| 1 |
*CMZ : 1.05/00 08/07/99 11.14.36 by Christian Zeitnitz |
| 2 |
*-- Author : Christian Zeitnitz |
| 3 |
SUBROUTINE GCALOR |
| 4 |
******************************************************************** |
| 5 |
* * |
| 6 |
* PURPOSE: GEANT interface to CALOR * |
| 7 |
* * |
| 8 |
* CALLED BY : GUHADR * |
| 9 |
* * |
| 10 |
* INPUT : particle, material, and probabilities via GEANT common * |
| 11 |
* * |
| 12 |
* OUTPUT : COMMON GCKING, DESTEP * |
| 13 |
* KCALL = -1 : Nothing done * |
| 14 |
* = 0 : NMTC has been called * |
| 15 |
* = 1 : MICAP has been called * |
| 16 |
* = 2 : HETC/SKALE has been called * |
| 17 |
* = 3 : FLUKA has been called * |
| 18 |
* * |
| 19 |
* AUTHOR : C.Zeitnitz (University of Arizona) * |
| 20 |
* * |
| 21 |
******************************************************************** |
| 22 |
C. |
| 23 |
C. --- GEANT Commons |
| 24 |
#include "gcbank.inc" |
| 25 |
#include "gcjloc.inc" |
| 26 |
#include "gckine.inc" |
| 27 |
#include "gcking.inc" |
| 28 |
#include "gcmate.inc" |
| 29 |
#include "gcphys.inc" |
| 30 |
#include "gctrak.inc" |
| 31 |
#include "gsecti.inc" |
| 32 |
#include "gconst.inc" |
| 33 |
#include "gccuts.inc" |
| 34 |
#include "gcflag.inc" |
| 35 |
#include "calgea.inc" |
| 36 |
#include "cerrcm.inc" |
| 37 |
#include "camass.inc" |
| 38 |
C |
| 39 |
C Avogadro number multiplied by 1.E-24 |
| 40 |
PARAMETER(XNAVO = 0.60221367) |
| 41 |
C |
| 42 |
DIMENSION NNPART(12) |
| 43 |
LOGICAL INIT,GOFLUK,DOSKAL,FMICAP,SKALEF,NABSOR,FSTOP |
| 44 |
DOUBLE PRECISION DECIN,DMASS |
| 45 |
C |
| 46 |
DATA INIT /.TRUE./ |
| 47 |
SAVE INIT |
| 48 |
C |
| 49 |
IF ( INIT ) THEN |
| 50 |
C |
| 51 |
C initialize CALOR |
| 52 |
CALL CALINI |
| 53 |
C |
| 54 |
INIT = .FALSE. |
| 55 |
C |
| 56 |
ENDIF |
| 57 |
KCALL = -1 |
| 58 |
C |
| 59 |
C get CALOR particle type |
| 60 |
IPINC = -1 |
| 61 |
IF(IPART .LE. 48 ) IPINC = IGECAL(IPART) |
| 62 |
C |
| 63 |
C energy in MeV |
| 64 |
|
| 65 |
EINC =GEKIN * 1000.0 |
| 66 |
UINC(1)=VECT(4) |
| 67 |
UINC(2)=VECT(5) |
| 68 |
UINC(3)=VECT(6) |
| 69 |
KCASE=NAMEC(12) |
| 70 |
NGKINE = 0 |
| 71 |
NABSOR = .FALSE. |
| 72 |
FSTOP = .FALSE. |
| 73 |
C ----- particle has to be stopped ? ------- |
| 74 |
IF(GEKIN.LT.CUTHAD.AND.ITRTYP.EQ.4) THEN |
| 75 |
FSTOP = .TRUE. |
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ISTOP = 2 |
| 77 |
IF(IPART .EQ. 9) THEN |
| 78 |
NABSOR = .TRUE. |
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ISTOP = 1 |
| 80 |
EINC = 1.0 |
| 81 |
IF(GEKIN.GT.EINC/1000.) DESTEP = DESTEP + GEKIN - EINC/ |
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+ 1000.0 |
| 83 |
GEKIN = 0.0 |
| 84 |
VECT(7) = 0.0 |
| 85 |
KCASE = NAMEC(18) |
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NMEC = NMEC + 1 |
| 87 |
LMEC(NMEC) = 18 |
| 88 |
ELSE |
| 89 |
DESTEP = DESTEP + GEKIN |
| 90 |
GEKIN = 0.0 |
| 91 |
VECT(7) = 0.0 |
| 92 |
IF(IPART.EQ.8.OR.IPART.EQ.11.OR.IPART.EQ.12) THEN |
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CALL GDECAY |
| 94 |
KCASE = NAMEC(5) |
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NMEC = NMEC + 1 |
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LMEC(NMEC) = 5 |
| 97 |
ENDIF |
| 98 |
RETURN |
| 99 |
ENDIF |
| 100 |
ELSE IF(GEKIN.LT.CUTNEU.AND.IPART.EQ.13) THEN |
| 101 |
IF(GEKIN.LT.1.E-14) EINC=1.E-11 |
| 102 |
ISTOP = 1 |
| 103 |
NABSOR = .TRUE. |
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ENDIF |
| 105 |
CZZZ IF(ISTOP.EQ.2.OR.GEKIN.EQ.0.0) RETURN |
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C |
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C ------------- check if FLUKA has to be called --------- |
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C ------------------------------------------------- Goto FLUKA ? |
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C |
| 110 |
DOSKAL = (IPINC.EQ.0 .OR. IPINC.EQ.1) .AND. GEKIN.GT.EMAXP |
| 111 |
DOSKAL = DOSKAL .OR. (GEKIN .GT. EMAXPI .AND. (IPINC .GT. 1)) |
| 112 |
IF(ICPROC.GE.0) THEN |
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GOFLUK = ICPROC.EQ.3 .OR. IPINC.EQ.-1 |
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DOSKAL = DOSKAL .AND. ICPROC.EQ.2 |
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ELSE |
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GOFLUK = IPINC .EQ. -1 .OR. GEKIN .GE. ESKALE |
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DOSKAL = DOSKAL .AND. .NOT.GOFLUK |
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GOFLUK = GOFLUK .OR. (DOSKAL.AND.SKALEF(IPINC,GEKIN,ESKALE)) |
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GOFLUK = GOFLUK .AND. .NOT.FSTOP .AND. .NOT.NABSOR |
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ENDIF |
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ICPROC = -1 |
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C ------------------------------------------- call FLUKA |
| 123 |
IF(GOFLUK) THEN |
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CALL FLUFIN |
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KCALL = 3 |
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RETURN |
| 127 |
ENDIF |
| 128 |
CERRF = .FALSE. |
| 129 |
IF(IPINC .EQ. 1 .AND. EINC .LE. 20.0) THEN |
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C MICAP needs only GEANT material number |
| 131 |
NCEL = NMAT |
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C --- low energetic neutron -> call micap |
| 133 |
CALL MICAP |
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KCALL = 1 |
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ELSE |
| 136 |
NCEL = 1 |
| 137 |
AMED(1) = A |
| 138 |
ZMED(1) = Z |
| 139 |
DMED(1) = DENS/A*XNAVO |
| 140 |
IF(INT(A) .EQ. 1) THEN |
| 141 |
HDEN = DMED(1) |
| 142 |
ELSE |
| 143 |
HDEN = 0.0 |
| 144 |
ENDIF |
| 145 |
C ------- get material parameter for a mixture--------------------- |
| 146 |
KK=MIN1(ABS(Q(JMA+11)),100.) |
| 147 |
NCEL = 1 |
| 148 |
IF(KK.GT.1) THEN |
| 149 |
HDEN = 0.0 |
| 150 |
NCEL = 0 |
| 151 |
AMOL = Q(LQ(JMIXT-1) + 2) |
| 152 |
DO 10 K=1,KK |
| 153 |
IF(NINT(Q(JMIXT+K)).EQ.1) THEN |
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C hydrogen density |
| 155 |
XMOLCM = DENS/AMOL*XNAVO |
| 156 |
WI = Q(JMIXT+K+2*KK)*AMOL/Q(JMIXT+K) |
| 157 |
HDEN = HDEN + XMOLCM * WI |
| 158 |
ELSE |
| 159 |
NCEL = NCEL + 1 |
| 160 |
AMED(NCEL) = Q(JMIXT+K) |
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ZMED(NCEL) = Q(JMIXT+K+KK) |
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C molekuls/cm^3 |
| 163 |
XMOLCM = DENS/AMOL*XNAVO |
| 164 |
C number of atoms per molecule |
| 165 |
WI = Q(JMIXT+K+2*KK)*AMOL/AMED(NCEL) |
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C atoms/cm^3 |
| 167 |
DMED(NCEL) = XMOLCM * WI |
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ENDIF |
| 169 |
10 CONTINUE |
| 170 |
ENDIF |
| 171 |
CALL CHETC(DOSKAL) |
| 172 |
KCALL = 0 |
| 173 |
IF(DOSKAL) KCALL = 2 |
| 174 |
ENDIF |
| 175 |
C error ocurred in CALOR ? |
| 176 |
IF(CERRF) THEN |
| 177 |
WRITE(IERRU,'('' NEVT,IPART,Ek,NMED,ISTOP,NABSOR,FSTOP :'', ' |
| 178 |
+ //' I10,I5,G15.6,2I6,2L6)') IEVENT,IPART,GEKIN,NMAT, |
| 179 |
+ ISTOP,NABSOR,FSTOP |
| 180 |
ENDIF |
| 181 |
ESUM =0. |
| 182 |
EKSUM = 0. |
| 183 |
PX = 0. |
| 184 |
PY = 0. |
| 185 |
PZ = 0. |
| 186 |
NGKINE = 0 |
| 187 |
PSUM = 0. |
| 188 |
C |
| 189 |
ZINTHA=GARNDM(6) |
| 190 |
SLHADR=SLENG |
| 191 |
STEPHA=BIG |
| 192 |
C |
| 193 |
IF(NPHETC.EQ.0.AND.NABSOR) ISTOP = 2 |
| 194 |
C neutron has been absorbed -> INTCAL=18 |
| 195 |
IF(INTCAL.EQ.18) ISTOP = 1 |
| 196 |
IF(NPHETC.LE.0) GOTO 160 |
| 197 |
C |
| 198 |
C too many particles in the CALOR array for GEANT |
| 199 |
C happens sometimes with deexcitation gammas and evaporation neutrons |
| 200 |
C simple approach to combine particles and sum up their energies, but |
| 201 |
C forget about momentum conservation |
| 202 |
C |
| 203 |
IF(NPHETC.GT.MXGKIN) THEN |
| 204 |
20 CONTINUE |
| 205 |
DO 30 I=1,12 |
| 206 |
NNPART(I)=0 |
| 207 |
30 CONTINUE |
| 208 |
NNTOT = 0 |
| 209 |
DO 40 I=1,NPHETC |
| 210 |
IF(IPCAL(I).NE.-1) THEN |
| 211 |
NNPART(IPCAL(I)+1)=NNPART(IPCAL(I)+1)+1 |
| 212 |
NNTOT = NNTOT + 1 |
| 213 |
ENDIF |
| 214 |
40 CONTINUE |
| 215 |
IF(NNTOT.LE.MXGKIN) GOTO 100 |
| 216 |
JMAX=0 |
| 217 |
IMAX=0 |
| 218 |
DO 50 I=1,12 |
| 219 |
IF(JMAX.LT.NNPART(I)) THEN |
| 220 |
JMAX=NNPART(I) |
| 221 |
IPI=I-1 |
| 222 |
ENDIF |
| 223 |
50 CONTINUE |
| 224 |
DO 60 I=1,NPHETC |
| 225 |
IF(IPCAL(I).EQ.IPI) GOTO 70 |
| 226 |
60 CONTINUE |
| 227 |
70 I1=I |
| 228 |
DO 80 I=I1+1,NPHETC |
| 229 |
IF(IPCAL(I).EQ.IPI) GOTO 90 |
| 230 |
80 CONTINUE |
| 231 |
90 I2=I |
| 232 |
ECINI = EKINET(I1) |
| 233 |
DMASS = DBLE(XMASS(IPI))*1.D3 |
| 234 |
DECIN = DBLE(ECINI) |
| 235 |
PPI = SNGL(DSQRT(DECIN*DECIN + 2.D0*DECIN*DMASS)) |
| 236 |
IPJ = IPCAL(I2) |
| 237 |
ECINJ = EKINET(I2) |
| 238 |
DECIN = DBLE(ECINJ) |
| 239 |
PPJ = SNGL(DSQRT(DECIN*DECIN + 2.D0*DECIN*DMASS)) |
| 240 |
ECIN = SNGL(DBLE(ECINI)+DBLE(ECINJ)+DMASS) |
| 241 |
EKINET(I1) = ECIN |
| 242 |
PP = SNGL(DSQRT(DBLE(ECIN*ECIN) + 2.D0*DBLE(ECIN)*DMASS)) |
| 243 |
C determine new direction cosines |
| 244 |
UCAL(I1,1) = (PPI*UCAL(I1,1)+PPJ*UCAL(I2,1))/PP |
| 245 |
UCAL(I1,2) = (PPI*UCAL(I1,2)+PPJ*UCAL(I2,2))/PP |
| 246 |
UCAL(I1,3) = (PPI*UCAL(I1,3)+PPJ*UCAL(I2,3))/PP |
| 247 |
USUM = SQRT(UCAL(I1,1)**2+UCAL(I1,2)**2+UCAL(I1,3)**2) |
| 248 |
C normalize direction cosines |
| 249 |
IF(USUM.LT.0.0001) THEN |
| 250 |
C direction is isotropic distributed |
| 251 |
CALL AZIRN(SINA,COSA) |
| 252 |
COSP = SFLRAF(DUM) |
| 253 |
SINP = SQRT(1.0-COSP*COSP) |
| 254 |
UCAL(I1,1) = SINP * COSA |
| 255 |
UCAL(I1,2) = SINP * SINA |
| 256 |
UCAL(I1,3) = COSP |
| 257 |
ELSE |
| 258 |
UCAL(I1,1) = UCAL(I1,1)/USUM |
| 259 |
UCAL(I1,2) = UCAL(I1,2)/USUM |
| 260 |
UCAL(I1,3) = UCAL(I1,3)/USUM |
| 261 |
ENDIF |
| 262 |
C particle I2 vanished |
| 263 |
IPCAL(I2)=-1 |
| 264 |
GOTO 20 |
| 265 |
C end of particle combination |
| 266 |
100 CONTINUE |
| 267 |
C sort particles |
| 268 |
I2=NPHETC |
| 269 |
DO 120 I = 1,NPHETC |
| 270 |
IF(I.GE.I2) GOTO 130 |
| 271 |
IF(IPCAL(I).EQ.-1) THEN |
| 272 |
DO 110 J = I2,I,-1 |
| 273 |
IF(IPCAL(J).NE.-1) THEN |
| 274 |
IPCAL(I) = IPCAL(J) |
| 275 |
EKINET(I) = EKINET(J) |
| 276 |
UCAL(I,1) = UCAL(J,1) |
| 277 |
UCAL(I,2) = UCAL(J,2) |
| 278 |
UCAL(I,3) = UCAL(J,3) |
| 279 |
I2 = J-1 |
| 280 |
GOTO 120 |
| 281 |
ENDIF |
| 282 |
110 CONTINUE |
| 283 |
ENDIF |
| 284 |
120 CONTINUE |
| 285 |
130 CONTINUE |
| 286 |
NPHETC=MXGKIN |
| 287 |
ENDIF |
| 288 |
C |
| 289 |
IF(INTCAL.LT.1.OR.INTCAL.GT.30) INTCAL=12 |
| 290 |
KCASE = NAMEC(INTCAL) |
| 291 |
IF(INTCAL.NE.12) THEN |
| 292 |
NMEC = NMEC + 1 |
| 293 |
LMEC(NMEC) = INTCAL |
| 294 |
ENDIF |
| 295 |
DO 140 I=1,NPHETC |
| 296 |
IP=IPCAL(I) |
| 297 |
IGPART=ICALGE(IP) |
| 298 |
IF ( IGPART.EQ.0 ) THEN |
| 299 |
PRINT*,'>>> ERROR GCALOR: Particle type ',IP, ' not ' |
| 300 |
+ //'implemented in GEANT' |
| 301 |
GOTO 140 |
| 302 |
ENDIF |
| 303 |
C |
| 304 |
C store particle |
| 305 |
ECIN = EKINET(I)/1000.0 |
| 306 |
IF(ECIN.LT.1.E-15) GOTO 140 |
| 307 |
DECIN = DBLE(ECIN) |
| 308 |
DMASS = DBLE(XMASS(IP)) |
| 309 |
PP = SNGL(DSQRT(DECIN*DECIN + 2.0D0*DECIN*DMASS)) |
| 310 |
PX = PX + PP*UCAL(I,1) |
| 311 |
PY = PY + PP*UCAL(I,2) |
| 312 |
PZ = PZ + PP*UCAL(I,3) |
| 313 |
C generated particle eq incoming |
| 314 |
IF(NPHETC.EQ.1 .AND. IGPART.EQ.IPART) THEN |
| 315 |
VECT(4) = UCAL(I,1) |
| 316 |
VECT(5) = UCAL(I,2) |
| 317 |
VECT(6) = UCAL(I,3) |
| 318 |
VECT(7) = PP |
| 319 |
GEKIN = ECIN |
| 320 |
GETOT = SNGL(DECIN + DMASS) |
| 321 |
TOFG = TOFG + CALTIM(I) |
| 322 |
ISTOP = 0 |
| 323 |
IF(NABSOR) ISTOP = 2 |
| 324 |
GOTO 160 |
| 325 |
ENDIF |
| 326 |
C |
| 327 |
NGKINE=NGKINE+1 |
| 328 |
GKIN(1,NGKINE) = PP*UCAL(I,1) |
| 329 |
GKIN(2,NGKINE) = PP*UCAL(I,2) |
| 330 |
GKIN(3,NGKINE) = PP*UCAL(I,3) |
| 331 |
C the total energy is critical for ECIN below 1.E-8 GeV because of |
| 332 |
C single precision of GKIN (normalization when mass is added)!! |
| 333 |
C luckely GEANT does use only the momentum components when storing the |
| 334 |
C particle on the stack. |
| 335 |
GKIN(4,NGKINE) = SNGL(DECIN+DMASS) |
| 336 |
GKIN(5,NGKINE) = FLOAT(IGPART) |
| 337 |
TOFD(NGKINE) = CALTIM(I) |
| 338 |
GPOS(1,NGKINE) = VECT(1) |
| 339 |
GPOS(2,NGKINE) = VECT(2) |
| 340 |
GPOS(3,NGKINE) = VECT(3) |
| 341 |
IF(NGKINE.GE.MXGKIN) GOTO 150 |
| 342 |
C |
| 343 |
140 CONTINUE |
| 344 |
150 CONTINUE |
| 345 |
C particle lost its identity |
| 346 |
ISTOP=1 |
| 347 |
160 CONTINUE |
| 348 |
C |
| 349 |
C |
| 350 |
NGKINE = MIN(NGKINE,MXGKIN) |
| 351 |
C |
| 352 |
C score kinetic energy of recoil nucleus (given in MeV) |
| 353 |
CZ DESTEP = DESTEP + ERMED * 1.E-3 |
| 354 |
170 RETURN |
| 355 |
END |
| 356 |
*CMZ : 1.05/02 16/05/2000 17.18.13 by Christian Zeitnitz |
| 357 |
*-- Author : Christian Zeitnitz 27/05/92 |
| 358 |
SUBROUTINE CALINI |
| 359 |
C************************************************************** |
| 360 |
C |
| 361 |
C INITIALIZATION of CALOR |
| 362 |
C ======================= |
| 363 |
C |
| 364 |
C Called by : CALSIG , GCALOR |
| 365 |
C |
| 366 |
C Author: Christian Zeitnitz 27.5.92 |
| 367 |
C |
| 368 |
C************************************************************** |
| 369 |
C |
| 370 |
C GEANT COMMON |
| 371 |
#include "gccuts.inc" |
| 372 |
#include "gctime.inc" |
| 373 |
#include "gcbank.inc" |
| 374 |
C CALOR COMMONS |
| 375 |
#include "calgea.inc" |
| 376 |
#include "ccomon.inc" |
| 377 |
#include "cjoint.inc" |
| 378 |
#include "cinout.inc" |
| 379 |
#include "cxpd.inc" |
| 380 |
#include "cmagnt.inc" |
| 381 |
#include "chie.inc" |
| 382 |
#include "cgeos.inc" |
| 383 |
#include "ctncol.inc" |
| 384 |
#include "minput.inc" |
| 385 |
#include "cerrcm.inc" |
| 386 |
#include "camass.inc" |
| 387 |
C |
| 388 |
DIMENSION IPID(0:11) |
| 389 |
LOGICAL INIT,OPENED,EXISTS |
| 390 |
CHARACTER*100 BERTF |
| 391 |
CHARACTER*8 VERSQQ |
| 392 |
CHARACTER*10 DATE |
| 393 |
CHARACTER*20 NAP |
| 394 |
CHARACTER*100 CHROOT |
| 395 |
DATA INIT/.TRUE./ |
| 396 |
C GEANT Particle IDs used to extract masses from GEANT |
| 397 |
DATA IPID /14 , 13 , 8 , 7 , 9 , 5 , 6 , 45 , 46 , 49 , 47 , 1/ |
| 398 |
C |
| 399 |
IF(.NOT.INIT) RETURN |
| 400 |
INIT = .FALSE. |
| 401 |
*KEEP,VERSQQ. |
| 402 |
VERSQQ = ' 1.05/04' |
| 403 |
IVERSQ = 10504 |
| 404 |
*KEND. |
| 405 |
CALL GCDATE(IDAT,ITIM) |
| 406 |
IYEAR = IDAT/10000 |
| 407 |
IMONTH= (IDAT-IYEAR*10000)/100 |
| 408 |
IDAY = IDAT-(IDAT/100)*100 |
| 409 |
WRITE(DATE,'(I2,''.'',I2,''.'',I4)') IDAY,IMONTH,IYEAR |
| 410 |
PRINT*,'******************************************************' |
| 411 |
PRINT*,'* *' |
| 412 |
PRINT*,'* GEANT - CALOR Interface Version ',VERSQQ,' *' |
| 413 |
PRINT*,'* ----------------------------------------- *' |
| 414 |
PRINT*,'* ',DATE,' C.Zeitnitz, T.A.Gabriel *' |
| 415 |
PRINT*,'* *' |
| 416 |
PRINT*,'* NMTC is used for hadronic interactions of *' |
| 417 |
PRINT*,'* protons,neutrons and charged pions *' |
| 418 |
PRINT*,'* up to 3.5 GeV (proton,neutron), 2.5 GeV(pion) *' |
| 419 |
PRINT*,'* *' |
| 420 |
PRINT*,'* A Scaling Model is used for the energy range *' |
| 421 |
PRINT*,'* up to 10 GeV. *' |
| 422 |
PRINT*,'* *' |
| 423 |
PRINT*,'* MICAP is calculating the interaction of *' |
| 424 |
PRINT*,'* Neutrons with an energy below 20 MeV *' |
| 425 |
PRINT*,'* *' |
| 426 |
PRINT*,'* For interactions of hadrons not implemented in *' |
| 427 |
PRINT*,'* CALOR or with an energy above 10 GeV *' |
| 428 |
PRINT*,'* GEANT-FLUKA is called *' |
| 429 |
PRINT*,'* *' |
| 430 |
PRINT*,'* The transport of electrons, positrons and gammas *' |
| 431 |
PRINT*,'* is done by GEANT *' |
| 432 |
PRINT*,'* *' |
| 433 |
PRINT*,'* All output is written to file calor.out *' |
| 434 |
PRINT*,'* *' |
| 435 |
PRINT*,'******************************************************' |
| 436 |
PRINT '('' * Neutron cutoff energy='',G10.2, ' |
| 437 |
+ //' '' eV *'')',CUTNEU*1.E9 |
| 438 |
PRINT*,'******************************************************' |
| 439 |
C |
| 440 |
C fill particle mass array |
| 441 |
DO 10 I=0,11 |
| 442 |
CALL GFPART(IPID(I),NAP,ITR,AM,CH,TL,UB,NW) |
| 443 |
XMASS(I)=AM |
| 444 |
10 CONTINUE |
| 445 |
INIT = .FALSE. |
| 446 |
ICPROC = -1 |
| 447 |
IN = 5 |
| 448 |
EHIN = 3495.0 |
| 449 |
EHIPI = 2495.0 |
| 450 |
EMAX = 3500.0 |
| 451 |
NBERTP = 30 |
| 452 |
INQUIRE(UNIT=NBERTP,OPENED=OPENED) |
| 453 |
IF(OPENED) THEN |
| 454 |
REWIND NBERTP |
| 455 |
ELSE |
| 456 |
BERTF = 'chetc.dat' |
| 457 |
INQUIRE(FILE=BERTF,EXIST=EXISTS) |
| 458 |
IF(.NOT.EXISTS) THEN |
| 459 |
CHROOT = ' ' |
| 460 |
CALL GETENV('CERN_ROOT',CHROOT) |
| 461 |
LNROOT = LNBLNK(CHROOT) |
| 462 |
IF(LNROOT.GT.0)BERTF = CHROOT(1:LNROOT)//'/lib/chetc.dat' |
| 463 |
ENDIF |
| 464 |
INQUIRE(FILE=BERTF,EXIST=EXISTS) |
| 465 |
IF(.NOT.EXISTS) THEN |
| 466 |
PRINT*,'**********************************' |
| 467 |
PRINT*,'* G C A L O R *' |
| 468 |
PRINT*,'* ----------- *' |
| 469 |
PRINT*,'* File CHETC.DAT not found *' |
| 470 |
PRINT*,'* Program STOP *' |
| 471 |
PRINT*,'**********************************' |
| 472 |
STOP |
| 473 |
ENDIF |
| 474 |
OPEN(UNIT = NBERTP,FILE=BERTF, FORM = 'FORMATTED',STATUS= |
| 475 |
+ 'OLD') |
| 476 |
ENDIF |
| 477 |
C Output unit for Neutron information and error messages |
| 478 |
IOUT = 32 |
| 479 |
IERRU = IOUT |
| 480 |
OPEN(UNIT=IOUT,FILE='calor.out',FORM='FORMATTED', |
| 481 |
+ STATUS='UNKNOWN') |
| 482 |
IO = IOUT |
| 483 |
WRITE(IOUT,'(/, ' |
| 484 |
+ //' 18X,''GEANT-CALOR INTERFACE V'',A8,'' Output File'', ' |
| 485 |
+ //'/,18X,''==========================================='',/)') |
| 486 |
+ VERSQQ |
| 487 |
C read bert cascade and evaporation dataset |
| 488 |
CALL CRBERT |
| 489 |
CLOSE(UNIT=NBERTP) |
| 490 |
ELOP = AMAX1(1.0,CUTHAD * 1000.0) |
| 491 |
ELON = AMAX1(20.0,CUTNEU * 1000.0) |
| 492 |
NPOWR2 = 11 |
| 493 |
NGROUP = 2**NPOWR2 |
| 494 |
EMUCUT = AMAX1(1.0,CUTMUO * 1000.0) |
| 495 |
EPICUT = ELOP |
| 496 |
NPIDK = -1 |
| 497 |
CTOFE = 0.0 |
| 498 |
CTOFEN = 0.0 |
| 499 |
ANDIT = 0.0 |
| 500 |
NEXITE = 1 |
| 501 |
NBOGUS = NEXITE |
| 502 |
ELAS = 0.0 |
| 503 |
BODGE = 0.0 |
| 504 |
EMIN(1) = ELOP |
| 505 |
EMIN(2) = ELON |
| 506 |
EMIN(3) = EPICUT |
| 507 |
EMIN(4) = EPICUT |
| 508 |
EMIN(5) = EPICUT |
| 509 |
EMIN(6) = EMUCUT |
| 510 |
EMIN(7) = EMUCUT |
| 511 |
C now get some cross sections |
| 512 |
CALL CREADG(GEOSIG) |
| 513 |
CALL GTHSIG(1) |
| 514 |
C No decay cross-section needed in GEANT |
| 515 |
C SGPIMX = 0.001259/SQRT ((EMIN(3)/139.9+1.)**2 -1.) |
| 516 |
C SGMUMX = 1.587E-5/SQRT ((EMIN(6)/107.+1.)**2 -1.) |
| 517 |
SGPIMX = 0.0 |
| 518 |
SGMUMX = 0.0 |
| 519 |
NCOL = 1 |
| 520 |
C ------------ initialize MICAP ------------------------ |
| 521 |
CALL MORINI |
| 522 |
C perform garbage collection in constant division |
| 523 |
CALL MZGARB(IXCONS,0) |
| 524 |
RETURN |
| 525 |
END |
| 526 |
*CMZ : 1.01/04 10/06/93 14.43.36 by Christian Zeitnitz |
| 527 |
*-- Author : |
| 528 |
SUBROUTINE CREADG(GEOSIG) |
| 529 |
C |
| 530 |
#include "cjoint.inc" |
| 531 |
#include "cbert.inc" |
| 532 |
C |
| 533 |
DIMENSION GEOSIG(240) |
| 534 |
C |
| 535 |
K=1 |
| 536 |
DO 20 J = 1,4 |
| 537 |
CZ data already read by CRBERT called by CALINI 19.june 92 CZ |
| 538 |
CZ changed 5-28-92 crazy number for A=240 set to GEOSIG(239) |
| 539 |
DO 10 I = 4,594,10 |
| 540 |
IF(K.LT.240) THEN |
| 541 |
GEOSIG(K) = SNGL(CRSC(I + (J-1)*600)) |
| 542 |
GEOSIG(K) = 3.1416 * GEOSIG(K)**2 * 1.E+24 |
| 543 |
ELSE |
| 544 |
GEOSIG(K) = GEOSIG(K-1) |
| 545 |
ENDIF |
| 546 |
10 K = K + 1 |
| 547 |
20 CONTINUE |
| 548 |
RETURN |
| 549 |
END |
| 550 |
*CMZ : 1.01/04 10/06/93 14.43.36 by Christian Zeitnitz |
| 551 |
*-- Author : Christian Zeitnitz 06/06/92 |
| 552 |
FUNCTION ICALGE(IP) |
| 553 |
C******************************************* |
| 554 |
C |
| 555 |
C INPUT : CALOR particle type |
| 556 |
C OUTPUT: GEANT particle type |
| 557 |
C |
| 558 |
C****************************************** |
| 559 |
C |
| 560 |
C |
| 561 |
DIMENSION NCALGE(0:11) |
| 562 |
C convert CALOR particle code to GEANT |
| 563 |
C p n pi+ pi0 pi- mu+ mu- D T He3 Alpha Gamma |
| 564 |
DATA NCALGE/ 14, 13, 8, 7, 9, 5, 6, 45, 46, 49, 47, 1/ |
| 565 |
C |
| 566 |
IF(IP .LE. 11 .AND. IP.GE.0) THEN |
| 567 |
ICALGE = NCALGE(IP) |
| 568 |
ELSE |
| 569 |
ICALGE = 0 |
| 570 |
ENDIF |
| 571 |
RETURN |
| 572 |
END |
| 573 |
*CMZ : 1.01/04 10/06/93 14.43.36 by Christian Zeitnitz |
| 574 |
*-- Author : Christian Zeitnitz 06/06/92 |
| 575 |
FUNCTION IGECAL(IP) |
| 576 |
C******************************************* |
| 577 |
C |
| 578 |
C INPUT : GEANT particle type |
| 579 |
C OUTPUT: CALOR particle type or -1 |
| 580 |
C |
| 581 |
C****************************************** |
| 582 |
C |
| 583 |
C |
| 584 |
DIMENSION NGECAL(48) |
| 585 |
C |
| 586 |
C convert GEANT particle code to CALOR |
| 587 |
C -1 indicates a particle not implemented in CALOR |
| 588 |
DATA NGECAL/ -1, -1, -1, -1, -1, -1, -1, 2, 4, -1, |
| 589 |
+ -1, -1, 1, 0, -1, -1, -1, -1, -1, -1, |
| 590 |
+ 28*-1/ |
| 591 |
C |
| 592 |
C |
| 593 |
IF(IP .LE. 48 .AND. IP.GT.0) THEN |
| 594 |
IGECAL = NGECAL(IP) |
| 595 |
ELSE |
| 596 |
IGECAL = -1 |
| 597 |
ENDIF |
| 598 |
RETURN |
| 599 |
END |
| 600 |
*CMZ : 1.01/04 10/06/93 14.43.36 by Christian Zeitnitz |
| 601 |
*-- Author : Christian Zeitnitz 19/06/92 |
| 602 |
SUBROUTINE CRBERT |
| 603 |
C********************************************************* |
| 604 |
C |
| 605 |
C Read BERT Data into commons used by BERT,PCOL,GTHSIG |
| 606 |
C DRES |
| 607 |
C |
| 608 |
C********************************************************* |
| 609 |
C |
| 610 |
#include "cjoint.inc" |
| 611 |
#include "cbert.inc" |
| 612 |
#include "cdresc.inc" |
| 613 |
#include "cevcm.inc" |
| 614 |
*KEND. |
| 615 |
C |
| 616 |
REWIND NBERTP |
| 617 |
C ---- read cascade data -------------- |
| 618 |
I1 = 1 |
| 619 |
I2 = 600 |
| 620 |
DO 10 J=1,4 |
| 621 |
READ(NBERTP,10000) (CRSC(I),I=I1,I2) |
| 622 |
I1 = I1 + 600 |
| 623 |
I2 = I2 + 600 |
| 624 |
10 CONTINUE |
| 625 |
READ(NBERTP,10000) (TAPCRS(I),I=1,29849) |
| 626 |
C ----- read evaporation data ----------- |
| 627 |
DO 30 K=1,250 |
| 628 |
DO 20 J=1,20 |
| 629 |
WAPS(K,J) = 0.0 |
| 630 |
20 CONTINUE |
| 631 |
30 CONTINUE |
| 632 |
READ(NBERTP,10000) (P0(J),P1(J),P22(J),J=1,1001) |
| 633 |
READ(NBERTP,10100) (IA(J),J=1,6),(IZ(J),J=1,6) |
| 634 |
READ(NBERTP,10000) (RHO(J),J=1,6),(OMEGA(J),J=1,6) |
| 635 |
READ(NBERTP,10000) (EXMASS(J),J=1,6) |
| 636 |
READ(NBERTP,10000) (CAM2(J),J=1,130) |
| 637 |
READ(NBERTP,10000) (CAM3(J),J=1,200) |
| 638 |
READ(NBERTP,10000) (CAM4(J),J=1,130) |
| 639 |
READ(NBERTP,10000) (CAM5(J),J=1,200) |
| 640 |
READ(NBERTP,10000) ((T(I,J),J=1,7),I=1,3) |
| 641 |
READ(NBERTP,10000) (RMASS(J),J=1,297) |
| 642 |
READ(NBERTP,10000) (ALPH(J),J=1,297) |
| 643 |
READ(NBERTP,10000) (BET(J),J=1,297) |
| 644 |
READ(NBERTP,10000) ((WAPS(I,J),I=1,250),J=1,20) |
| 645 |
10000 FORMAT(5E16.8) |
| 646 |
10100 FORMAT(6I10) |
| 647 |
RETURN |
| 648 |
END |
| 649 |
*CMZ : 1.01/04 10/06/93 14.43.36 by Christian Zeitnitz |
| 650 |
*-- Author : Christian Zeitnitz 30/10/92 |
| 651 |
LOGICAL FUNCTION SKALEF(IP,EIP,ESKALE) |
| 652 |
C************************************************************* |
| 653 |
C |
| 654 |
C Called by: GCALOR |
| 655 |
C Purpose : function is true, when scaling applies to FLUKA |
| 656 |
C linear transition from NMTC to FLUKA |
| 657 |
C Author : C.Zeitnitz |
| 658 |
C |
| 659 |
C************************************************************* |
| 660 |
#include "crandm.inc" |
| 661 |
*KEND. |
| 662 |
C |
| 663 |
SKALEF = .TRUE. |
| 664 |
ENMTC = 3.495 |
| 665 |
IF(IP.GT.1) ENMTC = 2.495 |
| 666 |
IF(EIP.LE.ENMTC) SKALEF = .FALSE. |
| 667 |
IF(EIP.LT.ESKALE.AND.EIP.GT.ENMTC) THEN |
| 668 |
X1 = (EIP - ENMTC) / (ESKALE - ENMTC) |
| 669 |
X2 = SNGL(RANDC(ISEED)) |
| 670 |
IF(X2.GT.X1) SKALEF = .FALSE. |
| 671 |
ENDIF |
| 672 |
RETURN |
| 673 |
END |
| 674 |
*CMZ : 1.02/02 28/01/94 09.09.15 by Christian Zeitnitz |
| 675 |
*-- Author : Christian Zeitnitz 30/07/93 |
| 676 |
* |
| 677 |
* simple utility to generate date and time of GCALOR version |
| 678 |
* When running kumac file vers.kumac this file is written as fortran |
| 679 |
* and then read again, in order to fix date and time |
| 680 |
* |
| 681 |
SUBROUTINE GCDATE(IDATQQ,ITIMQQ) |
| 682 |
*KEEP,DATEQQ. |
| 683 |
IDATQQ = 20051130 |
| 684 |
*KEEP,TIMEQQ. |
| 685 |
ITIMQQ = 1129 |
| 686 |
*KEND. |
| 687 |
RETURN |
| 688 |
END |
| 689 |
*CMZ : 0.92/00 02/12/92 16.02.28 by Christian Zeitnitz |
| 690 |
*-- Author : |
| 691 |
SUBROUTINE AZIRN(SIN,COS) |
| 692 |
#include "crandm.inc" |
| 693 |
*KEND. |
| 694 |
C THIS ROUTINE SELECTS THE AZIMUTHAL ANGLE UNIFORMLY IN THETA |
| 695 |
10 R1 = SFLRAF(DUM) |
| 696 |
R1SQ = R1 * R1 |
| 697 |
R2 = RANDC(ISEED) |
| 698 |
R2SQ = R2 * R2 |
| 699 |
RSQ = R1SQ + R2SQ |
| 700 |
IF(1.0-RSQ) 10 ,20 ,20 |
| 701 |
20 SIN = 2.0 * R1 * R2 / RSQ |
| 702 |
COS = (R2SQ-R1SQ) / RSQ |
| 703 |
RETURN |
| 704 |
END |
| 705 |
*CMZ : 0.94/00 08/03/93 12.50.48 by Christian Zeitnitz |
| 706 |
*-- Author : |
| 707 |
SUBROUTINE DKLOS |
| 708 |
C |
| 709 |
#include "ccomon.inc" |
| 710 |
#include "cmagnt.inc" |
| 711 |
#include "ctuctw.inc" |
| 712 |
#include "celstc.inc" |
| 713 |
*KEND. |
| 714 |
C |
| 715 |
MT = MAT |
| 716 |
GOTO(10,10,20,30,20,40,40),ITYP |
| 717 |
10 DKWT =1. |
| 718 |
C*************ADD MAGNET BODGE TO DELSIG******************** |
| 719 |
DELSIG=SIGMX(ITYP,MT)+TOTELS+BODGE |
| 720 |
C DELSIG = SIGMX(ITYP,MT ) + TOTELS |
| 721 |
RETURN |
| 722 |
20 SIGDK= 0.001259/SQRT ((EC(NO)/139.9+1.)**2. -1.) |
| 723 |
GO TO 50 |
| 724 |
30 CALL CERROR('DKLOS$') |
| 725 |
40 SIGDK= 1.587E-5/SQRT ((EC(NO)/107.+1.)**2. -1.) |
| 726 |
C 50 DELSIG = SIGMX(ITYP,MT ) - SIGDK |
| 727 |
C********ADD MAGNET BODGE TO DELSIG AND ALLOW FOR IT IN DKWT******* |
| 728 |
50 DELSIG = SIGMX(ITYP,MT ) - SIGDK+BODGE |
| 729 |
C DKWT = DELSIG/SIGMX(ITYP,MT ) |
| 730 |
DKWT = DELSIG/(SIGMX(ITYP,MT )+BODGE) |
| 731 |
RETURN |
| 732 |
END |
| 733 |
*CMZ : 0.92/00 02/12/92 16.02.28 by Christian Zeitnitz |
| 734 |
*-- Author : |
| 735 |
SUBROUTINE CESWH |
| 736 |
C** ELASTIC SCATTERING WITH HYDROGEN, |
| 737 |
C* STRUCK PARTICLE AT REST. |
| 738 |
#include "cbert.inc" |
| 739 |
*KEND. |
| 740 |
SAVE |
| 741 |
C |
| 742 |
CALL CAAZIO(SOPC,SOPS) |
| 743 |
PM(4) = DNCMS |
| 744 |
PT(1) = 0. |
| 745 |
DO 10 I=3,13 |
| 746 |
10 PT(I) = 0. |
| 747 |
DO 20 I=15,48 |
| 748 |
20 PT(I) = 0. |
| 749 |
DO 30 I=1,24 |
| 750 |
30 COL(I) = 0. |
| 751 |
A=PM(4)*PM(4) |
| 752 |
COL(1)=E(1)+E(2) |
| 753 |
C TOTAL ENERGY PARTICLES 1 AND 2 |
| 754 |
DO40 I=1,3 |
| 755 |
40 COL(I+1)=PM(I)*PM(I) |
| 756 |
C MASS PARTICLE I SQD. |
| 757 |
COL(5)=COL(3)+COL(2)+2.0*(E(1)*E(2)-(PXYZ(1)*PXYZ(2)+PXYZ(5)* |
| 758 |
1PXYZ(6)+PXYZ(9)*PXYZ(10))) |
| 759 |
COL(6)=DSQRT(COL(5)) |
| 760 |
COL(7)=COL(6)/COL(1) |
| 761 |
C GAM |
| 762 |
COL(8)=2.0*COL(6) |
| 763 |
COL(9)=(COL(4)+COL(5)-A)/COL(8) |
| 764 |
COM2 = COL(9)*COL(9) |
| 765 |
50 COL(10)=DSQRT(COM2-COL(4)) |
| 766 |
C P3 PRIME |
| 767 |
COL(18)=PXYZ(9)*PM(2)/COL(6) |
| 768 |
C P(1),Z *M2/M=P(BAR PRIME)1,Z |
| 769 |
COL(21)=PXYZ(9)/COL(1) |
| 770 |
C VZ VELOCITY |
| 771 |
PXYZ(3)=COL(10)*SNT*SOPC |
| 772 |
C X COMPONENT P3 BAR =P3 PRIME X SIN THETA X COS PHI |
| 773 |
PXYZ(7)=COL(10)*SNT*SOPS |
| 774 |
C Y COMP. P3 BAR =P3 PRIME X SIN THETA X SIN PHI |
| 775 |
PXYZ(11)=COL(10)*CST |
| 776 |
Z=PXYZ(9)/COL(6) |
| 777 |
PXYZ(11)=PXYZ(11)+(Z*PXYZ(9)*PXYZ(11))/(COL(1)+COL(6))+Z*COL(9) |
| 778 |
C Z COMP. P3 BAR=P3 PRIME COS THETA+(P1Z SQ*P3Z (PRIME)COS |
| 779 |
C THETA/(E PRIME*(E+E PRIME))+P1Z*E3 PRIME/E PRIME |
| 780 |
E(3)=DSQRT(PXYZ(3)*PXYZ(3)+PXYZ(7)*PXYZ(7)+PXYZ(11)*PXYZ(11)+ |
| 781 |
1PM(3)*PM(3)) |
| 782 |
DO60 I=1,9,4 |
| 783 |
60 PXYZ(I+3)=PXYZ(I)-PXYZ(I+2) |
| 784 |
E(4)=DSQRT(PXYZ(4)*PXYZ(4)+PXYZ(8)*PXYZ(8)+PXYZ(12)*PXYZ(12) |
| 785 |
1+PM(4)*PM(4)) |
| 786 |
C** KINETIC ENERGY OF 3 AND 4 |
| 787 |
PT(3) = (E(3) - PM(3))/RCPMV |
| 788 |
PT(15) = (E(4) - PM(4))/RCPMV |
| 789 |
C** MOMENTUM OF 3 AND 4, IN LAB. |
| 790 |
P3 = DSQRT(PXYZ(3)*PXYZ(3) + PXYZ(7)*PXYZ(7) + PXYZ(11)*PXYZ(11)) |
| 791 |
P4 = DSQRT(PXYZ(4)*PXYZ(4) + PXYZ(8)*PXYZ(8) + PXYZ(12) *PXYZ(12)) |
| 792 |
C** DIRECT COSINES OF 3 AND 4 |
| 793 |
PT(8) = PXYZ(3)/P3 |
| 794 |
PT(9) = PXYZ(7)/P3 |
| 795 |
PT(10) = PXYZ(11)/P3 |
| 796 |
PT(20) = PXYZ(4)/P4 |
| 797 |
PT(21) = PXYZ(8)/P4 |
| 798 |
PT(22) = PXYZ(12) /P4 |
| 799 |
RETURN |
| 800 |
END |
| 801 |
*CMZ : 1.01/17 22/11/93 12.22.58 by Christian Zeitnitz |
| 802 |
*-- Author : |
| 803 |
FUNCTION EXPRNF(A) |
| 804 |
C |
| 805 |
#include "crandm.inc" |
| 806 |
*KEND. |
| 807 |
C |
| 808 |
REAL I |
| 809 |
C |
| 810 |
I = 0.0 |
| 811 |
10 X = RANDC(ISEED) |
| 812 |
Z = X |
| 813 |
20 Y = RANDC(ISEED) |
| 814 |
IF(Z-Y) 50 ,50 ,30 |
| 815 |
30 Z = RANDC(ISEED) |
| 816 |
IF(Z-Y) 20 ,40 ,40 |
| 817 |
40 I = I + 1.0 |
| 818 |
GO TO 10 |
| 819 |
50 EXPRNF = X + I |
| 820 |
RETURN |
| 821 |
END |
| 822 |
*CMZ : 0.92/00 02/12/92 16.02.28 by Christian Zeitnitz |
| 823 |
*-- Author : |
| 824 |
FUNCTION GAURN(X) |
| 825 |
C |
| 826 |
#include "crandm.inc" |
| 827 |
*KEND. |
| 828 |
C |
| 829 |
10 Y = EXPRNF(X1) |
| 830 |
Z = EXPRNF(X2) |
| 831 |
TEST = (Y-1.0)**2/2. |
| 832 |
IF(TEST-Z) 20,20,10 |
| 833 |
20 R1 = 2.0 * RANDC(ISEED) - 1.0 |
| 834 |
IF(R1) 30,40,40 |
| 835 |
30 Y = -Y |
| 836 |
40 GAURN = Y |
| 837 |
RETURN |
| 838 |
END |
| 839 |
*CMZ : 1.01/04 10/06/93 14.43.41 by Christian Zeitnitz |
| 840 |
*-- Author : |
| 841 |
SUBROUTINE GTHSIG(ISGNL) |
| 842 |
C |
| 843 |
#include "cjoint.inc" |
| 844 |
#include "ccomon.inc" |
| 845 |
#include "cxpd.inc" |
| 846 |
#include "chie.inc" |
| 847 |
#include "cbert2.inc" |
| 848 |
*KEND. |
| 849 |
C |
| 850 |
C |
| 851 |
C ** DE IS THE CONST. ENERGY SPACING COMMON T0 P-P,N-P,PI+P,PI-P XSECTS |
| 852 |
DIMENSION ISA(4),EMX(4) |
| 853 |
SAVE ISA,EMX |
| 854 |
C |
| 855 |
GO TO (10,180),ISGNL |
| 856 |
10 CONTINUE |
| 857 |
CZ BERT dataset already read by CRBERT called by CALINI 19.june 92 |
| 858 |
CALL CSHXD |
| 859 |
DO 20 I=1,4 |
| 860 |
20 ISA(I) = LOCX(3,I) |
| 861 |
C**** COMPUTE TOTAL P-P AND N-P XSECTS (SINGLE PRODUCTION + DOUBLE PRODU |
| 862 |
C**** + ELASTIC) AND STORE P-P BEGINNING AT CS(3794) ANP N-P BEGINNING |
| 863 |
C**** CS(3970). |
| 864 |
ISP=995 |
| 865 |
IDP=1153 |
| 866 |
DO 50 IT=1,2 |
| 867 |
IS= ISA(IT) |
| 868 |
DO 30 I=1,158 |
| 869 |
TEMP= CS(IS+18+I) |
| 870 |
30 CS(IS+18+I) = TEMP + CS(ISP+I) |
| 871 |
ISP = ISP + 288 |
| 872 |
DO 40 I=1,130 |
| 873 |
TEMP = CS(IS+46+I) |
| 874 |
40 CS(IS+46+I) = TEMP + CS(IDP+I) |
| 875 |
50 IDP = IDP + 288 |
| 876 |
C**** COMPUTE TOTAL PI+(SNGL PROD.+ELAS) AND PI-(SNGL PROD.+EXCHNG +ELAS |
| 877 |
C**** AND STORE PI+-P BEGINNING AT CS(3668) AND PI--P BEGINNING AT CS(35 |
| 878 |
ISP =2009 |
| 879 |
DO 70 IT =3,4 |
| 880 |
IS= ISA(IT) |
| 881 |
DO 60 I=1,117 |
| 882 |
TEMP = CS(IS +9+I) |
| 883 |
60 CS(IS+9+I) = TEMP + CS(ISP+I) |
| 884 |
70 ISP = ISP +234 |
| 885 |
IEX =3415 |
| 886 |
IS = ISA(4) |
| 887 |
DO 80 I=1,126 |
| 888 |
TEMP = CS(IS+I) |
| 889 |
80 CS(IS+I) = TEMP + CS(IEX+I) |
| 890 |
DO 100 IT = 1,2 |
| 891 |
IS = ISA(IT) |
| 892 |
DO 90 I=1,176 |
| 893 |
90 NPSG(IT,I) = SNGL( CS(IS+I) ) |
| 894 |
100 CONTINUE |
| 895 |
DO 120 IT = 1,2 |
| 896 |
IS = ISA(IT+2) |
| 897 |
DO 110 I=1,126 |
| 898 |
110 PIPSG(IT,I) = SNGL( CS(IS+I) ) |
| 899 |
120 CONTINUE |
| 900 |
C ***** |
| 901 |
C **** SELECT MAX. TOT.XSECTS FOR X ON PROT. IN ENERGY RANGE EMIN(X) TO |
| 902 |
C **** WHERE X = PROT.,NEUT.,PI+,PI-. |
| 903 |
IF(EMAX.LT.EHIN)GO TO 130 |
| 904 |
EMX(1)=EHIN |
| 905 |
EMX(2)=EHIN |
| 906 |
EMX(3)=EHIPI |
| 907 |
EMX(4)=EHIPI |
| 908 |
GO TO 140 |
| 909 |
130 CONTINUE |
| 910 |
EMX(1)= EMAX |
| 911 |
EMX(2)= EMAX |
| 912 |
EMX(3)= 2500. |
| 913 |
EMX(4)= 2500. |
| 914 |
140 CONTINUE |
| 915 |
DO 160 ITP =1,4 |
| 916 |
IS= ISA(ITP) |
| 917 |
IT = ITP + ITP/4 |
| 918 |
CALL CALSGM(1,ITP,IS,DE,EMIN(IT),IL,EL,SL) |
| 919 |
CALL CALSGM(1,ITP,IS,DE,EMX(ITP),IH,EH,SH) |
| 920 |
HSIGMX(IT) = AMAX1(SL,SH) |
| 921 |
IF(IL.GE.IH) GO TO 160 |
| 922 |
IL = IL +1 |
| 923 |
DO 150 I= IL,IH |
| 924 |
SIG = SNGL(CS(I+IS)) |
| 925 |
IF(SIG. LE. HSIGMX(IT)) GO TO 150 |
| 926 |
HSIGMX(IT) = SIG |
| 927 |
150 CONTINUE |
| 928 |
160 CONTINUE |
| 929 |
HSIGMX(4)=0.0 |
| 930 |
10000 FORMAT(1H0,7HHSIGMX ,5E15.5) |
| 931 |
170 RETURN |
| 932 |
180 IT = ITYP - ITYP/5 |
| 933 |
IS = ISA(IT) |
| 934 |
CALL CALSGM(2,IT,IS,DE,EC(NO),I,EI,HSIG) |
| 935 |
GO TO 170 |
| 936 |
END |
| 937 |
*CMZ : 1.01/04 10/06/93 14.43.41 by Christian Zeitnitz |
| 938 |
*-- Author : |
| 939 |
SUBROUTINE CISOB |
| 940 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 941 |
C |
| 942 |
#include "crandm.inc" |
| 943 |
#include "cbert3.inc" |
| 944 |
#include "cisob2.inc" |
| 945 |
*KEND. |
| 946 |
C |
| 947 |
INTEGER*2 RANDI |
| 948 |
REAL*8 DCLN(80),DCIN(115),PPAC(19),POAC(19), |
| 949 |
+ FMXSN(161),FMXDN(130),FMXSP(117),PDCI(60),PDCH(55),DCHN(143), |
| 950 |
+ DCHNA(36),DCHNB(60),PSPCL(158),PDPCL(130),SPCLN(158),DPCLN(130), |
| 951 |
+ FSLN(176),FRINN(161),DMIN(101),PPSCL(117),PNSCL(117),PMSCL(117), |
| 952 |
+ PNNSL(117),PCFSL(234),FRIPN(117),PNMI(101),PNFSL(234),PNEC(126), |
| 953 |
+ PNNEC(126),PMXC(126),PMEC(126),PPEC(126),PEC(176),ECN(176), |
| 954 |
+ PPDC(6426),PMDD(6426),PMDX(6426),PNDD(6426) |
| 955 |
REAL*8 CALCIN(3) |
| 956 |
EQUIVALENCE (TAPCRS(1),DCLN(1)) ,(TAPCRS(81),DCIN(1)) , |
| 957 |
+ (TAPCRS(196),PPAC(1)) ,(TAPCRS(215),POAC(1)) , |
| 958 |
+ (TAPCRS(234),FMXSN(1)) ,(TAPCRS(395),FMXDN(1)) , |
| 959 |
+ (TAPCRS(525),FMXSP(1)) ,(TAPCRS(642),PDCI(1)) , |
| 960 |
+ (TAPCRS(702),PDCH(1)) ,(TAPCRS(757),DCHN(1)) , |
| 961 |
+ (TAPCRS(900),DCHNA(1)) ,(TAPCRS(936),DCHNB(1)) , |
| 962 |
+ (TAPCRS(996),PSPCL(1)) ,(TAPCRS(1154),PDPCL(1)), |
| 963 |
+ (TAPCRS(1284),SPCLN(1)),(TAPCRS(1442),DPCLN(1)), |
| 964 |
+ (TAPCRS(1572),FSLN(1)) ,(TAPCRS(1748),FRINN(1)) |
| 965 |
C |
| 966 |
EQUIVALENCE (TAPCRS(1909),DMIN(1)) ,(TAPCRS(2010),PPSCL(1)), |
| 967 |
+ (TAPCRS(2127),PNSCL(1)),(TAPCRS(2244),PMSCL(1)), |
| 968 |
+ (TAPCRS(2361),PNNSL(1)),(TAPCRS(2478),PCFSL(1)), |
| 969 |
+ (TAPCRS(2712),FRIPN(1)),(TAPCRS(2829),PNMI(1)) , |
| 970 |
+ (TAPCRS(2930),PNFSL(1)),(TAPCRS(3164),PNEC(1)) , |
| 971 |
+ (TAPCRS(3290),PNNEC(1)),(TAPCRS(3416),PMXC(1)) , |
| 972 |
+ (TAPCRS(3542),PMEC(1)) ,(TAPCRS(3668),PPEC(1)) , |
| 973 |
+ (TAPCRS(3794),PEC(1)) ,(TAPCRS(3970),ECN(1)) , |
| 974 |
+ (TAPCRS(4146),PPDC(1)) ,(TAPCRS(10572),PMDD(1)), |
| 975 |
+ (TAPCRS(16998),PMDX(1)),(TAPCRS(23424),PNDD(1)) |
| 976 |
C |
| 977 |
SAVE |
| 978 |
DATA NTER/0/ |
| 979 |
IF(NTER.NE.0) GO TO 10 |
| 980 |
NTER =1 |
| 981 |
JP = 0 |
| 982 |
IK = 0 |
| 983 |
CASESN = 1.D0 |
| 984 |
LN=2 |
| 985 |
PNMS=.708E13 |
| 986 |
SQNM=2.2638564E27 |
| 987 |
DNCMS=4.758E13 |
| 988 |
POMS=.684E13 |
| 989 |
RCPMV=.50613E11 |
| 990 |
10 CONTINUE |
| 991 |
LOOP=0 |
| 992 |
INPT=0 |
| 993 |
DO20 I=1,48 |
| 994 |
20 PT(I)=0.0 |
| 995 |
NOF = 0 |
| 996 |
30 BEGRU=0.0 |
| 997 |
NOR=0 |
| 998 |
C NOR=NUMBER OF RECORD |
| 999 |
NOF=NOF+1 |
| 1000 |
C EINC=INC.PART.EN. |
| 1001 |
C CASESN=NO.OF INC.PART. |
| 1002 |
C ANDIT=ANG.DIST. |
| 1003 |
C PRTIN=INC.PART. |
| 1004 |
C TRSYM=STRUCK PART. |
| 1005 |
C RANDI=INPUT RAND NO. |
| 1006 |
C IP=TYPE OF REACTION(-1=S.P.,0=D.P.,1=CHOICE) |
| 1007 |
C IK=0,STRUCK PART.AT REST--OTHERWISE ASSUME ENERGY |
| 1008 |
C JP=0, NO PRINT OUT |
| 1009 |
KASE=0 |
| 1010 |
C SENTINEL FOR GETTING CROSS SECTIONS WHEN STRUCK PARTICLE HAS ENERGY |
| 1011 |
DO40 I=1,3 |
| 1012 |
40 CALCIN(I)=0.0 |
| 1013 |
STRKP = -1.D0 |
| 1014 |
GOTO(50 ,50 ,60 ,70 ,60 ),NO |
| 1015 |
50 PM(1)=DNCMS |
| 1016 |
GOTO110 |
| 1017 |
60 PM(1)=PNMS |
| 1018 |
GOTO80 |
| 1019 |
70 PM(1)=POMS |
| 1020 |
80 IF(NO-4)90 ,100,100 |
| 1021 |
90 ISW(11)=1 |
| 1022 |
GOTO110 |
| 1023 |
100 ISW(11)=0 |
| 1024 |
110 PM(2)=DNCMS |
| 1025 |
KA = 1 |
| 1026 |
E(1)=EINC*RCPMV+PM(1) |
| 1027 |
PXYZ(1)=0.0 |
| 1028 |
PXYZ(5)=0.0 |
| 1029 |
PXYZ(9) = DSQRT (E(1)*E(1) - PM(1)*PM(1) ) |
| 1030 |
RLKE=EINC |
| 1031 |
IF(IK)140,120,140 |
| 1032 |
120 P2=0.0 |
| 1033 |
PXYZ(2)=0.0 |
| 1034 |
PXYZ(6)=0.0 |
| 1035 |
PXYZ(10)=0.0 |
| 1036 |
E(2)=DNCMS |
| 1037 |
GOTO140 |
| 1038 |
130 CONTINUE |
| 1039 |
140 IF(NO-3)150,160,160 |
| 1040 |
150 IF(RLKE-3500.0)230,230,190 |
| 1041 |
160 IF(RLKE-180.0)190,190,170 |
| 1042 |
170 IF(RLKE-2500.0)180,180,190 |
| 1043 |
180 IF(KASE)970 ,230,970 |
| 1044 |
190 IF(IK)200,210,200 |
| 1045 |
200 IF(KASE)220,210,220 |
| 1046 |
210 NE=3 |
| 1047 |
C RLKE IN CERROR('CISOB1') |
| 1048 |
GOTO1050 |
| 1049 |
220 LOOP=LOOP+1 |
| 1050 |
IF(LOOP-1000)130,130,210 |
| 1051 |
230 IF(IP)240,460,460 |
| 1052 |
240 IF(NO-3)460,370,370 |
| 1053 |
250 LK=2 |
| 1054 |
I3=1 |
| 1055 |
260 CALL QRDET(1,PSPCL(1),CALCIN(1)) |
| 1056 |
C ARGUMENT=PSPCL, P-P, N-N, S.P. |
| 1057 |
CALCIN(1)=CRDT(1) |
| 1058 |
IF(LK-6)270,320,320 |
| 1059 |
270 CALL QRDET(1, PEC(1), RLKE) |
| 1060 |
C ELASTIC CROSS SECTION |
| 1061 |
280 CALCIN(3)=CRDT(1)+CALCIN(1)+CALCIN(2) |
| 1062 |
C TOTAL |
| 1063 |
C P-P, N-N, ELASTIC |
| 1064 |
GO TO 630 |
| 1065 |
290 LK=3 |
| 1066 |
I3=2 |
| 1067 |
300 CALL QRDET(1, SPCLN(1),CALCIN(1)) |
| 1068 |
C ARGUMENT=NSPCL, N-P, P-N, S.P. |
| 1069 |
CALCIN(1)=CRDT(1) |
| 1070 |
IF(LK-6)310,320,320 |
| 1071 |
310 CALL QRDET(1, ECN(1), RLKE) |
| 1072 |
GO TO 280 |
| 1073 |
C P-N, N-P, ELASTIC |
| 1074 |
320 CRATIO=CALCIN(1)/(CALCIN(1)+CALCIN(2)) |
| 1075 |
VALUE1 = RANDC(ISEED) |
| 1076 |
IF(VALUE1-CRATIO)330 ,330 ,350 |
| 1077 |
330 IF(KA-NO)360 ,340 ,360 |
| 1078 |
340 I3=1 |
| 1079 |
GOTO270 |
| 1080 |
350 IF(KA-NO)310,270,310 |
| 1081 |
360 I3=2 |
| 1082 |
GOTO310 |
| 1083 |
370 ISW(10)=0 |
| 1084 |
ISW(9)=0 |
| 1085 |
C 9 SET FOR PI0,10 SET FOR PI+-N,PI--P,PI0-P, AND PI0-N |
| 1086 |
CALCIN(1)=RLKE-180.0 |
| 1087 |
LK=1 |
| 1088 |
C PION |
| 1089 |
I3=0 |
| 1090 |
IF(NO-4)380,420,450 |
| 1091 |
380 GOTO(390,400),KA |
| 1092 |
390 CALL QRDET(1, PPSCL(1),CALCIN(1)) |
| 1093 |
CALCIN(1)=CRDT(1) |
| 1094 |
CALL QRDET(1, PPEC(1),RLKE) |
| 1095 |
GOTO280 |
| 1096 |
C PI(PLUS)-P, S.P. OR PI(MINUS)-N |
| 1097 |
400 CALL QRDET(1, PMSCL(1),CALCIN(1)) |
| 1098 |
CALCIN(1)=CRDT(1) |
| 1099 |
CALL QRDET(1, PMEC(1) , RLKE) |
| 1100 |
410 CALCIN(3)=CRDT(1) |
| 1101 |
ISW(10)=2 |
| 1102 |
CALL QRDET(1, PMXC(1) , RLKE) |
| 1103 |
CALCIN(3)=CALCIN(3)+CRDT(1)+CALCIN(1)+CALCIN(2) |
| 1104 |
C PI(PLUS)-N, S.P) OR PI(MINUS)-P |
| 1105 |
GOTO630 |
| 1106 |
420 ISW(9)=2 |
| 1107 |
GOTO(430,440),KA |
| 1108 |
430 CALL QRDET(1, PNSCL(1),CALCIN(1)) |
| 1109 |
CALCIN(1)=CRDT(1) |
| 1110 |
CALL QRDET(1, PNEC(1) ,RLKE) |
| 1111 |
GOTO410 |
| 1112 |
C PI(0)-P, S.P. |
| 1113 |
440 CALL QRDET(1,PNNSL(1) ,CALCIN(1)) |
| 1114 |
CALCIN(1)=CRDT(1) |
| 1115 |
CALL QRDET(1,PNNEC(1) ,RLKE ) |
| 1116 |
GOTO410 |
| 1117 |
C PI(0)-N, S.P. |
| 1118 |
450 GOTO(400,390),KA |
| 1119 |
C PI(-)-P, PI(-)-N, S.P. |
| 1120 |
460 IF(RLKE-920.0)470,470,530 |
| 1121 |
470 IF(IP)480,190,480 |
| 1122 |
480 IF(RLKE-360.0)190,190,490 |
| 1123 |
490 IF(KASE)970 ,500,970 |
| 1124 |
500 CALCIN(1)=RLKE-360.0 |
| 1125 |
GOTO(510,520 ),NO |
| 1126 |
510 ISW(4)=1 |
| 1127 |
GOTO(570,600),KA |
| 1128 |
520 ISW(4)=0 |
| 1129 |
GOTO(600,570),KA |
| 1130 |
530 IF(KASE)970 ,540,970 |
| 1131 |
540 CALCIN(2)=RLKE-920.0 |
| 1132 |
CALCIN(1)=RLKE-360.0 |
| 1133 |
GOTO(550,620),NO |
| 1134 |
550 ISW(4)=1 |
| 1135 |
GOTO(560,590),KA |
| 1136 |
560 CALL QRDET(1,PDPCL(1) ,CALCIN(2)) |
| 1137 |
C ARGUMENT=PDPCL, P-P, N-N, D.P. |
| 1138 |
CALCIN(2)=CRDT(1) |
| 1139 |
C N-N, OR P-P, D.P. |
| 1140 |
570 IF(IP)250,580,580 |
| 1141 |
580 LK=4+2*(IP) |
| 1142 |
I3=3 |
| 1143 |
GOTO260 |
| 1144 |
590 CALL QRDET(1,DPCLN(1) ,CALCIN(2)) |
| 1145 |
C ARGUMENT=NDPCL, N-P, P-N, D.P. |
| 1146 |
CALCIN(2)=CRDT(1) |
| 1147 |
600 IF(IP)290,610,610 |
| 1148 |
610 LK=5+IP |
| 1149 |
I3=4 |
| 1150 |
GOTO300 |
| 1151 |
C N-P, OR P-N, D.P. |
| 1152 |
620 ISW(4)=0 |
| 1153 |
GOTO(590,560),KA |
| 1154 |
630 IF(JP)1050,650,640 |
| 1155 |
C JP=0, NO PRINT OUT |
| 1156 |
640 WRITE(6,10000)EINC,NO,KA,CASESN,(RANDS(I),I=2,4),(CALCIN(I),I=1, |
| 1157 |
+3) , IP,NOF,IK |
| 1158 |
10000 FORMAT(1H1,' EINC NO KA CASESN RANDI CAL |
| 1159 |
+CIN IP NOF IK'/1H0,D11.3,2I8,D11.3,1X,3Z4, |
| 1160 |
+ 3D11.3,3I8) |
| 1161 |
650 CONTINUE |
| 1162 |
KASE=1 |
| 1163 |
IF(IK)130,660,130 |
| 1164 |
660 GOTO(990 ,990 ,680 ,680 ,680 ),NO |
| 1165 |
670 I3=0 |
| 1166 |
680 CALL QOUT17(FRIPN(1),PNMI(1),FMXSP(1),PCFSL(1),PNFSL(1)) |
| 1167 |
IF(I3)1090,730 ,690 |
| 1168 |
690 IF(COL(15)-1.0)730 ,790 ,700 |
| 1169 |
700 IF(COL(15)-3.0)770 ,760 ,710 |
| 1170 |
710 IF(COL(15)-5.0)780 ,1020,720 |
| 1171 |
720 NE=11 |
| 1172 |
GOTO1050 |
| 1173 |
730 CALL QOLLM |
| 1174 |
IF(PT(38))750 ,740 ,750 |
| 1175 |
740 I3=1 |
| 1176 |
GOTO800 |
| 1177 |
750 I3=2 |
| 1178 |
GOTO800 |
| 1179 |
760 I3=4 |
| 1180 |
GOTO800 |
| 1181 |
770 I3=5 |
| 1182 |
GOTO800 |
| 1183 |
780 I3=6 |
| 1184 |
GOTO800 |
| 1185 |
790 I3=3 |
| 1186 |
800 CALL QOUT18 |
| 1187 |
I3=I3 |
| 1188 |
GOTO(690 ,810 ,690 ,820 ),I3 |
| 1189 |
810 NE=12 |
| 1190 |
GOTO1050 |
| 1191 |
820 PM(4)=DNCMS |
| 1192 |
K=IP |
| 1193 |
J=2 |
| 1194 |
IF(IP)830 ,860 ,840 |
| 1195 |
830 NWRIT=22 |
| 1196 |
MM=26 |
| 1197 |
GO TO 870 |
| 1198 |
840 IF(PT(38))850 ,830 ,850 |
| 1199 |
850 K=K+1 |
| 1200 |
860 NWRIT=29 |
| 1201 |
MM=38 |
| 1202 |
870 OUT(1)=K |
| 1203 |
DO900 I=2,MM,12 |
| 1204 |
M=I |
| 1205 |
K=M+3 |
| 1206 |
DO890 N=1,2 |
| 1207 |
DO880 L=M,K |
| 1208 |
OUT(J)=PT(L) |
| 1209 |
880 J=J+1 |
| 1210 |
M=I+6 |
| 1211 |
890 K=M+2 |
| 1212 |
900 CONTINUE |
| 1213 |
NOR=NOR+1 |
| 1214 |
910 IF(JP)1050,930,920 |
| 1215 |
C JP=0, NO PRINT OUT |
| 1216 |
920 WRITE(6,10100)NOR,(OUT(I),I=1,NWRIT),E(2),(PXYZ(I),I=2,10,4) |
| 1217 |
10100 FORMAT(1H ,I7/(7D14.5)) |
| 1218 |
930 NWDS=NWRIT+4 |
| 1219 |
C NO.OF WORDS IN RECORD |
| 1220 |
940 DO950 I=1,48 |
| 1221 |
950 PT(I)=0.0 |
| 1222 |
PGCNT=0.0 |
| 1223 |
PACNT=0.0 |
| 1224 |
LOOP=0 |
| 1225 |
BEGRU=BEGRU+1.0 |
| 1226 |
IF(CASESN-BEGRU)1050,1080,960 |
| 1227 |
960 IF(IK)130,970 ,130 |
| 1228 |
970 GOTO(670 ,980 ,1000,1010,1040,1100),LK |
| 1229 |
980 I3=1 |
| 1230 |
990 CALL QOUT21(FRINN(1),DMIN(1),FMXSN(1),FMXDN(1),FSLN(1)) |
| 1231 |
GOTO680 |
| 1232 |
1000 I3=2 |
| 1233 |
GOTO990 |
| 1234 |
1010 I3=3 |
| 1235 |
GOTO990 |
| 1236 |
1020 CALL QOUT19 |
| 1237 |
IF(I3)1030,820 ,820 |
| 1238 |
1030 NE=13 |
| 1239 |
GOTO1050 |
| 1240 |
1040 I3=4 |
| 1241 |
GOTO990 |
| 1242 |
1050 CALL CERROR('CISOB$') |
| 1243 |
IF(NE-3)1080,1060,1060 |
| 1244 |
1060 IF(CALCIN(1))1070,1080,1070 |
| 1245 |
1070 CONTINUE |
| 1246 |
NOR=NOR+1 |
| 1247 |
1080 CONTINUE |
| 1248 |
RETURN |
| 1249 |
1090 NE=10 |
| 1250 |
GOTO1050 |
| 1251 |
1100 VALUE1 = RANDC(ISEED) |
| 1252 |
IF(VALUE1-CRATIO)1110,1110,1120 |
| 1253 |
1110 IF(KA-NO)1000,980 ,1000 |
| 1254 |
1120 IF(KA-NO)1130,1010,1130 |
| 1255 |
1130 GO TO 1040 |
| 1256 |
END |
| 1257 |
*CMZ : 1.01/04 10/06/93 14.43.41 by Christian Zeitnitz |
| 1258 |
*-- Author : |
| 1259 |
SUBROUTINE CPCOL(IB,ITYP,HSIG,EC,NOPART,KIND,EP,ALF,BET,GAM) |
| 1260 |
C |
| 1261 |
#include "cinpu.inc" |
| 1262 |
#include "cjoint.inc" |
| 1263 |
#include "cisobr.inc" |
| 1264 |
#include "cxpd.inc" |
| 1265 |
#include "crun.inc" |
| 1266 |
#include "cinout.inc" |
| 1267 |
#include "crandm.inc" |
| 1268 |
#include "cbert.inc" |
| 1269 |
*KEND. |
| 1270 |
REAL*8 DCLN(80),DCIN(115),PPAC(19),POAC(19), |
| 1271 |
+ FMXSN(161),FMXDN(130),FMXSP(117),PDCI(60),PDCH(55),DCHN(143), |
| 1272 |
+ DCHNA(36),DCHNB(60),PSPCL(158),PDPCL(130),SPCLN(158),DPCLN(130), |
| 1273 |
+ FSLN(176),FRINN(161),DMIN(101),PPSCL(117),PNSCL(117),PMSCL(117), |
| 1274 |
+ PNNSL(117),PCFSL(234),FRIPN(117),PNMI(101),PNFSL(234),PNEC(126), |
| 1275 |
+ PNNEC(126),PMXC(126),PMEC(126),PPEC(126),PEC(176),ECN(176), |
| 1276 |
+ PPDC(6426),PMDD(6426),PMDX(6426),PNDD(6426) |
| 1277 |
EQUIVALENCE (TAPCRS(1),DCLN(1)) ,(TAPCRS(81),DCIN(1)) , (TAPCRS(1 |
| 1278 |
+96),PPAC(1)) ,(TAPCRS(215),POAC(1)) , (TAPCRS(234),FMXSN(1)) , |
| 1279 |
+(TAPCRS(395),FMXDN(1)) , (TAPCRS(525),FMXSP(1)) ,(TAPCRS(642), |
| 1280 |
+PDCI(1)) , (TAPCRS(702),PDCH(1)) ,(TAPCRS(757),DCHN(1)) , (TAPCRS |
| 1281 |
+(900),DCHNA(1)) ,(TAPCRS(936),DCHNB(1)) , (TAPCRS(996),PSPCL(1)) |
| 1282 |
+,(TAPCRS(1154),PDPCL(1)), (TAPCRS(1284),SPCLN(1)),(TAPCRS(1442), |
| 1283 |
+DPCLN(1)), (TAPCRS(1572),FSLN(1)) ,(TAPCRS(1748),FRINN(1)) |
| 1284 |
EQUIVALENCE (TAPCRS(1909),DMIN(1)) ,(TAPCRS(2010),PPSCL(1)), |
| 1285 |
+ (TAPCRS(2127),PNSCL(1)),(TAPCRS(2244),PMSCL(1)), |
| 1286 |
+ (TAPCRS(2361),PNNSL(1)),(TAPCRS(2478),PCFSL(1)), |
| 1287 |
+ (TAPCRS(2712),FRIPN(1)),(TAPCRS(2829),PNMI(1)) , |
| 1288 |
+ (TAPCRS(2930),PNFSL(1)),(TAPCRS(3164),PNEC(1)) , |
| 1289 |
+ (TAPCRS(3290),PNNEC(1)),(TAPCRS(3416),PMXC(1)) , |
| 1290 |
+ (TAPCRS(3542),PMEC(1)) ,(TAPCRS(3668),PPEC(1)) , |
| 1291 |
+ (TAPCRS(3794),PEC(1)) ,(TAPCRS(3970),ECN(1)) , |
| 1292 |
+ (TAPCRS(4146),PPDC(1)) ,(TAPCRS(10572),PMDD(1)), |
| 1293 |
+ (TAPCRS(16998),PMDX(1)),(TAPCRS(23424),PNDD(1)) |
| 1294 |
C |
| 1295 |
DIMENSION KIND(60),EP(60),ALF(60),BET(60),GAM(60) |
| 1296 |
DIMENSION ICC(12) |
| 1297 |
SAVE |
| 1298 |
C |
| 1299 |
KE =1 |
| 1300 |
IF(IB)30,10,30 |
| 1301 |
10 IB =1 |
| 1302 |
AND1T = DBLE(ANDT) |
| 1303 |
CZ BERT dataset already read by CRBERT called by CALINI 19.june 92 |
| 1304 |
SF = 1.D0 |
| 1305 |
RANDI(1) = 16896 |
| 1306 |
PNMS = .708D13 |
| 1307 |
C PI+ OR - MASS IN PER CM. |
| 1308 |
DNCMS = 4.758D13 |
| 1309 |
C NUCLEON MASS IN PER CM. |
| 1310 |
SQNM=DNCMS*DNCMS |
| 1311 |
C NUCLEON MASS SQD. |
| 1312 |
RCPMV = .50613D11 |
| 1313 |
C RECIPROCAL CM PER MEV. |
| 1314 |
POMS = .684D13 |
| 1315 |
C PIO MASS IN RECIP. CM |
| 1316 |
DO 20 I = 1,19 |
| 1317 |
POAC(I) = POAC(I) + POAC(I) |
| 1318 |
20 PPAC(I) = PPAC(I)/SF |
| 1319 |
C POAC(19),PPAC(19) |
| 1320 |
30 DO 40 I =1,60 |
| 1321 |
40 IPEC(I) =0 |
| 1322 |
DO 50 I =1,2114 |
| 1323 |
50 ESPS(I) = 0.D0 |
| 1324 |
DO 60 I = 4515,4849 |
| 1325 |
60 ESPS(I) = 0.D0 |
| 1326 |
DO 70 I=1,12 |
| 1327 |
70 ICC(I)= 0 |
| 1328 |
DO 80 I = 1,4 |
| 1329 |
80 RANDS(I) = RANDI(I) |
| 1330 |
PM(1) = DNCMS |
| 1331 |
GO TO(110,110,100,90,100,90,90),ITYP |
| 1332 |
C P N PI+ PI0 PI- MU+ MU- |
| 1333 |
90 CALL CERROR('CPCOL1$') |
| 1334 |
WRITE(IO,10000) ITYP |
| 1335 |
10000 FORMAT(' Wrong particle type = ',I2,' in CPCOL') |
| 1336 |
100 PM(1) = PNMS |
| 1337 |
110 INC =1 |
| 1338 |
CLSM = 1.D0 |
| 1339 |
PM(2) = DNCMS |
| 1340 |
E(2) = DNCMS |
| 1341 |
E(1) = DBLE(EC)*RCPMV + PM(1) |
| 1342 |
PXYZ(2) = 0. |
| 1343 |
PXYZ(6) = 0. |
| 1344 |
PXYZ(10) = 0. |
| 1345 |
CALL P1CLI |
| 1346 |
C CALC'S X,Y,Z MOM COORD'S OF INC. PART.(PXYZ(1-5-9))AND P1OE1 = PZ1 |
| 1347 |
RLKE =(((E(1)*E(2)-PXYZ(1)*PXYZ(2)-PXYZ(5)*PXYZ(6)-PXYZ(9)*PXYZ(10 |
| 1348 |
+ )) /DNCMS)-PM(1))/RCPMV |
| 1349 |
VALUE1 = RANDC(ISEED) |
| 1350 |
R = SNGL(VALUE1) |
| 1351 |
VALUE1 = RLKE |
| 1352 |
ITP = ITYP - ITYP/5 |
| 1353 |
NOPART = 2 |
| 1354 |
GO TO (170,170,200,120),ITP |
| 1355 |
120 CONTINUE |
| 1356 |
C TRY (PI-,P) EXCHANGE. |
| 1357 |
R = R - XSECHE(4,ITP,EC)/HSIG |
| 1358 |
IF( R.GT.0.) GO TO 200 |
| 1359 |
C A (PI-,P) EXCHANGE EVENT HAS OCCURRED |
| 1360 |
IT = 5 |
| 1361 |
KIND(1) = 3 |
| 1362 |
C PI 0 |
| 1363 |
KIND(2) = 1 |
| 1364 |
C NEUTRON |
| 1365 |
PT(2) = 4.D0 |
| 1366 |
PT(14) = 2.D0 |
| 1367 |
IK = IT |
| 1368 |
PM(3) = POMS |
| 1369 |
IF(RLKE - 340.D0) 130,130,140 |
| 1370 |
130 CALL CALMUD(SNT,INPT) |
| 1371 |
CALL CRDET(51,PMDX,RLKE) |
| 1372 |
C DIF PI--P EXCHG |
| 1373 |
GO TO 370 |
| 1374 |
140 I3 = 1 |
| 1375 |
IF(RLKE-1000.D0) 150,160,160 |
| 1376 |
150 I3 = 2 |
| 1377 |
VALUE1 = RLKE - 340.D0 |
| 1378 |
160 CALL ROUT16(PMDX) |
| 1379 |
C DIF PI--P EXCHG 2500-1000, 1000-340, 340- 0 |
| 1380 |
GO TO 440 |
| 1381 |
170 CONTINUE |
| 1382 |
C TRY NUCLEON - P DBLE PRODUCTION. |
| 1383 |
IF(EC.LT.ETH(2,ITP)) GO TO 200 |
| 1384 |
R = R - XSECHE(2,ITP,EC)/HSIG |
| 1385 |
IF( R.GT.0. ) GO TO 200 |
| 1386 |
C DBLE PRODUCTION HAS OCCURRED. |
| 1387 |
NOPART =4 |
| 1388 |
IPPP = 0 |
| 1389 |
180 NNO = ITYP |
| 1390 |
E1NC = DBLE(EC) |
| 1391 |
CALL CISOB |
| 1392 |
KNO = 2 |
| 1393 |
DO 190 NOO = 1,NOPART |
| 1394 |
KIND(NOO) = IDINT( DOUT(KNO)) - 1 |
| 1395 |
EP(NOO) = SNGL ( DOUT(KNO+1)) |
| 1396 |
ALF(NOO) = SNGL ( DOUT(KNO+4)) |
| 1397 |
BET(NOO) = SNGL ( DOUT(KNO+5)) |
| 1398 |
GAM(NOO) = SNGL ( DOUT(KNO+6)) |
| 1399 |
190 KNO = KNO + 7 |
| 1400 |
GO TO 310 |
| 1401 |
200 CONTINUE |
| 1402 |
C TRY SNGL PRODUCTION. |
| 1403 |
IF(EC .LT. ETH(1,ITP)) GO TO 210 |
| 1404 |
R = R - XSECHE(1,ITP,EC)/HSIG |
| 1405 |
IF( R.GT.0.) GO TO 210 |
| 1406 |
C NUCLEON - P ,PI+ -P, OR PI- -P SNGL PRODUCTION HAS OCCURRED. |
| 1407 |
NOPART =3 |
| 1408 |
IPPP = -1 |
| 1409 |
GO TO 180 |
| 1410 |
210 CONTINUE |
| 1411 |
C AN ELASTIC EVENT HAS OCCURRED. |
| 1412 |
GO TO (230,240,340,220,390,220,220),ITYP |
| 1413 |
220 CALL CERROR('CPCOL2$') |
| 1414 |
WRITE(IO,10100) ITYP |
| 1415 |
10100 FORMAT(' Wrong particle type = ',I2,' in CPCOL ') |
| 1416 |
230 I3 =7 |
| 1417 |
IT =18 |
| 1418 |
GO TO 250 |
| 1419 |
240 I3 = 4 |
| 1420 |
IT = 15 |
| 1421 |
250 CALL ROUT20(DCIN(1),DCLN(1),DCHN(1),PDCI(1),PDCH(1)) |
| 1422 |
C ELAS DIF XSECTS-NP 300-740,NP 0-300, NP 660-3500, PP 500-1000,PP 660-3 |
| 1423 |
C SETS PT(2)=1.-PROT,2.-NEUT,PT(14)=1.,PM(3)= DNCMS |
| 1424 |
C CALC'S CST(SCAT COS) FOR EC GT (500 FOR PROT,740 FOR NEUTS) |
| 1425 |
I3 = I3 |
| 1426 |
IGO = I3-4 |
| 1427 |
GO TO (330 ,260 ,270 ,280 ),IGO |
| 1428 |
C I3 = 5 6 7 8 |
| 1429 |
260 SNT = DSQRT(1.D0 - CST*CST) |
| 1430 |
GO TO 280 |
| 1431 |
270 CALL CAPOL1(CST,SNT) |
| 1432 |
280 CALL CESWH |
| 1433 |
290 IF(IT.EQ.5) GO TO 300 |
| 1434 |
KIND(1) = ITYP - 1 |
| 1435 |
KIND(2) = 0 |
| 1436 |
C PROTON |
| 1437 |
300 CONTINUE |
| 1438 |
EP(1)= SNGL( PT(3) ) |
| 1439 |
ALF(1)=SNGL( PT(8) ) |
| 1440 |
BET(1)=SNGL( PT(9) ) |
| 1441 |
GAM(1)=SNGL( PT(10)) |
| 1442 |
EP(2)= SNGL( PT(15)) |
| 1443 |
ALF(2)=SNGL( PT(20)) |
| 1444 |
BET(2)=SNGL( PT(21)) |
| 1445 |
GAM(2)=SNGL( PT(22)) |
| 1446 |
310 DO 320 I = 2,4 |
| 1447 |
320 RANDI(I) = RANDS(I) |
| 1448 |
RETURN |
| 1449 |
330 I3=4 |
| 1450 |
CALL ROUT15(PPDC(1)) |
| 1451 |
C CALC'S CST(SCAT COS) FOR EC LT 740 MEV |
| 1452 |
GO TO 260 |
| 1453 |
340 I3 =1 |
| 1454 |
IT =1 |
| 1455 |
C PI+-P ELAS |
| 1456 |
350 CALL ROUT11(PPDC (1)) |
| 1457 |
C TAPCRS(248) PI+-P LT 340 MEV. |
| 1458 |
I3 = I3 |
| 1459 |
GO TO (380,360,360,370),I3 |
| 1460 |
360 CALL CERROR('CPCOL3$') |
| 1461 |
WRITE(IO,10200) I3 |
| 1462 |
10200 FORMAT(' I3 = ',I3,' IN CPCOL') |
| 1463 |
370 CST = CRDT(2)- DABS(SNT*(CRDT(2)-CRDT(1))) |
| 1464 |
GO TO 260 |
| 1465 |
380 I3 =1 |
| 1466 |
CALL ROUT15(PPDC(1)) |
| 1467 |
C PI+-P DIF ELAS FOR1.-2.5 GEV AT 3401,FOR .34 -1. AT 3231. |
| 1468 |
I3 = I3 |
| 1469 |
GO TO 260 |
| 1470 |
390 IT= 3 |
| 1471 |
C PI--P ELAS |
| 1472 |
I3= 2 |
| 1473 |
PT(2) = 5.D0 |
| 1474 |
PT(14)= 1.D0 |
| 1475 |
IK= IT |
| 1476 |
PM(3) = PNMS |
| 1477 |
IF(RLKE - 340.D0) 400,400,410 |
| 1478 |
400 CALL CALMUD(SNT,INPT) |
| 1479 |
CALL CRDET(51,PMDD(1),RLKE) |
| 1480 |
GO TO 370 |
| 1481 |
410 I3 =1 |
| 1482 |
IF(RLKE - 1000.D0) 420,430,430 |
| 1483 |
420 I3 = 2 |
| 1484 |
VALUE1 = RLKE - 340.D0 |
| 1485 |
430 CALL ROUT16(PMDD(1)) |
| 1486 |
440 I3 = I3 |
| 1487 |
IF( I3) 260,450,460 |
| 1488 |
450 I3 = 3 |
| 1489 |
CALL ROUT15(PPDC(1)) |
| 1490 |
GO TO 260 |
| 1491 |
460 CONTINUE |
| 1492 |
GO TO 360 |
| 1493 |
END |
| 1494 |
*CMZ : 1.01/04 10/06/93 14.43.41 by Christian Zeitnitz |
| 1495 |
*-- Author : |
| 1496 |
SUBROUTINE CALQDK |
| 1497 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 1498 |
#include "cbert3.inc" |
| 1499 |
#include "cisob2.inc" |
| 1500 |
*KEND. |
| 1501 |
SAVE |
| 1502 |
C |
| 1503 |
UNIV=PNIDK(6)*PNIDK(6) |
| 1504 |
C M(P1) SQUARED DECAY PION MASS SQUARED |
| 1505 |
PNIDK(7)=(PNIDK(1)*PNIDK(1)+UNIV-SQNM)/(2.0*PNIDK(1)) |
| 1506 |
C E(PI)PRIME DECAY PION ENERGY PRIME |
| 1507 |
PNIDK(8)=DSQRT(PNIDK(7)*PNIDK(7)-UNIV) |
| 1508 |
C DECAY PION MOMENTUM PRIME P(D) |
| 1509 |
CALL CAPOL1(PNIDK(20),PNIDK(21)) |
| 1510 |
C COS THETA, SIN THETA |
| 1511 |
CALL CAAZIO(PNIDK(22),PNIDK(23)) |
| 1512 |
C COS PHI, SIN PHI |
| 1513 |
PNIDK(9)=PNIDK(22)*PNIDK(21)*PNIDK(8) |
| 1514 |
C DECAY PION X MOMENTUM COMPONENT PRIME |
| 1515 |
PNIDK(10)=PNIDK(21)*PNIDK(23)*PNIDK(8) |
| 1516 |
C P(P1)PRIME Y |
| 1517 |
PNIDK(11)=PNIDK(20)*PNIDK(8) |
| 1518 |
C P(P1)PRIME Z |
| 1519 |
UNIV=PNIDK(9)*PNIDK(2)+PNIDK(10)*PNIDK(3)+PNIDK(11)*PNIDK(4) |
| 1520 |
C P P1 PRIME DOT P |
| 1521 |
PNIDK(12)=(PNIDK(7)*PNIDK(5)+UNIV)/PNIDK(1) |
| 1522 |
C DECAY PION ENERGY E(PI) |
| 1523 |
PNIDK(13)=PNIDK(5)-PNIDK(12) |
| 1524 |
UNIV=(((PNIDK(5)/PNIDK(1))-1.0)*UNIV)/(PNIDK(2)*PNIDK(2)+ |
| 1525 |
+PNIDK(3)*PNIDK(3)+PNIDK(4)*PNIDK(4)) |
| 1526 |
C (E/M-1.0)*P(P1)PRIME DOT P/P SQUARED |
| 1527 |
UNIVE=PNIDK(7)/PNIDK(1) |
| 1528 |
C E PI PRIME OVER MASS |
| 1529 |
DO10 I=2,4 |
| 1530 |
PNIDK(I+12)=PNIDK(I)*(UNIV+UNIVE) +PNIDK(I+7) |
| 1531 |
10 PNIDK(I+15)=PNIDK(I)-PNIDK(I+12) |
| 1532 |
RETURN |
| 1533 |
C PION MOMENTUM COMPONENTS AND NUCLEON MOMENTUM |
| 1534 |
C COMPONENTS |
| 1535 |
END |
| 1536 |
*CMZ : 0.92/00 02/12/92 16.02.29 by Christian Zeitnitz |
| 1537 |
*-- Author : |
| 1538 |
SUBROUTINE CQENE(Z) |
| 1539 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 1540 |
#include "cbert3.inc" |
| 1541 |
#include "cisob2.inc" |
| 1542 |
*KEND. |
| 1543 |
DIMENSION Z(380) |
| 1544 |
SAVE |
| 1545 |
C |
| 1546 |
CD=COM*1.0D2 |
| 1547 |
I=IDINT(CD+1.00D0) |
| 1548 |
AZ=Z(I) |
| 1549 |
IF(I.EQ.1)GOTO150 |
| 1550 |
10 BZ=Z(I+1) |
| 1551 |
IF(101-(I+1))70,20,30 |
| 1552 |
20 CZ=BZ+5.0D-1*(BZ-AZ) |
| 1553 |
GOTO40 |
| 1554 |
30 CZ=Z(I+2) |
| 1555 |
40 XZ=CD-DFLOAT(I-1) |
| 1556 |
SCA=CZ-AZ |
| 1557 |
C F(2)-F(0) |
| 1558 |
50 SBA=BZ-AZ |
| 1559 |
C F(1)-F(0) |
| 1560 |
SQA=AZ*AZ |
| 1561 |
C F(0)**2 |
| 1562 |
SQAC=SQA-CZ*CZ |
| 1563 |
C F(0)**2-F(2)**2 |
| 1564 |
SQBA=BZ*BZ-SQA |
| 1565 |
C F(1)**2-F(0)**2 |
| 1566 |
RB=SQAC+SQBA+SQBA |
| 1567 |
C (ASQ-CSQ)+2(BSQ-ASQ) |
| 1568 |
CZ |
| 1569 |
CZ changed in order to keep exponent small 5/21/92 |
| 1570 |
RC=AZ*1.0D-20*CZ*SCA-SBA*1.0D-20*(2.0D0*AZ*BZ+XZ*(BZ-CZ)*SCA) |
| 1571 |
CZ RC is 1E-20 smaller than it supposed to be !!!! |
| 1572 |
RA=SCA-SBA-SBA |
| 1573 |
C (C-A)-2(B-A) |
| 1574 |
IF(RA.NE.0.0)GOTO60 |
| 1575 |
COM=AZ+XZ*SBA |
| 1576 |
GOTO80 |
| 1577 |
60 CONTINUE |
| 1578 |
CZ \/ factor 1E-20 in RC !! |
| 1579 |
DISC=RB*1.0D-20*RB-4.0D0*RA*RC |
| 1580 |
IF(DISC)70,90,90 |
| 1581 |
C B**2-4AC |
| 1582 |
70 CALL CERROR('CQENE1$') |
| 1583 |
80 RETURN |
| 1584 |
CZ \/ correct for factor 1E-20 |
| 1585 |
90 DISC=DSQRT(DISC)*1.0D10 |
| 1586 |
CZ end of change |
| 1587 |
CZ |
| 1588 |
PLUS=(DISC-RB)/(RA+RA) |
| 1589 |
AMINUS=(-RB-DISC)/(RA+RA) |
| 1590 |
IF(I.EQ.1)GOTO160 |
| 1591 |
100 IF(PLUS.GT.BZ)GOTO120 |
| 1592 |
IF(PLUS.LT.AZ)GOTO120 |
| 1593 |
IF(AMINUS.GT.BZ)GOTO110 |
| 1594 |
IF(AMINUS.GE.AZ)GOTO140 |
| 1595 |
110 COM=PLUS |
| 1596 |
GOTO80 |
| 1597 |
120 IF(AMINUS.GT.BZ)GOTO70 |
| 1598 |
IF(AMINUS.LT.AZ)GOTO70 |
| 1599 |
130 COM=AMINUS |
| 1600 |
GOTO80 |
| 1601 |
140 RA=XZ*SBA+AZ |
| 1602 |
RB=DABS(RA-AMINUS) |
| 1603 |
RC=DABS(RA-PLUS) |
| 1604 |
IF(RB.GT.RC)GOTO110 |
| 1605 |
GOTO130 |
| 1606 |
150 CZ=Z(I+1) |
| 1607 |
SCA=CZ-AZ |
| 1608 |
BZ=AZ+SCA*7.071067812D-1 |
| 1609 |
XZ=CD+CD |
| 1610 |
GOTO50 |
| 1611 |
C (CZ-AZ)(CZ-AZ)=C,CZ=MASS FOR R=1,AZ=MASS FOR R=0, C=CONST.FOR PARABOLA |
| 1612 |
C (M-AZ)(M-AZ)=0.5*C,DETERMINES MASS,BZ,FOR R=1/2 |
| 1613 |
160 BZ=CZ |
| 1614 |
XZ=XZ-CD |
| 1615 |
SBA=CZ-AZ |
| 1616 |
GOTO100 |
| 1617 |
END |
| 1618 |
*CMZ : 0.92/00 02/12/92 16.02.29 by Christian Zeitnitz |
| 1619 |
*-- Author : |
| 1620 |
SUBROUTINE CQLP19 |
| 1621 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 1622 |
C |
| 1623 |
#include "crandm.inc" |
| 1624 |
#include "cbert3.inc" |
| 1625 |
#include "cisob2.inc" |
| 1626 |
*KEND. |
| 1627 |
SAVE |
| 1628 |
C |
| 1629 |
UNIV = RANDC(ISEED) |
| 1630 |
PT(2)=1.0 |
| 1631 |
PT(26)=1.0 |
| 1632 |
PT(14)=3.0 |
| 1633 |
PT(16)=POMS |
| 1634 |
IF(ISW(12))10,10,140 |
| 1635 |
10 IF(UNIV-.25)20,20,110 |
| 1636 |
20 IF(ISW(4))40,30,40 |
| 1637 |
30 PT(2)=2.0 |
| 1638 |
40 UNIV = RANDC(ISEED) |
| 1639 |
IF(UNIV-.66666667)50,50,90 |
| 1640 |
50 PT(14)=4.0 |
| 1641 |
60 IF(ISW(4))80,70,80 |
| 1642 |
70 PT(26)=2.0 |
| 1643 |
80 RETURN |
| 1644 |
90 PT(16)=PNMS |
| 1645 |
IF(ISW(4))70,100,70 |
| 1646 |
100 PT(14)=5.0 |
| 1647 |
GOTO80 |
| 1648 |
110 IF(ISW(4))130,120,130 |
| 1649 |
120 PT(26)=2.0 |
| 1650 |
GOTO90 |
| 1651 |
130 PT(2)=2.0 |
| 1652 |
PT(16)=PNMS |
| 1653 |
GOTO80 |
| 1654 |
140 IF(UNIV-.5)150,150,190 |
| 1655 |
150 IF(ISW(4))160,170,160 |
| 1656 |
160 PT(2)=2.0 |
| 1657 |
170 UNIV = RANDC(ISEED) |
| 1658 |
IF(UNIV-.33333333)90,90,180 |
| 1659 |
180 PT(14)=4.0 |
| 1660 |
GOTO60 |
| 1661 |
190 IF(ISW(4))210,200,210 |
| 1662 |
200 PT(2)=2.0 |
| 1663 |
210 UNIV = RANDC(ISEED) |
| 1664 |
IF(UNIV-.66666667)220,220,230 |
| 1665 |
220 PT(14)=4.0 |
| 1666 |
IF(ISW(4))70,80,70 |
| 1667 |
230 PT(16)=PNMS |
| 1668 |
IF(ISW(4))240,70,240 |
| 1669 |
240 GO TO 100 |
| 1670 |
END |
| 1671 |
*CMZ : 0.92/00 02/12/92 16.02.29 by Christian Zeitnitz |
| 1672 |
*-- Author : |
| 1673 |
SUBROUTINE CQLP28 |
| 1674 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 1675 |
C |
| 1676 |
#include "crandm.inc" |
| 1677 |
#include "cbert3.inc" |
| 1678 |
#include "cisob2.inc" |
| 1679 |
*KEND. |
| 1680 |
SAVE |
| 1681 |
C |
| 1682 |
R = RANDC(ISEED) |
| 1683 |
IF(ISW(13))230,10,230 |
| 1684 |
10 IF(R-.6)20,20,120 |
| 1685 |
20 PT(4)=PNMS |
| 1686 |
R = RANDC(ISEED) |
| 1687 |
IF(ISW(4))30,90,30 |
| 1688 |
30 IF(R-.33333333)40,40,70 |
| 1689 |
40 PT(26)=5.0 |
| 1690 |
50 PT(28)=PNMS |
| 1691 |
60 RETURN |
| 1692 |
70 PT(26)=4.0 |
| 1693 |
80 PT(38)=2.0 |
| 1694 |
GOTO60 |
| 1695 |
90 PT(2)=5.0 |
| 1696 |
PT(14)=2.0 |
| 1697 |
IF(R-.33333333)100,100,110 |
| 1698 |
100 PT(28)=PNMS |
| 1699 |
GOTO80 |
| 1700 |
110 PT(26)=4.0 |
| 1701 |
GOTO60 |
| 1702 |
120 R = RANDC(ISEED) |
| 1703 |
IF(ISW(4))130,180,130 |
| 1704 |
130 IF(R-.66666667)140,140,160 |
| 1705 |
140 PT(2)=4.0 |
| 1706 |
150 R = RANDC(ISEED) |
| 1707 |
IF(R-.66666667)110,110,100 |
| 1708 |
160 PT(14)=2.0 |
| 1709 |
170 PT(4)=PNMS |
| 1710 |
GOTO150 |
| 1711 |
180 IF(R-.66666667)190,190,220 |
| 1712 |
190 PT(2)=4.0 |
| 1713 |
200 PT(14)=2.0 |
| 1714 |
210 R = RANDC(ISEED) |
| 1715 |
IF(R-.66666667)70,70,40 |
| 1716 |
220 PT(2)=5.0 |
| 1717 |
PT(4)=PNMS |
| 1718 |
GOTO210 |
| 1719 |
230 IF(R-VALUE1)240,240,270 |
| 1720 |
240 PT(4)=PNMS |
| 1721 |
IF(ISW(4))260,250,260 |
| 1722 |
250 PT(2)=5.0 |
| 1723 |
PT(14)=2.0 |
| 1724 |
GOTO50 |
| 1725 |
260 PT(38)=2.0 |
| 1726 |
GOTO40 |
| 1727 |
270 R = RANDC(ISEED) |
| 1728 |
IF(ISW(4))280,310,280 |
| 1729 |
280 IF(R-.33333333)290,290,300 |
| 1730 |
290 PT(4)=PNMS |
| 1731 |
GOTO200 |
| 1732 |
300 PT(2)=4.0 |
| 1733 |
GOTO210 |
| 1734 |
310 IF(R-.33333333)320,320,330 |
| 1735 |
320 PT(2)=5.0 |
| 1736 |
GOTO170 |
| 1737 |
330 PT(14)=2.0 |
| 1738 |
GOTO140 |
| 1739 |
END |
| 1740 |
*CMZ : 0.92/00 02/12/92 16.02.29 by Christian Zeitnitz |
| 1741 |
*-- Author : |
| 1742 |
SUBROUTINE CQLPHA |
| 1743 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 1744 |
C |
| 1745 |
#include "crandm.inc" |
| 1746 |
#include "cbert3.inc" |
| 1747 |
#include "cisob2.inc" |
| 1748 |
*KEND. |
| 1749 |
SAVE |
| 1750 |
C |
| 1751 |
UNIV = RANDC(ISEED) |
| 1752 |
IF(VALUE3)300,10,140 |
| 1753 |
10 IF(UNIV-VALUE1)20,20,120 |
| 1754 |
20 IF(ISW(11))40,30,40 |
| 1755 |
30 PT(2)=5.0 |
| 1756 |
PT(26)=2.0 |
| 1757 |
40 PT(4)=PNMS |
| 1758 |
PM(4)=PNMS |
| 1759 |
UNIV = RANDC(ISEED) |
| 1760 |
IF(UNIV-VALUE2)50,50,70 |
| 1761 |
50 PT(14)=4.0 |
| 1762 |
60 RETURN |
| 1763 |
70 IF(ISW(11))110,80,110 |
| 1764 |
80 PT(26)=1.0 |
| 1765 |
90 PT(14)=5.0 |
| 1766 |
100 PT(16)=PNMS |
| 1767 |
GOTO60 |
| 1768 |
110 PT(26)=2.0 |
| 1769 |
GOTO100 |
| 1770 |
120 PT(2)=4.0 |
| 1771 |
IF(ISW(11))100,130,100 |
| 1772 |
130 PT(14)=5.0 |
| 1773 |
GOTO110 |
| 1774 |
140 IF(UNIV-VALUE1)150,150,200 |
| 1775 |
150 PM(4)=PNMS |
| 1776 |
IF(ISW(11))160,190,160 |
| 1777 |
160 PT(2)=5.0 |
| 1778 |
170 PT(16)=PNMS |
| 1779 |
180 PT(4)=PNMS |
| 1780 |
GOTO60 |
| 1781 |
190 PT(14)=5.0 |
| 1782 |
PT(26)=2.0 |
| 1783 |
GOTO170 |
| 1784 |
200 IF(UNIV-VALUE2)210,210,250 |
| 1785 |
210 PT(2)=4.0 |
| 1786 |
UNIV = RANDC(ISEED) |
| 1787 |
IF(UNIV-VALUE3)240,240,220 |
| 1788 |
220 IF(ISW(11))50,230,50 |
| 1789 |
230 PT(26)=2.0 |
| 1790 |
GOTO50 |
| 1791 |
240 IF(ISW(11))110,90,110 |
| 1792 |
250 PM(4)=PNMS |
| 1793 |
PT(4)=PNMS |
| 1794 |
UNIV = RANDC(ISEED) |
| 1795 |
IF(UNIV-.66666667)260,260,280 |
| 1796 |
260 IF(ISW(11))230,270,230 |
| 1797 |
270 PT(2)=5.0 |
| 1798 |
GOTO50 |
| 1799 |
280 IF(ISW(11))90,290,90 |
| 1800 |
290 PT(26)=2.0 |
| 1801 |
GOTO160 |
| 1802 |
300 IF(UNIV-VALUE1)310,310,340 |
| 1803 |
310 PM(4)=PNMS |
| 1804 |
PT(4)=PNMS |
| 1805 |
UNIV = RANDC(ISEED) |
| 1806 |
IF(VALUE3+1.0)330,320,330 |
| 1807 |
320 IF(UNIV-.33333333)90,90,230 |
| 1808 |
330 PT(2)=5.0 |
| 1809 |
IF(UNIV-.33333333)110,110,50 |
| 1810 |
340 IF(UNIV-VALUE2)350,350,380 |
| 1811 |
350 PT(2)=4.0 |
| 1812 |
UNIV = RANDC(ISEED) |
| 1813 |
IF(VALUE3+1.0)370,360,370 |
| 1814 |
360 IF(UNIV-.66666667)50,50,110 |
| 1815 |
370 IF(UNIV-.66666667)230,230,90 |
| 1816 |
380 PM(4)=PNMS |
| 1817 |
PT(4)=PNMS |
| 1818 |
IF(VALUE3+1.0)390,160,390 |
| 1819 |
390 PT(14)=5.0 |
| 1820 |
GOTO110 |
| 1821 |
END |
| 1822 |
*CMZ : 1.01/00 03/06/93 19.40.16 by Christian Zeitnitz |
| 1823 |
*-- Author : |
| 1824 |
SUBROUTINE CQNGID |
| 1825 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 1826 |
C |
| 1827 |
#include "crandm.inc" |
| 1828 |
#include "cbert3.inc" |
| 1829 |
#include "cisob2.inc" |
| 1830 |
*KEND. |
| 1831 |
SAVE |
| 1832 |
C |
| 1833 |
C ****************************************************************** |
| 1834 |
C**** CALCULATES COS AND SIN THETA,SIN AND COS PHI ************** |
| 1835 |
C ****************************************************************** |
| 1836 |
ICURR= CURR(1) |
| 1837 |
IT=0 |
| 1838 |
GO TO(10,10,30,30,30),ICURR |
| 1839 |
C**** INCIDENT PARTICLE - NUCLEON |
| 1840 |
10 IF(IT.EQ.21.OR.IT.EQ.22)GO TO 20 |
| 1841 |
C**** SINGLE PRODUCTION |
| 1842 |
IF(RLKE.GT.3500.0D0) CALL CERROR('CQNGID1$') |
| 1843 |
IF(RLKE.LT.500.0D0)GO TO 70 |
| 1844 |
TESISO= 0.75D0 |
| 1845 |
IF(RLKE.LT.1000.0D0)GO TO 50 |
| 1846 |
TESISO= 0.5D0 |
| 1847 |
IF(RLKE.LT.1300.0D0)GO TO 50 |
| 1848 |
TESISO= 0.25D0 |
| 1849 |
IF(RLKE.LT.2500.0D0)GO TO 50 |
| 1850 |
GO TO 60 |
| 1851 |
C**** DOUBLE PRODUCTION |
| 1852 |
20 IF(RLKE.GT.3500.0D0) CALL CERROR('CQNGID2$') |
| 1853 |
GO TO 60 |
| 1854 |
C**** INCIDENT PARTICLE-PION |
| 1855 |
30 R = RANDC(ISEED) |
| 1856 |
IF(RLKE.GT.2500.0D0) CALL CERROR('CQNGID3$') |
| 1857 |
CST= -0.9999995D0 |
| 1858 |
SNT= 0.003162D0 |
| 1859 |
IF(IT.NE.11)GO TO 40 |
| 1860 |
IF(R.LE.0.75D0)GO TO 70 |
| 1861 |
GO TO 80 |
| 1862 |
C**** (PI+)-(P),(PI-)-(N) |
| 1863 |
C**** (PI0)-(N),(PI0)-(P) |
| 1864 |
40 IF(IT.NE.12.AND.IT.NE.28) CALL CERROR('CQNGID4$') |
| 1865 |
IF(RLKE.LT.500.0D0)CST=-CST |
| 1866 |
IF(R.LE.0.80D0)GO TO 70 |
| 1867 |
GO TO 80 |
| 1868 |
50 R = RANDC(ISEED) |
| 1869 |
IF(R.LE.TESISO)GO TO 70 |
| 1870 |
C**** BACKWARD/FORWARD |
| 1871 |
60 R = RANDC(ISEED) |
| 1872 |
C**** TEST FOR DIRECTION |
| 1873 |
CST= 0.9999995D0 |
| 1874 |
SNT= 0.003162D0 |
| 1875 |
IF(R.LE.0.5)GO TO 80 |
| 1876 |
CST= -0.9999995D0 |
| 1877 |
GO TO 80 |
| 1878 |
C**** ISOTROPIC |
| 1879 |
70 CALL CAPOL1(CST,SNT) |
| 1880 |
C**** CALCULATES COS,SIN PHI |
| 1881 |
80 CALL CAAZIO(SOPC,SOPS) |
| 1882 |
RETURN |
| 1883 |
END |
| 1884 |
*CMZ : 0.92/00 02/12/92 16.02.29 by Christian Zeitnitz |
| 1885 |
*-- Author : |
| 1886 |
SUBROUTINE CQOLL |
| 1887 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 1888 |
#include "cbert3.inc" |
| 1889 |
#include "cisob2.inc" |
| 1890 |
*KEND. |
| 1891 |
SAVE |
| 1892 |
C |
| 1893 |
A=PM(4)*PM(4) |
| 1894 |
COL(15)=0.0 |
| 1895 |
COL(1)=E(1)+E(2) |
| 1896 |
C TOTAL ENERGY PARTICLES 1 AND 2 |
| 1897 |
DO10 I=1,3 |
| 1898 |
10 COL(I+1)=PM(I)*PM(I) |
| 1899 |
C MASS PARTICLE I SQD. |
| 1900 |
COL(5)=COL(3)+COL(2)+2.0*(E(1)*E(2)-(PXYZ(1)*PXYZ(2)+PXYZ(5)* |
| 1901 |
1PXYZ(6)+PXYZ(9)*PXYZ(10))) |
| 1902 |
COL(6)=DSQRT(COL(5)) |
| 1903 |
COL(7)=COL(6)/COL(1) |
| 1904 |
C GAM |
| 1905 |
COL(8)=2.0*COL(6) |
| 1906 |
COL(9)=(COL(4)+COL(5)-A)/COL(8) |
| 1907 |
COM2=COL(9)*COL(9) |
| 1908 |
20 IF(COL(4)-2.9882156E27)30,30,50 |
| 1909 |
C GT,PM(3)=ISOBAR--LTE,TEST FOR ROUNDOFF RANGE,(MIN)SQD+OR-5E23 |
| 1910 |
30 IF(COL(4)-2.9872156E27)60,40 ,40 |
| 1911 |
C LT,PION OR NUCLEON MASS=PM(3) |
| 1912 |
40 COL(4)=2.9877156E27 |
| 1913 |
PM(3) = 5.466005D13 |
| 1914 |
50 IF(COM2-COL(4))70,90,90 |
| 1915 |
60 IF(COL(4)-SQNM)50,50,120 |
| 1916 |
C LTE,HAVE NUCLEON OR PION--GT,GO TO ERROR |
| 1917 |
70 IF(COM2-9.9D-1*COL(4)) 90,80,80 |
| 1918 |
80 COM2 = COL(4) |
| 1919 |
COL(9) = PM(3) |
| 1920 |
90 COL(10)=DSQRT(COM2-COL(4)) |
| 1921 |
C P3 PRIME |
| 1922 |
IF(IK)100,170,100 |
| 1923 |
100 COL(11)=(COL(5)+COL(2)-COL(3))/COL(8) |
| 1924 |
C E1 PRIME |
| 1925 |
COL(12)=DSQRT(COL(11)*COL(11)-COL(2)) |
| 1926 |
C P1 PRIME |
| 1927 |
COL(13)=(COL(7)*E(1)-COL(11))/COL(12) |
| 1928 |
C BETA |
| 1929 |
COM=1.0-(COL(13)*COL(13)+COL(7)*COL(7)) |
| 1930 |
IF(COM-5.0E-6)110,150,150 |
| 1931 |
110 IF(COM+5.0E-6)120,140,140 |
| 1932 |
120 COL(15)=1.0 |
| 1933 |
C ERROR |
| 1934 |
130 RETURN |
| 1935 |
140 COL(14)=.002236067977 |
| 1936 |
GOTO160 |
| 1937 |
150 COL(14)=DSQRT(COM) |
| 1938 |
C ALPHA |
| 1939 |
160 E(3)=(COL(9)+COL(10)*(COL(13)*CST+COL(14)*SOPC*SNT))/COL(7) |
| 1940 |
E(4)=COL(1)-E(3) |
| 1941 |
GOTO130 |
| 1942 |
170 DO180 I=11,14 |
| 1943 |
180 COL(I)=0.0 |
| 1944 |
E(3)=0.0 |
| 1945 |
E(4)=0.0 |
| 1946 |
GOTO130 |
| 1947 |
C FOR PART AT REST E1 AND P1 PRIME,ALPHA AND BETA NOT |
| 1948 |
C CALCULATED. E(3) ANDE(4) DONE LATER |
| 1949 |
END |
| 1950 |
*CMZ : 1.01/04 10/06/93 14.43.41 by Christian Zeitnitz |
| 1951 |
*-- Author : |
| 1952 |
SUBROUTINE QOLLM |
| 1953 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 1954 |
#include "cbert3.inc" |
| 1955 |
#include "cisob2.inc" |
| 1956 |
*KEND. |
| 1957 |
SAVE |
| 1958 |
C |
| 1959 |
IF(IK)10,60,10 |
| 1960 |
10 UNIV=E(2)+COL(6)-COL(11) |
| 1961 |
UNIVE=E(1)+COL(11) |
| 1962 |
UNIVER=COL(1)+COL(6) |
| 1963 |
K=16 |
| 1964 |
DO20 I=1,9,4 |
| 1965 |
COL(K)=(PXYZ(I)*UNIV-PXYZ(I+1)*UNIVE)/UNIVER |
| 1966 |
COL(K+3)=(PXYZ(I)+PXYZ(I+1))/COL(1) |
| 1967 |
C VX |
| 1968 |
20 K=K+1 |
| 1969 |
COL(22)=(-PXYZ(9)*PXYZ(6))/COL(1) |
| 1970 |
C QX |
| 1971 |
C ABBREVIATED FORM SINCE PXYZ(1)=PXYZ(5)=0.0 |
| 1972 |
COL(23)=(PXYZ(2)*PXYZ(9))/COL(1) |
| 1973 |
C QY |
| 1974 |
C ABBREVIATED FORM SINCE PXYZ(1)=PXYZ(5)=0.0 |
| 1975 |
COL(24)=0.0 |
| 1976 |
C ABBREVIATED FORM SINCE PXYZ(1)=PXYZ(5)=0.0 |
| 1977 |
A=SNT/COL(14) |
| 1978 |
B=A*COL(10) |
| 1979 |
C (-BETA*COS PHI*SIN THETA/ALPHA + COS THETA)/P1P*P3P |
| 1980 |
UNIV=COL(10)*(CST-A*SOPC*COL(13))/COL(12) |
| 1981 |
UNIVE=B*SOPS/COL(12) |
| 1982 |
C P3P*SIN PHI*SIN THETA/P1P*ALPHA |
| 1983 |
UNIVER=(SOPC*B)+((E(3)+COL(9))/(COL(7)+1.0)) |
| 1984 |
C COS PHI*SIN THETA*P3P/ALPHA + (E3+E3P)/(1.0+GAMMA) |
| 1985 |
K=19 |
| 1986 |
DO30 I=3,11,4 |
| 1987 |
PXYZ(I)=COL(K)*UNIVER+COL(K+3)*UNIVE+COL(K-3)*UNIV |
| 1988 |
30 K=K+1 |
| 1989 |
DO40 I=1,9,4 |
| 1990 |
40 PXYZ(I+3)=PXYZ(I)+PXYZ(I+1)-PXYZ(I+2) |
| 1991 |
50 RETURN |
| 1992 |
60 DO70 I=16,17 |
| 1993 |
COL(I)=0.0 |
| 1994 |
70 COL(I+3)=0.0 |
| 1995 |
COL(18)=PXYZ(9)*PM(2)/COL(6) |
| 1996 |
C P(1),Z *M2/M=P(BAR PRIME)1,Z |
| 1997 |
COL(21)=PXYZ(9)/COL(1) |
| 1998 |
C VZ VELOCITY |
| 1999 |
DO80 I=22,24 |
| 2000 |
80 COL(I)=0.0 |
| 2001 |
C CROSS PRODUCT P1 PRIME X V |
| 2002 |
PXYZ(3)=COL(10)*SNT*SOPC |
| 2003 |
C X COMPONENT P3 BAR =P3 PRIME X SIN THETA X COS PHI |
| 2004 |
PXYZ(7)=COL(10)*SNT*SOPS |
| 2005 |
C Y COMP. P3 BAR =P3 PRIME X SIN THETA X SIN PHI |
| 2006 |
PXYZ(11)=COL(10)*CST |
| 2007 |
Z=PXYZ(9)/COL(6) |
| 2008 |
PXYZ(11)=PXYZ(11)+(Z*PXYZ(9)*PXYZ(11))/(COL(1)+COL(6))+Z*COL(9) |
| 2009 |
C Z COMP. P3 BAR=P3 PRIME COS THETA+(P1Z SQ*P3Z (PRIME)COS |
| 2010 |
C THETA/(E PRIME*(E+E PRIME))+P1Z*E3 PRIME/E PRIME |
| 2011 |
E(3)=DSQRT(PXYZ(3)*PXYZ(3)+PXYZ(7)*PXYZ(7)+PXYZ(11)*PXYZ(11)+ |
| 2012 |
+PM(3)*PM(3)) |
| 2013 |
DO90 I=1,9,4 |
| 2014 |
90 PXYZ(I+3)=PXYZ(I)-PXYZ(I+2) |
| 2015 |
E(4)=DSQRT(PXYZ(4)*PXYZ(4)+PXYZ(8)*PXYZ(8)+PXYZ(12)*PXYZ(12) |
| 2016 |
++PM(4)*PM(4)) |
| 2017 |
IF(PT(38))50,100,50 |
| 2018 |
100 PT(3)=((E(4)-PM(4))/RCPMV)+PT(3) |
| 2019 |
GOTO50 |
| 2020 |
END |
| 2021 |
*CMZ : 0.92/00 02/12/92 16.02.29 by Christian Zeitnitz |
| 2022 |
*-- Author : |
| 2023 |
SUBROUTINE QOUT17(T,B,R,W,G) |
| 2024 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 2025 |
C |
| 2026 |
#include "crandm.inc" |
| 2027 |
#include "cbert3.inc" |
| 2028 |
#include "cisob2.inc" |
| 2029 |
*KEND. |
| 2030 |
C |
| 2031 |
DIMENSIONT(117),B(101),R(117),W(234),G(234) |
| 2032 |
SAVE |
| 2033 |
C |
| 2034 |
IF(I3)10 ,10 ,160 |
| 2035 |
10 PT(38)=0.0 |
| 2036 |
C 1-ALPHA PART.6+1 |
| 2037 |
VALUE1=RLKE-180.0 |
| 2038 |
CALL QRDET(1,T(1),VALUE1) |
| 2039 |
20 COM2=CRDT(1) |
| 2040 |
FTR =DNCMS*RLKE*2.0*RCPMV+2.9877156E27 |
| 2041 |
C E**2=MIN**2+NCNMS*RLKE*2*RCPMV |
| 2042 |
UNIVER=DSQRT(FTR ) |
| 2043 |
C E |
| 2044 |
30 VALUE2 = RANDC(ISEED) |
| 2045 |
COM=VALUE2*COM2 |
| 2046 |
C R-PRIME |
| 2047 |
CALL CQENE (B(1)) |
| 2048 |
COM1=(COM*COM+FTR -.501264E26)/(2.0*UNIVER) |
| 2049 |
C M1R PRIME)**2+E**2-2(PNMS)/2E=E ALPHA |
| 2050 |
A=COM1*COM1-COM*COM |
| 2051 |
IF(A)40 ,50 ,50 |
| 2052 |
40 PACNT=PACNT+1.0 |
| 2053 |
GOTO30 |
| 2054 |
50 UNIVE=(UNIVER-COM1)*COM1*(DSQRT(A)/UNIVER) |
| 2055 |
C ((E BETA*E ALPHA*P ALPHA)/E)=F(M,TR) |
| 2056 |
CALL QRDET(1,R(1),VALUE1) |
| 2057 |
C (PI-NUC)FMAX(RLKE)ISOBAR SAMPLING S.P. |
| 2058 |
COM1 = RANDC(ISEED) |
| 2059 |
IF((UNIVE/CRDT(1))-COM1)30 ,60 ,60 |
| 2060 |
C RANDOM NO. LESS OR EQUAL THAN F(M,TR)/FMAX(TR) |
| 2061 |
60 CALL CQNGID |
| 2062 |
PM(4)=POMS |
| 2063 |
PM(3)=COM |
| 2064 |
PT(2)=3.0 |
| 2065 |
PT(4)=POMS |
| 2066 |
PT(14)=3.0 |
| 2067 |
PT(16)=POMS |
| 2068 |
PT(26)=1.0 |
| 2069 |
PT(28)=DNCMS |
| 2070 |
IF(ISW(9))80 ,70 ,80 |
| 2071 |
70 IF(ISW(10))120 ,110 ,120 |
| 2072 |
80 IF(ISW(10))130 ,90 ,130 |
| 2073 |
90 I3=-1 |
| 2074 |
100 RETURN |
| 2075 |
110 VALUE1=.4 |
| 2076 |
VALUE2=.66666667 |
| 2077 |
VALUE3=0.0 |
| 2078 |
GOTO150 |
| 2079 |
120 CALL QRDET(2,W(1),VALUE1) |
| 2080 |
C (PICH-P)FRACT. FIN.STA.WITH RECL. PI1 PI0 L.E. |
| 2081 |
VALUE3=.33333333 |
| 2082 |
GOTO140 |
| 2083 |
130 CALL QRDET(2,G(1),VALUE1) |
| 2084 |
VALUE3=STRKP |
| 2085 |
C (PIN-P)FRACT.FIN.STA.WITH RECL.PI1 PIO L.E. |
| 2086 |
140 VALUE1=CRDT(1) |
| 2087 |
VALUE2=CRDT(2) |
| 2088 |
150 CALL CQLPHA |
| 2089 |
160 PT(3)=0.0 |
| 2090 |
PT(15)=0.0 |
| 2091 |
PT(27)=0.0 |
| 2092 |
PT(39)=0.0 |
| 2093 |
170 CALL CQOLL |
| 2094 |
IF(COL(15))90 ,180 ,90 |
| 2095 |
180 IF(PT(38))190 ,200 ,190 |
| 2096 |
190 I3=0 |
| 2097 |
GOTO100 |
| 2098 |
200 PT(39)=0.0 |
| 2099 |
IF(IK)210 ,220 ,210 |
| 2100 |
210 PT(3)=((E(4)-PM(4))/RCPMV)+PT(3) |
| 2101 |
220 I3=1 |
| 2102 |
GOTO100 |
| 2103 |
END |
| 2104 |
*CMZ : 1.01/04 10/06/93 14.43.41 by Christian Zeitnitz |
| 2105 |
*-- Author : |
| 2106 |
SUBROUTINE QOUT18 |
| 2107 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 2108 |
#include "cbert3.inc" |
| 2109 |
#include "cisob2.inc" |
| 2110 |
*KEND. |
| 2111 |
SAVE |
| 2112 |
GOTO(10 ,20 ,80 ,120 ,80 ,100 ),I3 |
| 2113 |
10 I=3 |
| 2114 |
COL(15)=1.0 |
| 2115 |
K=27 |
| 2116 |
GOTO30 |
| 2117 |
20 I=3 |
| 2118 |
COL(15)=4.0 |
| 2119 |
K=15 |
| 2120 |
30 PNIDK(1)=PM(I) |
| 2121 |
J=I |
| 2122 |
DO40 L=2,4 |
| 2123 |
PNIDK(L)=PXYZ(J) |
| 2124 |
40 J=J+4 |
| 2125 |
PNIDK(5)=E(I) |
| 2126 |
PNIDK(6)=PT(K-11) |
| 2127 |
CALL CALQDK |
| 2128 |
IF(K-27)60 ,50 ,60 |
| 2129 |
50 PT(15)=PT(15)+((PNIDK(12)-PNIDK( 6))/RCPMV) |
| 2130 |
60 PT(K)=PT(K)+((PNIDK(13)-DNCMS)/RCPMV) |
| 2131 |
I3=1 |
| 2132 |
70 IV=K |
| 2133 |
RETURN |
| 2134 |
80 COL(15)=3.0 |
| 2135 |
K=15 |
| 2136 |
IF(PT(14)-2.0)90 ,90 ,120 |
| 2137 |
90 I3=2 |
| 2138 |
GOTO70 |
| 2139 |
100 L=14 |
| 2140 |
DO110 M=5,7 |
| 2141 |
PT(M)=PNIDK(L) |
| 2142 |
PT(M+12)=PNIDK(L+3) |
| 2143 |
110 L=L+1 |
| 2144 |
PT(11)=PNIDK(12) |
| 2145 |
PT(12)=PNIDK(6) |
| 2146 |
I=4 |
| 2147 |
K=39 |
| 2148 |
COL(15)=5.0 |
| 2149 |
GOTO30 |
| 2150 |
120 I1=3 |
| 2151 |
130 K=12*I1-33 |
| 2152 |
140 IF(I1-4)150 ,160 ,170 |
| 2153 |
150 I2=-1 |
| 2154 |
GOTO200 |
| 2155 |
160 I2=0 |
| 2156 |
GOTO200 |
| 2157 |
170 IF(I1-5)160 ,190 ,180 |
| 2158 |
180 I3=4 |
| 2159 |
GOTO70 |
| 2160 |
190 I2=1 |
| 2161 |
200 IF(PT(K))210 ,220 ,210 |
| 2162 |
210 CALL CQSTOR |
| 2163 |
220 I1=I1+1 |
| 2164 |
GOTO130 |
| 2165 |
END |
| 2166 |
*CMZ : 0.92/00 02/12/92 16.02.29 by Christian Zeitnitz |
| 2167 |
*-- Author : |
| 2168 |
SUBROUTINE QOUT19 |
| 2169 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 2170 |
#include "cbert3.inc" |
| 2171 |
#include "cisob2.inc" |
| 2172 |
*KEND. |
| 2173 |
SAVE |
| 2174 |
C |
| 2175 |
10 PT(3)=PT(3)+((PT(11)-PT(12))/RCPMV) |
| 2176 |
C COLLISION ALLOWED |
| 2177 |
K=3 |
| 2178 |
GOTO100 |
| 2179 |
20 I3=-1 |
| 2180 |
30 RETURN |
| 2181 |
40 I2=2 |
| 2182 |
50 I1=(K/12)+3 |
| 2183 |
60 CALL CQSTOR |
| 2184 |
70 IF(K-15)80 ,90 ,120 |
| 2185 |
80 K=15 |
| 2186 |
GOTO40 |
| 2187 |
90 K=27 |
| 2188 |
PT(27)=PT(27)+((PNIDK(12)-PT(K+1))/RCPMV) |
| 2189 |
100 IF(K-15)40 ,110 ,110 |
| 2190 |
110 I2=0 |
| 2191 |
GOTO50 |
| 2192 |
120 IF(K-27)20 ,130 ,140 |
| 2193 |
130 IF(PT(39))140 ,140 ,150 |
| 2194 |
140 I3=0 |
| 2195 |
GOTO30 |
| 2196 |
150 I2=1 |
| 2197 |
K=39 |
| 2198 |
GOTO50 |
| 2199 |
END |
| 2200 |
*CMZ : 0.92/00 02/12/92 16.02.29 by Christian Zeitnitz |
| 2201 |
*-- Author : |
| 2202 |
SUBROUTINE QOUT21(V,W,X,Y,Z) |
| 2203 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 2204 |
C |
| 2205 |
#include "crandm.inc" |
| 2206 |
#include "cbert3.inc" |
| 2207 |
#include "cisob2.inc" |
| 2208 |
*KEND. |
| 2209 |
C |
| 2210 |
REAL*8 V(161),W(101),X(161),Y(130),Z(176) |
| 2211 |
SAVE |
| 2212 |
C |
| 2213 |
VALUE2=RLKE*4.81633308E24+9.0554256E27 |
| 2214 |
C E(TR)**2=RLKE*RCPMV*2*NCMS+4*NCMS**2 |
| 2215 |
VALUE3=DSQRT(VALUE2) |
| 2216 |
GOTO(10 ,130 ,140 ,270 ),I3 |
| 2217 |
10 ISW(12)=0 |
| 2218 |
20 PT(38)=0.0 |
| 2219 |
I1=0 |
| 2220 |
30 ANS=RLKE |
| 2221 |
40 VALUE1=ANS-300.0 |
| 2222 |
CALL QRDET(1,V(1),VALUE1) |
| 2223 |
C (NUC-NUC) F(TR) ISOBAR SAMPLING |
| 2224 |
FTR=CRDT(1) |
| 2225 |
50 SN = RANDC(ISEED) |
| 2226 |
COM=SN*FTR |
| 2227 |
C R PRIME=F(TR)*RANDOM |
| 2228 |
CALL CQENE (W(1)) |
| 2229 |
C (NUC-NUC)MASS OF ISOBAR S.P. M(R PRIME) |
| 2230 |
IF(I1)160 ,60 ,170 |
| 2231 |
60 COM1=(COM*COM-SQNM+VALUE2)/(2.0*VALUE3) |
| 2232 |
C E GAMMA |
| 2233 |
A=COM1*COM1-COM*COM |
| 2234 |
IF(A)70 ,80 ,80 |
| 2235 |
70 PGCNT=PGCNT+1.0 |
| 2236 |
GOTO50 |
| 2237 |
80 UNIVER=DSQRT(A)*COM1*((VALUE3-COM1)/VALUE3) |
| 2238 |
C F(M,TR)=P GAMMA*E GAMMA*E DELTA/E |
| 2239 |
CALL QRDET(1,X(1),VALUE1) |
| 2240 |
C (NUC-NUC)FMAX(TR) ISOBAR SAMPLING S.P. |
| 2241 |
COM1 = RANDC(ISEED) |
| 2242 |
IF(COM1-(UNIVER/CRDT(1)))90 ,90 ,50 |
| 2243 |
90 PM(4)=DNCMS |
| 2244 |
PM(3)=COM |
| 2245 |
100 CALL CQNGID |
| 2246 |
PT(4)=DNCMS |
| 2247 |
PT(28)=DNCMS |
| 2248 |
110 CALL CQLP19 |
| 2249 |
120 RETURN |
| 2250 |
130 ISW(12)=2 |
| 2251 |
GOTO20 |
| 2252 |
140 ISW(13)=0 |
| 2253 |
150 I1=-1 |
| 2254 |
ANS=((VALUE3-.708E13)**2-9.0554256E27)/4.81633308E24 |
| 2255 |
GOTO40 |
| 2256 |
C TR PRIME COM1=RLKE PRIME |
| 2257 |
160 COM1=((VALUE3+DNCMS-COM)**2-9.0554256E27)/4.81633308E24 |
| 2258 |
COM2=COM |
| 2259 |
ANS=COM1 |
| 2260 |
COM4=FTR |
| 2261 |
I1=1 |
| 2262 |
GOTO40 |
| 2263 |
170 COM1=(COM2*COM2-COM*COM+VALUE2)/(2.0*VALUE3) |
| 2264 |
C E EPSILON |
| 2265 |
A=COM1*COM1-COM2*COM2 |
| 2266 |
IF(A)180 ,190 ,190 |
| 2267 |
180 PECNT=PECNT+1.0 |
| 2268 |
GOTO200 |
| 2269 |
C F(M1,M2,TR)=P EPSILON*E EPSILON*E ZETA/E |
| 2270 |
190 UNIVER=DSQRT(A)*COM1*((VALUE3-COM1)/VALUE3) |
| 2271 |
VALUE1=RLKE-920.0 |
| 2272 |
CALL QRDET(1,Y(1),VALUE1) |
| 2273 |
C (NUC-NUC)FMAX(TR) ISOBAR SAMPLING D.P. FMAX(M1,M2,TR) |
| 2274 |
SN = RANDC(ISEED) |
| 2275 |
IF(SN-(UNIVER*FTR/(CRDT(1)*COM4)))210 ,210 ,200 |
| 2276 |
200 FTR=COM4 |
| 2277 |
I1=-1 |
| 2278 |
GOTO50 |
| 2279 |
210 VALUE1 = RANDC(ISEED) |
| 2280 |
IF(VALUE1-.5)220 ,220 ,230 |
| 2281 |
220 PM(3)=COM2 |
| 2282 |
PM(4)=COM |
| 2283 |
GOTO240 |
| 2284 |
230 PM(3)=COM |
| 2285 |
PM(4)=COM2 |
| 2286 |
240 CALL CQNGID |
| 2287 |
PT(16)=DNCMS |
| 2288 |
PT(40)=DNCMS |
| 2289 |
IF(ISW(13))250 ,260 ,250 |
| 2290 |
250 CALL QRDET(1,Z(1),RLKE) |
| 2291 |
VALUE1=CRDT(1) |
| 2292 |
C (N-P)FRACT.FIN.STA.3/2 L.E. |
| 2293 |
260 PT(2)=3.0 |
| 2294 |
PT(4)=POMS |
| 2295 |
PT(14)=1.0 |
| 2296 |
PT(26)=3.0 |
| 2297 |
PT(28)=POMS |
| 2298 |
PT(38)=1.0 |
| 2299 |
CALL CQLP28 |
| 2300 |
GOTO120 |
| 2301 |
270 ISW(13)=2.0 |
| 2302 |
GOTO150 |
| 2303 |
END |
| 2304 |
*CMZ : 1.01/04 10/06/93 14.43.41 by Christian Zeitnitz |
| 2305 |
*-- Author : |
| 2306 |
SUBROUTINE QRDET(NODATA,DATA,ENER) |
| 2307 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 2308 |
#include "cbert3.inc" |
| 2309 |
#include "cisob2.inc" |
| 2310 |
*KEND. |
| 2311 |
DIMENSION DATA(380) |
| 2312 |
SAVE |
| 2313 |
C |
| 2314 |
IE=DABS(ENER/20.0) |
| 2315 |
UNIV=(ENER-DFLOAT(IE)*20.0)/20.0 |
| 2316 |
DO10 I=1,25 |
| 2317 |
10 CRDT(I)=0.0 |
| 2318 |
K=(NODATA*IE)+1 |
| 2319 |
IF(INPT)50 ,20 ,50 |
| 2320 |
20 N=NODATA |
| 2321 |
30 L=K+NODATA |
| 2322 |
DO40 I=1,N |
| 2323 |
CRDT(I)=(DATA(L)-DATA(K))*UNIV+DATA(K) |
| 2324 |
K=K+1 |
| 2325 |
40 L=L+1 |
| 2326 |
INPT=0 |
| 2327 |
RETURN |
| 2328 |
50 K=INPT-1+K |
| 2329 |
N=2 |
| 2330 |
GOTO30 |
| 2331 |
END |
| 2332 |
*CMZ : 1.01/04 10/06/93 14.43.41 by Christian Zeitnitz |
| 2333 |
*-- Author : |
| 2334 |
SUBROUTINE CQSTOR |
| 2335 |
IMPLICIT REAL *8 (A-H,O-Z) |
| 2336 |
#include "cbert3.inc" |
| 2337 |
#include "cisob2.inc" |
| 2338 |
*KEND. |
| 2339 |
SAVE |
| 2340 |
C |
| 2341 |
L=(I1*12)-28 |
| 2342 |
IF(I2)10,60,70 |
| 2343 |
10 JJ=0 |
| 2344 |
IF(PM(3)-DNCMS)30,30,20 |
| 2345 |
20 I1=I1+1 |
| 2346 |
JJ=1 |
| 2347 |
C X-Y-Z-COORDINATES OF COLLISION POINT |
| 2348 |
30 UNIV=DSQRT(PXYZ(I1)*PXYZ(I1)+PXYZ(I1+4)*PXYZ(I1+4)+PXYZ(I1+8)* |
| 2349 |
+PXYZ(I1+8)) |
| 2350 |
K=I1+8 |
| 2351 |
DO40 I=I1,K,4 |
| 2352 |
PT(L)=PXYZ(I)/UNIV |
| 2353 |
40 L=L+1 |
| 2354 |
I1=I1-JJ |
| 2355 |
50 RETURN |
| 2356 |
60 K=14 |
| 2357 |
GOTO90 |
| 2358 |
70 IF(I2-2)80,110,110 |
| 2359 |
80 K=17 |
| 2360 |
90 UNIV=DSQRT(PNIDK(K)*PNIDK(K)+PNIDK(K+1)*PNIDK(K+1)+PNIDK |
| 2361 |
+(K+2)*PNIDK(K+2)) |
| 2362 |
PT(L-3)=1.0 |
| 2363 |
J=K+2 |
| 2364 |
DO100 I=K,J |
| 2365 |
PT(L)=PNIDK(I)/UNIV |
| 2366 |
100 L=L+1 |
| 2367 |
GOTO50 |
| 2368 |
110 UNIV=DSQRT(PT(L-3)*PT(L-3)+PT(L-2)*PT(L-2)+PT(L-1)*PT(L-1)) |
| 2369 |
K=L-1 |
| 2370 |
M=L-3 |
| 2371 |
DO120 I=M,K |
| 2372 |
PT(L)=PT(I)/UNIV |
| 2373 |
120 L=L+1 |
| 2374 |
PT(M)=1.0 |
| 2375 |
GOTO50 |
| 2376 |
END |
| 2377 |
*CMZ : 0.92/00 02/12/92 16.02.29 by Christian Zeitnitz |
| 2378 |
*-- Author : |
| 2379 |
FUNCTION SFLRAF(X) |
| 2380 |
C |
| 2381 |
#include "crandm.inc" |
| 2382 |
*KEND. |
| 2383 |
C |
| 2384 |
SFLRAF = 2.0 * RANDC(ISEED) |
| 2385 |
TEMP = 1.0 - SFLRAF |
| 2386 |
IF(TEMP) 10 ,20 ,20 |
| 2387 |
10 SFLRAF = TEMP |
| 2388 |
20 RETURN |
| 2389 |
END |
| 2390 |
*CMZ : 1.01/04 10/06/93 14.43.41 by Christian Zeitnitz |
| 2391 |
*-- Author : |
| 2392 |
SUBROUTINE CALSGM(NSGNL,IT,IS,DDE,EM,I,E,S) |
| 2393 |
C |
| 2394 |
#include "cinout.inc" |
| 2395 |
#include "cxpd.inc" |
| 2396 |
#include "cbert2.inc" |
| 2397 |
*KEND. |
| 2398 |
C |
| 2399 |
DIMENSION PPNP(9,2),ENRGY(9) |
| 2400 |
DATA ENRGY/1., 3., 5., 8., 10., 12.5,15., 17.5,20./ |
| 2401 |
DATA PPNP /1.20,.890,.620,.392,.310,.250,.208,.178,.155, |
| 2402 |
+ 4.25,2.28,1.62,1.14,.940,.765,.645,.555,.480/ |
| 2403 |
DATA IEMX /9/ |
| 2404 |
SAVE |
| 2405 |
C |
| 2406 |
I= IFIX(EM/DDE + 1.) |
| 2407 |
E= FLOAT(I-1)*DDE |
| 2408 |
IF(EM.LT.20.0.AND.IT.LE.2) GO TO 70 |
| 2409 |
GO TO (10,30),NSGNL |
| 2410 |
10 TEMP = SNGL(CS(I+IS)) |
| 2411 |
S = TEMP + (EM-E)/DDE*(SNGL(CS(I+1+IS))- TEMP) |
| 2412 |
20 RETURN |
| 2413 |
30 IF(IT.GT.2) GO TO 60 |
| 2414 |
IF(I.LT.176) GO TO 50 |
| 2415 |
40 CALL CERROR('CALSGM1$') |
| 2416 |
50 S= NPSG(IT,I) +(EM-E)/DDE*(NPSG(IT,I+1) - NPSG(IT,I) ) |
| 2417 |
GO TO 20 |
| 2418 |
60 IF(I.GT.125) GO TO 40 |
| 2419 |
IT = IT - 2 |
| 2420 |
S= PIPSG(IT,I) + (EM-E)/DDE *(PIPSG(IT,I+1) - PIPSG(IT,I) ) |
| 2421 |
GO TO 20 |
| 2422 |
C** LOW ENERGY (.LT. 20 MEV) P-P OF N-P XSECTS FOR ELAST. SCATT. WITH H. |
| 2423 |
70 CONTINUE |
| 2424 |
IF(EM.LT.ENRGY(1)) CALL CERROR('CALSGM2$') |
| 2425 |
DO 80 IE = 2,IEMX |
| 2426 |
IF(EM.LE.ENRGY(IE)) GO TO 90 |
| 2427 |
80 CONTINUE |
| 2428 |
CALL CERROR('CALSGM3$') |
| 2429 |
90 S = ALOG(PPNP(IE-1,IT)) + (EM - ENRGY(IE-1)) / |
| 2430 |
+ (ENRGY(IE) - ENRGY(IE-1)) * |
| 2431 |
+ (ALOG(PPNP(IE,IT)) - ALOG(PPNP(IE-1,IT))) |
| 2432 |
S = EXP(S) * 1.0E-24 |
| 2433 |
GO TO 20 |
| 2434 |
END |
| 2435 |
*CMZ : 1.01/04 10/06/93 14.43.41 by Christian Zeitnitz |
| 2436 |
*-- Author : |
| 2437 |
SUBROUTINE CSHXD |
| 2438 |
C |
| 2439 |
#include "cxpd.inc" |
| 2440 |
*KEND. |
| 2441 |
C |
| 2442 |
DE = 20. |
| 2443 |
LOCX(1,1) = 995 |
| 2444 |
LOCX(2,1) = 1153 |
| 2445 |
LOCX(3,1) = 3793 |
| 2446 |
LOCX(4,1)= 0 |
| 2447 |
LOCX(1,2) = 1283 |
| 2448 |
LOCX(2,2) = 1441 |
| 2449 |
LOCX(3,2) = 3969 |
| 2450 |
LOCX(4,2)= 0 |
| 2451 |
LOCX(1,3) = 2009 |
| 2452 |
LOCX(2,3)= 0 |
| 2453 |
LOCX(3,3) = 3667 |
| 2454 |
LOCX(4,3)= 0 |
| 2455 |
LOCX(1,4) = 2243 |
| 2456 |
LOCX(2,4)= 0 |
| 2457 |
LOCX(3,4) = 3541 |
| 2458 |
LOCX(4,4) = 3415 |
| 2459 |
DO 10 IT =1,4 |
| 2460 |
DO 10 ID =1,4 |
| 2461 |
10 ETH(ID,IT) = 0. |
| 2462 |
DO 20 IT=1,2 |
| 2463 |
ETH(1,IT)= 360. |
| 2464 |
20 ETH(2,IT)= 920. |
| 2465 |
DO 30 IT =3,4 |
| 2466 |
30 ETH(1,IT)= 180. |
| 2467 |
RETURN |
| 2468 |
END |
| 2469 |
*CMZ : 0.90/04 11/09/92 05.11.48 by Christian Zeitnitz |
| 2470 |
*-- Author : |
| 2471 |
FUNCTION XSECHE(ID,ITP,EC) |
| 2472 |
#include "cbert2.inc" |
| 2473 |
#include "cxpd.inc" |
| 2474 |
*KEND. |
| 2475 |
C |
| 2476 |
C ID = 1 2 3 4 |
| 2477 |
C SNGL PROD DBLE PROD ELASTIC EXCHANGE |
| 2478 |
C ITP = 1 2 3 4 |
| 2479 |
C PROT NEUT PI+ PI- |
| 2480 |
ET = ETH(ID,ITP) |
| 2481 |
LC =LOCX(ID,ITP) |
| 2482 |
I= IFIX( (EC-ET)/DE + 1.) |
| 2483 |
E = FLOAT(I-1)*DE + ET |
| 2484 |
TEMP = SNGL( CS(I+LC) ) |
| 2485 |
XSECHE=TEMP + (EC-E)/DE * ( SNGL( CS(I+1+LC) ) - TEMP ) |
| 2486 |
RETURN |
| 2487 |
END |
| 2488 |
*CMZ : 0.90/00 27/05/92 16.43.05 by Christian Zeitnitz |
| 2489 |
*-- Author : |
| 2490 |
FUNCTION CZFOI(Z) |
| 2491 |
C** USING REVISED DATA (1-70,TWA) |
| 2492 |
DIMENSION FLI(13) |
| 2493 |
DATA FLI/18.7,42.0,39.0,60.0,68.0,78.0,99.5,98.5,117.0,140.0, |
| 2494 |
1150.0,157.0,163.0/,A1/9.76/,A2/58.8/,XP/-0.19/ |
| 2495 |
IF(Z.GT.13.) GO TO 10 |
| 2496 |
IZ=IFIX(Z) |
| 2497 |
CZFOI=FLI(IZ) |
| 2498 |
RETURN |
| 2499 |
10 CZFOI=A1*Z + A2 *(Z**XP) |
| 2500 |
RETURN |
| 2501 |
END |
| 2502 |
*CMZ : 1.04/03 17/02/95 12.38.47 by Christian Zeitnitz |
| 2503 |
*-- Author : Christian Zeitnitz 21/05/92 |
| 2504 |
SUBROUTINE CHETC(DOSKAL) |
| 2505 |
C************************************************************* |
| 2506 |
C |
| 2507 |
C process intranuclear-cascade and evaporation |
| 2508 |
C call scaling for smooth transition to FLUKA |
| 2509 |
C If H-Atoms present -> special particle-H collision |
| 2510 |
C generate de-exitation gammas |
| 2511 |
C |
| 2512 |
C************************************************************* |
| 2513 |
C |
| 2514 |
C Interface common |
| 2515 |
#include "calgea.inc" |
| 2516 |
*KEND. |
| 2517 |
C |
| 2518 |
C CALOR commons |
| 2519 |
#include "ccomon.inc" |
| 2520 |
#include "ccomn2.inc" |
| 2521 |
#include "ccomn3.inc" |
| 2522 |
#include "cjoint.inc" |
| 2523 |
#include "cxpd.inc" |
| 2524 |
#include "cgeos.inc" |
| 2525 |
#include "chevap.inc" |
| 2526 |
#include "ctncol.inc" |
| 2527 |
#include "crandm.inc" |
| 2528 |
#include "cmass.inc" |
| 2529 |
*KEND. |
| 2530 |
C |
| 2531 |
DIMENSION F(8),PCAP(100,2),NPCOL(12),AP(12),ZP(12) |
| 2532 |
C |
| 2533 |
LOGICAL DOSKAL,INIT |
| 2534 |
INTEGER IBERT |
| 2535 |
SAVE |
| 2536 |
C |
| 2537 |
DATA AP/ 1., 1., 0., 0., 0., 0., 0., 2., 3., 3., 4., 0./ |
| 2538 |
DATA ZP/ 1., 0., 0., 0., 0., 0., 0., 1., 1., 2., 2., 0./ |
| 2539 |
C |
| 2540 |
DATA INIT/.TRUE./ |
| 2541 |
C |
| 2542 |
IF(INIT) THEN |
| 2543 |
IBERT = 0 |
| 2544 |
INIT = .FALSE. |
| 2545 |
ENDIF |
| 2546 |
INTCAL = 12 |
| 2547 |
NO = 1 |
| 2548 |
ATARGT = 0.0 |
| 2549 |
ZTARGT = 0.0 |
| 2550 |
ITYP = IPINC + 1 |
| 2551 |
TIP(1) = FLOAT(IPINC) |
| 2552 |
WT(NO) = 1.0 |
| 2553 |
EC(1) = EINC |
| 2554 |
MAT = 1 |
| 2555 |
MXMAT = 1 |
| 2556 |
NEL(1) = NCEL |
| 2557 |
C copy material data to CALOR |
| 2558 |
DO 10 I=1,NCEL |
| 2559 |
DEN(I,1) = DMED(I) |
| 2560 |
ZZ(I,1) = ZMED(I) |
| 2561 |
A(I,1) = AMED(I) |
| 2562 |
DENH(1) = HDEN |
| 2563 |
10 CONTINUE |
| 2564 |
C calculate x-section for given material |
| 2565 |
CALL CALCXS |
| 2566 |
20 CONTINUE |
| 2567 |
C |
| 2568 |
C --------- start of intranuclear cascade ---------------------- |
| 2569 |
C |
| 2570 |
C |
| 2571 |
R = RANDC(ISEED) |
| 2572 |
IF(E(NO) - 1.0)100,30 ,100 |
| 2573 |
C* PI- CAPTURE ? |
| 2574 |
30 IF(TIP(NO).NE.4) GOTO 100 |
| 2575 |
INTCAL = 18 |
| 2576 |
M=1 |
| 2577 |
LMX=NEL(M) |
| 2578 |
DO 40 L=1,LMX |
| 2579 |
40 PCAP(L,M)=DEN(L,M)*ZZ(L,M) |
| 2580 |
PCAPS=0. |
| 2581 |
DO 50 L=1,LMX |
| 2582 |
50 PCAPS=PCAPS+PCAP(L,M) |
| 2583 |
DO 60 L=1,LMX |
| 2584 |
60 PCAP(L,M)=PCAP(L,M)/PCAPS |
| 2585 |
LMX=NEL(MAT) |
| 2586 |
DO 80 L=1,LMX |
| 2587 |
R0=R |
| 2588 |
R=R-PCAP(L,MAT) |
| 2589 |
IF(R.LE.0.) GO TO 70 |
| 2590 |
GO TO 80 |
| 2591 |
70 LELEM=L |
| 2592 |
GO TO 90 |
| 2593 |
80 CONTINUE |
| 2594 |
CALL CERROR('NMTC$') |
| 2595 |
90 DKWT=1. |
| 2596 |
GO TO 250 |
| 2597 |
100 CONTINUE |
| 2598 |
C |
| 2599 |
IF(ITYP.GE.6) GO TO 220 |
| 2600 |
R = R-HSIGG(ITYP,MAT)/SIGMX(ITYP,MAT) |
| 2601 |
IF(R) 110,110 ,230 |
| 2602 |
110 CONTINUE |
| 2603 |
CZ 10/11/92 SCALING added |
| 2604 |
C scaling selected ? |
| 2605 |
IF(DOSKAL) THEN |
| 2606 |
INC = ITYP - 1 |
| 2607 |
C get H cross-section |
| 2608 |
CALL SHXSEC(EC(1),INC,HEHT,HEHEL,HELNEL) |
| 2609 |
R = RANDC(ISEED) |
| 2610 |
IF(HEHT*DENH(MAT)*1.E 24/HSIGG(ITYP,MAT)-R) 210,120,120 |
| 2611 |
120 CONTINUE |
| 2612 |
ATARGT = 1. |
| 2613 |
ZTARGT = 1. |
| 2614 |
R = RANDC(ISEED) |
| 2615 |
IF(HEHEL/HEHT.GT.R) THEN |
| 2616 |
C ---- elastic |
| 2617 |
CALL CSCATT(INC,EC(NO),KIND,EP,ALPHA,BETA,GAM) |
| 2618 |
NOPART = 2 |
| 2619 |
GOTO 160 |
| 2620 |
ELSE |
| 2621 |
C ---- nonelastic |
| 2622 |
EHICUT = EMAXPI*1000. |
| 2623 |
IF(TIP(NO).LE.1.) EHICUT = EMAXP*1000. |
| 2624 |
CALL SKALEH(IBERT,INC,HEHT,EC(NO),NOPART,KIND,EP,ALPHA, |
| 2625 |
+ BETA,GAM,EHICUT) |
| 2626 |
GOTO 160 |
| 2627 |
ENDIF |
| 2628 |
ELSE |
| 2629 |
CALL GTHSIG(2) |
| 2630 |
R = RANDC(ISEED) |
| 2631 |
IF(HSIG*DENH(MAT)*1.E 24/HSIGG(ITYP,MAT)-R) 210,130,130 |
| 2632 |
130 CONTINUE |
| 2633 |
140 CONTINUE |
| 2634 |
ATARGT = 1.0 |
| 2635 |
ZTARGT = 1.0 |
| 2636 |
UU = 0.0 |
| 2637 |
CALL CPCOL(IBERT,ITYP,HSIG,EC(NO),NOPART,KIND,EP,ALPHA,BETA, |
| 2638 |
+ GAM) |
| 2639 |
C CHANGED NOV.1,1986 |
| 2640 |
IBERT = 1 |
| 2641 |
ENDIF |
| 2642 |
IF(NOPART.LE.0) GO TO 170 |
| 2643 |
DO 150 I=1,NOPART |
| 2644 |
KINDI(I)=KIND(I)+1 |
| 2645 |
IBB=1 |
| 2646 |
IF(KINDI(I).GT.2)IBB=0 |
| 2647 |
IBBARR(I)=IBB |
| 2648 |
150 CONTINUE |
| 2649 |
160 APR = 0.0 |
| 2650 |
ZPR = 0.0 |
| 2651 |
GOTO 190 |
| 2652 |
170 CONTINUE |
| 2653 |
C END OF CHANGE |
| 2654 |
C |
| 2655 |
180 CONTINUE |
| 2656 |
LELEM = 1 |
| 2657 |
APR=A(LELEM,MAT) |
| 2658 |
ZPR =ZZ(LELEM,MAT) |
| 2659 |
190 EX= 0. |
| 2660 |
EREC =0. |
| 2661 |
DO 200 I = 1,6 |
| 2662 |
200 NPART(I) = 0 |
| 2663 |
UU = 0. |
| 2664 |
GOTO 430 |
| 2665 |
210 CONTINUE |
| 2666 |
220 CONTINUE |
| 2667 |
NOPART = -1 |
| 2668 |
GO TO 180 |
| 2669 |
230 NNN = NEL(MAT) |
| 2670 |
DO 240 LEM = 1,NNN |
| 2671 |
LELEM = LEM |
| 2672 |
CZ no hydrogen accepted in BERT ; CZ 2 JUN 92 |
| 2673 |
IF(A(LELEM,MAT) .LT. 2.0) GOTO 240 |
| 2674 |
R = R - SIGG(LEM,MAT)/SIGMX(ITYP,MAT) |
| 2675 |
IF(R) 250,250,240 |
| 2676 |
240 CONTINUE |
| 2677 |
GOTO 220 |
| 2678 |
C------------- elastic neutron-nucleus scattering not implemented ----- |
| 2679 |
C |
| 2680 |
250 ETOT = EINC + PMASS(IPINC+1)*1.E3 |
| 2681 |
CZ |
| 2682 |
CZ check if mass number to low for BERT (A>=4) |
| 2683 |
IF(A(LELEM,MAT).LT.4.0) THEN |
| 2684 |
C |
| 2685 |
CZ 2.95 CALL CERROR('NMTC: A < 4$') |
| 2686 |
CZ set A=4 (brute force, but will work ) |
| 2687 |
A(LELEM,MAT) = 4.0 |
| 2688 |
ENDIF |
| 2689 |
F(1) = A(LELEM,MAT) |
| 2690 |
F(2) = ZZ(LELEM,MAT) |
| 2691 |
F(3) = EC(NO) |
| 2692 |
F(4) = 0.0 |
| 2693 |
F(5) = 1.0 |
| 2694 |
F(6) = 0.0 |
| 2695 |
F(7) = TIP(NO) |
| 2696 |
F(8) = 0.0 |
| 2697 |
C |
| 2698 |
CZ 10/11/92 SCALING added |
| 2699 |
IF(DOSKAL) THEN |
| 2700 |
EHICUT = EMAXPI*1000. |
| 2701 |
IF(TIP(NO).LE.1.) EHICUT = EMAXP*1000. |
| 2702 |
CALL CSKALE(IBERT,F,NOPART,KIND,EP,ALPHA,BETA,GAM,EHICUT, |
| 2703 |
+ RMFAS,EX,EREC) |
| 2704 |
ELSE |
| 2705 |
CALL CABERT(IBERT,F,NOPART,KIND,EP,ALPHA,BETA,GAM) |
| 2706 |
ENDIF |
| 2707 |
IBERT = 1 |
| 2708 |
C |
| 2709 |
IF(NOPART.GT.0) THEN |
| 2710 |
DO 260 I=1,NOPART |
| 2711 |
KINDI(I)=KIND(I)+1 |
| 2712 |
IBB=1 |
| 2713 |
IF(KINDI(I).GT.2) IBB=0 |
| 2714 |
IBBARR(I)=IBB |
| 2715 |
260 CONTINUE |
| 2716 |
ENDIF |
| 2717 |
IF(NOPART.LT.0) THEN |
| 2718 |
C ----------- Pseudo collision ------------------------- |
| 2719 |
C if incident particle pi- with 1 MeV -> repeat BERT, |
| 2720 |
C reason : pi- capture (below cutoff) |
| 2721 |
IF(IPINC.EQ.4 .AND. EINC.EQ.1.0) GO TO 250 |
| 2722 |
C pi- capture ? -> retry |
| 2723 |
IF(EINC.EQ.1.0) GOTO 20 |
| 2724 |
GOTO 420 |
| 2725 |
ELSE IF(NOPART.EQ.0) THEN |
| 2726 |
C ------------------- no particle escaped nucleus ------ |
| 2727 |
GO TO(270,270,280,290,280,290,290),ITYP |
| 2728 |
270 APR = A(LELEM,MAT) + 1. |
| 2729 |
ZPR = ZZ(LELEM,MAT) + 1. - TIP(1) |
| 2730 |
EX = EC(NO) + 7. |
| 2731 |
GO TO 400 |
| 2732 |
280 APR = A(LELEM,MAT) |
| 2733 |
ZPR = ZZ(LELEM,MAT) + 3.- TIP(1) |
| 2734 |
EX= EC(NO) + PMASS(ITYP)*1.E3 |
| 2735 |
GO TO 400 |
| 2736 |
290 CALL CERROR('NMTC: PI0,MU+-$') |
| 2737 |
C ---------------NOPART GT 0 -------------------------- |
| 2738 |
ELSE |
| 2739 |
300 PI0 =0. |
| 2740 |
SUME = 0. |
| 2741 |
PRONO = 0. |
| 2742 |
PIPOS = 0. |
| 2743 |
PINEG = 0. |
| 2744 |
DO 360 N=1,NOPART |
| 2745 |
LK= KIND(N)+1 |
| 2746 |
GO TO(310,350,320,330,340,370,370),LK |
| 2747 |
310 PRONO =PRONO +1. |
| 2748 |
GO TO 350 |
| 2749 |
320 PIPOS = PIPOS +1. |
| 2750 |
GO TO 350 |
| 2751 |
330 PI0 = PI0+1. |
| 2752 |
GO TO 350 |
| 2753 |
340 PINEG= PINEG +1. |
| 2754 |
350 SUME = SUME + EP(N) |
| 2755 |
360 CONTINUE |
| 2756 |
CHGPIS =PIPOS +PINEG |
| 2757 |
FPT = NOPART |
| 2758 |
FPT = FPT -CHGPIS-PI0 |
| 2759 |
IF(TIP(1)-1.) 380,380,390 |
| 2760 |
370 CALL CERROR('NMTC: MU+-$') |
| 2761 |
380 APR=A(LELEM,MAT) + 1. - FPT |
| 2762 |
ZPR= ZZ(LELEM,MAT) + 1. - TIP(1) - PRONO - PIPOS + PINEG |
| 2763 |
IF(ZPR.LT.0.) THEN |
| 2764 |
CALL CERROR(' NMTC: Zpr < 0$') |
| 2765 |
EREC = 0.0 |
| 2766 |
EX = 0.0 |
| 2767 |
ZPR = 0 |
| 2768 |
GOTO 410 |
| 2769 |
ENDIF |
| 2770 |
IF(.NOT.DOSKAL) EX= EINC + (1.-FPT)*7.0-SUME- CHGPIS*PMASS(3)* |
| 2771 |
+ 1.E3-PI0*PMASS(4)*1.E3 |
| 2772 |
GO TO 400 |
| 2773 |
390 APR = A(LELEM,MAT) - FPT |
| 2774 |
ZPR = ZZ(LELEM,MAT)+ 3.-TIP(1)-PRONO-PIPOS + PINEG |
| 2775 |
IF(ZPR.LT.0.) THEN |
| 2776 |
CALL CERROR(' NMTC: Zpr < 0$') |
| 2777 |
EREC = 0.0 |
| 2778 |
ZPR = 0 |
| 2779 |
GOTO 410 |
| 2780 |
ENDIF |
| 2781 |
IF(.NOT.DOSKAL) EX= EINC+(1.-CHGPIS)*PMASS(3)*1.E3-SUME |
| 2782 |
+ -FPT*7.-PI0*PMASS(4)*1.E3 |
| 2783 |
ENDIF |
| 2784 |
C calculate recoil energy of nucleus |
| 2785 |
400 CONTINUE |
| 2786 |
IF(.NOT.DOSKAL) CALL RECOIL |
| 2787 |
410 EX=EX-EREC |
| 2788 |
IF(EX.LT.0.0) EX = 0.0 |
| 2789 |
C |
| 2790 |
C -------- evaporation ------------------------------ |
| 2791 |
C |
| 2792 |
CALL CERUP |
| 2793 |
C ------------------ fill return variables ------------- |
| 2794 |
420 CONTINUE |
| 2795 |
IBERT = 1 |
| 2796 |
430 CONTINUE |
| 2797 |
CZ set target nucleus |
| 2798 |
IF(ATARGT.EQ.0.0) THEN |
| 2799 |
ATARGT = A(LELEM,MAT) |
| 2800 |
ZTARGT = ZZ(LELEM,MAT) |
| 2801 |
ENDIF |
| 2802 |
EXMED = EX |
| 2803 |
IF(APR.GE.0 .AND. ZPR.GE.0) THEN |
| 2804 |
ERMED(1) = EREC |
| 2805 |
AMED(1) = APR |
| 2806 |
ZMED(1) = ZPR |
| 2807 |
NRECOL = 1 |
| 2808 |
ELSE |
| 2809 |
AMED(1) = 0.0 |
| 2810 |
ZMED(1) = 0.0 |
| 2811 |
ERMED(1) = 0.0 |
| 2812 |
NRECOL = 0 |
| 2813 |
ENDIF |
| 2814 |
IF(NOPART.LT.0) THEN |
| 2815 |
C Pseudo collision |
| 2816 |
NCOL = 5 |
| 2817 |
NPHETC = 0 |
| 2818 |
EKINET(1) = EINC |
| 2819 |
IPCAL(1) = IPINC |
| 2820 |
CALTIM(1) = 0.0 |
| 2821 |
UCAL(1,1) = UINC(1) |
| 2822 |
UCAL(1,2) = UINC(2) |
| 2823 |
UCAL(1,3) = UINC(3) |
| 2824 |
EXMED = 0.0 |
| 2825 |
NRECOL = 1 |
| 2826 |
ERMED(1) = 0.0 |
| 2827 |
INTCAL = 24 |
| 2828 |
AMED(1) = A(LELEM,MAT) |
| 2829 |
ZMED(1) = ZZ(LELEM,MAT) |
| 2830 |
ELSE |
| 2831 |
C get particles from intranuclear cascade |
| 2832 |
NCOL = 2 |
| 2833 |
NPHETC = 0 |
| 2834 |
AMED(1) = APR |
| 2835 |
ZMED(1) = ZPR |
| 2836 |
IF(NOPART.GT.0) THEN |
| 2837 |
DO 440 I=1,NOPART |
| 2838 |
NPHETC = NPHETC + 1 |
| 2839 |
IF(NPHETC.GT.MXCP) NPHETC=MXCP |
| 2840 |
EKINET(NPHETC) = EP(I) |
| 2841 |
IPCAL(NPHETC) = KIND(I) |
| 2842 |
CALTIM(NPHETC) = 0.0 |
| 2843 |
C transformation into Lab ssystem |
| 2844 |
CALL CB2LAB(ALPHA(I),BETA(I),GAM(I), UINC(1),UINC(2), |
| 2845 |
+ UINC(3),UCAL(NPHETC,1),UCAL(NPHETC,2),UCAL(NPHETC,3)) |
| 2846 |
440 CONTINUE |
| 2847 |
ENDIF |
| 2848 |
C get evaporated neutrons |
| 2849 |
IF(NPART(1).GT.0) THEN |
| 2850 |
DO 450 I=1,NPART(1) |
| 2851 |
NPHETC = NPHETC + 1 |
| 2852 |
IF(NPHETC.GT.MXCP) NPHETC=MXCP |
| 2853 |
EKINET(NPHETC) = EPART(I,1) |
| 2854 |
IPCAL(NPHETC) = 1 |
| 2855 |
CALTIM(NPHETC) = 0.0 |
| 2856 |
CALL GTISO(ALP,BET,CAM) |
| 2857 |
UCAL(NPHETC,1) = ALP |
| 2858 |
UCAL(NPHETC,2) = BET |
| 2859 |
UCAL(NPHETC,3) = CAM |
| 2860 |
450 CONTINUE |
| 2861 |
ENDIF |
| 2862 |
C get evaporated protons |
| 2863 |
IF(NPART(2).GT.0) THEN |
| 2864 |
DO 460 I=1,NPART(2) |
| 2865 |
NPHETC = NPHETC + 1 |
| 2866 |
IF(NPHETC.GT.MXCP) NPHETC=MXCP |
| 2867 |
EKINET(NPHETC) = EPART(I,2) |
| 2868 |
IPCAL(NPHETC) = 0 |
| 2869 |
CALTIM(NPHETC) = 0.0 |
| 2870 |
CALL GTISO(ALP,BET,CAM) |
| 2871 |
UCAL(NPHETC,1) = ALP |
| 2872 |
UCAL(NPHETC,2) = BET |
| 2873 |
UCAL(NPHETC,3) = CAM |
| 2874 |
460 CONTINUE |
| 2875 |
ENDIF |
| 2876 |
C get evaporated heavy particles (alpha,deuteron, triton, He3) |
| 2877 |
C particle type 10 7 8 9 |
| 2878 |
DO 480 I=3,6 |
| 2879 |
IF(NPART(I).GT.0) THEN |
| 2880 |
DO 470 K=1,NPART(I) |
| 2881 |
NPHETC = NPHETC + 1 |
| 2882 |
IF(NPHETC.GT.MXCP) NPHETC=MXCP |
| 2883 |
EKINET(NPHETC) = HEPART(K,I-2) |
| 2884 |
IPCAL(NPHETC) = I + 4 |
| 2885 |
CALTIM(NPHETC) = 0.0 |
| 2886 |
CALL GTISO(ALP,BET,CAM) |
| 2887 |
UCAL(NPHETC,1) = ALP |
| 2888 |
UCAL(NPHETC,2) = BET |
| 2889 |
UCAL(NPHETC,3) = CAM |
| 2890 |
470 CONTINUE |
| 2891 |
ENDIF |
| 2892 |
480 CONTINUE |
| 2893 |
C generate de-exitation gammas |
| 2894 |
C |
| 2895 |
IF(UU.GT.0.0) THEN |
| 2896 |
EEX = UU |
| 2897 |
EGTOT = 0.0 |
| 2898 |
490 CONTINUE |
| 2899 |
EGAM = EEX * RANDC(ISEED) |
| 2900 |
IF((EGTOT+EGAM) .GT. EEX) THEN |
| 2901 |
EGAM = EEX - EGTOT |
| 2902 |
EEX = 0.0 |
| 2903 |
ENDIF |
| 2904 |
EGTOT = EGTOT + EGAM |
| 2905 |
CALL AZIRN(SINA,COSA) |
| 2906 |
COSP = SFLRAF(DUM) |
| 2907 |
SINP = SQRT(1.0-COSP*COSP) |
| 2908 |
NPHETC = NPHETC + 1 |
| 2909 |
IF(NPHETC.GT.MXCP) NPHETC=MXCP |
| 2910 |
EKINET(NPHETC) = EGAM |
| 2911 |
UCAL(NPHETC,1) = SINP * COSA |
| 2912 |
UCAL(NPHETC,2) = SINP * SINA |
| 2913 |
UCAL(NPHETC,3) = COSP |
| 2914 |
IPCAL(NPHETC) = 11 |
| 2915 |
CALTIM(NPHETC) = 0.0 |
| 2916 |
IF(EEX.GT.0.0) GOTO 490 |
| 2917 |
ENDIF |
| 2918 |
ENDIF |
| 2919 |
RETURN |
| 2920 |
END |
| 2921 |
*CMZ : 1.01/04 10/06/93 14.43.37 by Christian Zeitnitz |
| 2922 |
*-- Author : |
| 2923 |
SUBROUTINE CABRAN(K1) |
| 2924 |
C |
| 2925 |
#include "crandm.inc" |
| 2926 |
*KEND. |
| 2927 |
C |
| 2928 |
#include "cbert.inc" |
| 2929 |
*KEND. |
| 2930 |
C |
| 2931 |
VALUE1 = RANDC(ISEED) |
| 2932 |
VALUE1=VALUE1*SIGN |
| 2933 |
VALUE2=0.0 |
| 2934 |
NOT=1 |
| 2935 |
DO10 I=2,K1 |
| 2936 |
VALUE2=CE(I)+VALUE2 |
| 2937 |
IF(VALUE2-VALUE1)10,20,20 |
| 2938 |
10 NOT=NOT+1 |
| 2939 |
20 RETURN |
| 2940 |
C VALUE2=SUM OF CE FOR A PARTICULAR REGION--SUM F(I1)MASS |
| 2941 |
END |
| 2942 |
*CMZ : 0.92/00 02/12/92 16.02.23 by Christian Zeitnitz |
| 2943 |
*-- Author : |
| 2944 |
SUBROUTINE CALP19 |
| 2945 |
#include "crandm.inc" |
| 2946 |
#include "cbert.inc" |
| 2947 |
*KEND. |
| 2948 |
SAVE |
| 2949 |
C |
| 2950 |
C |
| 2951 |
UNIV = RANDC(ISEED) |
| 2952 |
PT(2)=1.0 |
| 2953 |
PT(26)=1.0 |
| 2954 |
PT(14)=3.0 |
| 2955 |
PT(16)=POMS |
| 2956 |
IF(ISW(12))10,10,140 |
| 2957 |
10 IF(UNIV-.25)20,20,110 |
| 2958 |
20 IF(ISW(4))40,30,40 |
| 2959 |
30 PT(2)=2.0 |
| 2960 |
40 UNIV = RANDC(ISEED) |
| 2961 |
IF(UNIV-6.6666667D-1)50,50,90 |
| 2962 |
50 PT(14)=4.0 |
| 2963 |
60 IF(ISW(4))80,70,80 |
| 2964 |
70 PT(26)=2.0 |
| 2965 |
80 GO TO 240 |
| 2966 |
90 PT(16)=PNMS |
| 2967 |
IF(ISW(4))70,100,70 |
| 2968 |
100 PT(14)=5.0 |
| 2969 |
GOTO80 |
| 2970 |
110 IF(ISW(4))130,120,130 |
| 2971 |
120 PT(26)=2.0 |
| 2972 |
GOTO90 |
| 2973 |
130 PT(2)=2.0 |
| 2974 |
PT(16)=PNMS |
| 2975 |
GOTO80 |
| 2976 |
140 IF(UNIV-.5)150,150,190 |
| 2977 |
150 IF(ISW(4))160,170,160 |
| 2978 |
160 PT(2)=2.0 |
| 2979 |
170 UNIV = RANDC(ISEED) |
| 2980 |
IF(UNIV-3.3333333D-1)90,90,180 |
| 2981 |
180 PT(14)=4.0 |
| 2982 |
GOTO60 |
| 2983 |
190 IF(ISW(4))210,200,210 |
| 2984 |
200 PT(2)=2.0 |
| 2985 |
210 UNIV = RANDC(ISEED) |
| 2986 |
IF(UNIV-6.6666667D-1)220,220,230 |
| 2987 |
220 PT(14)=4.0 |
| 2988 |
IF(ISW(4))70,80,70 |
| 2989 |
230 PT(16)=PNMS |
| 2990 |
IF(ISW(4))100,70,100 |
| 2991 |
240 RETURN |
| 2992 |
END |
| 2993 |
*CMZ : 0.92/00 02/12/92 16.02.24 by Christian Zeitnitz |
| 2994 |
*-- Author : |
| 2995 |
SUBROUTINE CALP28 |
| 2996 |
#include "cbert.inc" |
| 2997 |
#include "crandm.inc" |
| 2998 |
*KEND. |
| 2999 |
REAL *8 R |
| 3000 |
C |
| 3001 |
SAVE |
| 3002 |
C |
| 3003 |
R = RANDC(ISEED) |
| 3004 |
IF(ISW(13))230,10,230 |
| 3005 |
10 IF(R-6.0D-1)20,20,120 |
| 3006 |
20 PT(4)=PNMS |
| 3007 |
R = RANDC(ISEED) |
| 3008 |
IF(ISW(4))30,90,30 |
| 3009 |
30 IF(R-3.3333333D-1)40,40,70 |
| 3010 |
40 PT(26)=5.0 |
| 3011 |
50 PT(28)=PNMS |
| 3012 |
60 RETURN |
| 3013 |
70 PT(26)=4.0 |
| 3014 |
80 PT(38)=2.0 |
| 3015 |
GO TO 60 |
| 3016 |
90 PT(2)=5.0 |
| 3017 |
PT(14)=2.0 |
| 3018 |
IF(R-3.3333333D-1)100,100,110 |
| 3019 |
100 PT(28)=PNMS |
| 3020 |
GO TO 80 |
| 3021 |
110 PT(26)=4.0 |
| 3022 |
GO TO 60 |
| 3023 |
120 R = RANDC(ISEED) |
| 3024 |
IF(ISW(4))130,180,130 |
| 3025 |
130 IF(R-6.6666667D-1)140,140,160 |
| 3026 |
140 PT(2)=4.0 |
| 3027 |
150 R = RANDC(ISEED) |
| 3028 |
IF(R-6.6666667D-1)110,110,100 |
| 3029 |
160 PT(14)=2.0 |
| 3030 |
170 PT(4)=PNMS |
| 3031 |
GO TO 150 |
| 3032 |
180 IF(R-6.6666667D-1)190,190,220 |
| 3033 |
190 PT(2)=4.0 |
| 3034 |
200 PT(14)=2.0 |
| 3035 |
210 R = RANDC(ISEED) |
| 3036 |
IF(R-6.6666667D-1)70,70,40 |
| 3037 |
220 PT(2)=5.0 |
| 3038 |
PT(4)=PNMS |
| 3039 |
GO TO 210 |
| 3040 |
230 IF(R-VALUE1)240,240,270 |
| 3041 |
240 PT(4)=PNMS |
| 3042 |
IF(ISW(4))260,250,260 |
| 3043 |
250 PT(2)=5.0 |
| 3044 |
PT(14)=2.0 |
| 3045 |
GO TO 50 |
| 3046 |
260 PT(38)=2.0 |
| 3047 |
GO TO 40 |
| 3048 |
270 R = RANDC(ISEED) |
| 3049 |
IF(ISW(4))280,310,280 |
| 3050 |
280 IF(R-3.3333333D-1)290,290,300 |
| 3051 |
290 PT(4)=PNMS |
| 3052 |
GO TO 200 |
| 3053 |
300 PT(2)=4.0 |
| 3054 |
GOTO210 |
| 3055 |
310 IF(R-3.3333333D-1)320,320,330 |
| 3056 |
320 PT(2)=5.0 |
| 3057 |
GOTO170 |
| 3058 |
330 PT(14)=2.0 |
| 3059 |
GOTO140 |
| 3060 |
END |
| 3061 |
*CMZ : 0.92/00 02/12/92 16.02.24 by Christian Zeitnitz |
| 3062 |
*-- Author : |
| 3063 |
SUBROUTINE CALPHA |
| 3064 |
#include "cbert.inc" |
| 3065 |
#include "crandm.inc" |
| 3066 |
*KEND. |
| 3067 |
SAVE |
| 3068 |
C |
| 3069 |
UNIV = RANDC(ISEED) |
| 3070 |
IF(VALUE3)300,10,140 |
| 3071 |
10 IF(UNIV-VALUE1)20,20,120 |
| 3072 |
20 IF(ISW(11))40,30,40 |
| 3073 |
30 PT(2)=5.0 |
| 3074 |
PT(26)=2.0 |
| 3075 |
40 PT(4)=PNMS |
| 3076 |
PM(4)=PNMS |
| 3077 |
UNIV = RANDC(ISEED) |
| 3078 |
IF(UNIV-VALUE2)50,50,70 |
| 3079 |
50 PT(14)=4.0 |
| 3080 |
60 RETURN |
| 3081 |
70 IF(ISW(11))110,80,110 |
| 3082 |
80 PT(26)=1.0 |
| 3083 |
90 PT(14)=5.0 |
| 3084 |
100 PT(16)=PNMS |
| 3085 |
GO TO 60 |
| 3086 |
110 PT(26)=2.0 |
| 3087 |
GO TO 100 |
| 3088 |
120 PT(2)=4.0 |
| 3089 |
IF(ISW(11))100,130,100 |
| 3090 |
130 PT(14)=5.0 |
| 3091 |
GO TO 110 |
| 3092 |
140 IF(UNIV-VALUE1)150,150,200 |
| 3093 |
150 PM(4)=PNMS |
| 3094 |
IF(ISW(11))160,190,160 |
| 3095 |
160 PT(2)=5.0 |
| 3096 |
170 PT(16)=PNMS |
| 3097 |
180 PT(4)=PNMS |
| 3098 |
GO TO 60 |
| 3099 |
190 PT(14)=5.0 |
| 3100 |
PT(26)=2.0 |
| 3101 |
GO TO 170 |
| 3102 |
200 IF(UNIV-VALUE2)210,210,250 |
| 3103 |
210 PT(2)=4.0 |
| 3104 |
UNIV = RANDC(ISEED) |
| 3105 |
IF(UNIV-VALUE3)240,240,220 |
| 3106 |
220 IF(ISW(11))50,230,50 |
| 3107 |
230 PT(26)=2.0 |
| 3108 |
GO TO 50 |
| 3109 |
240 IF(ISW(11))110,90,110 |
| 3110 |
250 PM(4)=PNMS |
| 3111 |
PT(4)=PNMS |
| 3112 |
UNIV = RANDC(ISEED) |
| 3113 |
IF(UNIV-6.6666667D-1)260,260,280 |
| 3114 |
260 IF(ISW(11))230,270,230 |
| 3115 |
270 PT(2)=5.0 |
| 3116 |
GO TO 50 |
| 3117 |
280 IF(ISW(11))90,290,90 |
| 3118 |
290 PT(26)=2.0 |
| 3119 |
GO TO 160 |
| 3120 |
300 IF(UNIV-VALUE1)310,310,340 |
| 3121 |
310 PM(4)=PNMS |
| 3122 |
PT(4)=PNMS |
| 3123 |
UNIV = RANDC(ISEED) |
| 3124 |
IF(VALUE3+1.0)330,320,330 |
| 3125 |
320 IF(UNIV-3.3333333D-1)90,90,230 |
| 3126 |
330 PT(2)=5.0 |
| 3127 |
IF(UNIV-3.3333333D-1)110,110,50 |
| 3128 |
340 IF(UNIV-VALUE2)350,350,380 |
| 3129 |
350 PT(2)=4.0 |
| 3130 |
UNIV = RANDC(ISEED) |
| 3131 |
IF(VALUE3+1.0)370,360,370 |
| 3132 |
360 IF(UNIV-6.6666667D-1)50,50,110 |
| 3133 |
370 IF(UNIV-6.6666667D-1)230,230,90 |
| 3134 |
380 PM(4)=PNMS |
| 3135 |
PT(4)=PNMS |
| 3136 |
IF(VALUE3+1.0)390,160,390 |
| 3137 |
390 PT(14)=5.0 |
| 3138 |
GOTO110 |
| 3139 |
END |
| 3140 |
*CMZ : 0.92/00 02/12/92 16.02.24 by Christian Zeitnitz |
| 3141 |
*-- Author : |
| 3142 |
SUBROUTINE CANGID |
| 3143 |
#include "cbert.inc" |
| 3144 |
#include "crandm.inc" |
| 3145 |
*KEND. |
| 3146 |
REAL*8 R,TESISO |
| 3147 |
SAVE |
| 3148 |
C |
| 3149 |
C ****************************************************************** |
| 3150 |
C**** CALCULATES COS AND SIN THETA,SIN AND COS PHI ************** |
| 3151 |
C ****************************************************************** |
| 3152 |
ICURR = CURR(1) |
| 3153 |
GO TO(10,10,30,30,30),ICURR |
| 3154 |
C**** INCIDENT PARTICLE - NUCLEON |
| 3155 |
10 IF(IT.EQ.21.OR.IT.EQ.22)GO TO 20 |
| 3156 |
C**** SINGLE PRODUCTION |
| 3157 |
IF(RLKE.GT.3500.0D0) CALL CERROR('CANGID1$') |
| 3158 |
IF(RLKE.LT.500.0D0)GO TO 70 |
| 3159 |
TESISO= 0.75D0 |
| 3160 |
IF(RLKE.LT.1000.0D0)GO TO 50 |
| 3161 |
TESISO= 0.5D0 |
| 3162 |
IF(RLKE.LT.1300.0D0)GO TO 50 |
| 3163 |
TESISO= 0.25D0 |
| 3164 |
IF(RLKE.LT.2500.0D0)GO TO 50 |
| 3165 |
GO TO 60 |
| 3166 |
C**** DOUBLE PRODUCTION |
| 3167 |
20 IF(RLKE.GT.3500.0D0) CALL CERROR('CANGID2$') |
| 3168 |
GO TO 60 |
| 3169 |
C**** INCIDENT PARTICLE-PION |
| 3170 |
30 R = RANDC(ISEED) |
| 3171 |
IF(RLKE.GT.2500.0D0) CALL CERROR('CANGID3$') |
| 3172 |
CST= -0.9999995D0 |
| 3173 |
SNT= 0.003162D0 |
| 3174 |
IF(IT.NE.11)GO TO 40 |
| 3175 |
IF(R.LE.0.75D0)GO TO 70 |
| 3176 |
GO TO 80 |
| 3177 |
C**** (PI+)-(P),(PI-)-(N) |
| 3178 |
C**** (PI0)-(N),(PI0)-(P) |
| 3179 |
40 IF(IT.NE.12.AND.IT.NE.28) CALL CERROR('CANGID4$') |
| 3180 |
IF(RLKE.LT.500.0D0)CST=-CST |
| 3181 |
IF(R.LE.0.80D0)GO TO 70 |
| 3182 |
GO TO 80 |
| 3183 |
50 R = RANDC(ISEED) |
| 3184 |
IF(R.LE.TESISO)GO TO 70 |
| 3185 |
C**** BACKWARD/FORWARD |
| 3186 |
60 R = RANDC(ISEED) |
| 3187 |
C**** TEST FOR DIRECTION |
| 3188 |
CST= 0.9999995D0 |
| 3189 |
SNT= 0.003162D0 |
| 3190 |
IF(R.LE.0.5)GO TO 80 |
| 3191 |
CST= -0.9999995D0 |
| 3192 |
GO TO 80 |
| 3193 |
C**** ISOTROPIC |
| 3194 |
70 CALL CAPOL1(CST,SNT) |
| 3195 |
C**** CALCULATES COS,SIN PHI |
| 3196 |
80 CALL CAAZIO(SOPC,SOPS) |
| 3197 |
RETURN |
| 3198 |
END |
| 3199 |
*CMZ : 0.92/00 02/12/92 16.02.24 by Christian Zeitnitz |
| 3200 |
*-- Author : |
| 3201 |
SUBROUTINE CAAZIO(SINE,COSINE) |
| 3202 |
C |
| 3203 |
#include "crandm.inc" |
| 3204 |
*KEND. |
| 3205 |
REAL * 8 SINE,COSINE,R1,R2,R1SQ,R2SQ,SUM |
| 3206 |
C |
| 3207 |
10 R1 = RANDC(ISEED) |
| 3208 |
R1SQ = R1 * R1 |
| 3209 |
C XSQ |
| 3210 |
R2 = RANDC(ISEED) |
| 3211 |
R2SQ = R2 * R2 |
| 3212 |
C YSQ |
| 3213 |
SUM = R1SQ + R2SQ |
| 3214 |
IF(SUM.GT.1.0) GO TO 10 |
| 3215 |
SUM = SUM * 0.5 |
| 3216 |
C (XSQ+YSQ)/2 |
| 3217 |
COSINE = (SUM-R1SQ) / SUM |
| 3218 |
C (YSQ-XSQ)/(XSQ+YSQ) |
| 3219 |
SINE = (R1*R2) / SUM |
| 3220 |
C (2*X*Y)/(XSQ+YSQ) |
| 3221 |
R1 = RANDC(ISEED) |
| 3222 |
IF(R1.LT.0.5) GO TO 20 |
| 3223 |
SINE = -SINE |
| 3224 |
20 RETURN |
| 3225 |
END |
| 3226 |
*CMZ : 1.01/04 10/06/93 14.43.37 by Christian Zeitnitz |
| 3227 |
*-- Author : Christian Zeitnitz 21/05/92 |
| 3228 |
SUBROUTINE CB2LAB(ALPHA,BETA,GAM,U,V,W,ULAB,VLAB,WLAB) |
| 3229 |
C*************************************************************** |
| 3230 |
C |
| 3231 |
C convert direction cosines of paticles produced in BERT |
| 3232 |
C into Lab system |
| 3233 |
C |
| 3234 |
C input: ALPHA,BETA,GAM : direction consine in BERT |
| 3235 |
C u,v,w : direction cosines in Lab system of |
| 3236 |
C the projectile |
| 3237 |
C output:ulab,vlab,wlab : direction cosine in Lab system |
| 3238 |
C |
| 3239 |
C |
| 3240 |
C************************************************************** |
| 3241 |
C |
| 3242 |
RT = SQRT(U*U + V*V) |
| 3243 |
if(RT.EQ.0.0) THEN |
| 3244 |
SINTH = 0.0 |
| 3245 |
COSTH = 1.0 |
| 3246 |
COSPHI = 1.0 |
| 3247 |
SINPHI = 0.0 |
| 3248 |
ELSE |
| 3249 |
SINTH = RT |
| 3250 |
COSTH = W |
| 3251 |
COSPHI = U/RT |
| 3252 |
SINPHI = V/RT |
| 3253 |
ENDIF |
| 3254 |
T1 = COSTH * ALPHA + SINTH * GAM |
| 3255 |
ULAB = COSPHI * T1 - SINPHI * BETA |
| 3256 |
VLAB = SINPHI * T1 + COSPHI * BETA |
| 3257 |
WLAB = COSTH * GAM - SINTH * ALPHA |
| 3258 |
C |
| 3259 |
C U = COSPHI*COSTH* ALPHA -SINPHI* BETA +COSPHI*SINTH* GAMA |
| 3260 |
C |
| 3261 |
C V = SINPHI*COSTH* ALPHA +COSPHI* BETA +SINPHI*SINTH* GAMA |
| 3262 |
C |
| 3263 |
C W = -SINTH* ALPHA + 0. * BETA +COSTH* GAMA |
| 3264 |
C ROTATION MATRIX |
| 3265 |
RETURN |
| 3266 |
END |
| 3267 |
*CMZ : 0.92/04 11/12/92 12.04.27 by Christian Zeitnitz |
| 3268 |
*-- Author : |
| 3269 |
SUBROUTINE CBBBBB |
| 3270 |
#include "cbert.inc" |
| 3271 |
*KEND. |
| 3272 |
SAVE |
| 3273 |
C |
| 3274 |
I=I2 |
| 3275 |
C COLLISION CUT-OFF ENERGY (PROTON) |
| 3276 |
IF(I1)10,20,10 |
| 3277 |
10 I=I+3 |
| 3278 |
C COLLISION CUT-OFF ENERGY (NEUTRON) |
| 3279 |
20 IF(KNOT-6)40,40,30 |
| 3280 |
30 IF(KNOT-12)50,50,40 |
| 3281 |
40 CLCFE=CFEPN(I) |
| 3282 |
50 E(1)=WKRPN(I)*RCPMV+PM(1) |
| 3283 |
C TOTAL ENERGY PARTICLE 1 |
| 3284 |
60 IF(IN)80,70,80 |
| 3285 |
70 CALLP1CLI |
| 3286 |
GOTO90 |
| 3287 |
80 CALL P1CLC |
| 3288 |
C P1OE1=CURRENT=MOMENT/TOTAL |
| 3289 |
90 RETURN |
| 3290 |
END |
| 3291 |
*CMZ : 1.01/04 10/06/93 14.43.37 by Christian Zeitnitz |
| 3292 |
*-- Author : |
| 3293 |
SUBROUTINE CABERT(IBERT,FINPUT,NOPART,KIND,ERAY,ARAY,BRAY,GRAY) |
| 3294 |
C************************************************************************* |
| 3295 |
C |
| 3296 |
C calculate collision of particle with nucleus |
| 3297 |
C |
| 3298 |
C input: Finput(1) = A of nucleus |
| 3299 |
C Finput(2) = Z of nucleus |
| 3300 |
C Finput(3) = Ekin of incident particle |
| 3301 |
C Finput(4) = energy cut off used in intranuclear cascade default = 0 |
| 3302 |
C Finput(5) = No. of incident particles = 1.0 |
| 3303 |
C Finput(6) = Angular distance |
| 3304 |
C Finput(7) = particle type a la CALOR + 1 |
| 3305 |
C Finput(8) = same as Finput(4) |
| 3306 |
C |
| 3307 |
C output:NOPART > 0 -> no. of particles generated |
| 3308 |
C = 0 -> collision with no escaping particle |
| 3309 |
C = -1 -> pseudo collision |
| 3310 |
C KIND(1-NOPART) -> particle type |
| 3311 |
C ERAY(1-NOPART) -> kinetic energy |
| 3312 |
C A,B,GRAY(1-NOPART) -> direction cosine (x,y,z-axis) |
| 3313 |
C incident particle with GRAY = 1 !!! |
| 3314 |
C |
| 3315 |
C************************************************************************* |
| 3316 |
C |
| 3317 |
DIMENSION FINPUT(*),KIND(*),ERAY(*),ARAY(*),BRAY(*),GRAY(*) |
| 3318 |
C |
| 3319 |
C A.C.3526(3410-44) CASCADE CALCULATION |
| 3320 |
C |
| 3321 |
#include "crandm.inc" |
| 3322 |
#include "cjoint.inc" |
| 3323 |
#include "cinout.inc" |
| 3324 |
#include "cbert.inc" |
| 3325 |
#include "crn.inc" |
| 3326 |
#include "cmunpu.inc" |
| 3327 |
#include "crun.inc" |
| 3328 |
*KEND. |
| 3329 |
REAL*8 DCLN(80) , DCIN(115) , PPAC(19) , POAC(19) , FMXSN(161), |
| 3330 |
+ FMXDN(130), FMXSP(117), PDCI(60) , PDCH(55) , DCHN(143) , |
| 3331 |
+ DCHNA(36) , DCHNB(60) , PSPCL(158), PDPCL(130), SPCLN(158), |
| 3332 |
+ DPCLN(130), FSLN(176) , FRINN(161), DMIN(101) , PPSCL(117), |
| 3333 |
+ PNSCL(117), PMSCL(117), PNNSL(117), PCFSL(234), FRIPN(117), |
| 3334 |
+ PNMI(101) , PNFSL(234), PNEC(126) , PNNEC(126), PMXC(126) , |
| 3335 |
+ PMEC(126) , PPEC(126) , PEC(176) , ECN(176) , PPDC(6426), |
| 3336 |
+ PMDD(6426), PMDX(6426), PNDD(6426) |
| 3337 |
DIMENSION ICC(12) |
| 3338 |
REAL * 8 ZERO,XINC |
| 3339 |
EQUIVALENCE (TAPCRS(1),DCLN(1)) , (TAPCRS(81),DCIN(1)) , |
| 3340 |
+ (TAPCRS(196),PPAC(1)) , (TAPCRS(215),POAC(1)) , |
| 3341 |
+ (TAPCRS(234),FMXSN(1)) , (TAPCRS(395),FMXDN(1)) , |
| 3342 |
+ (TAPCRS(525),FMXSP(1)) , (TAPCRS(642),PDCI(1)) , |
| 3343 |
+ (TAPCRS(702),PDCH(1)) , (TAPCRS(757),DCHN(1)) , |
| 3344 |
+ (TAPCRS(900),DCHNA(1)) , (TAPCRS(936),DCHNB(1)) , |
| 3345 |
+ (TAPCRS(996),PSPCL(1)) , (TAPCRS(1154),PDPCL(1)), |
| 3346 |
+ (TAPCRS(1284),SPCLN(1)), (TAPCRS(1442),DPCLN(1)), |
| 3347 |
+ (TAPCRS(1572),FSLN(1)) , (TAPCRS(1748),FRINN(1)), |
| 3348 |
+ (TAPCRS(1909),DMIN(1)) , (TAPCRS(2010),PPSCL(1)) |
| 3349 |
EQUIVALENCE (TAPCRS(2127),PNSCL(1)), (TAPCRS(2244),PMSCL(1)), |
| 3350 |
+ (TAPCRS(2361),PNNSL(1)), (TAPCRS(2478),PCFSL(1)), |
| 3351 |
+ (TAPCRS(2712),FRIPN(1)), (TAPCRS(2829),PNMI(1)) , |
| 3352 |
+ (TAPCRS(2930),PNFSL(1)), (TAPCRS(3164),PNEC(1)) , |
| 3353 |
+ (TAPCRS(3290),PNNEC(1)), (TAPCRS(3416),PMXC(1)) , |
| 3354 |
+ (TAPCRS(3542),PMEC(1)) , (TAPCRS(3668),PPEC(1)) , |
| 3355 |
+ (TAPCRS(3794),PEC(1)) , (TAPCRS(3970),ECN(1)) , |
| 3356 |
+ (TAPCRS(4146),PPDC(1)) , (TAPCRS(10572),PMDD(1)), |
| 3357 |
+ (TAPCRS(16998),PMDX(1)), (TAPCRS(23424),PNDD(1)) |
| 3358 |
C |
| 3359 |
SAVE |
| 3360 |
AMASNO =DBLE(FINPUT(1)) |
| 3361 |
ZEE = DBLE(FINPUT(2)) |
| 3362 |
EINC = DBLE(FINPUT(3)) |
| 3363 |
CTOFE = DBLE(FINPUT(4)) |
| 3364 |
CASESN = DBLE(FINPUT(5)) |
| 3365 |
ANDIT = DBLE(FINPUT(6)) |
| 3366 |
CTOFEN = DBLE(FINPUT(8)) |
| 3367 |
PRTIN = FINPUT(7) |
| 3368 |
KE = 0 |
| 3369 |
IF(IBERT)40,10,40 |
| 3370 |
C CHANGED SEPT.1,1987 |
| 3371 |
10 CONTINUE |
| 3372 |
CZ BERT dataset already read by CRBERT called by CALINI 19. june 92 |
| 3373 |
NRT = 0 |
| 3374 |
SF =1. |
| 3375 |
C SF=1.0 AT PRESENT |
| 3376 |
LN=2 |
| 3377 |
C NOR=RECORD NUMBER |
| 3378 |
C NRT=NUMBER OF FILES |
| 3379 |
RANDI(1)=16896 |
| 3380 |
PNMS=.708D13 |
| 3381 |
C PI+ OR - MASS IN RECIP. CM |
| 3382 |
DNCMS=4.758D13 |
| 3383 |
SQNM=DNCMS*DNCMS |
| 3384 |
C NUCLEON MASS SQUARED |
| 3385 |
C NUCLEON MASS IN RECIP. CM |
| 3386 |
RCPMV=.50613D11 |
| 3387 |
C RECIPROCAL CM PER MV |
| 3388 |
POMS=.684D13 |
| 3389 |
C PI0 MASS IN RECIP. CM |
| 3390 |
IFIVE=5 |
| 3391 |
ISIX=6 |
| 3392 |
ZERO=0.0 |
| 3393 |
NE=0 |
| 3394 |
BEGRU = 0.0 |
| 3395 |
DO 20 I=1,3 |
| 3396 |
20 XI(I)=0.0 |
| 3397 |
DO 30 I=1,19 |
| 3398 |
POAC(I)=POAC(I)+POAC(I) |
| 3399 |
30 PPAC(I)=PPAC(I)/SF |
| 3400 |
C P0AC(19),PPAC(19) |
| 3401 |
C SF IS A SCALE FACTOR SUBJECT TO CHANGE |
| 3402 |
C ANDIT |
| 3403 |
C ISOBAR ANGULAR DISTRIBUTION 0,50 PERCENT ISOTROPIC 50 |
| 3404 |
C PERCENT FORWARD-BACKWARD-1,ALL ISOTROPIC-2,ALL FORWARD-BACKWARD |
| 3405 |
C =0,ALL OF WORD IN CRDET TO BE CONSIDERED. NOT 0, ONLY PART. INPT |
| 3406 |
C ESCAPING PARTICLE STORAGE ESPS |
| 3407 |
C NUMBER OF FORBIDDEN COLLISIONS FOR NEUTRONS FCN |
| 3408 |
C NUMBER OF FORBIDDEN COLLISIONS FOR PROTONS FCP |
| 3409 |
C PARTICLE WITH VELOCITY LESS THAN CRITERION PLVC |
| 3410 |
C PARTICLE WITH VELOCITY GREATER THAN CRITERION PGVC |
| 3411 |
40 DO 50 I=1,60 |
| 3412 |
IPEC(I)=0 |
| 3413 |
50 CONTINUE |
| 3414 |
I18=0 |
| 3415 |
I19=0 |
| 3416 |
DO 60 I=1,2114 |
| 3417 |
ESPS(I)=0.0 |
| 3418 |
60 CONTINUE |
| 3419 |
DO 70 I= 4515,4849 |
| 3420 |
ESPS(I)=0.D0 |
| 3421 |
70 CONTINUE |
| 3422 |
DO 80 I=1,10 |
| 3423 |
COUNT(I)=0.0D0 |
| 3424 |
80 CONTINUE |
| 3425 |
DO 90 I=1,12 |
| 3426 |
ICC(I)=0 |
| 3427 |
90 CONTINUE |
| 3428 |
SPACE(13)=EINC |
| 3429 |
NO=AMASNO |
| 3430 |
NMAS=1+(NO-1)*10 |
| 3431 |
DO 100 I=1,10 |
| 3432 |
OUT(I)=CRSC(NMAS) |
| 3433 |
NMAS=NMAS+1 |
| 3434 |
100 CONTINUE |
| 3435 |
CALL ROUT1 |
| 3436 |
IF(PRTIN.GT.4) THEN |
| 3437 |
CALL CERROR(' BERT called for muon$') |
| 3438 |
NOPART=-1 |
| 3439 |
RETURN |
| 3440 |
ENDIF |
| 3441 |
NO= PRTIN + 1. |
| 3442 |
IF(SPACE(4).GT.100.0) SPACE(4)=100.0 |
| 3443 |
VALUE1=EINC+SPACE(4) |
| 3444 |
IF(NO.LT.3) GOTO 2540 |
| 3445 |
IF(NO.EQ.4) THEN |
| 3446 |
CALL CERROR(' BERT called for pi0$') |
| 3447 |
NOPART = -1 |
| 3448 |
RETURN |
| 3449 |
ENDIF |
| 3450 |
C ----- Charged pions ------ |
| 3451 |
CALL ROUT2(PPAC(1)) |
| 3452 |
IF(I1.EQ.0) THEN |
| 3453 |
CALL CERROR(' BERT Epion > 2.5 GeV$') |
| 3454 |
RETURN |
| 3455 |
ENDIF |
| 3456 |
IV=2 |
| 3457 |
IF(NO.EQ.5) IV=0 |
| 3458 |
CALL CALXYI(1,14,30) |
| 3459 |
IP=1 |
| 3460 |
110 CALL ROUT3 |
| 3461 |
IF(BEGRU.EQ.0.0) GOTO 2460 |
| 3462 |
C IF BEGRU=0, LAST RUN COMPLETED--BG6A |
| 3463 |
KK=I1 |
| 3464 |
XINC=XI(1) |
| 3465 |
C XINC=X-COORDINATE INC.PART. |
| 3466 |
CALL ROUT4 |
| 3467 |
IF(I1.LT.0.0) GOTO 2820 |
| 3468 |
I1=KK |
| 3469 |
120 IF(IN.NE.0) GOTO 2200 |
| 3470 |
IF(EX.GT.D(2)) GOTO 650 |
| 3471 |
130 CURR(2)=OUT(13) |
| 3472 |
WKRPN(3)=CURR(2) |
| 3473 |
C K.E. WITH RESPECT TOPROTONS RG.3 |
| 3474 |
WKRPN(6)=OUT(16) |
| 3475 |
C K.E. WITH RESPECT TONEUTRONS RG.3 |
| 3476 |
IFCA=0 |
| 3477 |
140 CALL CBG6CA(3,3) |
| 3478 |
150 IFCC=0 |
| 3479 |
CALL CABRAN(6) |
| 3480 |
KNOT=NOT |
| 3481 |
IF(NOT.EQ.4) GOTO 380 |
| 3482 |
CALL CABG6C(ISW(11)) |
| 3483 |
VALUE1=RLKE |
| 3484 |
IF(IN.NE.0) GOTO 1980 |
| 3485 |
IF(NOT.EQ.4) GOTO 380 |
| 3486 |
IF(NOT.LT.4) THEN |
| 3487 |
ANY=SPACE(NOT+13) |
| 3488 |
GOTO 170 |
| 3489 |
ELSE |
| 3490 |
ANY=S(NOT-4) |
| 3491 |
ENDIF |
| 3492 |
160 IF(NOT-5)170,600,630 |
| 3493 |
C IT=1-6 PIPPS(20051),BG129(21011),PIMPD(21004),PIPND(20644) |
| 3494 |
170 CALL ROUT5(PPEC(1),PMEC(1),PMXC(1)) |
| 3495 |
C PPEC(126),PMEC(126),PMXC(126) |
| 3496 |
180 IF(CLSM-2.0)880 ,740,190 |
| 3497 |
C (PIM-P)EXCHANGE SCATTERING CRS. |
| 3498 |
190 IF(VALUE1.GT.VALUE2) GOTO 300 |
| 3499 |
200 IF(ISW(1).NE.0) GOTO 240 |
| 3500 |
IFC=IFCC+1 |
| 3501 |
IF(IN.NE.0) GOTO 1990 |
| 3502 |
210 C(3)=0.0 |
| 3503 |
220 C(1)=CURR(4) |
| 3504 |
C(2)=CURR(5) |
| 3505 |
C(3)=C(3)+CURR(6)+EX+D(1) |
| 3506 |
230 CONTINUE |
| 3507 |
GOTO(960 ,1230,1240,1300,1310,1410,1420,1450,1460,1420,1470,1830,1 |
| 3508 |
+840 ,1460,1850,1860,1870,1880,1960,1930,1940,1950,2360,2420,2430,2 |
| 3509 |
+440 ,1420,2450),IT |
| 3510 |
240 IF(ISW(2))280,250,280 |
| 3511 |
250 IFC=2+IFCC |
| 3512 |
260 IF(IN)2000,270,2000 |
| 3513 |
270 C(3)=D(2)+D(3) |
| 3514 |
GOTO 220 |
| 3515 |
280 IFC=3+IFCC |
| 3516 |
IF(IN)480,290,480 |
| 3517 |
290 C(3)=D(2)+D(3)+D(4)+D(5) |
| 3518 |
GOTO 220 |
| 3519 |
C IFC(1-3),BG6C(1502),BG6F(3243),BG6K(4055) COLLISION |
| 3520 |
300 CALL SIGNEX |
| 3521 |
310 IF(ISW(1))320,120,320 |
| 3522 |
320 IF(IN)2010,330,2010 |
| 3523 |
330 IF(EX-D(6))130,130,340 |
| 3524 |
340 IF(ISW(2))360,350,360 |
| 3525 |
350 IPEC(7)=IPEC(7)+1 |
| 3526 |
C NO. OF ESCAPED PARTICLES ON REGION 2 |
| 3527 |
GOTO 110 |
| 3528 |
360 IPEC(11)=IPEC(11)+1 |
| 3529 |
C NO. OF ESCAPED PARTICES ON REGION 1 |
| 3530 |
GOTO 110 |
| 3531 |
370 I3=1 |
| 3532 |
GOTO 390 |
| 3533 |
380 I3=-1 |
| 3534 |
390 CALL ROUT6 |
| 3535 |
IF(I3)400 ,410,450 |
| 3536 |
400 CALL CERROR(' BERT CURR(1) < 3 or > 5$') |
| 3537 |
NOPART=-1 |
| 3538 |
RETURN |
| 3539 |
410 CALL ROUT6A |
| 3540 |
IF(CLSM-2.0)910 ,940 ,2180 |
| 3541 |
420 IFCA=1 |
| 3542 |
430 IF(ISW(1))440,210,440 |
| 3543 |
440 IF(ISW(2))290,270,290 |
| 3544 |
C NON-DEUTERON ABSORPTION |
| 3545 |
450 CALL ROUT7 |
| 3546 |
IF(I3)400 ,460,460 |
| 3547 |
460 CALL ROUT7A |
| 3548 |
I3=I3 |
| 3549 |
GOTO(480,470 ,590,540,210,290,500,510,270),I3 |
| 3550 |
470 CALL CERROR(' BERT PWD or NWD < 7$') |
| 3551 |
NOPART = -1 |
| 3552 |
RETURN |
| 3553 |
480 VALUE1=EX+D(4)+D(5) |
| 3554 |
490 IF(CURR(10)-2.0)500,510,510 |
| 3555 |
500 C(1)=VALUE1*CURR(7)+CURR(4) |
| 3556 |
C(2)=VALUE1*CURR(8)+CURR(5) |
| 3557 |
C(3)=VALUE1*CURR(9)+CURR(6) |
| 3558 |
GO TO 230 |
| 3559 |
510 VALUE1=VALUE1+D(3) |
| 3560 |
GO TO 520 |
| 3561 |
520 IF(CURR(10)-2.0)500,500,530 |
| 3562 |
530 VALUE1=VALUE1+D(2) |
| 3563 |
GO TO 500 |
| 3564 |
540 IF(INC)550,570,550 |
| 3565 |
550 C(3)=D(2) |
| 3566 |
IF(ISW(3))560,220,560 |
| 3567 |
560 C(3)=C(3)+D(3)+D(4) |
| 3568 |
GO TO 220 |
| 3569 |
570 IF(ISW(3))580,520,580 |
| 3570 |
580 VALUE1=EX+D(4) |
| 3571 |
GO TO 490 |
| 3572 |
590 VALUE1=EX |
| 3573 |
IF(INC)270,490,270 |
| 3574 |
600 IF(RLKE.GT.2500.0) THEN |
| 3575 |
CALL CERROR(' BERT RLKE > 2.5 GeV$') |
| 3576 |
RLKE = 2500.0 |
| 3577 |
ENDIF |
| 3578 |
IF(RLKE-180.0)610,610,620 |
| 3579 |
610 CALL SIGNEX |
| 3580 |
IF(CLSM-2.0)850 ,760,310 |
| 3581 |
620 VALUE1=VALUE1-180.0 |
| 3582 |
CALL CRJAB(1,PPSCL(1)) |
| 3583 |
C PPSCL(117) |
| 3584 |
C (PIP-P)SINGLE PROD. CRS. LOW ENERGY |
| 3585 |
GO TO 180 |
| 3586 |
630 IF(RLKE.GT.2500.0) THEN |
| 3587 |
CALL CERROR(' BERT RLKE > 2.5 GeV (2)$') |
| 3588 |
RLKE = 2500.0 |
| 3589 |
ENDIF |
| 3590 |
IF(RLKE-180.0)610,610,640 |
| 3591 |
640 VALUE1=VALUE1-180.0 |
| 3592 |
CALL CRJAB(1,PMSCL(1)) |
| 3593 |
C PMSCL(117) |
| 3594 |
C (PIM-P)SINGLE PROD. CRS. LOW ENERGY |
| 3595 |
GO TO 180 |
| 3596 |
650 IF(D(3))670,660,670 |
| 3597 |
660 IPEC(2)=IPEC(2)+1 |
| 3598 |
C NO. OF PARTICLES INCIDENT ON REGION 3 ESCAPING |
| 3599 |
GO TO 110 |
| 3600 |
670 ISW(1)=1 |
| 3601 |
CALL SPAC32(31) |
| 3602 |
680 IF(IN)2020,690 ,2020 |
| 3603 |
690 IF(EX-D(3))710,710,810 |
| 3604 |
700 IF(IN)720,710,720 |
| 3605 |
710 CURR(2)=OUT(14) |
| 3606 |
WKRPN(2)=CURR(2) |
| 3607 |
WKRPN(5)=OUT(17) |
| 3608 |
C K.E. FOR PROTONS AND NEUTRONS REGION 2 |
| 3609 |
720 CALL CBG6CA(2,2) |
| 3610 |
GO TO 150 |
| 3611 |
730 IV=-1 |
| 3612 |
GO TO 750 |
| 3613 |
740 IV=0 |
| 3614 |
750 CALL ROUT8 |
| 3615 |
I3=I3 |
| 3616 |
GOTO(760,2030,220,580),I3 |
| 3617 |
760 IF(ISW(3))770,680,770 |
| 3618 |
770 IF(EX-D(5))700 ,700 ,780 |
| 3619 |
780 IF(IN)2040,790 ,2040 |
| 3620 |
790 CALL SPAC32(32) |
| 3621 |
800 IF(EX-D(6))130,130,360 |
| 3622 |
810 IF(D(4))840 ,820 ,840 |
| 3623 |
820 CALL SPAC32(32) |
| 3624 |
830 IF(EX-D(6))130,130,350 |
| 3625 |
840 ISW(2)=1 |
| 3626 |
ISW(3)=1 |
| 3627 |
CALL SPAC32(30) |
| 3628 |
850 IF(IN)2050,860 ,2050 |
| 3629 |
860 CALL ROUT10 |
| 3630 |
IF(I3)770,870 ,870 |
| 3631 |
870 CALL CBG6CA(1,1) |
| 3632 |
GO TO 150 |
| 3633 |
880 IF(VALUE1-VALUE2)890 ,890 ,900 |
| 3634 |
890 IFC=9+IFCC |
| 3635 |
IF(IN)2060,270,2060 |
| 3636 |
900 CALL SIGNEX |
| 3637 |
IF(IN)2050,860 ,2050 |
| 3638 |
910 IF(IN)930 ,920 ,930 |
| 3639 |
920 IFCA=6 |
| 3640 |
GO TO 270 |
| 3641 |
930 IFCA=9*IABS(I6-2)+13*(I6-1)*(3-I6) |
| 3642 |
GOTO2060 |
| 3643 |
940 IF(IN)2070,950 ,2070 |
| 3644 |
950 IFCA=7 |
| 3645 |
GOTO550 |
| 3646 |
960 I3=1 |
| 3647 |
GOTO1000 |
| 3648 |
970 I3=4 |
| 3649 |
GOTO1000 |
| 3650 |
980 I3=2 |
| 3651 |
GOTO1000 |
| 3652 |
990 I3=3 |
| 3653 |
1000 CALLROUT11(PPDC(1)) |
| 3654 |
C PPDCL(378) |
| 3655 |
I3=I3 |
| 3656 |
GOTO(1180,1270,1400,1010),I3 |
| 3657 |
1010 CST=CRDT(2)-DABS(SNT*(CRDT(2)-CRDT(1))) |
| 3658 |
1020 SNT=DSQRT(1.0-CST*CST) |
| 3659 |
1030 CALL ROUT12 |
| 3660 |
IF(I3)1040,1050,1110 |
| 3661 |
1040 CALL CERROR(' BERT COM < -5E-6$') |
| 3662 |
NOPART=-1 |
| 3663 |
RETURN |
| 3664 |
1050 IF(EFRN-VALUE1)1150,1060,1060 |
| 3665 |
1060 FCN=FCN+1.0 |
| 3666 |
1070 IV=-1 |
| 3667 |
GOTO1090 |
| 3668 |
1080 IV=0 |
| 3669 |
1090 I1=0 |
| 3670 |
CALLROUT13 |
| 3671 |
IF(I3)460,1100,410 |
| 3672 |
1100 IFC=IFC |
| 3673 |
GOTO(120,830 ,800 ,2840,3210,3270,680,770,850 ,3150,3250,3230,2200 |
| 3674 |
+ ,2010,2010,2080,2090,2100,2020,770,2200,2010,2010,2050,2200,20 |
| 3675 |
+10 ,2010,2020,2110,2050),IFC |
| 3676 |
1110 IF(EFRP-VALUE1)1150,1120,1120 |
| 3677 |
1120 FCP=FCP+1.0 |
| 3678 |
GOTO1070 |
| 3679 |
1130 I3=0 |
| 3680 |
GOTO1160 |
| 3681 |
1140 I3=-1 |
| 3682 |
GOTO1160 |
| 3683 |
1150 I3=1 |
| 3684 |
1160 CALLROUT14 |
| 3685 |
I3=I3 |
| 3686 |
GOTO(1110,1050,1170,3560,2120),I3 |
| 3687 |
1170 CALL CERROR(' BERT I3=3$') |
| 3688 |
NOPART=-1 |
| 3689 |
RETURN |
| 3690 |
1180 I3=1 |
| 3691 |
GOTO1210 |
| 3692 |
1190 I3=3 |
| 3693 |
GOTO1210 |
| 3694 |
1200 I3=4 |
| 3695 |
1210 CALLROUT15(PPDC(1)) |
| 3696 |
C HPPDCI(45),PPDCI(170) |
| 3697 |
I3=I3 |
| 3698 |
GOTO(1250,1340,1020,1220,1260,1390),I3 |
| 3699 |
1220 CALL CERROR(' BERT I3=4$') |
| 3700 |
C SNN(RLKE GTE 1000) DCINTP(RLKE GTE CRS.SECT.VALUES) |
| 3701 |
NOPART=-1 |
| 3702 |
RETURN |
| 3703 |
1230 PT(2)=5.0 |
| 3704 |
IK=IT |
| 3705 |
C BG129 (PIM-N) |
| 3706 |
PT(14)=2.0 |
| 3707 |
GOTO980 |
| 3708 |
1240 PT(2)=5.0 |
| 3709 |
C PIPNX DIR. SCAT. |
| 3710 |
PT(14)=1.0 |
| 3711 |
IK=IT |
| 3712 |
GOTO 980 |
| 3713 |
1250 I3=1 |
| 3714 |
GOTO1280 |
| 3715 |
1260 I3=2 |
| 3716 |
GOTO1280 |
| 3717 |
1270 I3=3 |
| 3718 |
1280 CALLROUT16(PMDD(1)) |
| 3719 |
C HPMDDI(45),PMDDI(170),PMDDL(378) |
| 3720 |
1290 IF(I3)1020,1190,1020 |
| 3721 |
1300 PT(2)=3.0 |
| 3722 |
PT(14)=2.0 |
| 3723 |
IK=3 |
| 3724 |
GO TO 980 |
| 3725 |
1310 PT(14)=2.0 |
| 3726 |
1320 IK=IT |
| 3727 |
1330 PT(2)=4.0 |
| 3728 |
PM(3)=POMS |
| 3729 |
C PI 0 MASS/CM |
| 3730 |
GO TO 990 |
| 3731 |
1340 IF(IK-23)1350,2390,1350 |
| 3732 |
1350 I3=1 |
| 3733 |
GO TO 1380 |
| 3734 |
1360 I3=2 |
| 3735 |
GO TO 1380 |
| 3736 |
1370 I3=3 |
| 3737 |
1380 CALL ROUT16(PMDX(1)) |
| 3738 |
C HPMDXI(45),PMDXI(170),PMDXL(378) |
| 3739 |
GO TO 1290 |
| 3740 |
1390 IF(IK-23)1360,2370,1360 |
| 3741 |
1400 IF(IK-23)1370,2380,1370 |
| 3742 |
C (PIM-P)XCH. |
| 3743 |
1410 PT(14)=1.0 |
| 3744 |
GO TO 1320 |
| 3745 |
1420 PT(2)=1.0 |
| 3746 |
C PIM+(PP) ABS |
| 3747 |
C IT=10,PIP+(NN) ABS |
| 3748 |
1430 PT(14)=2.0 |
| 3749 |
1440 CALL CAPOL1(CST,SNT) |
| 3750 |
GO TO 1030 |
| 3751 |
1450 PT(2)=2.0 |
| 3752 |
C PIN+(NN) ABS |
| 3753 |
GO TO 1430 |
| 3754 |
1460 PT(2)=1.0 |
| 3755 |
C PIN+(PP) ABS ALS0 PI+ ABS |
| 3756 |
PT(14)=1.0 |
| 3757 |
GO TO 1440 |
| 3758 |
1470 ISW(9)=0 |
| 3759 |
ISW(10)=0 |
| 3760 |
1480 I3=0 |
| 3761 |
GO TO 1500 |
| 3762 |
1490 I3=-1 |
| 3763 |
1500 CALL ROUT17(FRIPN(1),PNMI(1),FMXSP(1),PCFSL(1),PNFSL(1)) |
| 3764 |
C FRIPN(117),PNMI(101),FMXSP(117),PCFSL(234),PNFSL(234) |
| 3765 |
IF(I3) 1510,1640,1520 |
| 3766 |
1510 CALL CERROR(' BERT I3 < 0$') |
| 3767 |
C COLL(COM LT -5.0E-6) ECPL(ERROR IN CURR ,STRKP,PT(26), |
| 3768 |
C PT(2),PT(14) OR PT(37)) ISW10=0 |
| 3769 |
NOPART=-1 |
| 3770 |
RETURN |
| 3771 |
1520 K=3 |
| 3772 |
1530 IF(PT(K-1)-1.0)1650,1540,1650 |
| 3773 |
1540 IF(PT(K))1560,1560,1550 |
| 3774 |
1550 IF(PT(K)-EFRP)1560,1560,1580 |
| 3775 |
1560 FCP=FCP+1.0 |
| 3776 |
C NO. FORBIDDEN COLLISIONS INVOLVING PROTONS |
| 3777 |
1570 PM(4)=DNCMS |
| 3778 |
GO TO 1080 |
| 3779 |
1580 M=PT(K-1) |
| 3780 |
IF(PT(K)-ECO (M)) 1590,1590,1600 |
| 3781 |
1590 PT(K)=0.0 |
| 3782 |
PNBC(M)=PNBC(M)+1.0 |
| 3783 |
1600 IF(COL(15)-1.0)1640,1740,1610 |
| 3784 |
1610 IF(COL(15)-3.0)1720,1710,1620 |
| 3785 |
1620 IF(COL(15)-5.0)1730,1780,1630 |
| 3786 |
1630 CALL CERROR(' BERT COL(15)>5$') |
| 3787 |
NOPART=-1 |
| 3788 |
RETURN |
| 3789 |
1640 CALL COLLM(0) |
| 3790 |
IF(PT(38)) 1700,1690,1700 |
| 3791 |
1650 IF(PT(K-1)-2.0) 1810,1660,1810 |
| 3792 |
1660 IF(PT(K)) 1680,1680,1670 |
| 3793 |
1670 IF(PT(K)-EFRN) 1680,1680,1580 |
| 3794 |
1680 FCN = FCN+1.0 |
| 3795 |
GO TO 1570 |
| 3796 |
1690 I3=1 |
| 3797 |
GO TO 1750 |
| 3798 |
1700 I3=2 |
| 3799 |
GO TO 1750 |
| 3800 |
1710 I3=4 |
| 3801 |
GO TO 1750 |
| 3802 |
1720 I3=5 |
| 3803 |
GO TO 1750 |
| 3804 |
1730 I3=6 |
| 3805 |
GO TO 1750 |
| 3806 |
1740 I3=3 |
| 3807 |
1750 CALL ROUT18 |
| 3808 |
I3=I3 |
| 3809 |
K=IV |
| 3810 |
GO TO (1530,1760,1600,1900,1770),I3 |
| 3811 |
1760 CALL CERROR(' BERT PT(K-1) < 3$') |
| 3812 |
NOPART=-1 |
| 3813 |
RETURN |
| 3814 |
1770 I18=I18+1 |
| 3815 |
GO TO 1570 |
| 3816 |
1780 CALL ROUT19 |
| 3817 |
IF(I3)1790,1900,1800 |
| 3818 |
1790 CALL CERROR(' BERT PT(K-1)<3, >6 K<27$') |
| 3819 |
NOPART=-1 |
| 3820 |
RETURN |
| 3821 |
1800 I19=I19+1 |
| 3822 |
GO TO 1570 |
| 3823 |
1810 IF(COL(15)-1.0)1640,1820,1820 |
| 3824 |
1820 CALL CERROR(' BERT COL(15) >=1$') |
| 3825 |
NOPART=-1 |
| 3826 |
RETURN |
| 3827 |
1830 I3=2 |
| 3828 |
GO TO 1910 |
| 3829 |
1840 I3=3 |
| 3830 |
GO TO 1910 |
| 3831 |
1850 I3=4 |
| 3832 |
GOTO1910 |
| 3833 |
1860 I3=5 |
| 3834 |
GOTO1910 |
| 3835 |
1870 I3=6 |
| 3836 |
GOTO1910 |
| 3837 |
1880 I3=7 |
| 3838 |
GOTO1910 |
| 3839 |
1890 I3=8 |
| 3840 |
GOTO1910 |
| 3841 |
1900 I3=1 |
| 3842 |
1910 CALL ROUT20(DCIN(1),DCLN(1),DCHN(1),PDCI(1),PDCH(1)) |
| 3843 |
C DCIN(115),DCLN(80),DCHN(64),PDCI(52),PDCH(64) |
| 3844 |
I3=I3 |
| 3845 |
GOTO(1920,1140,1490,1430,1200,1020,1440,1030),I3 |
| 3846 |
1920 CALL CERROR(' BERT RLKE>3.5GeV$') |
| 3847 |
NOPART=-1 |
| 3848 |
RETURN |
| 3849 |
1930 I3=2 |
| 3850 |
GOTO1970 |
| 3851 |
1940 I3=3 |
| 3852 |
GOTO1970 |
| 3853 |
1950 I3=4 |
| 3854 |
GOTO1970 |
| 3855 |
1960 I3=1 |
| 3856 |
1970 CALL ROUT21(FRINN(1),DMIN(1), FMXSN(1),FMXDN(1),FSLN(1)) |
| 3857 |
C FRINN(161),DMIN(101),FMXSN(161),FMXDN(130),FSLN(176) |
| 3858 |
GOTO1500 |
| 3859 |
1980 IV=2 |
| 3860 |
GOTO2210 |
| 3861 |
1990 IV=3 |
| 3862 |
GOTO2210 |
| 3863 |
2000 IV=4 |
| 3864 |
GOTO2210 |
| 3865 |
2010 IV=5 |
| 3866 |
GOTO2210 |
| 3867 |
2020 IV=6 |
| 3868 |
GOTO2210 |
| 3869 |
2030 IV=7 |
| 3870 |
GOTO2210 |
| 3871 |
2040 IV=8 |
| 3872 |
GOTO2210 |
| 3873 |
2050 IV=9 |
| 3874 |
GOTO2210 |
| 3875 |
2060 IV=10 |
| 3876 |
GOTO2210 |
| 3877 |
2070 IV=11 |
| 3878 |
GOTO2210 |
| 3879 |
2080 IV=12 |
| 3880 |
GOTO2210 |
| 3881 |
2090 IV=13 |
| 3882 |
GOTO2210 |
| 3883 |
2100 IV=14 |
| 3884 |
GOTO2210 |
| 3885 |
2110 IV=15 |
| 3886 |
GOTO2210 |
| 3887 |
2120 IV=16 |
| 3888 |
GOTO2210 |
| 3889 |
2130 IV=17 |
| 3890 |
GOTO2210 |
| 3891 |
2140 IV=18 |
| 3892 |
GOTO2210 |
| 3893 |
2150 IV=19 |
| 3894 |
GOTO2210 |
| 3895 |
2160 IV=20 |
| 3896 |
GOTO2210 |
| 3897 |
2170 IV=21 |
| 3898 |
GOTO2210 |
| 3899 |
2180 IV=22 |
| 3900 |
GOTO2210 |
| 3901 |
2190 IV=23 |
| 3902 |
GOTO2210 |
| 3903 |
2200 IV=1 |
| 3904 |
2210 CALLROUT22(PPAC(1),POAC(1),PNEC(1),PMXC(1),PNNEC(1)) |
| 3905 |
C PPAC(19),POAC(19),PNEC(126),PMXC(126),PNNEC(126) |
| 3906 |
IV=IV |
| 3907 |
IF(I1)2820,2220,2220 |
| 3908 |
2220 GOTO(2350,2230,770,1130,2890,500,520,490,3400,3010,2990,3310,720,1 |
| 3909 |
+60 ,870 ,420,480,580,2900,140,2330,3020,2240),IV |
| 3910 |
2230 CALL CERROR(' BERT COM>3500,ESPS(1)>=30. COM>2500$') |
| 3911 |
NOPART=-1 |
| 3912 |
RETURN |
| 3913 |
2240 CALL CERROR(' BERT IV > 22$') |
| 3914 |
NOPART=-1 |
| 3915 |
RETURN |
| 3916 |
2250 XABS=1.0 |
| 3917 |
VALUE1 = RANDC(ISEED) |
| 3918 |
IF(VALUE1-PPNDA)2260,450,450 |
| 3919 |
C PROB. PIN-DEUT ABS |
| 3920 |
2260 IT=27 |
| 3921 |
C BG117(20040) PI0 ABS |
| 3922 |
MED=MED |
| 3923 |
ABSEC=-HVP(MED) |
| 3924 |
GO TO 370 |
| 3925 |
2270 IF(RLKE-2500.0)2290,2290,2280 |
| 3926 |
2280 CALL CERROR(' BERT RLKE > 2.5GeV$') |
| 3927 |
RLKE=2500.0 |
| 3928 |
2290 IF(RLKE-180.0) 2320,2320,2300 |
| 3929 |
2300 IF(NOT-6) 2310,2310,2340 |
| 3930 |
2310 VALUE1=RLKE-180.0 |
| 3931 |
CALL CRJAB(1,PNSCL(1)) |
| 3932 |
C PNSCL(117) |
| 3933 |
C (PIN-P)SINGLE PRODUCTION CRS. LOW EN. |
| 3934 |
GO TO 3020 |
| 3935 |
2320 IF(CLSM-2.0)3550,3510,3040 |
| 3936 |
2330 IF(NOT-6)2190,2270,2270 |
| 3937 |
2340 VALUE1=RLKE-180.0 |
| 3938 |
CALL CRJAB(1,PNNSL(1)) |
| 3939 |
C PNNSL(117) |
| 3940 |
C (PIN-N)SINGLE PROD. CRS. LOW EN. |
| 3941 |
GOTO3020 |
| 3942 |
2350 ISW(11)=0 |
| 3943 |
GOTO2130 |
| 3944 |
2360 PT(14)=1.0 |
| 3945 |
GO TO 1320 |
| 3946 |
2370 I3=2 |
| 3947 |
GO TO 2400 |
| 3948 |
2380 I3=3 |
| 3949 |
GO TO 2400 |
| 3950 |
2390 I3=1 |
| 3951 |
2400 CALL ROUT16(PNDD(1)) |
| 3952 |
C HPNDDI(45),PNDDI(170),PNDDL(378) |
| 3953 |
C (PIN-P)DRCT. CROSS SECTION INT. EN. |
| 3954 |
C (PIN-P)DRCT DIFF. CRS. SEC. LOW ENERGY |
| 3955 |
2410 GO TO 1290 |
| 3956 |
2420 PT(2)=3.0 |
| 3957 |
PT(14)=2.0 |
| 3958 |
IK=IT |
| 3959 |
GO TO 980 |
| 3960 |
2430 PT(14)=2.0 |
| 3961 |
IK=23 |
| 3962 |
GO TO 1330 |
| 3963 |
2440 PT(2)=5.0 |
| 3964 |
GO TO 970 |
| 3965 |
2450 ISW(9)=2 |
| 3966 |
GO TO 1890 |
| 3967 |
2460 ITOTE =IPEC(2)+IPEC(7)+IPEC(11) |
| 3968 |
IF(ITOTE-1)2500,2480,2470 |
| 3969 |
2470 CALL CERROR('BERT1$') |
| 3970 |
2480 NOPART = -1 |
| 3971 |
2490 CONTINUE |
| 3972 |
RETURN |
| 3973 |
2500 NOPART = ESPS(1) |
| 3974 |
IF(NOPART-60)2520,2520,2510 |
| 3975 |
2510 WRITE(IO ,10000) NOPART |
| 3976 |
10000 FORMAT(' BERT : NOPART HAS EXCEEDED THE MAXIMUM = ',I6) |
| 3977 |
NOPART = 60 |
| 3978 |
2520 CONTINUE |
| 3979 |
DO 2530 NDEX = 1,NOPART |
| 3980 |
KLMN = 8*(NDEX-1) + 1 |
| 3981 |
KIND(NDEX) = ESPS(KLMN+1)-1. |
| 3982 |
ERAY(NDEX) = ESPS(KLMN+2) |
| 3983 |
ARAY(NDEX) = ESPS(KLMN+3) |
| 3984 |
BRAY(NDEX) = ESPS(KLMN+4) |
| 3985 |
2530 GRAY(NDEX) = ESPS(KLMN+5) |
| 3986 |
GO TO 2490 |
| 3987 |
2540 VALUE2=EINC+SPACE(12) |
| 3988 |
IF(VALUE1-160.0)2550,2550,2570 |
| 3989 |
2550 SPACE(33)=1.4D-24 |
| 3990 |
C NO PRODUCTION POSSIBLE |
| 3991 |
FMAX(2)=1.4D-24 |
| 3992 |
SPACE(34)=0.46D-24 |
| 3993 |
FMAX(1)=0.46D-24 |
| 3994 |
DO2560 I=9,12 |
| 3995 |
2560 S(I)=0.0 |
| 3996 |
C EINC+50.0 IS LESS THAN 160.0 |
| 3997 |
GOTO2740 |
| 3998 |
2570 CALLCBOVER(VALUE2,DNCMS,ANS) |
| 3999 |
C NUCLEON MASS=CONSTANT ANS=P1/E1 |
| 4000 |
IF(VALUE1-560.0)2580,2580,2660 |
| 4001 |
2580 S(11)=0.0 |
| 4002 |
S(12)=0.0 |
| 4003 |
C SINGLE PRODUCTION POSSIBLE--S(11),S(12) DOUBLE PROD. |
| 4004 |
IF(VALUE1-400.0)2600,2590,2590 |
| 4005 |
2590 S(9)=22.6D-27*ANS |
| 4006 |
S(10)=14.0D-27*ANS |
| 4007 |
SPACE(44)=56.0D-27 |
| 4008 |
SPACE(45)=27.0D-27*ANS |
| 4009 |
GOTO2650 |
| 4010 |
2600 IF(VALUE1-300.0)2620,2610,2610 |
| 4011 |
2610 S(9)=20.0D-27*ANS |
| 4012 |
S(10)=14.0D-27*ANS |
| 4013 |
SPACE(44)=0.106D-24 |
| 4014 |
SPACE(45)=36.0D-27*ANS |
| 4015 |
GOTO2650 |
| 4016 |
2620 IF(VALUE1-200.0)2640,2630,2630 |
| 4017 |
2630 S(9)=11.4D-27*ANS |
| 4018 |
S(10)=11.2D-27*ANS |
| 4019 |
SPACE(44)=0.313D-24 |
| 4020 |
SPACE(45)=0.103D-24 |
| 4021 |
GOTO2650 |
| 4022 |
2640 S(9)=1.95D-27*ANS |
| 4023 |
S(10)=1.7D-27*ANS |
| 4024 |
SPACE(44)=0.52D-24 |
| 4025 |
SPACE(45)=0.176D-24 |
| 4026 |
2650 SPACE(33)=SPACE(44) |
| 4027 |
SPACE(34)=SPACE(45) |
| 4028 |
GOTO2740 |
| 4029 |
2660 IF(VALUE1-3600.0)2680,2680,2670 |
| 4030 |
2670 CALL CERROR(' BERT VALUE1 > 3.6GeV$') |
| 4031 |
NOPART=-1 |
| 4032 |
RETURN |
| 4033 |
2680 S(9)=22.6D-27*ANS |
| 4034 |
C DOUBLE PRODUCTION POSSIBLE |
| 4035 |
S(10)=14.0D-27*ANS |
| 4036 |
IF(VALUE1-800.0)2690,2700,2700 |
| 4037 |
2690 S(11)=1.9D-27*ANS |
| 4038 |
S(12)=9.0D-27*ANS |
| 4039 |
SPACE(46)=38.4D-27*ANS |
| 4040 |
SPACE(47)=27.2D-27*ANS |
| 4041 |
GOTO2730 |
| 4042 |
2700 IF(VALUE1-1680.0)2710,2720,2720 |
| 4043 |
2710 S(11)=10.8D-27*ANS |
| 4044 |
S(12)=17.4D-27*ANS |
| 4045 |
SPACE(46)=33.0D-27*ANS |
| 4046 |
SPACE(47)=27.2D-27*ANS |
| 4047 |
GOTO2730 |
| 4048 |
2720 SPACE(46)=25.0D-27*ANS |
| 4049 |
SPACE(47)=26.5D-27*ANS |
| 4050 |
S(10)=13.6D-27*ANS |
| 4051 |
S(11)=18.0D-27*ANS |
| 4052 |
S(12)=23.6D-27*ANS |
| 4053 |
2730 SPACE(33)=SPACE(46) |
| 4054 |
SPACE(34)=SPACE(47) |
| 4055 |
2740 GO TO (2750,3630), NO |
| 4056 |
2750 IV=1 |
| 4057 |
2760 CALL CALXYI(9,33,41) |
| 4058 |
IP=2 |
| 4059 |
2770 IF(NO-2)2790,2780,2780 |
| 4060 |
2780 ISW(4)=0 |
| 4061 |
GO TO 2800 |
| 4062 |
2790 ISW(4)=1 |
| 4063 |
2800 CALL UNDIS |
| 4064 |
IF(BEGRU) 2810,2460,2810 |
| 4065 |
2810 XABS=0.0 |
| 4066 |
XINC=XI(1) |
| 4067 |
C XINC=X-COORDINATE INC.PART. |
| 4068 |
INC=1 |
| 4069 |
C 0 IF PARTICLE CASCADE |
| 4070 |
CURR(1)=NO |
| 4071 |
CURR(3)=DNCMS |
| 4072 |
C NUCLEON MASS/CM |
| 4073 |
CALL CALGEO |
| 4074 |
IF(I1) 2820,2830,2830 |
| 4075 |
2820 CALL CERROR(' BERT error in GEOM$') |
| 4076 |
NOPART=-1 |
| 4077 |
RETURN |
| 4078 |
2830 CALL PARTIN |
| 4079 |
CALL SPAC32(43) |
| 4080 |
2840 IF(EX-D(2))2850,2850,3120 |
| 4081 |
2850 WKRPN(3)=OUT(13) |
| 4082 |
WKRPN(6)=OUT(16) |
| 4083 |
CURR(2)=WKRPN(6) |
| 4084 |
IF(ISW(4))2860,2870,2860 |
| 4085 |
2860 CURR(2)=WKRPN(3) |
| 4086 |
C K.E.WITH RESPECT TO NEUTRONS(PROTONS), RG.3 |
| 4087 |
2870 CALL CBG6CA(3,0) |
| 4088 |
IFCA=3 |
| 4089 |
2880 IFCC=3 |
| 4090 |
2890 KA=6 |
| 4091 |
2900 CALL CABRAN(KA) |
| 4092 |
KNOT=NOT+6 |
| 4093 |
IF(IN)2920,2920,2910 |
| 4094 |
2910 KNOT=KNOT+6 |
| 4095 |
2920 IF(KNOT-17)2930,2250,2930 |
| 4096 |
2930 CALL CABG6C(ISW(4)) |
| 4097 |
IF(RLKE)2940,2940,2950 |
| 4098 |
2940 CALL CERROR(' BERT RLKE <= 0.0$') |
| 4099 |
NOPART=-1 |
| 4100 |
RETURN |
| 4101 |
2950 VALUE1=RLKE |
| 4102 |
IF(IN) 2140,2960,2140 |
| 4103 |
2960 IF(NOT-5) 2970,3400,3400 |
| 4104 |
2970 IF(NOT-2)2980,3000,3310 |
| 4105 |
2980 ANY=SPACE(33) |
| 4106 |
2990 CALL CRJAB(1,ECN(1)) |
| 4107 |
C ECN(176) |
| 4108 |
C (N-P)ELASTIC CRS. SCATTERING |
| 4109 |
GOTO3020 |
| 4110 |
3000 ANY=SPACE(34) |
| 4111 |
3010 CALL CRJAB(1,PEC(1)) |
| 4112 |
C PEC(176) |
| 4113 |
C (P-P)ELASTIC SCAT. CRS. |
| 4114 |
3020 IF(CLSM-2.0)3540,3500,3030 |
| 4115 |
3030 IF(VALUE1-VALUE2)200,200,3040 |
| 4116 |
3040 CALLSIGNEX |
| 4117 |
IF(ISW(1))3070,3050,3070 |
| 4118 |
3050 IF(IN)3060 ,2840,3060 |
| 4119 |
3060 IF(CURR(1)-2.0)2200,2200,2150 |
| 4120 |
3070 IF(IN)2010,3080,2010 |
| 4121 |
3080 IF(EX-D(6))2850,2850,3090 |
| 4122 |
3090 IF(ISW(2))3110,3100,3110 |
| 4123 |
3100 IPEC(7)=IPEC(7)+1 |
| 4124 |
C NO. OF ESCAPED PARTICLES ON RG.2 |
| 4125 |
GOTO 2770 |
| 4126 |
3110 IPEC(11)=IPEC(11)+1 |
| 4127 |
GOTO 2770 |
| 4128 |
C NO. OF PARTICLES ESCAPED ON RG.1 |
| 4129 |
3120 IF(D(3))3140,3130,3140 |
| 4130 |
3130 IPEC(2)=IPEC(2)+1 |
| 4131 |
GOTO 2770 |
| 4132 |
C NO. OF PARTICLES INCIDENT ON RG.3 ESCAPING |
| 4133 |
3140 ISW(1)=1 |
| 4134 |
CALL SPAC32(42) |
| 4135 |
3150 IF(EX-D(3))3160,3160,3190 |
| 4136 |
3160 WKRPN(2)=OUT(14) |
| 4137 |
WKRPN(5)=OUT(17) |
| 4138 |
CURR(2)=WKRPN(5) |
| 4139 |
IF(ISW(4))3170,3180,3170 |
| 4140 |
3170 CURR(2)=WKRPN(2) |
| 4141 |
C K.E.WITH RESPECT TO NEUTRONS(PROTONS) RG.2 |
| 4142 |
3180 CALL CBG6CA(2,0) |
| 4143 |
GOTO2880 |
| 4144 |
3190 IF(D(4))3220,3200,3220 |
| 4145 |
3200 CALL SPAC32(43) |
| 4146 |
3210 IF(EX-D(6))2850,2850,3100 |
| 4147 |
3220 ISW(2)=1 |
| 4148 |
ISW(3)=1 |
| 4149 |
CALL SPAC32(41) |
| 4150 |
3230 IF(EX-D(4))3280,3280,3240 |
| 4151 |
3240 CALL SPAC32(42) |
| 4152 |
3250 IF(EX-D(5))3160,3160,3260 |
| 4153 |
3260 CALL SPAC32(43) |
| 4154 |
3270 IF(EX-D(6))2850,2850,3110 |
| 4155 |
3280 WKRPN(1)=OUT(15) |
| 4156 |
WKRPN(4)=OUT(18) |
| 4157 |
CURR(2)=WKRPN(4) |
| 4158 |
IF(ISW(4))3290,3300,3290 |
| 4159 |
3290 CURR(2)=WKRPN(1) |
| 4160 |
C K.E. WITH RESPECT TO NEUTRONS(PROTONS) RG.1 |
| 4161 |
3300 CALL CBG6CA(1,0) |
| 4162 |
GOTO 2880 |
| 4163 |
3310 IF(RLKE-3500.0)3330,3330,3320 |
| 4164 |
3320 CALL CERROR(' BERT RLKE>3.5GeV (2)$') |
| 4165 |
RLKE=3500.0 |
| 4166 |
3330 IF(RLKE-360.0)3530,3530,3340 |
| 4167 |
3340 VALUE1=RLKE-360.0 |
| 4168 |
IF(IN)3360,3350,3360 |
| 4169 |
3350 ANY=S(KNOT) |
| 4170 |
3360 IF(NOT-4)3380,3390,3370 |
| 4171 |
3370 CALL CERROR(' BERT NOT=5$') |
| 4172 |
NOPART=-1 |
| 4173 |
RETURN |
| 4174 |
3380 CALL CRJAB(1,PSPCL(1)) |
| 4175 |
C PSPCL(158) |
| 4176 |
C (P-P) SING. PROD. CRS. LOW ENERGY |
| 4177 |
GOTO 3020 |
| 4178 |
3390 CALL CRJAB(1,SPCLN(1)) |
| 4179 |
C SPCLN(158) |
| 4180 |
C (N-P) SINGLE PROD. CRS. LOW ENERGY |
| 4181 |
GOTO 3020 |
| 4182 |
3400 IF(RLKE-3500.0)3410,3410,3320 |
| 4183 |
3410 IF(RLKE-920.0)3530,3530,3420 |
| 4184 |
3420 VALUE1=RLKE-920.0 |
| 4185 |
IF(NOT-6)3440,3470,3430 |
| 4186 |
3430 CALL CERROR(' BERT NOT > 6$') |
| 4187 |
NOPART=-1 |
| 4188 |
RETURN |
| 4189 |
3440 IF(IN)3460,3450,3460 |
| 4190 |
3450 ANY=S(11) |
| 4191 |
3460 CALL CRJAB(1,PDPCL(1)) |
| 4192 |
C PDPCL(130) |
| 4193 |
C (P-P) DOUBLE PRODUCTION CRS. LOW ENERGY |
| 4194 |
GOTO 3020 |
| 4195 |
3470 IF(IN)3490,3480,3490 |
| 4196 |
3480 ANY=S(12) |
| 4197 |
3490 CALL CRJAB(1,DPCLN(1)) |
| 4198 |
C DPCLN(130) |
| 4199 |
C (N-P) DOUBLE PRODUCTION CRS. LOW ENERGY |
| 4200 |
GOTO 3020 |
| 4201 |
3500 IF(VALUE1-VALUE2)730,730,3510 |
| 4202 |
3510 CALL SIGNEX |
| 4203 |
IF(IN)2160,3520,2160 |
| 4204 |
3520 IF(ISW(3))3250,3150,3250 |
| 4205 |
3530 IF(CLSM-2.0)3550,3510,3040 |
| 4206 |
3540 IF(VALUE1-VALUE2)890 ,890 ,3550 |
| 4207 |
3550 CALL SIGNEX |
| 4208 |
IF(IN)2170,3230,2170 |
| 4209 |
3560 IF(ESPS(1))3580,3570,3580 |
| 4210 |
3570 NWDS=1 |
| 4211 |
GOTO 3610 |
| 4212 |
3580 NWDS=ESPS(1)*8.0+1.5 |
| 4213 |
C TOTAL NO. OF WORDS(ESCAPING PARTICLES) |
| 4214 |
IF(COUNT(6).GE.0.0) GO TO 3610 |
| 4215 |
C MINUS,RECORD NOT REPRESENTATIVE,SKIP |
| 4216 |
DO 3590 I=1,NWDS |
| 4217 |
3590 ESPS(I) = 0.0 |
| 4218 |
DO 3600 I=1,5 |
| 4219 |
3600 COUNT(I) = 0.0D0 |
| 4220 |
3610 NOR=NOR+1 |
| 4221 |
3620 IN=0 |
| 4222 |
GOTO(110,2770),IP |
| 4223 |
3630 IV=-1 |
| 4224 |
GOTO 2760 |
| 4225 |
C1370 RETURN |
| 4226 |
END |
| 4227 |
*CMZ : 1.01/04 10/06/93 14.43.37 by Christian Zeitnitz |
| 4228 |
*-- Author : |
| 4229 |
SUBROUTINE CABG6B |
| 4230 |
#include "cbert.inc" |
| 4231 |
*KEND. |
| 4232 |
C |
| 4233 |
SAVE |
| 4234 |
CALL CZERO |
| 4235 |
J=I2 |
| 4236 |
DO10 I=2,I4 |
| 4237 |
CE(I)=SPACE(J) |
| 4238 |
10 J=J+1 |
| 4239 |
J=I4+1 |
| 4240 |
DO20 I=J,6 |
| 4241 |
CE(I)=S(I3) |
| 4242 |
20 I3=I3+1 |
| 4243 |
RETURN |
| 4244 |
END |
| 4245 |
*CMZ : 0.92/03 10/12/92 10.53.07 by Christian Zeitnitz |
| 4246 |
*-- Author : |
| 4247 |
SUBROUTINE CABG6C(INT1) |
| 4248 |
SAVE |
| 4249 |
C |
| 4250 |
#include "cbert.inc" |
| 4251 |
*KEND. |
| 4252 |
C |
| 4253 |
IF(KNOT-7)10,190,190 |
| 4254 |
10 XABS=0.0 |
| 4255 |
IF(KNOT-2)20,30,30 |
| 4256 |
20 IF(INT1)70,100,70 |
| 4257 |
30 IF(KNOT-5)40,50,60 |
| 4258 |
40 IF(INT1)100,70,100 |
| 4259 |
50 IT=11 |
| 4260 |
IF(INT1)80,110,80 |
| 4261 |
60 IT=12 |
| 4262 |
IF(INT1)110,80,110 |
| 4263 |
70 IT=2*KNOT-1 |
| 4264 |
80 STRKP=-1.0 |
| 4265 |
90 I1=0 |
| 4266 |
GOTO130 |
| 4267 |
100 IT=2*KNOT |
| 4268 |
110 STRKP=-2.0 |
| 4269 |
120 I1=1 |
| 4270 |
130 I2=CLSM |
| 4271 |
CALLCBBBBB |
| 4272 |
140 CALLCAISOM |
| 4273 |
GOTO(150,150,150,160,150,150,180,180,180,180,180,180,150,150,150, |
| 4274 |
+150,160,150,150), KNOT |
| 4275 |
150 IF(RLKE-2500.0)170,170,140 |
| 4276 |
160 RLKE=0.0 |
| 4277 |
170 RETURN |
| 4278 |
180 IF(RLKE-3500.0)170,170,140 |
| 4279 |
190 IF(KNOT-12)200,200,310 |
| 4280 |
200 IF(IN)370,210,370 |
| 4281 |
210 IF(KNOT-8)220,270,320 |
| 4282 |
220 IF(INT1)230,250,230 |
| 4283 |
230 IT=2*(KNOT+1) |
| 4284 |
240 STRKP=-2.0 |
| 4285 |
GOTO90 |
| 4286 |
250 IT=2*KNOT+1 |
| 4287 |
260 STRKP=-1.0 |
| 4288 |
GOTO120 |
| 4289 |
270 IF(INT1)280,300,280 |
| 4290 |
280 IT=2*(KNOT+1) |
| 4291 |
290 GOTO80 |
| 4292 |
300 IT=2*KNOT+1 |
| 4293 |
GOTO110 |
| 4294 |
310 IF(KNOT-18)320,450,450 |
| 4295 |
320 IT=KNOT+10 |
| 4296 |
330 IF(KNOT-10)340,350,360 |
| 4297 |
340 IF(INT1)80,110,80 |
| 4298 |
350 IF(INT1)240,260,240 |
| 4299 |
360 IF(KNOT-12)340,350,430 |
| 4300 |
370 IF(KNOT-8)380,400,320 |
| 4301 |
380 IF(INT1)390,320,390 |
| 4302 |
390 IT=KNOT+11 |
| 4303 |
GOTO80 |
| 4304 |
400 IF(INT1)420,410,420 |
| 4305 |
410 IT=2*KNOT-1 |
| 4306 |
GOTO260 |
| 4307 |
420 IT=KNOT+KNOT |
| 4308 |
GOTO240 |
| 4309 |
430 XABS=0.0 |
| 4310 |
IF(KNOT-15)80,110,440 |
| 4311 |
440 IF(KNOT-18)110,80,110 |
| 4312 |
450 IT=28 |
| 4313 |
GOTO430 |
| 4314 |
END |
| 4315 |
*CMZ : 0.92/00 02/12/92 16.02.24 by Christian Zeitnitz |
| 4316 |
*-- Author : |
| 4317 |
SUBROUTINE CBG6CA(K,L) |
| 4318 |
C |
| 4319 |
#include "cbert.inc" |
| 4320 |
*KEND. |
| 4321 |
SAVE |
| 4322 |
C |
| 4323 |
CLSM=K |
| 4324 |
IF(IN)20,10,20 |
| 4325 |
10 CURR(10)=CLSM |
| 4326 |
CURR(11)=CLSM |
| 4327 |
C COLLISION MED. STORED IN REGION OF INITIAL COLL. AND |
| 4328 |
C MEDIUM WHERE PARTICLE WAS BORN |
| 4329 |
20 EFRP=SPACE(K+9)-7.0 |
| 4330 |
C PROTON WELL DEPTH + BINDING ENERGY=FERMI ENERGY PROTONS--MEV |
| 4331 |
EFRN=SPACE(K+3)-7.0 |
| 4332 |
PM(2)=DNCMS |
| 4333 |
C NUCLEON MASS PER CM |
| 4334 |
PM(1)=DNCMS |
| 4335 |
IF(K-L)30,40,50 |
| 4336 |
30 PM(1)=POMS |
| 4337 |
C PI0 MASS PER CM |
| 4338 |
GOTO50 |
| 4339 |
40 PM(1)=PNMS |
| 4340 |
C PI(+OR-) MASS PER CM |
| 4341 |
50 RETURN |
| 4342 |
END |
| 4343 |
*CMZ : 1.01/04 10/06/93 14.43.37 by Christian Zeitnitz |
| 4344 |
*-- Author : |
| 4345 |
SUBROUTINE CABIG7(C,GREAT,IX) |
| 4346 |
C |
| 4347 |
#include "crandm.inc" |
| 4348 |
*KEND. |
| 4349 |
C |
| 4350 |
REAL*8 C, GREAT |
| 4351 |
C |
| 4352 |
GREAT = C |
| 4353 |
I = IX + 1 |
| 4354 |
DO 10 K = 1,I |
| 4355 |
C = RANDC(ISEED) |
| 4356 |
IF(C.LT.GREAT) GO TO 10 |
| 4357 |
GREAT = C |
| 4358 |
10 CONTINUE |
| 4359 |
C GREAT IS THE LARGEST OF I RANDOM NOS. |
| 4360 |
RETURN |
| 4361 |
END |
| 4362 |
*CMZ : 0.90/00 05/06/92 10.53.27 by Christian Zeitnitz |
| 4363 |
*-- Author : |
| 4364 |
SUBROUTINE CBOVER(V,VE,VER) |
| 4365 |
SAVE |
| 4366 |
C |
| 4367 |
#include "cbert.inc" |
| 4368 |
*KEND. |
| 4369 |
REAL *8 V,VE,VER |
| 4370 |
C |
| 4371 |
VER=DSQRT(1.0-((VE*VE)/((V*RCPMV+VE)**2))) |
| 4372 |
VER=(DSQRT(VER*(6.91D-1+(VER*11.09D-1))+1.08D-1))/VER |
| 4373 |
RETURN |
| 4374 |
END |
| 4375 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 4376 |
*-- Author : |
| 4377 |
SUBROUTINE CCPES |
| 4378 |
SAVE |
| 4379 |
#include "cbert.inc" |
| 4380 |
*KEND. |
| 4381 |
C |
| 4382 |
#include "crn.inc" |
| 4383 |
*KEND. |
| 4384 |
C |
| 4385 |
I1=0 |
| 4386 |
I = IDINT(CURR(1) + 5.0D-2) |
| 4387 |
COUNT(I) = COUNT(I) + 1.0D0 |
| 4388 |
C*** COUNT NO. OF TIMES EACH TYPE OF PARTICLE ESCAPES |
| 4389 |
IF(CURR(1)-2.0)10,20,10 |
| 4390 |
10 K=CURR(10)+9.05 |
| 4391 |
GOTO30 |
| 4392 |
20 K=CURR(10)+3.05 |
| 4393 |
30 IF(ESPS(1)-60.0)60,40,40 |
| 4394 |
40 I1=1 |
| 4395 |
C STORAGE ALREADY FILLED |
| 4396 |
50 RETURN |
| 4397 |
60 L=ESPS(1)*8.D0 + 2.05D0 |
| 4398 |
ESPS(L)=CURR(1) |
| 4399 |
ESPS(L+1)=CURR(2)-SPACE(K) |
| 4400 |
M=13.05-CURR(11) |
| 4401 |
CC(M)=CC(M)+1.0 |
| 4402 |
M=4 |
| 4403 |
L=L+2 |
| 4404 |
N=L+2 |
| 4405 |
DO70 I=L,N |
| 4406 |
ESPS(I)=CURR(M+3) |
| 4407 |
ESPS(I+3)=CURR(M) |
| 4408 |
70 M=M+1 |
| 4409 |
ESPS(1)=ESPS(1)+1.0 |
| 4410 |
GOTO50 |
| 4411 |
END |
| 4412 |
*CMZ : 0.92/03 10/12/92 10.53.26 by Christian Zeitnitz |
| 4413 |
*-- Author : |
| 4414 |
SUBROUTINE COLE4 |
| 4415 |
SAVE |
| 4416 |
C |
| 4417 |
#include "cbert.inc" |
| 4418 |
*KEND. |
| 4419 |
C |
| 4420 |
K=CLSM |
| 4421 |
COM=(E(4)-DNCMS)/RCPMV |
| 4422 |
C K.E. OF PARTICLE 4 IN MEV |
| 4423 |
C TYPE OF PARTIL. 1-5 CURRENT NUCLEON |
| 4424 |
IF(CURR(1)-3.0)120,10,10 |
| 4425 |
10 IF(XABS)20,30,20 |
| 4426 |
20 COM=COM+ABSEC |
| 4427 |
GOTO120 |
| 4428 |
30 IF(IT-5)40,70,40 |
| 4429 |
40 IF(IT-24)50,70,50 |
| 4430 |
50 IF(IT-6)60,80,60 |
| 4431 |
60 IF(IT-26)120,80,120 |
| 4432 |
70 UNIV=0.0 |
| 4433 |
C NEUT WITH WRONG ENERGY |
| 4434 |
GOTO90 |
| 4435 |
80 UNIV=1.0 |
| 4436 |
90 UNIVE=SPACE(K+3)-SPACE(K+9) |
| 4437 |
C REGION I N-P WELL DEPTH DIFFERENCE |
| 4438 |
IF(UNIV)110,100,110 |
| 4439 |
100 COM=COM+UNIVE |
| 4440 |
GOTO120 |
| 4441 |
110 COM=COM-UNIVE |
| 4442 |
120 RETURN |
| 4443 |
END |
| 4444 |
*CMZ : 0.92/00 02/12/92 16.02.25 by Christian Zeitnitz |
| 4445 |
*-- Author : |
| 4446 |
SUBROUTINE CACOLL(M) |
| 4447 |
SAVE |
| 4448 |
#include "cbert.inc" |
| 4449 |
*KEND. |
| 4450 |
IF(M)10,20,20 |
| 4451 |
10 A=PM(4)*PM(4) |
| 4452 |
GOTO30 |
| 4453 |
20 A=SQNM |
| 4454 |
30 COL(15)=0.0 |
| 4455 |
MED=CLSM |
| 4456 |
ECO (1)=CFEPN(MED) |
| 4457 |
ECO (2)=CFEPN(MED+3) |
| 4458 |
C PROTON(NEUTRON) ENERGY CUT-OFF |
| 4459 |
COL(1)=E(1)+E(2) |
| 4460 |
C TOTAL ENERGY PARTICLES 1 AND 2 |
| 4461 |
DO40 I=1,3 |
| 4462 |
40 COL(I+1)=PM(I)*PM(I) |
| 4463 |
C MASS PARTICLE I SQD. |
| 4464 |
COL(5)=COL(3)+COL(2)+2.0*(E(1)*E(2)-(PXYZ(1)*PXYZ(2)+PXYZ(5)* |
| 4465 |
1PXYZ(6)+PXYZ(9)*PXYZ(10))) |
| 4466 |
COL(6)=DSQRT(COL(5)) |
| 4467 |
COL(7)=COL(6)/COL(1) |
| 4468 |
C GAM |
| 4469 |
COL(8)=2.0*COL(6) |
| 4470 |
COL(9)=(COL(4)+COL(5)-A)/COL(8) |
| 4471 |
COM2=COL(9)*COL(9) |
| 4472 |
50 IF(COL(4)-2.9882156D27)60,60,80 |
| 4473 |
C GT,PM(3)=ISOBAR--LTE,TEST FOR ROUNDOFF RANGE,(MIN)SQD+OR-5D23 |
| 4474 |
60 IF(COL(4)-2.9872156D27)90,70 ,70 |
| 4475 |
C LT,PION OR NUCLEON MASS=PM(3) |
| 4476 |
70 COL(4)=2.9877156D27 |
| 4477 |
PM(3) = 5.466005D13 |
| 4478 |
80 IF(COM2-COL(4))100,120,120 |
| 4479 |
90 IF(COL(4) - SQNM) 80,80,140 |
| 4480 |
C LTE,HAVE NUCLEON OR PION--GT,GO TO ERROR |
| 4481 |
100 IF(COM2 - 9.9D-1 * COL(4)) 120,110,110 |
| 4482 |
110 COM2 = COL(4) |
| 4483 |
COL(9) = PM(3) |
| 4484 |
120 COL(10)=DSQRT(COM2-COL(4)) |
| 4485 |
C P3 PRIME |
| 4486 |
COL(11)=(COL(5)+COL(2)-COL(3))/COL(8) |
| 4487 |
C E1 PRIME |
| 4488 |
COL(12)=DSQRT(COL(11)*COL(11)-COL(2)) |
| 4489 |
C P1 PRIME |
| 4490 |
COL(13)=(COL(7)*E(1)-COL(11))/COL(12) |
| 4491 |
C BETA |
| 4492 |
COM=1.0-(COL(13)*COL(13)+COL(7)*COL(7)) |
| 4493 |
IF(COM-5.0D-6)130,170,170 |
| 4494 |
130 IF(COM+5.0D-6)140,160,160 |
| 4495 |
140 COL(15)=1.0 |
| 4496 |
C ERROR |
| 4497 |
150 RETURN |
| 4498 |
160 COL(14)=2.236067977D-3 |
| 4499 |
GOTO180 |
| 4500 |
170 COL(14)=DSQRT(COM) |
| 4501 |
C ALPHA |
| 4502 |
180 E(3)=(COL(9)+COL(10)*(COL(13)*CST+COL(14)*SOPC*SNT))/COL(7) |
| 4503 |
E(4)=COL(1)-E(3) |
| 4504 |
GOTO150 |
| 4505 |
END |
| 4506 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 4507 |
*-- Author : |
| 4508 |
SUBROUTINE COLLM(M) |
| 4509 |
SAVE |
| 4510 |
#include "cbert.inc" |
| 4511 |
*KEND. |
| 4512 |
C |
| 4513 |
REAL *8 B |
| 4514 |
UNIV=E(2)+COL(6)-COL(11) |
| 4515 |
UNIVE=E(1)+COL(11) |
| 4516 |
UNIVER=COL(1)+COL(6) |
| 4517 |
K=16 |
| 4518 |
DO10 I=1,9,4 |
| 4519 |
COL(K)=(PXYZ(I)*UNIV-PXYZ(I+1)*UNIVE)/UNIVER |
| 4520 |
COL(K+3)=(PXYZ(I)+PXYZ(I+1))/COL(1) |
| 4521 |
C VX |
| 4522 |
10 K=K+1 |
| 4523 |
COL(22)=(PXYZ(10)*PXYZ(5)-PXYZ(9)*PXYZ(6))/COL(1) |
| 4524 |
C QX |
| 4525 |
COL(23)=(PXYZ(2)*PXYZ(9)-PXYZ(10)*PXYZ(1))/COL(1) |
| 4526 |
C QY |
| 4527 |
COL(24)=(PXYZ(6)*PXYZ(1)-PXYZ(5)*PXYZ(2))/COL(1) |
| 4528 |
A=SNT/COL(14) |
| 4529 |
B=A*COL(10) |
| 4530 |
C (-BETA*COS PHI*SIN THETA/ALPHA + COS THETA)/P1P*P3P |
| 4531 |
UNIV=COL(10)*(CST-A*SOPC*COL(13))/COL(12) |
| 4532 |
UNIVE=B*SOPS/COL(12) |
| 4533 |
C P3P*SIN PHI*SIN THETA/P1P*ALPHA |
| 4534 |
UNIVER=(SOPC*B)+((E(3)+COL(9))/(COL(7)+1.0)) |
| 4535 |
C COS PHI*SIN THETA*P3P/ALPHA + (E3+E3P)/(1.0+GAMMA) |
| 4536 |
K=19 |
| 4537 |
DO20 I=3,11,4 |
| 4538 |
PXYZ(I)=COL(K)*UNIVER+COL(K+3)*UNIVE+COL(K-3)*UNIV |
| 4539 |
20 K=K+1 |
| 4540 |
IF(M)30,40,30 |
| 4541 |
30 IF(PT(15))40,60,40 |
| 4542 |
40 DO50 I=1,9,4 |
| 4543 |
50 PXYZ(I+3)=PXYZ(I)+PXYZ(I+1)-PXYZ(I+2) |
| 4544 |
IF(M)60,130,60 |
| 4545 |
60 IF(PT(3))70,100,70 |
| 4546 |
70 PT(4)=PM(3) |
| 4547 |
I1=3 |
| 4548 |
80 I2=-1 |
| 4549 |
CALLPSTOR |
| 4550 |
90 IF(I1-3)100,100,120 |
| 4551 |
100 IF(PT(15))110,120,110 |
| 4552 |
110 PT(16)=DNCMS |
| 4553 |
C NUCLEON MASS PER CM |
| 4554 |
I1=4 |
| 4555 |
GOTO80 |
| 4556 |
120 PT(27)=0.0 |
| 4557 |
PT(39)=0.0 |
| 4558 |
130 RETURN |
| 4559 |
END |
| 4560 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 4561 |
*-- Author : |
| 4562 |
SUBROUTINE CRDET(NODATA,DATA,ENER) |
| 4563 |
REAL*8 DATA(6426),ENER |
| 4564 |
#include "cbert.inc" |
| 4565 |
*KEND. |
| 4566 |
SAVE |
| 4567 |
C |
| 4568 |
IE=DABS(ENER/20.0) |
| 4569 |
C ENERGY INTERVAL |
| 4570 |
UNIV=(ENER-DFLOAT(IE)*20.0)/20.0 |
| 4571 |
C INPT=0 IF WHOLE INTERVAL CONSIDERED |
| 4572 |
C NODATA=DATA PER ENERGY INTERVAL |
| 4573 |
DO10 I=1,25 |
| 4574 |
10 CRDT(I)=0.0 |
| 4575 |
C ANSWERS STORED IN CRDT |
| 4576 |
20 K=(NODATA*IE)+1 |
| 4577 |
30 IF(INPT)40,50 ,80 |
| 4578 |
40 WRITE(6,*) ' CALOR: ERROR in CRDET ====> STOP' |
| 4579 |
STOP |
| 4580 |
50 N=NODATA |
| 4581 |
60 L=K+NODATA |
| 4582 |
DO70 I=1,N |
| 4583 |
CRDT(I)=(DATA(L)-DATA(K))*UNIV+DATA(K) |
| 4584 |
K=K+1 |
| 4585 |
70 L=L+1 |
| 4586 |
INPT=0 |
| 4587 |
RETURN |
| 4588 |
80 K=INPT-1+K |
| 4589 |
N=2 |
| 4590 |
GOTO60 |
| 4591 |
C NOT ALL PARTS EVALUATED |
| 4592 |
END |
| 4593 |
*CMZ : 0.90/00 29/07/92 13.00.25 by Christian Zeitnitz |
| 4594 |
*-- Author : |
| 4595 |
SUBROUTINE CRJAB(K1,PP) |
| 4596 |
#include "cbert.inc" |
| 4597 |
#include "crandm.inc" |
| 4598 |
*KEND. |
| 4599 |
REAL*8 PP(380) |
| 4600 |
C |
| 4601 |
CALL CRDET(K1,PP(1),VALUE1) |
| 4602 |
VALUE1=(PXYZ(1)*PXYZ(2)+PXYZ(5)*PXYZ(6)+PXYZ(9)*PXYZ(10)) |
| 4603 |
1/E(1) |
| 4604 |
C P1.P2/E(1) |
| 4605 |
VALUE2=(VALUE1/(P2*P2))*((E(2)/DNCMS)-1.0)-(1.0/DNCMS) |
| 4606 |
C S=((P1.P2)/(E1*P2*P2))*((E2/M)-1.0)-1.0/M |
| 4607 |
VALUE2=DNCMS*CRDT(1)*DSQRT(P1OE1*P1OE1+2.0*VALUE1 |
| 4608 |
1*VALUE2+P2*P2*VALUE2*VALUE2)/(E(2)*P1OE1*ANY) |
| 4609 |
C (M)(C.S)(J**2+2S(P1.P2)/E1+(P2)(P2)(S)(S) |
| 4610 |
CZ changed 20.june 92 CZ |
| 4611 |
IF(VALUE2.GT.1.0) VALUE2 = 1.0 |
| 4612 |
C THIS TESTS SAMPLING TECH.TO ENSURE FMAXS WERE SELECTED SO THAT |
| 4613 |
C VALUE2 LTE ONE. |
| 4614 |
VALUE1 = RANDC(ISEED) |
| 4615 |
RETURN |
| 4616 |
END |
| 4617 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 4618 |
*-- Author : |
| 4619 |
SUBROUTINE DCINTP(W) |
| 4620 |
#include "cbert.inc" |
| 4621 |
*KEND. |
| 4622 |
C |
| 4623 |
#include "crandm.inc" |
| 4624 |
*KEND. |
| 4625 |
REAL*8 W(250),Z(24),FLTI |
| 4626 |
SAVE |
| 4627 |
C |
| 4628 |
Z(1)=RLKE-6.6D2 |
| 4629 |
IE=IDINT(Z(1)/2.0D1+5.0D-6) |
| 4630 |
UNIV=(Z(1)-DFLOAT(IE)*2.0D1)/2.0D1 |
| 4631 |
IE=IE+1 |
| 4632 |
UNIVE=(W(IE+1)-W(IE))*UNIV+W(IE) |
| 4633 |
C RATIO |
| 4634 |
I2=0 |
| 4635 |
K=1 |
| 4636 |
UNIV = RANDC(ISEED) |
| 4637 |
IF(UNIV.GE.UNIVE)GOTO190 |
| 4638 |
C LT=BACKWARD |
| 4639 |
C N-P ELASTIC SCAT.,RLKE GT 660 |
| 4640 |
LLL=179 |
| 4641 |
IF(W(180).GT.RLKE) GO TO 20 |
| 4642 |
DO 10 I = 1,5 |
| 4643 |
IF(W(179+K).GT.RLKE)GO TO 40 |
| 4644 |
10 K=K+12 |
| 4645 |
20 I1=-1 |
| 4646 |
C ERROR |
| 4647 |
30 RETURN |
| 4648 |
40 M=12 |
| 4649 |
50 DO60 L=1,M |
| 4650 |
Z(L+M)=W(LLL+K) |
| 4651 |
Z(L)=W(LLL+K-M) |
| 4652 |
60 K=K+1 |
| 4653 |
UNIV = RANDC(ISEED) |
| 4654 |
UNIVE=(RLKE-Z(1))/(Z(M+1)-Z(1)) |
| 4655 |
DO70 I=2,M |
| 4656 |
P=(Z(I+M)-Z(I))*UNIVE+Z(I) |
| 4657 |
IF(P.GE.UNIV) GO TO 80 |
| 4658 |
70 CONTINUE |
| 4659 |
GO TO 20 |
| 4660 |
80 I1=I |
| 4661 |
UNIV = RANDC(ISEED) |
| 4662 |
FLTI=UNIV+DFLOAT(I1-2) |
| 4663 |
IF(M.LE.9) GO TO 230 |
| 4664 |
90 GOTO(20,100,100,110,120,130,130,140,150,160,170,180),I1 |
| 4665 |
100 CST=1.0D-2*FLTI-0.1D1 |
| 4666 |
GO TO 30 |
| 4667 |
110 CST=2.0D-2*UNIV-9.8D-1 |
| 4668 |
GO TO 30 |
| 4669 |
120 CST=4.0D-2*UNIV-9.6D-1 |
| 4670 |
GO TO 30 |
| 4671 |
130 CST=6.0D-2*FLTI-0.116D1 |
| 4672 |
GO TO 30 |
| 4673 |
140 CST=8.0D-2*UNIV-8.0D-1 |
| 4674 |
GO TO 30 |
| 4675 |
150 CST=1.0D-1*UNIV-7.2D-1 |
| 4676 |
GO TO 30 |
| 4677 |
160 CST=1.2D-1*UNIV-6.2D-1 |
| 4678 |
GO TO 30 |
| 4679 |
170 CST=2.0D-1*UNIV-5.0D-1 |
| 4680 |
GO TO 30 |
| 4681 |
180 CST=3.0D-1*(UNIV-1.0D0) |
| 4682 |
GO TO 30 |
| 4683 |
C FORWARD |
| 4684 |
190 LLL=143 |
| 4685 |
IF(W(144).GT.RLKE) GO TO 20 |
| 4686 |
200 DO 210 I = 1,4 |
| 4687 |
IF(W(143+K).GT.RLKE) GO TO 220 |
| 4688 |
210 K=K+9 |
| 4689 |
GOTO20 |
| 4690 |
220 M=9 |
| 4691 |
GOTO50 |
| 4692 |
230 GOTO(20,240,240,240,240,250,260,270,280),I1 |
| 4693 |
240 CST=1.0D0-2.5D-2*FLTI |
| 4694 |
GOTO30 |
| 4695 |
250 CST=8.5D-1+0.5D-1*UNIV |
| 4696 |
GOTO30 |
| 4697 |
260 CST=7.0D-1+1.5D-1*UNIV |
| 4698 |
GOTO30 |
| 4699 |
270 CST=5.0D-1+2.0D-1*UNIV |
| 4700 |
GOTO30 |
| 4701 |
280 CST=5.0D-1*UNIV |
| 4702 |
GOTO30 |
| 4703 |
END |
| 4704 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 4705 |
*-- Author : |
| 4706 |
SUBROUTINE CADCPR(W,LK) |
| 4707 |
#include "cbert.inc" |
| 4708 |
*KEND. |
| 4709 |
C |
| 4710 |
#include "crandm.inc" |
| 4711 |
*KEND. |
| 4712 |
REAL*8 W(60),Z(24) |
| 4713 |
REAL*8 FRACT,R,SUM,FLTI |
| 4714 |
SAVE |
| 4715 |
C |
| 4716 |
C PDCI HAS KK=12, PDCH HAS KK=11 |
| 4717 |
I2=0 |
| 4718 |
KK=LK |
| 4719 |
K=1 |
| 4720 |
DO10 I=1,5 |
| 4721 |
IF(W(K).GE.RLKE)GOTO40 |
| 4722 |
10 K=K+KK |
| 4723 |
20 I2=1 |
| 4724 |
C ERROR RETURN |
| 4725 |
30 RETURN |
| 4726 |
40 DO 50 L = 1,KK |
| 4727 |
Z(L+KK)=W(K) |
| 4728 |
Z(L)=W(K-KK) |
| 4729 |
50 K=K+1 |
| 4730 |
SUM=0.0D0 |
| 4731 |
R = RANDC(ISEED) |
| 4732 |
FRACT=(RLKE-Z(1))/(Z(KK+1)-Z(1)) |
| 4733 |
DO 60 I = 2,KK |
| 4734 |
SUM=SUM+Z(I)+((Z(I+KK)-Z(I))*FRACT) |
| 4735 |
IF(R.LT.SUM) GO TO 70 |
| 4736 |
60 CONTINUE |
| 4737 |
GO TO 20 |
| 4738 |
C ERROR |
| 4739 |
70 R = RANDC(ISEED) |
| 4740 |
I1=I |
| 4741 |
IF(KK.GT.11) GO TO 90 |
| 4742 |
IF(I1.GT.2) GO TO 80 |
| 4743 |
CST=4.0D-1*R |
| 4744 |
GO TO 150 |
| 4745 |
80 I1=I1+1 |
| 4746 |
90 FLTI=DFLOAT(I1-2)+R |
| 4747 |
100 GO TO (20,110,110,110,120,120,130,130,130,130,140,140),I1 |
| 4748 |
110 CST=2.0D-1*(FLTI) |
| 4749 |
GO TO 150 |
| 4750 |
120 CST=3.0D-1+1.0D-1*(FLTI) |
| 4751 |
GO TO 150 |
| 4752 |
130 CST=6.0D-1+4.0D-2*(FLTI) |
| 4753 |
GO TO 150 |
| 4754 |
140 CST=7.8D-1+2.0D-2*(FLTI) |
| 4755 |
150 R = RANDC(ISEED) |
| 4756 |
IF(R.GT.5.0D-1) GO TO 30 |
| 4757 |
CST=-(CST) |
| 4758 |
GO TO 30 |
| 4759 |
END |
| 4760 |
*CMZ : 0.92/00 02/12/92 16.02.25 by Christian Zeitnitz |
| 4761 |
*-- Author : |
| 4762 |
SUBROUTINE DFMAX |
| 4763 |
SAVE |
| 4764 |
#include "cbert.inc" |
| 4765 |
*KEND. |
| 4766 |
REAL*8 WK |
| 4767 |
C |
| 4768 |
I=I2 |
| 4769 |
IF(CURR(1)-2.0)20,10,10 |
| 4770 |
10 I=I+3 |
| 4771 |
20 WK=WKRPN(I) |
| 4772 |
30 CALL CBOVER(WK,DNCMS,UNIV) |
| 4773 |
IF(WK-560.0)40,40,60 |
| 4774 |
40 FMAX(1)=27.2D-27*UNIV |
| 4775 |
C 820 MEV |
| 4776 |
C (P-P)S |
| 4777 |
FMAX(2)=38.0D-27*UNIV |
| 4778 |
C 230 MEV |
| 4779 |
C (P-N)S |
| 4780 |
FMAX(3)=22.6D-27*UNIV |
| 4781 |
C 1020 MEV |
| 4782 |
C (P-P)S.P. |
| 4783 |
FMAX(4)=14.0D-27*UNIV |
| 4784 |
C 750 MEV |
| 4785 |
C (P-N)S.P. |
| 4786 |
FMAX(5)=0.0 |
| 4787 |
C (P-P)D.P. |
| 4788 |
FMAX(6)=0.0 |
| 4789 |
C (P-N)D.P.) |
| 4790 |
50 RETURN |
| 4791 |
60 IF(WK-800.0)70,90,90 |
| 4792 |
70 FMAX(2)=37.0D-27*UNIV |
| 4793 |
C 250 MEV |
| 4794 |
FMAX(5)=1.9D-27*UNIV |
| 4795 |
C 5 AN6 AT 1380 MEV |
| 4796 |
FMAX(6)=9.0D-27*UNIV |
| 4797 |
80 FMAX(1)=27.2D-27*UNIV |
| 4798 |
C 820 MEV |
| 4799 |
FMAX(3)=22.6D-27*UNIV |
| 4800 |
C 1020 |
| 4801 |
FMAX(4)=14.0D-27*UNIV |
| 4802 |
C 750 |
| 4803 |
GO TO 50 |
| 4804 |
90 IF(WK-1680.0)100,110,110 |
| 4805 |
100 FMAX(2)=33.0D-27*UNIV |
| 4806 |
C 400 |
| 4807 |
FMAX(5)=10.8D-27*UNIV |
| 4808 |
C 5 AND 6 AT 2600 |
| 4809 |
FMAX(6)=17.4D-27*UNIV |
| 4810 |
GO TO 80 |
| 4811 |
110 FMAX(1)=26.3D-27*UNIV |
| 4812 |
C 1000 |
| 4813 |
FMAX(2)=24.7D-27*UNIV |
| 4814 |
C 1000 |
| 4815 |
FMAX(3)=22.6D-27*UNIV |
| 4816 |
C 1020 |
| 4817 |
FMAX(4)=13.5D-27*UNIV |
| 4818 |
C 1000 |
| 4819 |
FMAX(5)=18.0D-27*UNIV |
| 4820 |
FMAX(6)=23.6D-27*UNIV |
| 4821 |
C 3500 |
| 4822 |
GO TO 50 |
| 4823 |
END |
| 4824 |
*CMZ : 0.92/00 02/12/92 16.02.25 by Christian Zeitnitz |
| 4825 |
*-- Author : |
| 4826 |
SUBROUTINE CAECPL |
| 4827 |
#include "cbert.inc" |
| 4828 |
*KEND. |
| 4829 |
C |
| 4830 |
SAVE |
| 4831 |
I1=0 |
| 4832 |
MED=CLSM |
| 4833 |
IF(PT(38))590,10,590 |
| 4834 |
10 IF(CURR(1)-1.0)380,540,20 |
| 4835 |
20 IF(CURR(1)-3.0)450,420,30 |
| 4836 |
30 IF(CURR(1)-5.0)320,40,380 |
| 4837 |
40 IF(STRKP+1.0)50,60,380 |
| 4838 |
50 IF(STRKP+2.0)380,230,380 |
| 4839 |
60 IF(PT(2)-2.0)80,70,80 |
| 4840 |
70 PT(3)=VNVP(MED) |
| 4841 |
GOTO90 |
| 4842 |
C PI-,CURR(1)=5.0,PT6+1=0,STRKP=1.0 |
| 4843 |
80 PT(3)=0.0 |
| 4844 |
90 PT(15)=HVP(MED) |
| 4845 |
IF(PT(26)-1.0)380,190,100 |
| 4846 |
100 IF(PT(26)-2.0)380,110,380 |
| 4847 |
110 PT(27)=-PPAN(MED) |
| 4848 |
IF(CURR(1)-2.0)580,120,120 |
| 4849 |
C PPAN=-VNHP(NEUT.WELL DEPTH-1/2PROTON WELL DEPTH) |
| 4850 |
120 IF(CURR(1)-4.0)440,380,130 |
| 4851 |
130 IF(PT(2)-3.0)380,150,140 |
| 4852 |
140 IF(PT(2)-5.0)170,180,380 |
| 4853 |
150 IF(PT(14)-5.0)380,160,380 |
| 4854 |
160 RETURN |
| 4855 |
170 IF(PT(14)-4.0)380,160,380 |
| 4856 |
180 IF(PT(14)-3.0)380,160,380 |
| 4857 |
C 1/2PROT.WELL DEPTH |
| 4858 |
190 PT(27)=HVP(MED) |
| 4859 |
IF(CURR(1)-2.0)560,200,200 |
| 4860 |
200 IF(CURR(1)-4.0)400,380,210 |
| 4861 |
210 IF(PT(2)-4.0)380,150,220 |
| 4862 |
220 IF(PT(2)-5.0)380,170,380 |
| 4863 |
230 PT(3)=-VNVP(MED) |
| 4864 |
240 PT(15)=-PMAC(MED) |
| 4865 |
250 IF(PT(26)-1.0)380,270,260 |
| 4866 |
260 IF(PT(26)-2.0)380,300,380 |
| 4867 |
270 PT(27)=-PMAC(MED) |
| 4868 |
IF(CURR(1)-2.0)150,150,280 |
| 4869 |
280 IF(CURR(1)-4.0)130,210,290 |
| 4870 |
290 IF(PT(2)-5.0)380,150,380 |
| 4871 |
300 PT(27)=HVN(MED) |
| 4872 |
IF(CURR(1)-2.0)170,170,310 |
| 4873 |
310 IF(CURR(1)-4.0)400,130,210 |
| 4874 |
320 IF(STRKP+1.0)330,340,380 |
| 4875 |
330 IF(STRKP+2.0)380,230,380 |
| 4876 |
C PI0 |
| 4877 |
340 PT(3)=0.0 |
| 4878 |
350 PT(15)=HVP(MED) |
| 4879 |
IF(PT(26)-1.0)380,370,360 |
| 4880 |
360 IF(PT(26)-2.0)380,390,380 |
| 4881 |
370 PT(27)=HVP(MED) |
| 4882 |
IF(CURR(1)-4.0)170,130,380 |
| 4883 |
380 I1=1 |
| 4884 |
GOTO160 |
| 4885 |
390 PT(27)=-PPAN(MED) |
| 4886 |
IF(CURR(1)-4.0)180,400,380 |
| 4887 |
400 IF(PT(2)-3.0)380,170,410 |
| 4888 |
410 IF(PT(2)-4.0)380,180,380 |
| 4889 |
420 IF(STRKP+1.0)430,60,380 |
| 4890 |
C PI+ |
| 4891 |
430 IF(STRKP+2.0)380,230,380 |
| 4892 |
440 IF(PT(2)-3.0)380,180,380 |
| 4893 |
450 IF(STRKP+1.0)460,470,380 |
| 4894 |
C NEUTRON |
| 4895 |
460 IF(STRKP+2.0)380,490,380 |
| 4896 |
470 PT(3)=0.0 |
| 4897 |
IF(PT(2)-1.0)380,240,480 |
| 4898 |
480 IF(PT(2)-2.0)380,350,380 |
| 4899 |
490 PT(15)=-PMAC(MED) |
| 4900 |
IF(PT(2)-1.0)380,510,500 |
| 4901 |
500 IF(PT(2)-2.0)380,530,380 |
| 4902 |
510 IF(PT(26)-2.0)380,520,380 |
| 4903 |
520 PT(3)=-VNVP(MED) |
| 4904 |
PT(27)=HVN(MED) |
| 4905 |
GOTO150 |
| 4906 |
530 PT(3)=0.0 |
| 4907 |
GOTO250 |
| 4908 |
540 IF(STRKP+1.0)550,60,380 |
| 4909 |
550 IF(STRKP+2.0)380,470,380 |
| 4910 |
C PROTON |
| 4911 |
560 IF(PT(2)-1.0)380,170,570 |
| 4912 |
570 IF(PT(2)-2.0)380,180,380 |
| 4913 |
580 IF(PT(2)-1.0)380,180,380 |
| 4914 |
590 IF(CURR(1)-1.0)380,610,600 |
| 4915 |
600 IF(CURR(1)-2.0)380,630,380 |
| 4916 |
610 IF(STRKP+1.0)620,840,380 |
| 4917 |
620 IF(STRKP+2.0)380,650,380 |
| 4918 |
630 IF(STRKP+1.0)640,650,380 |
| 4919 |
640 IF(STRKP+2.0)380,960,380 |
| 4920 |
650 IF(PT(14))380,380,660 |
| 4921 |
660 IF(PT(38))380,380,670 |
| 4922 |
670 IF(PT(38)-2.0)680,740,380 |
| 4923 |
680 IF(PT(14)-2.0)690,800,380 |
| 4924 |
690 PT(3)=TFFN(MED) |
| 4925 |
PT(15)=TFFN(MED) |
| 4926 |
PT(27)=TFFN(MED) |
| 4927 |
PT(39)=TFFN(MED) |
| 4928 |
700 IF(PT(2)-3.0)380,380,710 |
| 4929 |
710 IF(PT(2)-5.0)730,720,380 |
| 4930 |
720 IF(PT(26)-4.0)380,160,380 |
| 4931 |
730 IF(PT(26)-5.0)380,160,380 |
| 4932 |
740 IF(PT(14)-2.0)750,810,380 |
| 4933 |
750 PT(27)=FFPTFN(MED) |
| 4934 |
PT(3)=FVNP(MED) |
| 4935 |
760 PT(39)=FVNP(MED) |
| 4936 |
PT(15)=FVNP(MED) |
| 4937 |
770 IF(PT(2)-3.0)380,730,780 |
| 4938 |
780 IF(PT(2)-5.0)720,790,380 |
| 4939 |
790 IF(PT(26)-3.0)380,160,380 |
| 4940 |
800 PT(3)=FFPTFN(MED) |
| 4941 |
PT(27)=FVNP(MED) |
| 4942 |
GOTO760 |
| 4943 |
810 PT(3)=TFFN(MED) |
| 4944 |
PT(27)=TFFN(MED) |
| 4945 |
PT(15)=TFFP(MED) |
| 4946 |
PT(39)=TFFP(MED) |
| 4947 |
820 IF(PT(2)-3.0)380,720,830 |
| 4948 |
830 IF(PT(2)-4.0)380,790,380 |
| 4949 |
840 IF(PT(14))380,380,850 |
| 4950 |
850 IF(PT(38)-1.0)380,870,860 |
| 4951 |
860 IF(PT(38)-2.0)380,930,380 |
| 4952 |
870 IF(PT(14)-2.0)880,900,380 |
| 4953 |
880 PT(3)=HVP(MED) |
| 4954 |
890 PT(15)=HVP(MED) |
| 4955 |
PT(27)=HVP(MED) |
| 4956 |
PT(39)=HVP(MED) |
| 4957 |
IF(PT(14)-2.0)770,700,380 |
| 4958 |
900 PT(27)=HVN(MED) |
| 4959 |
910 PT(3)=-PMAC(MED) |
| 4960 |
920 PT(39)=HVN(MED) |
| 4961 |
PT(15)=HVN(MED) |
| 4962 |
IF(PT(38)-2.0)820,770,380 |
| 4963 |
930 IF(PT(14)-2.0)940,950,380 |
| 4964 |
940 PT(3)=HVN(MED) |
| 4965 |
PT(15)=HVN(MED) |
| 4966 |
PT(27)=-PMAC(MED) |
| 4967 |
PT(39)=HVN(MED) |
| 4968 |
GOTO820 |
| 4969 |
950 PT(15)=-PPAN(MED) |
| 4970 |
PT(39)=-PPAN(MED) |
| 4971 |
PT(3)=HVP(MED) |
| 4972 |
PT(27)=HVP(MED) |
| 4973 |
IF(PT(2)-3.0)380,790,380 |
| 4974 |
960 IF(PT(14))380,380,970 |
| 4975 |
970 IF(PT(38)-1.0)380,990,980 |
| 4976 |
980 IF(PT(38)-2.0)380,1020,380 |
| 4977 |
990 IF(PT(14)-2.0)1000,1010,380 |
| 4978 |
1000 PT(39)=-PMAC(MED) |
| 4979 |
PT(15)=-PMAC(MED) |
| 4980 |
PT(27)=-PMAC(MED) |
| 4981 |
PT(3)=-PMAC(MED) |
| 4982 |
IF(PT(2)-5.0)380,730,380 |
| 4983 |
1010 PT(3)=THPN(MED) |
| 4984 |
GOTO890 |
| 4985 |
1020 IF(PT(14)-2.0)1030,1040,380 |
| 4986 |
1030 PT(3)=HVP(MED) |
| 4987 |
PT(15)=HVP(MED) |
| 4988 |
PT(39)=HVP(MED) |
| 4989 |
PT(27)=THPN(MED) |
| 4990 |
GOTO700 |
| 4991 |
1040 PT(27)=-PMAC(MED) |
| 4992 |
GOTO910 |
| 4993 |
END |
| 4994 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 4995 |
*-- Author : |
| 4996 |
SUBROUTINE CERROR(CARG) |
| 4997 |
C |
| 4998 |
#include "minput.inc" |
| 4999 |
#include "cerrcm.inc" |
| 5000 |
*KEND. |
| 5001 |
C |
| 5002 |
CHARACTER*1 CARG(50),CPRT(50) |
| 5003 |
CHARACTER*1 ZEI,CEND |
| 5004 |
DATA CEND/'$'/ |
| 5005 |
C |
| 5006 |
DO 10 I=1,50 |
| 5007 |
ZEI=CARG(I) |
| 5008 |
IF(ZEI.EQ.CEND) GOTO 20 |
| 5009 |
CPRT(I)=CARG(I) |
| 5010 |
10 CONTINUE |
| 5011 |
20 DO 30 J=I,50 |
| 5012 |
CPRT(J)=' ' |
| 5013 |
30 CONTINUE |
| 5014 |
WRITE(IOUT,*) ' HETC : ERROR in ',CPRT |
| 5015 |
C |
| 5016 |
CERRF = .TRUE. |
| 5017 |
RETURN |
| 5018 |
END |
| 5019 |
*CMZ : 0.92/00 02/12/92 16.02.25 by Christian Zeitnitz |
| 5020 |
*-- Author : |
| 5021 |
SUBROUTINE EXPRN(EXPA) |
| 5022 |
C |
| 5023 |
#include "crandm.inc" |
| 5024 |
*KEND. |
| 5025 |
C |
| 5026 |
REAL * 8 EXPA,EXPB,WHOLE,EXPAO |
| 5027 |
C |
| 5028 |
WHOLE=0.0 |
| 5029 |
10 EXPA = RANDC(ISEED) |
| 5030 |
EXPAO=EXPA |
| 5031 |
20 EXPB = RANDC(ISEED) |
| 5032 |
IF(EXPB.LT.EXPA) GO TO 40 |
| 5033 |
C RANDOM2 IS.GTE.TO RANDOM1 |
| 5034 |
30 EXPA=EXPAO+WHOLE |
| 5035 |
RETURN |
| 5036 |
40 EXPA = RANDC(ISEED) |
| 5037 |
IF(EXPA.LT.EXPB) GO TO 20 |
| 5038 |
WHOLE=WHOLE+1.0 |
| 5039 |
GO TO 10 |
| 5040 |
END |
| 5041 |
*CMZ : 0.92/00 02/12/92 16.02.25 by Christian Zeitnitz |
| 5042 |
*-- Author : |
| 5043 |
SUBROUTINE FRMICC(GPART) |
| 5044 |
#include "crandm.inc" |
| 5045 |
*KEND. |
| 5046 |
DIMENSION G(3) |
| 5047 |
REAL * 8 GPART,G |
| 5048 |
SAVE |
| 5049 |
C |
| 5050 |
DO 10 I = 1,3 |
| 5051 |
10 G(I) = RANDC(ISEED) |
| 5052 |
C FIND LARGEST OF 3 RANDOM NOS. |
| 5053 |
IF(G(3).LT.G(2)) GO TO 40 |
| 5054 |
C 3.GTE.2 |
| 5055 |
IF(G(3).LT.G(1))GO TO 30 |
| 5056 |
C 3.GTE.2,AND 3.GTE.1 |
| 5057 |
GPART=G(3) |
| 5058 |
20 RETURN |
| 5059 |
30 GPART=G(1) |
| 5060 |
C 3.GTE.2 AND 3.LT.1 OR 3.LT.2 AND 2.LT.1 |
| 5061 |
GO TO 20 |
| 5062 |
40 IF(G(2).LT.G(1))GO TO 30 |
| 5063 |
GPART=G(2) |
| 5064 |
C 3.LT.2,AND 2.GTE.1 |
| 5065 |
GO TO 20 |
| 5066 |
END |
| 5067 |
*CMZ : 0.92/00 02/12/92 16.02.25 by Christian Zeitnitz |
| 5068 |
*-- Author : |
| 5069 |
SUBROUTINE CAGENE(Z) |
| 5070 |
IMPLICIT REAL*8 (A-H,O-Z) |
| 5071 |
REAL*8 Z(101) |
| 5072 |
#include "cbert.inc" |
| 5073 |
*KEND. |
| 5074 |
SAVE |
| 5075 |
C |
| 5076 |
CD=COM*1.0D2 |
| 5077 |
I=IDINT(CD+1.00D0) |
| 5078 |
AZ=Z(I) |
| 5079 |
IF(I.EQ.1)GOTO150 |
| 5080 |
10 BZ=Z(I+1) |
| 5081 |
IF(101-(I+1))70,20,30 |
| 5082 |
20 CZ=BZ+5.0D-1*(BZ-AZ) |
| 5083 |
GOTO40 |
| 5084 |
30 CZ=Z(I+2) |
| 5085 |
40 XZ=CD-DFLOAT(I-1) |
| 5086 |
SCA=CZ-AZ |
| 5087 |
C F(2)-F(0) |
| 5088 |
50 SBA=BZ-AZ |
| 5089 |
C F(1)-F(0) |
| 5090 |
SQA=AZ*AZ |
| 5091 |
C F(0)**2 |
| 5092 |
SQAC=SQA-CZ*CZ |
| 5093 |
C F(0)**2-F(2)**2 |
| 5094 |
SQBA=BZ*BZ-SQA |
| 5095 |
C F(1)**2-F(0)**2 |
| 5096 |
RB=SQAC+SQBA+SQBA |
| 5097 |
C (ASQ-CSQ)+2(BSQ-ASQ) |
| 5098 |
CZ |
| 5099 |
CZ changed in order to keep exponent small 5/21/92 |
| 5100 |
RC=AZ*1.0D-20*CZ*SCA-SBA*1.0D-20*(2.0D0*AZ*BZ+XZ*(BZ-CZ)*SCA) |
| 5101 |
CZ RC is 1E-20 smaller than it supposed to be !!!! |
| 5102 |
RA=SCA-SBA-SBA |
| 5103 |
C (C-A)-2(B-A) |
| 5104 |
IF(RA.NE.0.0)GOTO60 |
| 5105 |
COM=AZ+XZ*SBA |
| 5106 |
GOTO80 |
| 5107 |
60 CONTINUE |
| 5108 |
CZ \/ factor 1E-20 in RC !! |
| 5109 |
DISC=RB*1.0D-20*RB-4.0D0*RA*RC |
| 5110 |
IF(DISC)70,90,90 |
| 5111 |
C B**2-4AC |
| 5112 |
70 CALL CERROR('CAGENE1$') |
| 5113 |
80 RETURN |
| 5114 |
CZ \/ correct for factor 1E-20 |
| 5115 |
90 DISC=DSQRT(DISC)*1.0D10 |
| 5116 |
CZ end of change |
| 5117 |
CZ |
| 5118 |
PLUS=(DISC-RB)/(RA+RA) |
| 5119 |
AMINUS=(-RB-DISC)/(RA+RA) |
| 5120 |
IF(I.EQ.1)GOTO160 |
| 5121 |
100 IF(PLUS.GT.BZ)GOTO120 |
| 5122 |
IF(PLUS.LT.AZ)GOTO120 |
| 5123 |
IF(AMINUS.GT.BZ)GOTO110 |
| 5124 |
IF(AMINUS.GE.AZ)GOTO140 |
| 5125 |
110 COM=PLUS |
| 5126 |
GOTO80 |
| 5127 |
120 IF(AMINUS.GT.BZ)GOTO70 |
| 5128 |
IF(AMINUS.LT.AZ)GOTO70 |
| 5129 |
130 COM=AMINUS |
| 5130 |
GOTO80 |
| 5131 |
140 RA=XZ*SBA+AZ |
| 5132 |
RB=DABS(RA-AMINUS) |
| 5133 |
RC=DABS(RA-PLUS) |
| 5134 |
IF(RB.GT.RC)GOTO110 |
| 5135 |
GOTO130 |
| 5136 |
150 CZ=Z(I+1) |
| 5137 |
SCA=CZ-AZ |
| 5138 |
BZ=AZ+SCA*7.071067812D-1 |
| 5139 |
XZ=CD+CD |
| 5140 |
GOTO50 |
| 5141 |
C (CZ-AZ)(CZ-AZ)=C,CZ=MASS FOR R=1,AZ=MASS FOR R=0, C=CONST.FOR PARABOLA |
| 5142 |
C (M-AZ)(M-AZ)=0.5*C,DETERMINES MASS,BZ,FOR R=1/2 |
| 5143 |
160 BZ=CZ |
| 5144 |
XZ=XZ-CD |
| 5145 |
SBA=CZ-AZ |
| 5146 |
GOTO100 |
| 5147 |
END |
| 5148 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 5149 |
*-- Author : |
| 5150 |
SUBROUTINE CALGEO |
| 5151 |
#include "cbert.inc" |
| 5152 |
*KEND. |
| 5153 |
REAL * 8 T1,T2,T3,T4,T5,T6,TEMP,TEMPO |
| 5154 |
SAVE |
| 5155 |
C |
| 5156 |
I1=0 |
| 5157 |
T1=OUT(2)*OUT(2) |
| 5158 |
C R1SQ |
| 5159 |
T2=OUT(3)*OUT(3) |
| 5160 |
C (R1+1)SQ |
| 5161 |
T3=OUT(4)*OUT(4) |
| 5162 |
C (R1+2)SQ |
| 5163 |
T4=2.0*T3 |
| 5164 |
C 2(R1+2)SQ |
| 5165 |
10 T5=XI(1)*XI(1)+XI(2)*XI(2)+XI(3)*XI(3) |
| 5166 |
C T5=R SQ |
| 5167 |
GO TO(20 ,70 ,130,190),MED |
| 5168 |
20 T6=T5-T1 |
| 5169 |
IF(T6)240,240,30 |
| 5170 |
C MED=1 |
| 5171 |
30 TEMP=T1 |
| 5172 |
40 IF((T6/TEMP)-5.0D-6)50 ,50 ,230 |
| 5173 |
50 DO60 I=1,3 |
| 5174 |
XI(I)=XI(I)*9.99995D-1 |
| 5175 |
60 CURR(I+3)=XI(I) |
| 5176 |
GOTO10 |
| 5177 |
70 T6=T5-T1 |
| 5178 |
C MED=2 |
| 5179 |
IF(T6)80 ,80 ,120 |
| 5180 |
80 TEMP=T1 |
| 5181 |
90 IF(5.0D-6+(T6/TEMP))230,100,100 |
| 5182 |
100 DO110 I=1,3 |
| 5183 |
XI(I)=XI(I)*10.00005D-1 |
| 5184 |
110 CURR(I+3)=XI(I) |
| 5185 |
GOTO10 |
| 5186 |
120 T6=T5-T2 |
| 5187 |
TEMP=T2 |
| 5188 |
IF(T6)240,240,40 |
| 5189 |
130 T6=T5-T2 |
| 5190 |
C MED=3 |
| 5191 |
IF(T6)140,140,150 |
| 5192 |
140 TEMP=T2 |
| 5193 |
GOTO90 |
| 5194 |
150 T6=T5-T3 |
| 5195 |
IF(T6)240,240,160 |
| 5196 |
160 TEMP=T3 |
| 5197 |
C****DUMMY IF ST. FOLLOWS TO KEEP ST. 175 |
| 5198 |
IF (TEMP.NE.T3) GO TO 170 |
| 5199 |
GOTO40 |
| 5200 |
170 IF(XI(2))230,180,230 |
| 5201 |
C MED=4 |
| 5202 |
180 IF(CURR(5))230,190,230 |
| 5203 |
190 T6=T5-T3 |
| 5204 |
IF(T6)200,200,210 |
| 5205 |
200 TEMP=T3 |
| 5206 |
GOTO90 |
| 5207 |
210 T6=T5-T4 |
| 5208 |
IF(T6)240,240,220 |
| 5209 |
220 TEMP=T4 |
| 5210 |
GOTO40 |
| 5211 |
230 I1=-1 |
| 5212 |
GOTO290 |
| 5213 |
240 T4=XI(1)*DCOS(1)+XI(2)*DCOS(2)+XI(3)*DCOS(3) |
| 5214 |
C T4=-B=-RCOS(THETA)=SUM OF XI(I)*DCOS(I) |
| 5215 |
T6=T4*T4 |
| 5216 |
C T5=R SQ. |
| 5217 |
T6=T5-T6 |
| 5218 |
C T6=R SQ.-B SQ. |
| 5219 |
IF(T3-T6)230,250 ,250 |
| 5220 |
250 T3=DSQRT(T3-T6) |
| 5221 |
C T3=A3=SQ.ROOT OF B SQ.-R SQ.+RADIUS3 SQ. SIMILAR |
| 5222 |
C FOR T2=A2 ANDT1=A1 |
| 5223 |
TEMP=T2-T6 |
| 5224 |
T2=DSQRT(DABS(TEMP)) |
| 5225 |
TEMPO=T1-T6 |
| 5226 |
T1=DSQRT(DABS(TEMPO)) |
| 5227 |
DO260 I=1,6 |
| 5228 |
260 D(I)=0.0 |
| 5229 |
GOTO(270,300,360,420),MED |
| 5230 |
270 IF(TEMP)230,280,280 |
| 5231 |
280 D(4)=T1-T4 |
| 5232 |
C B+A1 |
| 5233 |
D(5)=T2-T1 |
| 5234 |
C A2-A1 |
| 5235 |
D(6)=T3-T2 |
| 5236 |
C A3-A2 |
| 5237 |
290 RETURN |
| 5238 |
300 IF(TEMP)230,310,310 |
| 5239 |
310 D(6)=T3-T2 |
| 5240 |
320 IF(T4)340,330,330 |
| 5241 |
330 D(3)=T2-T4 |
| 5242 |
C B+A2 |
| 5243 |
GOTO290 |
| 5244 |
340 IF(TEMPO)330,350,350 |
| 5245 |
350 D(3)=-(T4+T1) |
| 5246 |
C B-A1 |
| 5247 |
D(4)=T1+T1 |
| 5248 |
C 2A1 |
| 5249 |
D(5)=T2-T1 |
| 5250 |
C A2-A1 |
| 5251 |
GOTO290 |
| 5252 |
360 IF(T4)380,370,370 |
| 5253 |
370 D(2)=T3-T4 |
| 5254 |
C B+A3 |
| 5255 |
GOTO290 |
| 5256 |
380 IF(TEMP)370,390,390 |
| 5257 |
390 D(2)=-(T4+T2) |
| 5258 |
C B-A2 |
| 5259 |
D(6)=T3-T2 |
| 5260 |
C A3-A2 |
| 5261 |
IF(TEMPO)400,410,410 |
| 5262 |
400 D(3)=T2+T2 |
| 5263 |
C 2A2 |
| 5264 |
GOTO290 |
| 5265 |
410 D(3)=T2-T1 |
| 5266 |
C A2-A1 |
| 5267 |
D(5)=D(3) |
| 5268 |
D(4)=T1+T1 |
| 5269 |
C 2A1 |
| 5270 |
GOTO290 |
| 5271 |
420 D(1)=-(T4+T3) |
| 5272 |
430 IF(TEMP)440,450,450 |
| 5273 |
440 D(2)=T3+T3 |
| 5274 |
GOTO290 |
| 5275 |
450 D(2)=T3-T2 |
| 5276 |
D(6)=D(2) |
| 5277 |
C B-A3, A3-A2,REGION 4 |
| 5278 |
IF(TEMPO)470,460,460 |
| 5279 |
460 D(3)=T2-T1 |
| 5280 |
C A2-A1 |
| 5281 |
D(5)=D(3) |
| 5282 |
D(4)=T1+T1 |
| 5283 |
GOTO290 |
| 5284 |
470 D(3)=T2+T2 |
| 5285 |
C 2A2 |
| 5286 |
GOTO290 |
| 5287 |
END |
| 5288 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 5289 |
*-- Author : |
| 5290 |
SUBROUTINE CALIDK |
| 5291 |
#include "cbert.inc" |
| 5292 |
*KEND. |
| 5293 |
SAVE |
| 5294 |
C |
| 5295 |
UNIV=PNIDK(6)*PNIDK(6) |
| 5296 |
C M(P1) SQUARED DECAY PION MASS SQUARED |
| 5297 |
PNIDK(7)=(PNIDK(1)*PNIDK(1)+UNIV-SQNM)/(2.0*PNIDK(1)) |
| 5298 |
C E(PI)PRIME DECAY PION ENERGY PRIME |
| 5299 |
PNIDK(8)=DSQRT(PNIDK(7)*PNIDK(7)-UNIV) |
| 5300 |
C DECAY PION MOMENTUM PRIME P(D) |
| 5301 |
CALL CAPOL1(PNIDK(20),PNIDK(21)) |
| 5302 |
C COS THETA, SIN THETA |
| 5303 |
CALL CAAZIO(PNIDK(22),PNIDK(23)) |
| 5304 |
C COS PHI, SIN PHI |
| 5305 |
PNIDK(9)=PNIDK(22)*PNIDK(21)*PNIDK(8) |
| 5306 |
C DECAY PION X MOMENTUM COMPONENT PRIME |
| 5307 |
PNIDK(10)=PNIDK(21)*PNIDK(23)*PNIDK(8) |
| 5308 |
C P(P1)PRIME Y |
| 5309 |
PNIDK(11)=PNIDK(20)*PNIDK(8) |
| 5310 |
C P(P1)PRIME Z |
| 5311 |
UNIV=PNIDK(9)*PNIDK(2)+PNIDK(10)*PNIDK(3)+PNIDK(11)*PNIDK(4) |
| 5312 |
C P P1 PRIME DOT P |
| 5313 |
PNIDK(12)=(PNIDK(7)*PNIDK(5)+UNIV)/PNIDK(1) |
| 5314 |
C DECAY PION ENERGY E(PI) |
| 5315 |
PNIDK(13)=PNIDK(5)-PNIDK(12) |
| 5316 |
UNIV=(((PNIDK(5)/PNIDK(1))-1.0)*UNIV)/(PNIDK(2)*PNIDK(2)+ |
| 5317 |
+PNIDK(3)*PNIDK(3)+PNIDK(4)*PNIDK(4)) |
| 5318 |
C (E/M-1.0)*P(P1)PRIME DOT P/P SQUARED |
| 5319 |
UNIVE=PNIDK(7)/PNIDK(1) |
| 5320 |
C E PI PRIME OVER MASS |
| 5321 |
DO10 I=2,4 |
| 5322 |
PNIDK(I+12)=PNIDK(I)*(UNIV+UNIVE) +PNIDK(I+7) |
| 5323 |
10 PNIDK(I+15)=PNIDK(I)-PNIDK(I+12) |
| 5324 |
RETURN |
| 5325 |
C PION MOMENTUM COMPONENTS AND NUCLEON MOMENTUM |
| 5326 |
C COMPONENTS |
| 5327 |
END |
| 5328 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 5329 |
*-- Author : |
| 5330 |
SUBROUTINE CAISOM |
| 5331 |
#include "cbert.inc" |
| 5332 |
*KEND. |
| 5333 |
REAL * 8 FERMN |
| 5334 |
SAVE |
| 5335 |
C |
| 5336 |
CALL CAPOL1(POLC,POLS) |
| 5337 |
CALL CAAZIO(SOPC,SOPS) |
| 5338 |
M = SNGL(CLSM) + .05 |
| 5339 |
IF(STRKP+2.0)20,20,10 |
| 5340 |
10 FERMN=FMPN(M) |
| 5341 |
C STRUCK PROTON |
| 5342 |
GOTO30 |
| 5343 |
20 FERMN=FMPN(M+3) |
| 5344 |
C STRUCK NEUTRON |
| 5345 |
30 CALL FRMICC(P2) |
| 5346 |
P2=FERMN*P2 |
| 5347 |
C FRMIC SELECTS LARGEST OF 3 RANDOM NUMBERS |
| 5348 |
C P2=MOMENTUM OF PARTICLE SELECTED FROM PROPER |
| 5349 |
C FERMI DISTRIBUTION |
| 5350 |
A=P2*POLS |
| 5351 |
C P2 SIN THETA |
| 5352 |
PXYZ(2)=A*SOPC |
| 5353 |
C P2 SIN THETA COS PHI |
| 5354 |
PXYZ(6)=A*SOPS |
| 5355 |
C P2 SIN PHI |
| 5356 |
PXYZ(10)=P2*POLC |
| 5357 |
C P2 COS THETA |
| 5358 |
E(2)=DSQRT(P2*P2+SQNM) |
| 5359 |
C SQ. RT. MOMENTUM STRUCK PART. SQD. +NUCLEON MASS SQD. |
| 5360 |
RLKE=(((E(1)*E(2)-PXYZ(1)*PXYZ(2)-PXYZ(5)*PXYZ(6)-PXYZ(9)* |
| 5361 |
1PXYZ(10))/DNCMS )-PM(1))/RCPMV |
| 5362 |
C RELATIVE K.E.(MEV)--CONSTANT=NUCLEON MASS /CM, |
| 5363 |
C SECOND=MEV/CM. |
| 5364 |
RETURN |
| 5365 |
END |
| 5366 |
*CMZ : 0.90/00 29/07/92 11.28.17 by Christian Zeitnitz |
| 5367 |
*-- Author : |
| 5368 |
SUBROUTINE CALMUD(SINE,INP) |
| 5369 |
C |
| 5370 |
#include "crandm.inc" |
| 5371 |
*KEND. |
| 5372 |
C |
| 5373 |
REAL * 8 SINE |
| 5374 |
C |
| 5375 |
SINE= RANDC(ISEED) |
| 5376 |
SINE = 5.0 D1 * SINE |
| 5377 |
INP = IDINT(SINE + 0.1D1) |
| 5378 |
SINE=DFLOAT(INP)-SINE |
| 5379 |
C SINE=(.02N-R)/.02=N-R/.02 N=INPT R/.02=(N-1)+X |
| 5380 |
RETURN |
| 5381 |
END |
| 5382 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 5383 |
*-- Author : |
| 5384 |
SUBROUTINE CALNNN |
| 5385 |
#include "cbert.inc" |
| 5386 |
*KEND. |
| 5387 |
C |
| 5388 |
FMAX(1) = 0.46 D-24 |
| 5389 |
FMAX(2) = 1.4 D-24 |
| 5390 |
DO10 I=3,6 |
| 5391 |
10 FMAX(I)=0.0 |
| 5392 |
RETURN |
| 5393 |
END |
| 5394 |
*CMZ : 0.90/00 19/05/92 17.08.07 by Christian Zeitnitz |
| 5395 |
*-- Author : |
| 5396 |
SUBROUTINE P1CLC |
| 5397 |
#include "cbert.inc" |
| 5398 |
*KEND. |
| 5399 |
C |
| 5400 |
P1OE1=DSQRT(E(1)*E(1)-PM(1)*PM(1)) |
| 5401 |
PXYZ(1)=P1OE1*CURR(7) |
| 5402 |
PXYZ(5)=P1OE1*CURR(8) |
| 5403 |
PXYZ(9)=P1OE1*CURR(9) |
| 5404 |
P1OE1=P1OE1/E(1) |
| 5405 |
RETURN |
| 5406 |
END |
| 5407 |
*CMZ : 0.90/00 06/06/92 14.08.24 by Christian Zeitnitz |
| 5408 |
*-- Author : |
| 5409 |
SUBROUTINE P1CLI |
| 5410 |
#include "cbert.inc" |
| 5411 |
*KEND. |
| 5412 |
C |
| 5413 |
PXYZ(1)=0.0 |
| 5414 |
PXYZ(5)=0.0 |
| 5415 |
PXYZ(9)=DSQRT(E(1)*E(1)-PM(1)*PM(1)) |
| 5416 |
P1OE1=PXYZ(9)/E(1) |
| 5417 |
RETURN |
| 5418 |
C MOMENTUM X AND Y COORDINATES,PARTICLE 1 =0.0 |
| 5419 |
C Z COORD. =TOTAL ENERGY SQUARED-MASS SQ. TO THE 1/2 |
| 5420 |
C FOR PARTICLE ONE. P1OE1=CURRENT(MOMENT/TOTAL) |
| 5421 |
END |
| 5422 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 5423 |
*-- Author : |
| 5424 |
SUBROUTINE PARTIN |
| 5425 |
#include "cbert.inc" |
| 5426 |
*KEND. |
| 5427 |
C |
| 5428 |
SAVE |
| 5429 |
IF(D(4))10 ,20 ,10 |
| 5430 |
10 IPEC(10)=IPEC(10)+1 |
| 5431 |
C NO. OF INC. PARTICLES ON REG.1 ONLY |
| 5432 |
GOTO50 |
| 5433 |
20 IF(D(3))30 ,40 ,30 |
| 5434 |
30 IPEC(6)=IPEC(6)+1 |
| 5435 |
C NO. OF INC. PARTICLES ON REG.2 ONLY |
| 5436 |
GOTO50 |
| 5437 |
40 IPEC(1)=IPEC(1)+1 |
| 5438 |
C NO. OF INC. PARTICLES ON REG.3 ONLY |
| 5439 |
50 DO60 I=1,3 |
| 5440 |
60 ISW(I)=0 |
| 5441 |
C 1=0 WHEN START IN RG.3 OR RG.4 |
| 5442 |
C 2=0 WHEN IN RG.3 NOT PASSING THROUGH RG.1 |
| 5443 |
C 3=0 WHEN IN RG.2 NOT PASSING THROUGH RG.1 |
| 5444 |
RETURN |
| 5445 |
END |
| 5446 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 5447 |
*-- Author : |
| 5448 |
SUBROUTINE PFMAX |
| 5449 |
#include "cbert.inc" |
| 5450 |
*KEND. |
| 5451 |
REAL * 8 WK |
| 5452 |
SAVE |
| 5453 |
C |
| 5454 |
I=I2 |
| 5455 |
IF(CURR(1)-2.0)20,10,10 |
| 5456 |
10 I=I+3 |
| 5457 |
20 WK=WKRPN(I) |
| 5458 |
IF(WK-160.0)30,30,50 |
| 5459 |
30 FMAX(1)=0.176D-24 |
| 5460 |
FMAX(2)=0.52D-24 |
| 5461 |
FMAX(3)=0.0 |
| 5462 |
FMAX(4)=0.0 |
| 5463 |
40 RETURN |
| 5464 |
50 CALL CBOVER(WK,DNCMS,UNIV) |
| 5465 |
IF(WK-400.0)60,110,110 |
| 5466 |
60 IF(WK-300.0)70,100,100 |
| 5467 |
70 IF(WK-200.0)80,90,90 |
| 5468 |
80 FMAX(3)=1.95D-27*UNIV |
| 5469 |
C 3 AND 4 AT 465 MEV |
| 5470 |
FMAX(4)=1.7D-27*UNIV |
| 5471 |
FMAX(1)=0.103D-24 |
| 5472 |
FMAX(2)=0.313D-24 |
| 5473 |
GOTO40 |
| 5474 |
90 FMAX(1)=0.09D-24 |
| 5475 |
C 1 AND 2 AT 35 MEV |
| 5476 |
FMAX(2)=0.26D-24 |
| 5477 |
FMAX(3)=11.4D-27*UNIV |
| 5478 |
C 3 AND 4 AT 630 MEV |
| 5479 |
FMAX(4)=11.2D-27*UNIV |
| 5480 |
GOTO40 |
| 5481 |
100 FMAX(1)=28.0D-27*UNIV |
| 5482 |
C 1 AND 2 AT 100 MEV |
| 5483 |
FMAX(2)=0.073D-24 |
| 5484 |
FMAX(3)=20.0D-27*UNIV |
| 5485 |
C 3 AND 4 AT 780 MEV |
| 5486 |
FMAX(4)=14.0D-27*UNIV |
| 5487 |
GOTO40 |
| 5488 |
110 FMAX(1)=27.2D-27*UNIV |
| 5489 |
C 1 AND 2 AT 155 MEV |
| 5490 |
FMAX(2)=48.0D-27*UNIV |
| 5491 |
FMAX(3)=22.6D-27*UNIV |
| 5492 |
C 3 AND 4 AT 1020 MEV |
| 5493 |
FMAX(4)=14.0D-27*UNIV |
| 5494 |
GOTO40 |
| 5495 |
C FMAX(1)=(P-P)S---(2)=(P-N)S---(3)=(P-P)S.P.---(4)=(P-N)S.P. |
| 5496 |
END |
| 5497 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 5498 |
*-- Author : |
| 5499 |
SUBROUTINE PINST |
| 5500 |
#include "cbert.inc" |
| 5501 |
*KEND. |
| 5502 |
SAVE |
| 5503 |
C |
| 5504 |
I1=0 |
| 5505 |
MED=CLSM |
| 5506 |
IF(INC)10,140,10 |
| 5507 |
10 INC=0 |
| 5508 |
IF(MED-1)20,50,40 |
| 5509 |
20 I1=1 |
| 5510 |
30 RETURN |
| 5511 |
40 IF(MED-3)60,90,20 |
| 5512 |
50 IPEC(12)=IPEC(12)+1 |
| 5513 |
C INCIDENT PARTICLE ON REG.1 COLLISION IN REG.1 |
| 5514 |
GOTO30 |
| 5515 |
60 IF(D(4))80,70,80 |
| 5516 |
70 IPEC(8)=IPEC(8)+1 |
| 5517 |
GOTO30 |
| 5518 |
C INC. PARTICLE ON REG.2 COLLISION IN REG.2 |
| 5519 |
80 IPEC(9)=IPEC(9)+1 |
| 5520 |
C INC. PARTICLE ON REG.1 COLLISION IN REG.2 |
| 5521 |
GOTO30 |
| 5522 |
90 IF(D(3))100,120,100 |
| 5523 |
100 IF(D(4))110,130,110 |
| 5524 |
110 IPEC(5)=IPEC(5)+1 |
| 5525 |
C INC. PARTICLE ON REG.1 COLLISION IN REG.3 |
| 5526 |
GOTO30 |
| 5527 |
120 IPEC(3)=IPEC(3)+1 |
| 5528 |
C INC. PARTICLE ON REG.3 COLLISION IN REG.3 |
| 5529 |
GOTO30 |
| 5530 |
130 IPEC(4)=IPEC(4)+1 |
| 5531 |
C INC. PARTICLE ON REG.2 COLLISION IN REG.3 |
| 5532 |
GOTO30 |
| 5533 |
140 K=CURR(11) |
| 5534 |
K=3*(MED-1)+K |
| 5535 |
CC(K)=CC(K)+1.0 |
| 5536 |
GOTO30 |
| 5537 |
C COLLISION REG.1 PARTICLE ORIGIN K |
| 5538 |
END |
| 5539 |
*CMZ : 0.90/00 29/07/92 11.28.53 by Christian Zeitnitz |
| 5540 |
*-- Author : |
| 5541 |
SUBROUTINE CAPOL1(CS,SI) |
| 5542 |
C |
| 5543 |
#include "crandm.inc" |
| 5544 |
*KEND. |
| 5545 |
C |
| 5546 |
REAL*8 CS, SI |
| 5547 |
C |
| 5548 |
CS = RANDC(ISEED) |
| 5549 |
S = 2.0 * RANDC(ISEED) - 1.0 |
| 5550 |
IF(S.LT.0) CS = -CS |
| 5551 |
SI = DSQRT(1.0-(CS*CS)) |
| 5552 |
RETURN |
| 5553 |
END |
| 5554 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 5555 |
*-- Author : |
| 5556 |
SUBROUTINE PSTOR |
| 5557 |
#include "cbert.inc" |
| 5558 |
*KEND. |
| 5559 |
SAVE |
| 5560 |
C |
| 5561 |
L=(I1*12)-28 |
| 5562 |
IF(I2)10,60,70 |
| 5563 |
10 JJ=0 |
| 5564 |
IF(PM(3)-DNCMS)30,30,20 |
| 5565 |
20 I1=I1+1 |
| 5566 |
JJ=1 |
| 5567 |
C X-Y-Z-COORDINATES OF COLLISION POINT |
| 5568 |
30 UNIV=DSQRT(PXYZ(I1)*PXYZ(I1)+PXYZ(I1+4)*PXYZ(I1+4)+PXYZ(I1+8) |
| 5569 |
+*PXYZ(I1+8)) |
| 5570 |
K=I1+8 |
| 5571 |
DO40 I=I1,K,4 |
| 5572 |
PT(L)=PXYZ(I)/UNIV |
| 5573 |
40 L=L+1 |
| 5574 |
I1=I1-JJ |
| 5575 |
50 PT(L)=CLSM |
| 5576 |
PT(L+1)=CURR(11) |
| 5577 |
PT(L-6)=C(1) |
| 5578 |
PT(L-5)=C(2) |
| 5579 |
PT(L-4)=C(3) |
| 5580 |
RETURN |
| 5581 |
60 K=14 |
| 5582 |
GOTO90 |
| 5583 |
70 IF(I2-2)80,110,110 |
| 5584 |
80 K=17 |
| 5585 |
90 UNIV=DSQRT(PNIDK(K)*PNIDK(K)+PNIDK(K+1)*PNIDK(K+1)+PNIDK |
| 5586 |
+(K+2)*PNIDK(K+2)) |
| 5587 |
J=K+2 |
| 5588 |
DO100 I=K,J |
| 5589 |
PT(L)=PNIDK(I)/UNIV |
| 5590 |
100 L=L+1 |
| 5591 |
GOTO50 |
| 5592 |
110 UNIV=DSQRT(PT(L-3)*PT(L-3)+PT(L-2)*PT(L-2)+PT(L-1)*PT(L-1)) |
| 5593 |
K=L-1 |
| 5594 |
M=L-3 |
| 5595 |
DO120 I=M,K |
| 5596 |
PT(L)=PT(I)/UNIV |
| 5597 |
120 L=L+1 |
| 5598 |
GOTO50 |
| 5599 |
END |
| 5600 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 5601 |
*-- Author : |
| 5602 |
SUBROUTINE CAPUNP |
| 5603 |
#include "cbert.inc" |
| 5604 |
#include "crn.inc" |
| 5605 |
#include "cmunpu.inc" |
| 5606 |
*KEND. |
| 5607 |
REAL*8 AC,ZC,AR,ZE |
| 5608 |
SAVE |
| 5609 |
C |
| 5610 |
IF(PGVC(1))10,60,30 |
| 5611 |
10 I1=-1 |
| 5612 |
20 RETURN |
| 5613 |
30 PGVC(1)=PGVC(1)-11.0 |
| 5614 |
K=PGVC(1)+2.005 |
| 5615 |
DO40 I=1,11 |
| 5616 |
CURR(I)=PGVC(K) |
| 5617 |
PGVC(K)=0.0 |
| 5618 |
40 K=K+1 |
| 5619 |
50 I1=1 |
| 5620 |
GOTO20 |
| 5621 |
60 IF(PLVC(1))10,130,70 |
| 5622 |
70 UNIV=0.0 |
| 5623 |
L=PLVC(1) |
| 5624 |
K=-10 |
| 5625 |
DO110 I=1,L |
| 5626 |
80 K=K+12 |
| 5627 |
IF(PLVC(K))10,80,90 |
| 5628 |
90 IF(PLVC(K)-UNIV)110,100,100 |
| 5629 |
100 UNIV=PLVC(K) |
| 5630 |
M=K |
| 5631 |
110 CONTINUE |
| 5632 |
PLVC(M)=0.0 |
| 5633 |
DO120 I=1,11 |
| 5634 |
M=M+1 |
| 5635 |
CURR(I)=PLVC(M) |
| 5636 |
120 PLVC(M)=0.0 |
| 5637 |
PLVC(1)=PLVC(1)-1.0 |
| 5638 |
GOTO50 |
| 5639 |
130 I1=0 |
| 5640 |
AC=AMASNO |
| 5641 |
IF(NO.GT.2)GOTO140 |
| 5642 |
ZC=ZEE |
| 5643 |
AC=AMASNO+1.0D0 |
| 5644 |
C AC-COMPOUND NUC,ZC=CHG.COMPOUND,AR=MASS CASCADE RESID.NUCLEUS |
| 5645 |
IF(NO.EQ.1)GOTO150 |
| 5646 |
GOTO160 |
| 5647 |
140 IF(NO.LT.5)GOTO150 |
| 5648 |
ZC=ZEE-1.0D0 |
| 5649 |
GOTO160 |
| 5650 |
150 ZC=ZEE+1.0D0 |
| 5651 |
160 AR=AC-COUNT(1)-COUNT(2) |
| 5652 |
ZE=COUNT(1)+COUNT(3)-COUNT(5) |
| 5653 |
IF(AR)170,180,190 |
| 5654 |
170 COUNT(7)=COUNT(7)+1.0D0 |
| 5655 |
GOTO210 |
| 5656 |
180 IF(ZC.EQ.ZE)GOTO20 |
| 5657 |
COUNT(8)=COUNT(8)+1.0D0 |
| 5658 |
GOTO210 |
| 5659 |
190 IF(AR.GE.(ZC-ZE))GOTO200 |
| 5660 |
COUNT(9)=COUNT(9)+1.0D0 |
| 5661 |
GOTO210 |
| 5662 |
200 IF(ZC.GE.ZE)GOTO20 |
| 5663 |
COUNT(10)=COUNT(10)+1.0D0 |
| 5664 |
210 IF(BEGRU.EQ.1.0D0)GOTO260 |
| 5665 |
BEGRU=BEGRU-1.0D0 |
| 5666 |
220 DO230 I=1,12 |
| 5667 |
CC(I)=PCC(I) |
| 5668 |
230 IPEC(I)=NIP(I) |
| 5669 |
DO 240 I = 1,5 |
| 5670 |
240 PNBC(I)=PPNB(I) |
| 5671 |
250 NOR=NOR-1 |
| 5672 |
COUNT(6)=-1.0D0 |
| 5673 |
GO TO 20 |
| 5674 |
260 BEGRU=-1.0D0 |
| 5675 |
GO TO 220 |
| 5676 |
C 1. PICKS UP LAST 11 ITEMS IN PGVC AND STORES |
| 5677 |
C THEM IN CURR. STORES ZERO IN THOSE 11 PGVC CELLS. |
| 5678 |
C GROUP IS GREATER THAN 1ST IN ALL OTHER GROUPS. STORES |
| 5679 |
C 2-12TH ITEMS IN CURR--ZEROES ITEMS 1-12 IN PLVC GROUP. |
| 5680 |
END |
| 5681 |
*CMZ : 1.05/03 27/06/2001 17.24.29 by Christian Zeitnitz |
| 5682 |
*-- Author : Christian Zeitnitz 20/05/92 |
| 5683 |
DOUBLE PRECISION FUNCTION RANDC(DUMMY) |
| 5684 |
C |
| 5685 |
integer DUMMY |
| 5686 |
DIMENSION RND1(1) |
| 5687 |
C |
| 5688 |
CALL GRNDM(RND1,1) |
| 5689 |
RANDC = RND1(1) |
| 5690 |
RETURN |
| 5691 |
END |
| 5692 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 5693 |
*-- Author : |
| 5694 |
SUBROUTINE ROUT10 |
| 5695 |
C |
| 5696 |
#include "cbert.inc" |
| 5697 |
*KEND. |
| 5698 |
C |
| 5699 |
I3=0 |
| 5700 |
IF(EX-D(4))40 ,40 ,10 |
| 5701 |
10 CALL SPAC32(31) |
| 5702 |
GO TO 20 |
| 5703 |
20 I3=-1 |
| 5704 |
30 RETURN |
| 5705 |
40 CURR(2)=OUT(15) |
| 5706 |
WKRPN(1)=OUT(15) |
| 5707 |
WKRPN(4)=OUT(18) |
| 5708 |
C K.E. FOR PROTONS AND NEUTRONS REGION 1 |
| 5709 |
GO TO 30 |
| 5710 |
END |
| 5711 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 5712 |
*-- Author : |
| 5713 |
SUBROUTINE ROUT11(T) |
| 5714 |
SAVE |
| 5715 |
C |
| 5716 |
#include "cbert.inc" |
| 5717 |
*KEND. |
| 5718 |
C |
| 5719 |
REAL *8 T(6426) |
| 5720 |
GO TO (10 ,30 ,40 ,20 ),I3 |
| 5721 |
10 PT(2)=3.0 |
| 5722 |
20 IK=IT |
| 5723 |
PT(14)=1.0 |
| 5724 |
30 PM(3)=PNMS |
| 5725 |
40 IF(340.0-RLKE)50 ,70 ,70 |
| 5726 |
50 I3=1 |
| 5727 |
60 RETURN |
| 5728 |
70 CALL CALMUD(SNT,INPT) |
| 5729 |
IF(IK-3)100,80 ,90 |
| 5730 |
80 I3=2 |
| 5731 |
GO TO 60 |
| 5732 |
90 I3=3 |
| 5733 |
GO TO 60 |
| 5734 |
100 CALL CRDET(51,T(1),RLKE) |
| 5735 |
I3=4 |
| 5736 |
GOTO60 |
| 5737 |
END |
| 5738 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 5739 |
*-- Author : |
| 5740 |
SUBROUTINE ROUT12 |
| 5741 |
C |
| 5742 |
#include "cbert.inc" |
| 5743 |
#include "crun.inc" |
| 5744 |
*KEND. |
| 5745 |
C |
| 5746 |
I3=0 |
| 5747 |
CALL CAAZIO(SOPC,SOPS) |
| 5748 |
CALL CACOLL(0) |
| 5749 |
IF(COL(15))10 ,30 ,10 |
| 5750 |
10 I3=-1 |
| 5751 |
20 RETURN |
| 5752 |
30 IF(KE)10 ,50 ,40 |
| 5753 |
40 COM = (E(4)-DNCMS)/RCPMV |
| 5754 |
GO TO 60 |
| 5755 |
50 CALL COLE4 |
| 5756 |
60 I1= -1 |
| 5757 |
VALUE1=COM |
| 5758 |
IF(PT(14)-2.0)70 ,20 ,20 |
| 5759 |
70 I3=1 |
| 5760 |
GOTO20 |
| 5761 |
END |
| 5762 |
*CMZ : 0.92/03 10/12/92 10.53.45 by Christian Zeitnitz |
| 5763 |
*-- Author : |
| 5764 |
SUBROUTINE ROUT13 |
| 5765 |
SAVE |
| 5766 |
#include "cbert.inc" |
| 5767 |
*KEND. |
| 5768 |
C |
| 5769 |
I3=0 |
| 5770 |
IF(IV)10 ,50 ,50 |
| 5771 |
10 IF(XABS)20 ,50 ,20 |
| 5772 |
20 IF(IFCA-2)30 ,70 ,60 |
| 5773 |
30 IN=0 |
| 5774 |
40 I3=1 |
| 5775 |
GOTO90 |
| 5776 |
50 CALLSIGNEX |
| 5777 |
IF(IFC-12)120,120,130 |
| 5778 |
60 IF(IFCA-6)70 ,30 ,100 |
| 5779 |
70 IN=0 |
| 5780 |
80 I3=-1 |
| 5781 |
90 RETURN |
| 5782 |
100 IF(IFCA-8)30 ,110,110 |
| 5783 |
110 IN=1 |
| 5784 |
GOTO40 |
| 5785 |
120 IN=0 |
| 5786 |
GOTO90 |
| 5787 |
130 IF(IFC-18)140,140,150 |
| 5788 |
140 IN=-1 |
| 5789 |
GOTO90 |
| 5790 |
150 IN=1 |
| 5791 |
GOTO90 |
| 5792 |
END |
| 5793 |
*CMZ : 0.92/03 10/12/92 10.54.08 by Christian Zeitnitz |
| 5794 |
*-- Author : |
| 5795 |
SUBROUTINE ROUT14 |
| 5796 |
SAVE |
| 5797 |
C |
| 5798 |
#include "cbert.inc" |
| 5799 |
#include "crun.inc" |
| 5800 |
*KEND. |
| 5801 |
C |
| 5802 |
IF(I3)310,270,10 |
| 5803 |
10 IF(I1)20 ,80 ,80 |
| 5804 |
20 I1=0 |
| 5805 |
VALUE1=(E(3)-PM(3))/RCPMV |
| 5806 |
IF(XABS)30 ,40 ,30 |
| 5807 |
30 VALUE1=VALUE1+ABSEC |
| 5808 |
40 IF(PT(2)-2.0)70 ,50 ,80 |
| 5809 |
C PT(2)=1=PROTON PT(2)=2=NEUTRON PT(2)=3,4,5=PION |
| 5810 |
50 I3=2 |
| 5811 |
60 GO TO 320 |
| 5812 |
70 I3=1 |
| 5813 |
GOTO60 |
| 5814 |
80 CALLPINST |
| 5815 |
IF(I1)90 ,100,90 |
| 5816 |
90 I3=3 |
| 5817 |
GOTO60 |
| 5818 |
100 I1=0 |
| 5819 |
M=PT(2) |
| 5820 |
VALUE2=VALUE1 |
| 5821 |
IF(M-3)110,150,150 |
| 5822 |
110 IF(ECO(M)-VALUE2)140,120,130 |
| 5823 |
120 IF(ECO(M))90 ,90 ,130 |
| 5824 |
130 PT(I1+3)=0.0 |
| 5825 |
PNBC(M)=PNBC(M)+1.0 |
| 5826 |
GOTO230 |
| 5827 |
140 PT(I1+3)=VALUE2 |
| 5828 |
IF(I1)300,240,300 |
| 5829 |
150 CCOFE=CLCFE |
| 5830 |
IF(M-4)160,170,170 |
| 5831 |
160 IF(STRKP+2.0)200,190,200 |
| 5832 |
170 IF(STRKP+2.0)200,200,180 |
| 5833 |
180 CCOFE=CLCFE-CTOFE+CTOFEN |
| 5834 |
GOTO200 |
| 5835 |
190 CCOFE=CLCFE+CTOFE-CTOFEN |
| 5836 |
200 IF(VALUE2-CCOFE)130,130,210 |
| 5837 |
210 IF(STRKP+2.0)220,220,140 |
| 5838 |
220 PT(3)=VALUE1-SPACE(MED+3)+SPACE(MED+9) |
| 5839 |
230 IF(I1)260,240,260 |
| 5840 |
240 M=PT(14) |
| 5841 |
IF(M-3)250,90 ,90 |
| 5842 |
250 VALUE2=COM |
| 5843 |
I1=12 |
| 5844 |
GOTO110 |
| 5845 |
260 IF(PT(3))300,270,300 |
| 5846 |
270 CALLCAPUNP |
| 5847 |
IF(I1)90 ,280 ,290 |
| 5848 |
C -, =ERROR 0=END OF RECORD +=PISCC(6607) |
| 5849 |
280 I3=4 |
| 5850 |
GOTO60 |
| 5851 |
290 I3=5 |
| 5852 |
GOTO60 |
| 5853 |
300 CALL COLLM(-1) |
| 5854 |
310 IF(KE.GT.0)GO TO 320 |
| 5855 |
CALL CASTPR |
| 5856 |
IF(I1)90 ,270,90 |
| 5857 |
320 RETURN |
| 5858 |
END |
| 5859 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 5860 |
*-- Author : |
| 5861 |
SUBROUTINE ROUT15(T) |
| 5862 |
SAVE |
| 5863 |
REAL*8 T(6426) |
| 5864 |
#include "cbert.inc" |
| 5865 |
#include "crandm.inc" |
| 5866 |
*KEND. |
| 5867 |
C |
| 5868 |
GOTO(10 ,80 ,20 ,100),I3 |
| 5869 |
10 IF(RLKE.LE.2.5D3) GO TO 40 |
| 5870 |
20 I3=4 |
| 5871 |
30 GO TO 160 |
| 5872 |
40 IF(IK-3)70 ,50 ,60 |
| 5873 |
50 I3=1 |
| 5874 |
GOTO30 |
| 5875 |
60 I3=2 |
| 5876 |
GOTO30 |
| 5877 |
70 CALL CALMUD(SNT,INPT) |
| 5878 |
CALL CRDET(51,T(1),RLKE) |
| 5879 |
I2 = 0 |
| 5880 |
CST = CRDT(2) - DABS(SNT*(CRDT(2) - CRDT(1))) |
| 5881 |
80 IF(I2)90 ,90 ,20 |
| 5882 |
90 I3=3 |
| 5883 |
GOTO30 |
| 5884 |
100 VALUE1 = RANDC(ISEED) |
| 5885 |
IF(VALUE1-CRDT(1))150,110,110 |
| 5886 |
110 VALUE2=1.0 |
| 5887 |
C SCATT. FORWARD |
| 5888 |
VALUE1= RANDC(ISEED) |
| 5889 |
IF(VALUE1-CRDT(4))120,140,140 |
| 5890 |
120 VALUE1 = RANDC(ISEED) |
| 5891 |
C TO SAMPLE FROM UNIFORM DIST. |
| 5892 |
130 CST=VALUE1*VALUE2 |
| 5893 |
GOTO90 |
| 5894 |
140 COM=0.0 |
| 5895 |
CALL CABIG7(COM,VALUE1,I1) |
| 5896 |
GOTO130 |
| 5897 |
150 VALUE2=-1.0 |
| 5898 |
VALUE1 = RANDC(ISEED) |
| 5899 |
I1=I1+I2 |
| 5900 |
IF(VALUE1-CRDT(2))120,140,140 |
| 5901 |
160 RETURN |
| 5902 |
END |
| 5903 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 5904 |
*-- Author : |
| 5905 |
SUBROUTINE ROUT16(T) |
| 5906 |
REAL*8 T(6426) |
| 5907 |
C |
| 5908 |
#include "cbert.inc" |
| 5909 |
*KEND. |
| 5910 |
C |
| 5911 |
CALL CALMUD(SNT,INPT) |
| 5912 |
CALL CRDET(51,T(1),RLKE) |
| 5913 |
I2 = 0 |
| 5914 |
CST = CRDT(2) - DABS(SNT*(CRDT(2) - CRDT(1))) |
| 5915 |
GO TO (10 ,30 ,40 ), I3 |
| 5916 |
10 I3=-1 |
| 5917 |
20 RETURN |
| 5918 |
30 I3=0 |
| 5919 |
GOTO20 |
| 5920 |
40 I3=1 |
| 5921 |
GOTO20 |
| 5922 |
END |
| 5923 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 5924 |
*-- Author : |
| 5925 |
SUBROUTINE ROUT17(T,B,R,W,G) |
| 5926 |
C |
| 5927 |
#include "crandm.inc" |
| 5928 |
#include "cbert.inc" |
| 5929 |
*KEND. |
| 5930 |
C |
| 5931 |
REAL*8 T(117),B(101),R(117),W(234),G(234) |
| 5932 |
SAVE |
| 5933 |
C |
| 5934 |
IF(I3)10 ,10 ,150 |
| 5935 |
10 PT(38)=0.0 |
| 5936 |
C 1-ALPHA PART.6+1 |
| 5937 |
VALUE1=RLKE-180.0 |
| 5938 |
CALL CRDET(1,T(1),VALUE1) |
| 5939 |
COM2=CRDT(1) |
| 5940 |
FTR=DNCMS*RLKE*2.0*RCPMV+2.9877156D27 |
| 5941 |
C E**2=MIN**2+NCNMS*RLKE*2*RCPMV |
| 5942 |
UNIVER=DSQRT(FTR) |
| 5943 |
C E |
| 5944 |
20 VALUE2 = RANDC(ISEED) |
| 5945 |
COM=VALUE2*COM2 |
| 5946 |
C R-PRIME |
| 5947 |
CALL CAGENE(B(1)) |
| 5948 |
COM1=(COM*COM+FTR-.501264D26)/(2.0*UNIVER) |
| 5949 |
C M1R PRIME)**2+E**2-2(PNMS)/2E=E ALPHA |
| 5950 |
A=COM1*COM1-COM*COM |
| 5951 |
IF(A)30 ,40 ,40 |
| 5952 |
30 PACNT=PACNT+1.0 |
| 5953 |
GO TO 20 |
| 5954 |
40 UNIVE=((UNIVER-COM1)*COM1/UNIVER)*DSQRT(A) |
| 5955 |
C ((E BETA*E ALPHA*P ALPHA)/E)=F(M,TR) |
| 5956 |
CALL CRDET(1,R(1),VALUE1) |
| 5957 |
C (PI-NUC)FMAX(RLKE)ISOBAR SAMPLING S.P. |
| 5958 |
COM1 = RANDC(ISEED) |
| 5959 |
IF((UNIVE/CRDT(1))-COM1)20 ,50 ,50 |
| 5960 |
C RANDOM NO. LESS OR EQUAL THAN F(M,TR)/FMAX(TR) |
| 5961 |
50 CALLCANGID |
| 5962 |
PM(3)=COM |
| 5963 |
PM(4)=POMS |
| 5964 |
PT(2)=3.0 |
| 5965 |
PT(4)=POMS |
| 5966 |
PT(14)=3.0 |
| 5967 |
PT(16)=POMS |
| 5968 |
PT(26)=1.0 |
| 5969 |
PT(28)=DNCMS |
| 5970 |
IF(ISW(9))70 ,60 ,70 |
| 5971 |
60 IF(ISW(10))110 ,100 ,110 |
| 5972 |
70 IF(ISW(10))120 ,80 ,120 |
| 5973 |
80 I3=-1 |
| 5974 |
90 RETURN |
| 5975 |
100 VALUE1=.4 |
| 5976 |
VALUE2=6.6666667D-1 |
| 5977 |
VALUE3=0.0 |
| 5978 |
GO TO 140 |
| 5979 |
110 CALL CRDET(2,W(1),VALUE1) |
| 5980 |
C (PICH-P)FRACT. FIN.STA.WITH RECL. PI1 PI0 L.E. |
| 5981 |
VALUE3=3.3333333D-1 |
| 5982 |
GO TO 130 |
| 5983 |
120 CALL CRDET(2,G(1),VALUE1) |
| 5984 |
VALUE3=STRKP |
| 5985 |
C (PIN-P)FRACT.FIN.STA.WITH RECL.PI1 PIO L.E. |
| 5986 |
130 VALUE1=CRDT(1) |
| 5987 |
VALUE2=CRDT(2) |
| 5988 |
140 CALL CALPHA |
| 5989 |
150 CALL CAECPL |
| 5990 |
IF(I1)160 ,160 ,80 |
| 5991 |
160 CALL CACOLL(-1) |
| 5992 |
IF(COL(15))80 ,170 ,80 |
| 5993 |
170 IF(PT(38))180 ,190 ,180 |
| 5994 |
180 I3=0 |
| 5995 |
GO TO 90 |
| 5996 |
190 PT(39)=0.0 |
| 5997 |
PT(3)=((E(4)-PM(4))/RCPMV)+PT(3) |
| 5998 |
I3=1 |
| 5999 |
GO TO 90 |
| 6000 |
END |
| 6001 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 6002 |
*-- Author : |
| 6003 |
SUBROUTINE ROUT18 |
| 6004 |
SAVE |
| 6005 |
C |
| 6006 |
#include "cbert.inc" |
| 6007 |
*KEND. |
| 6008 |
C |
| 6009 |
GOTO(10 ,20 ,80 ,210 ,170 ,190 ),I3 |
| 6010 |
10 I=3 |
| 6011 |
COL(15)=1.0 |
| 6012 |
K=27 |
| 6013 |
GO TO 30 |
| 6014 |
20 I=3 |
| 6015 |
COL(15)=4.0 |
| 6016 |
K=15 |
| 6017 |
30 PNIDK(1)=PM(I) |
| 6018 |
J=I |
| 6019 |
DO40 L=2,4 |
| 6020 |
PNIDK(L)=PXYZ(J) |
| 6021 |
40 J=J+4 |
| 6022 |
PNIDK(5)=E(I) |
| 6023 |
PNIDK(6)=PT(K-11) |
| 6024 |
CALLCALIDK |
| 6025 |
IF(K-27)60 ,50 ,60 |
| 6026 |
50 PT(15)=PT(15)+((PNIDK(12)-PNIDK( 6))/RCPMV) |
| 6027 |
60 PT(K)=PT(K)+((PNIDK(13)-DNCMS)/RCPMV) |
| 6028 |
I3=1 |
| 6029 |
70 IV=K |
| 6030 |
RETURN |
| 6031 |
80 K=3 |
| 6032 |
COL(15)=2.0 |
| 6033 |
IF(PT(2)-3.0)170 ,90 ,90 |
| 6034 |
90 IF(PT(K)-2500.0)110 ,110 ,100 |
| 6035 |
100 I3=5 |
| 6036 |
GOTO70 |
| 6037 |
110 IF(PT(K))150 ,150 ,120 |
| 6038 |
120 CCOFE = ECO(1) |
| 6039 |
IF(PT(K-1)-4.0) 140 ,130 ,130 |
| 6040 |
130 CCOFE = CCOFE - CTOFE + CTOFEN |
| 6041 |
140 IF(PT(K) - CCOFE ) 150 ,150 ,160 |
| 6042 |
150 M=PT(K-1) |
| 6043 |
PNBC(M)=PNBC(M)+1.0 |
| 6044 |
PT(K)=0.0 |
| 6045 |
I3=3 |
| 6046 |
GOTO70 |
| 6047 |
160 IF(K-3)170 ,170 ,210 |
| 6048 |
170 COL(15)=3.0 |
| 6049 |
K=15 |
| 6050 |
IF(PT(14)-2.0)180,180,90 |
| 6051 |
180 I3=2 |
| 6052 |
GOTO70 |
| 6053 |
190 L=14 |
| 6054 |
DO200 M=5,7 |
| 6055 |
PT(M)=PNIDK(L) |
| 6056 |
PT(M+12)=PNIDK(L+3) |
| 6057 |
200 L=L+1 |
| 6058 |
PT(11)=PNIDK(12) |
| 6059 |
PT(12)=PNIDK(6) |
| 6060 |
I=4 |
| 6061 |
K=39 |
| 6062 |
COL(15)=5.0 |
| 6063 |
GO TO 30 |
| 6064 |
210 I1=3 |
| 6065 |
220 K=12*I1-33 |
| 6066 |
IF(I1-4)230 ,240 ,250 |
| 6067 |
230 I2=-1 |
| 6068 |
GO TO 280 |
| 6069 |
240 I2=0 |
| 6070 |
GO TO 280 |
| 6071 |
250 IF(I1-5)240 ,270 ,260 |
| 6072 |
260 I3=4 |
| 6073 |
GO TO 70 |
| 6074 |
270 I2=1 |
| 6075 |
280 IF(PT(K))290 ,300 ,290 |
| 6076 |
290 CALL PSTOR |
| 6077 |
300 I1=I1+1 |
| 6078 |
GO TO 220 |
| 6079 |
END |
| 6080 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 6081 |
*-- Author : |
| 6082 |
SUBROUTINE ROUT19 |
| 6083 |
SAVE |
| 6084 |
C |
| 6085 |
#include "cbert.inc" |
| 6086 |
*KEND. |
| 6087 |
C |
| 6088 |
PT(3)=PT(3)+((PT(11)-PT(12))/RCPMV) |
| 6089 |
C COLLISION ALLOWED |
| 6090 |
K=3 |
| 6091 |
10 IF(PT(K)-2500.0)30 ,30 ,20 |
| 6092 |
20 I3=1 |
| 6093 |
GO TO 90 |
| 6094 |
30 IF(PT(K))70 ,70 ,40 |
| 6095 |
40 CCOFE = ECO(1) |
| 6096 |
IF(PT(K-1)-4.0) 60 ,50 ,50 |
| 6097 |
50 CCOFE = CCOFE - CTOFE + CTOFEN |
| 6098 |
60 IF(PT(K) - CCOFE) 70 ,70 ,170 |
| 6099 |
70 PT(K)=0.0 |
| 6100 |
IF(PT(K-1)-3.0)80 ,110 ,100 |
| 6101 |
80 I3=-1 |
| 6102 |
90 RETURN |
| 6103 |
100 IF(PT(K-1)-5.0)110 ,110 ,80 |
| 6104 |
110 M=PT(K-1) |
| 6105 |
PNBC(M)=PNBC(M)+1.0 |
| 6106 |
GOTO140 |
| 6107 |
120 I2=2 |
| 6108 |
130 I1=(K/12)+3 |
| 6109 |
CALLPSTOR |
| 6110 |
140 IF(K-15)150 ,160 ,190 |
| 6111 |
150 K=15 |
| 6112 |
IF(PT(15))160 ,160 ,120 |
| 6113 |
160 K=27 |
| 6114 |
PT(27)=PT(27)+((PNIDK(12)-PT(K+1))/RCPMV) |
| 6115 |
GOTO10 |
| 6116 |
170 IF(K-15)120 ,180 ,180 |
| 6117 |
180 I2=0 |
| 6118 |
GOTO130 |
| 6119 |
190 IF(K-27)80 ,200 ,210 |
| 6120 |
200 IF(PT(39))210 ,210 ,220 |
| 6121 |
210 I3=0 |
| 6122 |
GOTO90 |
| 6123 |
220 I2=1 |
| 6124 |
K=39 |
| 6125 |
GOTO130 |
| 6126 |
END |
| 6127 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 6128 |
*-- Author : |
| 6129 |
SUBROUTINE ROUT20(T,B,R,W,G) |
| 6130 |
REAL*8 T(115),B(80),R(239),W(60),G(55) |
| 6131 |
#include "cbert.inc" |
| 6132 |
*KEND. |
| 6133 |
SAVE |
| 6134 |
C |
| 6135 |
GO TO (10 ,50 ,70 ,80 ,190 ,200 ,290 ,60 ),I3 |
| 6136 |
10 PM(4)=DNCMS |
| 6137 |
CALL PINST |
| 6138 |
IF(I1)20 ,40 ,20 |
| 6139 |
20 I3=1 |
| 6140 |
30 RETURN |
| 6141 |
40 I3=2 |
| 6142 |
GOTO30 |
| 6143 |
50 ISW(9)=0 |
| 6144 |
60 ISW(10)=2 |
| 6145 |
I3=3 |
| 6146 |
GOTO30 |
| 6147 |
C PI MESON - SINGLE PRODUCTION |
| 6148 |
70 PT(2)=2.0 |
| 6149 |
I3=4 |
| 6150 |
GOTO30 |
| 6151 |
C COLLISION PARTICLE PI- |
| 6152 |
80 PT(2)=2.0 |
| 6153 |
PT(14)=1.0 |
| 6154 |
90 PM(3)=DNCMS |
| 6155 |
IF(740.0-RLKE)140 ,100 ,100 |
| 6156 |
100 IF(300.0-RLKE)110 ,130 ,130 |
| 6157 |
110 VALUE1=RLKE-300.0 |
| 6158 |
CALLCRDET(5,T(1),VALUE1) |
| 6159 |
C (N-P)DIFF.CRS.INT.EN. |
| 6160 |
I1=3 |
| 6161 |
I2=3 |
| 6162 |
120 I3=5 |
| 6163 |
GOTO30 |
| 6164 |
130 CALLCRDET(5,B(1),RLKE) |
| 6165 |
C (N-P)DIFF.CRS.LOW EN. |
| 6166 |
I1=3 |
| 6167 |
I2=1 |
| 6168 |
GOTO120 |
| 6169 |
140 IF(3500.0-RLKE)20 ,150 ,150 |
| 6170 |
150 IF(IT-17)160 ,20 ,20 |
| 6171 |
160 CALL DCINTP(R(1)) |
| 6172 |
C (N-P)DIFF.CRS.HIGH EN. |
| 6173 |
170 IF(I1)20 ,180,180 |
| 6174 |
180 I3=6 |
| 6175 |
GOTO30 |
| 6176 |
190 PT(2)=1.0 |
| 6177 |
PT(14)=2.0 |
| 6178 |
GOTO90 |
| 6179 |
200 PT(2)=2.0 |
| 6180 |
PT(14)=2.0 |
| 6181 |
210 PM(3)=DNCMS |
| 6182 |
IF(500.0-RLKE)230 ,220,220 |
| 6183 |
220 I3=7 |
| 6184 |
GOTO30 |
| 6185 |
230 IF(1000.0-RLKE)270 ,240 ,240 |
| 6186 |
240 CALL CADCPR(W(1),12) |
| 6187 |
IF(I2.EQ.1) GO TO 20 |
| 6188 |
C SAMPLE + MU IN CST |
| 6189 |
250 SNT=DSQRT(1.0-CST*CST) |
| 6190 |
C P-P SCATTERING |
| 6191 |
260 I3=8 |
| 6192 |
GOTO30 |
| 6193 |
C -, SCATTERING BACKWARD, MU LESS THAN 0 |
| 6194 |
270 IF(3500.0-RLKE)20 ,280 ,280 |
| 6195 |
280 CALL CADCPR(G(1),11) |
| 6196 |
IF(I2.EQ.1) GO TO 20 |
| 6197 |
C (P-P)DIFF.CRS.SEC.HIGH EN. |
| 6198 |
GOTO170 |
| 6199 |
290 PT(2)=1.0 |
| 6200 |
PT(14)=1.0 |
| 6201 |
GOTO210 |
| 6202 |
C NO PION PRODUCTION POSSIBLE |
| 6203 |
END |
| 6204 |
*CMZ : 0.92/00 02/12/92 16.02.26 by Christian Zeitnitz |
| 6205 |
*-- Author : |
| 6206 |
SUBROUTINE ROUT21(V,W,X,Y,Z) |
| 6207 |
C |
| 6208 |
#include "crandm.inc" |
| 6209 |
#include "cbert.inc" |
| 6210 |
*KEND. |
| 6211 |
C |
| 6212 |
REAL*8 V(161),W(101),X(161),Y(130),Z(176) |
| 6213 |
SAVE |
| 6214 |
C |
| 6215 |
VALUE2=RLKE*4.81633308D24+9.0554256D27 |
| 6216 |
C E(TR)**2=RLKE*RCPMV*2*NCMS+4*NCMS**2 |
| 6217 |
VALUE3=DSQRT(VALUE2) |
| 6218 |
GO TO (10 ,100 ,110 ,240 ),I3 |
| 6219 |
10 ISW(12)=0 |
| 6220 |
20 PT(38)=0.0 |
| 6221 |
I1=0 |
| 6222 |
ANS=RLKE |
| 6223 |
30 VALUE1=ANS-300.0 |
| 6224 |
CALL CRDET(1,V(1),VALUE1) |
| 6225 |
C (NUC-NUC) F(TR) ISOBAR SAMPLING |
| 6226 |
FTR=CRDT(1) |
| 6227 |
40 SN = RANDC(ISEED) |
| 6228 |
COM=SN*FTR |
| 6229 |
C R PRIME=F(TR)*RANDOM |
| 6230 |
CALL CAGENE(W(1)) |
| 6231 |
C (NUC-NUC)MASS OF ISOBAR S.P. M(R PRIME) |
| 6232 |
IF(I1)130 ,50 ,140 |
| 6233 |
50 COM1=(COM*COM-SQNM+VALUE2)/(2.0*VALUE3) |
| 6234 |
C E GAMMA |
| 6235 |
A=COM1*COM1-COM*COM |
| 6236 |
IF(A)60 ,70 ,70 |
| 6237 |
60 PGCNT=PGCNT+1.0 |
| 6238 |
GOTO40 |
| 6239 |
C |
| 6240 |
CZ changed in order to keep exponent small 5/21/92 |
| 6241 |
70 UNIVER=DSQRT(A)*COM1*(1.0D0-COM1/VALUE3) |
| 6242 |
CZ end of change |
| 6243 |
CZ |
| 6244 |
C F(M,TR)=P GAMMA*E GAMMA*E DELTA/E |
| 6245 |
CALL CRDET(1,X(1),VALUE1) |
| 6246 |
C (NUC-NUC)FMAX(TR) ISOBAR SAMPLING S.P. |
| 6247 |
COM1 = RANDC(ISEED) |
| 6248 |
IF(COM1-(UNIVER/CRDT(1)))80 ,80 ,40 |
| 6249 |
80 PM(4)=DNCMS |
| 6250 |
PM(3)=COM |
| 6251 |
CALL CANGID |
| 6252 |
PT(4)=DNCMS |
| 6253 |
PT(28)=DNCMS |
| 6254 |
CALL CALP19 |
| 6255 |
90 RETURN |
| 6256 |
100 ISW(12)=2 |
| 6257 |
GOTO20 |
| 6258 |
110 ISW(13)=0 |
| 6259 |
120 I1=-1 |
| 6260 |
ANS=((VALUE3-PNMS)**2-9.0554256D27)/4.81633308D24 |
| 6261 |
GO TO 30 |
| 6262 |
C TR PRIME COM1=RLKE PRIME |
| 6263 |
130 COM1=((VALUE3+DNCMS-COM)**2-9.0554256D27)/4.81633308D24 |
| 6264 |
COM2=COM |
| 6265 |
ANS=COM1 |
| 6266 |
COM4=FTR |
| 6267 |
I1=1 |
| 6268 |
GO TO 30 |
| 6269 |
140 COM1=(COM2*COM2-COM*COM+VALUE2)/(2.0*VALUE3) |
| 6270 |
C E EPSILON |
| 6271 |
A=COM1*COM1-COM2*COM2 |
| 6272 |
IF(A)150 ,160 ,160 |
| 6273 |
150 PECNT=PECNT+1.0 |
| 6274 |
GOTO170 |
| 6275 |
C F(M1,M2,TR)=P EPSILON*E EPSILON*E ZETA/E |
| 6276 |
C |
| 6277 |
CZ changed in order to keep exponent small 5/21/92 |
| 6278 |
160 UNIVER=DSQRT(A)*COM1*(1.0D0-COM1/VALUE3) |
| 6279 |
CZ end of change |
| 6280 |
CZ |
| 6281 |
VALUE1=RLKE-920.0 |
| 6282 |
CALLCRDET(1,Y(1),VALUE1) |
| 6283 |
C (NUC-NUC)FMAX(TR) ISOBAR SAMPLING D.P. FMAX(M1,M2,TR) |
| 6284 |
SN = RANDC(ISEED) |
| 6285 |
IF(SN-(UNIVER*FTR/(CRDT(1)*COM4)))180 ,180 ,170 |
| 6286 |
170 FTR=COM4 |
| 6287 |
I1=-1 |
| 6288 |
GOTO40 |
| 6289 |
180 VALUE1 = RANDC(ISEED) |
| 6290 |
IF(VALUE1-.5)190 ,190 ,200 |
| 6291 |
190 PM(3)=COM2 |
| 6292 |
PM(4)=COM |
| 6293 |
GOTO210 |
| 6294 |
200 PM(3)=COM |
| 6295 |
PM(4)=COM2 |
| 6296 |
210 CALLCANGID |
| 6297 |
PT(16)=DNCMS |
| 6298 |
PT(40)=DNCMS |
| 6299 |
IF(ISW(13))220 ,230 ,220 |
| 6300 |
220 CALL CRDET(1,Z(1),RLKE) |
| 6301 |
VALUE1=CRDT(1) |
| 6302 |
C (N-P)FRACT.FIN.STA.3/2 L.E. |
| 6303 |
230 PT(2)=3.0 |
| 6304 |
PT(4)=POMS |
| 6305 |
PT(14)=1.0 |
| 6306 |
PT(26)=3.0 |
| 6307 |
PT(28)=POMS |
| 6308 |
PT(38)=1.0 |
| 6309 |
CALL CALP28 |
| 6310 |
GO TO 90 |
| 6311 |
240 ISW(13)=2 |
| 6312 |
GO TO 120 |
| 6313 |
END |
| 6314 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 6315 |
*-- Author : |
| 6316 |
SUBROUTINE ROUT22(V,W,X,Y,Z) |
| 6317 |
REAL*8 V(19),W(19),X(126),Y(126),Z(126) |
| 6318 |
#include "cbert.inc" |
| 6319 |
*KEND. |
| 6320 |
SAVE |
| 6321 |
C |
| 6322 |
I5=CURR(1) |
| 6323 |
GOTO(270 ,1070,340 ,350 ,370 ,1040,520 ,1110,1170,460 ,1270,440 ,4 |
| 6324 |
+00 ,500 ,1440,10 ,700 ,590 ,260 ,530 ,430 ,1220,1570),IV |
| 6325 |
10 DO20 I=1,3 |
| 6326 |
XI(I)=CURR(I+3) |
| 6327 |
20 DCOS(I)=CURR(I+6) |
| 6328 |
IN=-1 |
| 6329 |
MED=CURR(10) |
| 6330 |
I5=CURR(1) |
| 6331 |
CALL CALGEO |
| 6332 |
IF(I1)60 ,30 ,30 |
| 6333 |
30 IF(CURR(1)-2.0)70 ,680 ,40 |
| 6334 |
40 IF(CURR(1)-4.0)690 ,700 ,50 |
| 6335 |
50 IV=1 |
| 6336 |
60 RETURN |
| 6337 |
70 ISW(4)=1 |
| 6338 |
C PROTON |
| 6339 |
80 XABS=0.0 |
| 6340 |
I4=1 |
| 6341 |
I2=MED |
| 6342 |
IF(I2-1)110,90 ,210 |
| 6343 |
90 I4=6 |
| 6344 |
GOTO210 |
| 6345 |
100 ISW(6)=1 |
| 6346 |
ISW(5)=1 |
| 6347 |
I3=0 |
| 6348 |
IF(COM-3600.0)120 ,120 ,110 |
| 6349 |
110 IV=2 |
| 6350 |
GOTO60 |
| 6351 |
C COM=GREATEST ENERGY INSIDE NUCLEUS FOR NUCLEONS ONLY |
| 6352 |
120 IF(COM-560.0)130 ,130 ,140 |
| 6353 |
130 IF(COM-160.0)200 ,200 ,190 |
| 6354 |
140 CALLDFMAX |
| 6355 |
C DFMAX FILLS OUT FMAX(1-6) |
| 6356 |
I1=6 |
| 6357 |
150 IF(CURR(1)-2.0)170 ,160 ,160 |
| 6358 |
160 I3=1 |
| 6359 |
170 CALLCSTORE |
| 6360 |
EX=0.0 |
| 6361 |
CALLSIGNEX |
| 6362 |
GOTO(260 ,370 ,430 ,480 ,400 ,580 ,920 ,1040,1170,180,1440),I4 |
| 6363 |
180 IV=3 |
| 6364 |
GOTO60 |
| 6365 |
190 ISW(6)=0 |
| 6366 |
CALLPFMAX |
| 6367 |
C PFMAX FILLS OUT FMAX(1-4) |
| 6368 |
I1=4 |
| 6369 |
GOTO150 |
| 6370 |
200 ISW(5)=0 |
| 6371 |
ISW(6)=0 |
| 6372 |
CALLCALNNN |
| 6373 |
C NN FILLS OUT FMAX(1-2),FMAX(3-6)=0 |
| 6374 |
I1=2 |
| 6375 |
GOTO150 |
| 6376 |
210 ISW(1)=0 |
| 6377 |
ISW(2)=0 |
| 6378 |
ISW(3)=0 |
| 6379 |
220 M=MED+ INT(15.0-6.0*SNGL(CURR(1))) |
| 6380 |
A=CURR(2)-SPACE(M) |
| 6381 |
230 DO240 I=1,3 |
| 6382 |
WKRPN(I)=A+SPACE(I+9) |
| 6383 |
240 WKRPN(I+3)=A+SPACE(I+3) |
| 6384 |
250 M=4-3*ISW(4) |
| 6385 |
COM=WKRPN(M) |
| 6386 |
GOTO100 |
| 6387 |
260 GOTO(1290,1290,270 ),I2 |
| 6388 |
270 IF(EX-D(2))310 ,310 ,280 |
| 6389 |
C ENTRY POINT FOR CASCADE CHARGED AND NEUTRAL PIONS AFTER CRJAB |
| 6390 |
C REJECTION,PROD.REACTION LT 180 FERMI REJECTION FOR NON-ABSORPTION |
| 6391 |
C REACTION ALSO ALL CASCADE NUCLEAR REJECTIONS INCLUDING CRJAB OR |
| 6392 |
C RLKE LT PROD.THRESHOLD |
| 6393 |
280 IF(D(3))560 ,290 ,560 |
| 6394 |
290 CALLCCPES |
| 6395 |
IF(I1)300,300,110 |
| 6396 |
C GO TO CAPUNP |
| 6397 |
300 IV=4 |
| 6398 |
GOTO60 |
| 6399 |
310 IF(IN) 320 ,320 ,1460 |
| 6400 |
320 CALLCBG6CA(3,0) |
| 6401 |
IFCC=12 |
| 6402 |
330 MED=CLSM |
| 6403 |
IV=5 |
| 6404 |
GOTO60 |
| 6405 |
340 VALUE1=EX |
| 6406 |
IV=6 |
| 6407 |
GOTO60 |
| 6408 |
350 VALUE1=EX+D(3) |
| 6409 |
360 IV=7 |
| 6410 |
GOTO60 |
| 6411 |
C E.P.FOR REJECTION FOLLOWING CRJAB OR RLKE LT 180 IN PROD.REACTIONS |
| 6412 |
C AND FOR FERMI REJECTION IN SCATTERING AND PRODUCTION REACTIONS |
| 6413 |
C FOR CASCADE CHARGED AND NEUTRAL PIONS |
| 6414 |
370 IF(EX-D(6))310 ,310 ,290 |
| 6415 |
380 ISW(1)=1 |
| 6416 |
390 GOTO(400 ,400 ,400 ,1040),I5 |
| 6417 |
C E.P.FOR ALL REJECTIONS,CRJAB,PRODUCTION,AND FERMI FOR CASCADE |
| 6418 |
C NUCLEONS |
| 6419 |
400 IF(EX-D(3))510 ,510 ,410 |
| 6420 |
410 I2=3 |
| 6421 |
I4=2 |
| 6422 |
I3=1 |
| 6423 |
I1=2 |
| 6424 |
IF(D(4))420 ,250 ,420 |
| 6425 |
420 ISW(2)=1 |
| 6426 |
ISW(3)=1 |
| 6427 |
I4=3 |
| 6428 |
I2=1 |
| 6429 |
GOTO250 |
| 6430 |
430 GOTO(440 ,440 ,440 ,1170),I5 |
| 6431 |
440 IF(EX-D(4))450 ,450 ,470 |
| 6432 |
450 CALLCBG6CA(1,0) |
| 6433 |
IFCC=7 |
| 6434 |
GOTO330 |
| 6435 |
460 VALUE1=EX |
| 6436 |
IV=8 |
| 6437 |
GOTO60 |
| 6438 |
470 I4=4 |
| 6439 |
I1=2 |
| 6440 |
I2=2 |
| 6441 |
I3=1 |
| 6442 |
GOTO250 |
| 6443 |
C E.P.FOR CASCADE NUCLEONS AND PI0,AFTER CRJAB AND PROD.THRESHOLD |
| 6444 |
C REJECTIONS |
| 6445 |
480 IF(I5-2)500 ,500 ,490 |
| 6446 |
490 IF(I5-4)110,1440,110 |
| 6447 |
C E.P.FOR CASCADE NUCLEONS AFTER ALL FERMI REJECTIONS |
| 6448 |
500 IF(EX-D(5))510 ,510 ,540 |
| 6449 |
510 CALLCBG6CA(2,0) |
| 6450 |
IFCC=10 |
| 6451 |
GOTO330 |
| 6452 |
520 VALUE1=EX |
| 6453 |
GOTO360 |
| 6454 |
530 IF(ISW(3))480 ,390 ,480 |
| 6455 |
540 I4=2 |
| 6456 |
I2=3 |
| 6457 |
550 I3=1 |
| 6458 |
I1=2 |
| 6459 |
GOTO250 |
| 6460 |
560 ISW(1)=1 |
| 6461 |
IF(CURR(1)-3.0)570 ,940 ,1390 |
| 6462 |
570 I4=5 |
| 6463 |
I2=2 |
| 6464 |
GOTO550 |
| 6465 |
C D.P. |
| 6466 |
580 ISW(1)=1 |
| 6467 |
ISW(2)=1 |
| 6468 |
ISW(3)=1 |
| 6469 |
GOTO260 |
| 6470 |
590 ANY=FMAX(NOT) |
| 6471 |
IF(NOT-5)620 ,600 ,610 |
| 6472 |
600 IV=9 |
| 6473 |
GOTO60 |
| 6474 |
610 IF(I5-4)600 ,630 ,600 |
| 6475 |
620 IF(KNOT-15)630 ,1560,1560 |
| 6476 |
630 GOTO(640 ,640 ,640 ,1510),I5 |
| 6477 |
640 IF(NOT-2)650 ,660 ,670 |
| 6478 |
650 IV=10 |
| 6479 |
GOTO60 |
| 6480 |
660 IV=11 |
| 6481 |
GOTO60 |
| 6482 |
670 IV=12 |
| 6483 |
GOTO60 |
| 6484 |
680 ISW(4)=0 |
| 6485 |
C NEUTRON |
| 6486 |
GOTO80 |
| 6487 |
690 ISW(11)=1 |
| 6488 |
C CURR(1)=3=PI+ MESON(11575)--PI 0=4(15100)--PI -(14646) |
| 6489 |
700 IN=1 |
| 6490 |
ISW(1)=0 |
| 6491 |
ISW(2)=0 |
| 6492 |
ISW(3)=0 |
| 6493 |
ISW(5)=1 |
| 6494 |
ISW(6)=0 |
| 6495 |
ISW(7)=0 |
| 6496 |
ISW(8)=1 |
| 6497 |
I6=I5-2 |
| 6498 |
I2=MED |
| 6499 |
COM=CURR(2)-SPACE(MED+9) |
| 6500 |
GOTO(720 ,710 ,730 ),MED |
| 6501 |
C E.P.FOR PI0 AFTER FERMI REJECTION |
| 6502 |
710 ISW(8)=0 |
| 6503 |
720 ISW(7)=1 |
| 6504 |
730 DO740 I=1,3 |
| 6505 |
WKRPN(I)=COM+SPACE(I+9) |
| 6506 |
740 WKRPN(I+3)=COM+SPACE(I+3) |
| 6507 |
COM=COM+SPACE(4) |
| 6508 |
750 IF(COM-2600.0)760 ,760 ,110 |
| 6509 |
760 IF(COM-100.0)770 ,770 ,780 |
| 6510 |
770 LG=4 |
| 6511 |
GOTO1330 |
| 6512 |
780 LG=6 |
| 6513 |
790 CALLCASPCN |
| 6514 |
IF(VALUE1)800 ,800 ,830 |
| 6515 |
800 COM=CURR(2)-SPACE(MED+9) |
| 6516 |
IF(COM-360.0)810 ,830 ,830 |
| 6517 |
810 GOTO(820 ,1350,820 ),I6 |
| 6518 |
820 CALLCRDET(1,V(1),COM) |
| 6519 |
FMAX(4)=CRDT(1) |
| 6520 |
830 GOTO(840 ,1360,840 ),I6 |
| 6521 |
840 I1=6 |
| 6522 |
850 I4=7 |
| 6523 |
I2=1 |
| 6524 |
I3=0 |
| 6525 |
GOTO(860 ,870 ,860 ),I6 |
| 6526 |
860 IF(ISW(11))870 ,910 ,870 |
| 6527 |
C PI+ |
| 6528 |
870 IF(ISW(7))880 ,900 ,880 |
| 6529 |
C PI- |
| 6530 |
880 IF(ISW(8))170 ,890 ,170 |
| 6531 |
890 I2=2 |
| 6532 |
GOTO170 |
| 6533 |
900 I2=3 |
| 6534 |
GOTO170 |
| 6535 |
910 I3=1 |
| 6536 |
GOTO870 |
| 6537 |
920 IF(CURR(1)-2.0)930 ,930 ,260 |
| 6538 |
930 A=CURR(2)-SPACE(MED+9) |
| 6539 |
GOTO230 |
| 6540 |
940 I4=8 |
| 6541 |
950 I2=2 |
| 6542 |
960 I3=0 |
| 6543 |
I1=LG |
| 6544 |
IF(CURR(1)-4.0)970 ,1030,970 |
| 6545 |
970 IF(ISW(11))990 ,980 ,990 |
| 6546 |
980 I3=1 |
| 6547 |
990 IF(CURR(1)-3.0)1000,1010,1010 |
| 6548 |
1000 IV=23 |
| 6549 |
GOTO60 |
| 6550 |
1010 IF(LG-4)1000,170 ,1020 |
| 6551 |
1020 M=5-IABS(I5-4) |
| 6552 |
UNIVER=FMAX(M) |
| 6553 |
CALLCASPCN |
| 6554 |
FMAX(M)=UNIVER |
| 6555 |
GOTO170 |
| 6556 |
1030 I1=I1+1 |
| 6557 |
GOTO1010 |
| 6558 |
C E.P.FOR CHARGED AND NEUTRAL PIONS AFTER CRJAB REJECTION ALSO,AFTER |
| 6559 |
C RLKE.LE.180 IN PROD.REACTIONS AND AFTER FERMI REJECTION IN SCATTER |
| 6560 |
C ING AND PROD.REACTIONS |
| 6561 |
1040 IF(EX-D(3))1050,1050,1140 |
| 6562 |
1050 GOTO(1060,1410,1060),I6 |
| 6563 |
1060 IV=13 |
| 6564 |
GOTO60 |
| 6565 |
1070 ANY=FMAX(NOT) |
| 6566 |
IF(CURR(1)-3.0)1080,1100,1100 |
| 6567 |
1080 IFC=12 |
| 6568 |
1090 IV=14 |
| 6569 |
GOTO60 |
| 6570 |
1100 IFCC=(CLSM-2.0)*((CLSM*5.5)-8.5)+12.05 |
| 6571 |
GOTO1090 |
| 6572 |
1110 IF(I4-10)1120,1210,1120 |
| 6573 |
C E.P.FOR ESCAPE PRIOR TO CHOOSING REACTIONS--CASCADE CHARGED PION |
| 6574 |
1120 IF(CLSM-2.0)1130,1210,1130 |
| 6575 |
1130 I4=2 |
| 6576 |
GOTO950 |
| 6577 |
1140 I4=2 |
| 6578 |
C E.P.WHEN CASCADE PARTICLE ESCAPES FROM REGION 2 |
| 6579 |
I2=3 |
| 6580 |
IF(D(4))1160,1150,1160 |
| 6581 |
1150 GOTO(960 ,1450,960 ),I6 |
| 6582 |
1160 ISW(2)=1 |
| 6583 |
ISW(3)=1 |
| 6584 |
I4=9 |
| 6585 |
I2=1 |
| 6586 |
GOTO1150 |
| 6587 |
C E.P.AFTER ALL REJECTIONS EXCEPT FERMI IN ABS.REACTIONS FOR |
| 6588 |
C CHARGED AND NEUTRAL CC PIONS--ESCAPE FROM REGION 1 PRIOR TO |
| 6589 |
C CHOOSING REACTION FOR CC CHARGED PION |
| 6590 |
1170 IF(EX-D(4))1180,1180,1200 |
| 6591 |
1180 GOTO(1190,1480,1190),I6 |
| 6592 |
1190 IV=15 |
| 6593 |
GOTO60 |
| 6594 |
1200 I4=10 |
| 6595 |
GOTO(950 ,1430,950 ),I6 |
| 6596 |
1210 I4=2 |
| 6597 |
I2=3 |
| 6598 |
GOTO960 |
| 6599 |
1220 IF(IN)1240,1230,1240 |
| 6600 |
1230 IV=16 |
| 6601 |
GOTO60 |
| 6602 |
1240 IFCA=8*IABS(I6-2)-11*(I6-1)*(I6-3) |
| 6603 |
IF(ISW(1))1250,340 ,1250 |
| 6604 |
1250 IF(ISW(2))1260,350,1260 |
| 6605 |
1260 IV=17 |
| 6606 |
GOTO60 |
| 6607 |
1270 IFCA=10*IABS(I6-2)+12*(I6-1)*(3-I6) |
| 6608 |
IF(ISW(3))1280,520,1280 |
| 6609 |
1280 IV=18 |
| 6610 |
GOTO60 |
| 6611 |
1290 IF(CURR(1)-3.0)1300,1310,1310 |
| 6612 |
1300 GOTO(430 ,380 ),MED |
| 6613 |
1310 ISW(1)=1 |
| 6614 |
GOTO(1320,1040),MED |
| 6615 |
1320 ISW(2)=1 |
| 6616 |
ISW(3)=1 |
| 6617 |
GOTO1170 |
| 6618 |
1330 ISW(5)=0 |
| 6619 |
GOTO(1340,1500,1340),I6 |
| 6620 |
1340 CALLCBOVER(CURR(2),PNMS,ANS) |
| 6621 |
FMAX(1)=.20 D-24*ANS |
| 6622 |
C (PI+P)SCATTERING |
| 6623 |
FMAX(2) = 23.0D-27*ANS |
| 6624 |
C (PIM+P)SCATTERING |
| 6625 |
FMAX(3)=45.1D-27*ANS |
| 6626 |
C (PIM+P)EXCHANGE |
| 6627 |
COM=CURR(2)-SPACE(MED+9) |
| 6628 |
C (K.E.OF PIONS OUTSIDE NUCLEUS |
| 6629 |
CALLCRDET(1,V(1),COM) |
| 6630 |
FMAX(4)=CRDT(1) |
| 6631 |
C C(PIP+P)ABS. |
| 6632 |
I1=4 |
| 6633 |
GOTO850 |
| 6634 |
1350 CALLCRDET(1,W(1),COM) |
| 6635 |
FMAX(5)=CRDT(1) |
| 6636 |
1360 I1=7 |
| 6637 |
GOTO850 |
| 6638 |
1370 CALLCBG6CA(3,4) |
| 6639 |
IFCC=24 |
| 6640 |
1380 KA=7 |
| 6641 |
MED=CLSM |
| 6642 |
IV=19 |
| 6643 |
GOTO60 |
| 6644 |
1390 I4=8 |
| 6645 |
1400 I2=2 |
| 6646 |
GOTO960 |
| 6647 |
1410 CALLCBG6CA(2,3) |
| 6648 |
1420 IFCC=21 |
| 6649 |
GOTO1380 |
| 6650 |
1430 I4=11 |
| 6651 |
GOTO1400 |
| 6652 |
1440 IF(EX-D(5))1410,1410,1490 |
| 6653 |
1450 I1=9-I5 |
| 6654 |
GOTO960 |
| 6655 |
1460 GOTO(1470,1370,1470),I6 |
| 6656 |
1470 IV=20 |
| 6657 |
GOTO60 |
| 6658 |
1480 CALLCBG6CA(1,2) |
| 6659 |
GOTO1420 |
| 6660 |
1490 I1=5 |
| 6661 |
GOTO1210 |
| 6662 |
1500 CALLCBOVER(CURR(2),POMS,ANS) |
| 6663 |
FMAX(1) = 89.2D-27*ANS |
| 6664 |
C (PI0+P)ELAST.SCAT. |
| 6665 |
FMAX(2)=45.1D-27*ANS |
| 6666 |
C (PI0+P)EX.SCAT. |
| 6667 |
FMAX(3)=FMAX(1) |
| 6668 |
SPACE(48)=FMAX(1) |
| 6669 |
FMAX(4)=FMAX(2) |
| 6670 |
SPACE(49)=FMAX(2) |
| 6671 |
COM=CURR(2)-SPACE(MED+9) |
| 6672 |
CALLCRDET(1,W(1),COM) |
| 6673 |
C (PIN-P)ABS. CRS.SEC. |
| 6674 |
FMAX(5)=CRDT(1) |
| 6675 |
C (PI0+P)ABS. |
| 6676 |
SPACE(50)=FMAX(5) |
| 6677 |
I1=5 |
| 6678 |
GOTO850 |
| 6679 |
1510 IF(NOT-2)1530,1550,1520 |
| 6680 |
1520 IV=21 |
| 6681 |
GOTO60 |
| 6682 |
1530 CALLCRJAB(1,X(1)) |
| 6683 |
C (PIN-P)DIRECT SCAT.CRS. |
| 6684 |
1540 IV=22 |
| 6685 |
GOTO60 |
| 6686 |
1550 CALLCRJAB(1,Y(1)) |
| 6687 |
C (PIM-P)XCH.SCAT.CRS. |
| 6688 |
GOTO1540 |
| 6689 |
1560 IF(KNOT-16)1570,1550,1550 |
| 6690 |
1570 CALLCRJAB(1,Z(1)) |
| 6691 |
C (PIN-N)DRCT.SCAT.CRS. |
| 6692 |
GOTO1540 |
| 6693 |
END |
| 6694 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 6695 |
*-- Author : |
| 6696 |
SUBROUTINE ROUT1 |
| 6697 |
SAVE |
| 6698 |
C |
| 6699 |
#include "cbert.inc" |
| 6700 |
*KEND. |
| 6701 |
C |
| 6702 |
OUT(11)=ZEE |
| 6703 |
VALUE2=ZEE**6.6666667D-1 |
| 6704 |
DO10 I=5,7 |
| 6705 |
SPACE(I+2)=OUT(I)*OUT(11) |
| 6706 |
10 SPACE(I+5)=(OUT(I+3)*VALUE2)+7.0 |
| 6707 |
C SCALED PROTONS PER CC AND POTENTIAL PROTON WELL DEPTH |
| 6708 |
C (MEV) IN EACH REGION |
| 6709 |
OUT(12)=AMASNO-OUT(11) |
| 6710 |
C NO. OF NEUTRONS N, STORED |
| 6711 |
VALUE2=OUT(12)**6.6666667D-1 |
| 6712 |
C N 2/3 |
| 6713 |
DO20 I=5,7 |
| 6714 |
SPACE(I-4)=OUT(I)*OUT(12) |
| 6715 |
20 SPACE(I-1)=(OUT(I+3)*VALUE2)+7.0 |
| 6716 |
C SCALED NEUTS. PER CC AND POT. NEUT. WELL DEPTH (MEV) |
| 6717 |
C IN EACH REGION |
| 6718 |
DO30 I=1,3 |
| 6719 |
HVN(I)=0.5*SPACE(I+3) |
| 6720 |
HVP(I)=0.5*SPACE(I+9) |
| 6721 |
AWD(I)=HVN(I)+HVP(I) |
| 6722 |
FVNP(I)=0.5*AWD(I) |
| 6723 |
VNVP(I)=SPACE(I+3)-SPACE(I+9) |
| 6724 |
PMAC(I)=VNVP(I)-HVN(I) |
| 6725 |
PPAN(I)=-VNVP(I)-HVP(I) |
| 6726 |
THPN(I)=HVP(I)-VNVP(I) |
| 6727 |
FFPTFN(I)=-VNVP(I)+FVNP(I) |
| 6728 |
TFFN(I)=SPACE(I+9)-FVNP(I) |
| 6729 |
30 TFFP(I)=VNVP(I)+TFFN(I) |
| 6730 |
PPPDA=(2.0*ZEE)/(ZEE+AMASNO-1.0) |
| 6731 |
PPMDA=(2.0*OUT(12))/(AMASNO+OUT(12)-1.0) |
| 6732 |
PPNDA=(2.0*ZEE*OUT(12))/(AMASNO*AMASNO-AMASNO) |
| 6733 |
PPNNA=(OUT(12)*OUT(12)-OUT(12))/(OUT(12)*OUT(12)+ZEE*ZEE-AMASNO) |
| 6734 |
C PION ABSORPTION CALC. FOR EACH REG. 1/2 NWD, (-PNAN, -PPAC) |
| 6735 |
C 1/2 PWD, (-PNAP, -PNAC) AV. WELL DEPTH, 1/4 AV. WELL DEPTH, |
| 6736 |
C (N-P)WELL DEPTH, (-VPVN), 1/2NWD -PWD, (PMAP, -VPHN), 1/2PWD -NWD, |
| 6737 |
C (-VNHP), 3/2PWD -NWD, 5/4PWD -3/4NWD, 3/4PWD -1/4NWD, |
| 6738 |
C 3/4NWD -1/4PWD, PROB. PIP DEUT ABS, PROB PIM DEUT ABS |
| 6739 |
C PROB PIN DEUT ABS, PROB PIN NN ABS RATHER THAN PP |
| 6740 |
K=15 |
| 6741 |
DO40 I=4,6 |
| 6742 |
OUT(K)=SPACE(I+6)+EINC |
| 6743 |
OUT(K+3)=SPACE(I)+EINC |
| 6744 |
40 K=K-1 |
| 6745 |
C TOTAL K.E. IN MEV INCIDENT PROTON(NEUTRON)PARTICLE IN EACH REGION |
| 6746 |
OUT(30)=(ZEE/OUT(4))*1.4412D-13 |
| 6747 |
C COULOMB POTENTIAL AT SURFACE IN MEV. CONVERSION |
| 6748 |
C FACTOR=MEV-CM PER PROTON (BG33) |
| 6749 |
IF(CTOFE)60,50,60 |
| 6750 |
50 CTOFE=OUT(30) |
| 6751 |
C IF CTOFE=0,THEN EQUATE IT TO1/2 POTENTIAL ENERGY AT SURFACE |
| 6752 |
60 DO70 I=1,3 |
| 6753 |
CFEPN(I+3)=SPACE(I+3)+CTOFEN |
| 6754 |
70 CFEPN(I)=SPACE(I+9)+CTOFE |
| 6755 |
C BG33P--CUTOFF ENERGIES IN EACH REGION FOR NEUTRONS(PROTONS) |
| 6756 |
IN=0 |
| 6757 |
VALUE1=6.28318531D10*(1.19366207D-1)**3.3333333D-1 |
| 6758 |
C CALC. OF FERMI MOMENTA PER CM. PF EQU. 2PI*((3/8PI)TO 1/3)*E10 |
| 6759 |
DO80 I=1,3 |
| 6760 |
FMPN(I)=VALUE1* (SPACE(I+6))**3.3333333D-1 |
| 6761 |
80 FMPN(I+3)=VALUE1* (SPACE(I))**3.3333333D-1 |
| 6762 |
C FERMI MOMENTA PER CM. OF PROTONS(NEUTRONS) |
| 6763 |
DO 90 I = 1,4 |
| 6764 |
90 RANDS(I)=RANDI(I) |
| 6765 |
RETURN |
| 6766 |
END |
| 6767 |
*CMZ : 0.92/05 19/12/92 15.36.43 by Christian Zeitnitz |
| 6768 |
*-- Author : |
| 6769 |
SUBROUTINE ROUT2(T) |
| 6770 |
REAL*8 T(19) |
| 6771 |
C |
| 6772 |
#include "cbert.inc" |
| 6773 |
*KEND. |
| 6774 |
SAVE |
| 6775 |
C |
| 6776 |
I1=1 |
| 6777 |
VALUE2=EINC+SPACE(12) |
| 6778 |
CALL CBOVER(VALUE2,PNMS,ANS) |
| 6779 |
SPACE(14)=0.20D-24*ANS |
| 6780 |
C PIP+P |
| 6781 |
SPACE(15)=0.023D-24*ANS |
| 6782 |
C (PIM+P)EL |
| 6783 |
SPACE(16)=.0451D-24*ANS |
| 6784 |
C (PIM+P)EX |
| 6785 |
C 180 |
| 6786 |
IF(VALUE1-100.0)10 ,10 ,50 |
| 6787 |
10 FMAX(1)=SPACE(14) |
| 6788 |
FMAX(2)=SPACE(15) |
| 6789 |
FMAX(3)=SPACE(16) |
| 6790 |
S(1)=0.0 |
| 6791 |
S(2)=0.0 |
| 6792 |
20 CALLCRDET(1,T(1),EINC) |
| 6793 |
C (PIP-P) ABSORPTION CROSS SECTION |
| 6794 |
SPACE(17)=CRDT(1) |
| 6795 |
IF(I1)40 ,40 ,30 |
| 6796 |
30 FMAX(4)=SPACE(17) |
| 6797 |
40 RETURN |
| 6798 |
50 IF(VALUE2-2600.0)70 ,70 ,60 |
| 6799 |
C VALUE2 IS GREATER THAN 2600 |
| 6800 |
60 I1=0 |
| 6801 |
GOTO40 |
| 6802 |
70 SPACE(17)=0.0 |
| 6803 |
IF(VALUE2-220.0)80 ,80 ,90 |
| 6804 |
80 S(1)=0.75D-27*ANS |
| 6805 |
C (PIP-P)S.P. 400MEV |
| 6806 |
S(2)=4.7D-27*ANS |
| 6807 |
C (PIM-P)S.P. 400MEV |
| 6808 |
GOTO110 |
| 6809 |
90 IF(VALUE2-400.0)100,100,120 |
| 6810 |
100 SPACE(14)=0.20D-24 |
| 6811 |
SPACE(16)=.0451D-24 |
| 6812 |
S(1)=7.8D-27*ANS |
| 6813 |
S(2)=21.8D-27*ANS |
| 6814 |
C 660 MEV |
| 6815 |
110 IF(EINC-360.0)20 ,40 ,40 |
| 6816 |
120 IF(VALUE2-500.0)130,130,140 |
| 6817 |
130 SPACE(14)=.113D-24 |
| 6818 |
C 250 MEV |
| 6819 |
SPACE(15)=20.5D-27*ANS |
| 6820 |
C 620 MEV |
| 6821 |
SPACE(16)=27.7D-27 |
| 6822 |
C 250 MEV |
| 6823 |
S(1)=13.8D-27*ANS |
| 6824 |
S(2)=24.4D-27*ANS |
| 6825 |
C 800 MEV |
| 6826 |
I1=-1 |
| 6827 |
GOTO110 |
| 6828 |
140 S(2)=30.4D-27*ANS |
| 6829 |
SPACE(15)=26.3D-27*ANS |
| 6830 |
C 900 |
| 6831 |
IF(VALUE2-600.0)150,150,160 |
| 6832 |
C 940,325 |
| 6833 |
150 SPACE(14)=53.0D-27 |
| 6834 |
C 325 |
| 6835 |
C VALUE2 LTE 600 |
| 6836 |
C 325 |
| 6837 |
SPACE(16)=16.2D-27 |
| 6838 |
S(1)=15.2D-27*ANS |
| 6839 |
C 940 |
| 6840 |
GOTO40 |
| 6841 |
160 IF(VALUE2-800.0)170,170,180 |
| 6842 |
C 1200,400 |
| 6843 |
170 SPACE(14)=33.0D-27 |
| 6844 |
C 400 |
| 6845 |
SPACE(16)=12.0D-27*ANS |
| 6846 |
C 400 |
| 6847 |
S(1)=20.9D-27*ANS |
| 6848 |
C 1200 |
| 6849 |
GOTO40 |
| 6850 |
180 SPACE(14)=19.3D-27*ANS |
| 6851 |
C 1300 |
| 6852 |
SPACE(16)=8.2D-27*ANS |
| 6853 |
C 540 |
| 6854 |
S(1)=23.3D-27*ANS |
| 6855 |
C 1400 |
| 6856 |
S(2)=30.4D-27*ANS |
| 6857 |
C SIGMA(A) 900+2MB FOR FUTURE CORRECTION |
| 6858 |
GOTO40 |
| 6859 |
C VALUES OF FI FOR BOTH INCIDENT AND CASCADE PARTICLES FOR |
| 6860 |
C CHARGED PIONS(PI +OR-) ,SINGLE PRODUCTION. S(1)=N)S.P., S(2)=P) |
| 6861 |
C S.P., SPACE(14)=N)S, SPACE(15)=P)D.S., SPACE(16)=P)ABS, SPACE(17) |
| 6862 |
C =P)ABS (PPAC) |
| 6863 |
END |
| 6864 |
*CMZ : 0.92/00 02/12/92 16.02.27 by Christian Zeitnitz |
| 6865 |
*-- Author : |
| 6866 |
SUBROUTINE ROUT3 |
| 6867 |
C |
| 6868 |
#include "cbert.inc" |
| 6869 |
*KEND. |
| 6870 |
C |
| 6871 |
IF(NO-4)10 ,20 ,20 |
| 6872 |
C BG6A IN ORIGINAL |
| 6873 |
10 ISW(11)=1 |
| 6874 |
GOTO30 |
| 6875 |
20 ISW(11)=0 |
| 6876 |
30 CALL UNDIS |
| 6877 |
INC=1 |
| 6878 |
RETURN |
| 6879 |
END |
| 6880 |
*CMZ : 0.92/00 02/12/92 16.02.27 by Christian Zeitnitz |
| 6881 |
*-- Author : |
| 6882 |
SUBROUTINE ROUT4 |
| 6883 |
C |
| 6884 |
#include "cbert.inc" |
| 6885 |
*KEND. |
| 6886 |
C |
| 6887 |
CALL CALGEO |
| 6888 |
IF(I1) 20,10,10 |
| 6889 |
10 CURR(3)=PNMS |
| 6890 |
C PI+ OR -MASS/CM |
| 6891 |
CURR(1)=NO |
| 6892 |
CALL PARTIN |
| 6893 |
CALL SPAC32(32) |
| 6894 |
20 RETURN |
| 6895 |
END |
| 6896 |
*CMZ : 0.92/00 02/12/92 16.02.27 by Christian Zeitnitz |
| 6897 |
*-- Author : |
| 6898 |
SUBROUTINE ROUT5(T,B,R) |
| 6899 |
REAL*8 T(126),B(126),R(126) |
| 6900 |
C |
| 6901 |
#include "cbert.inc" |
| 6902 |
*KEND. |
| 6903 |
C |
| 6904 |
IF(NOT-2) 10 ,20 ,30 |
| 6905 |
10 CALL CRJAB(1,T(1)) |
| 6906 |
GO TO 40 |
| 6907 |
C (PIP-P)ELASTIC SCATTERING CRS. |
| 6908 |
20 CALL CRJAB(1,B(1)) |
| 6909 |
GO TO 40 |
| 6910 |
C (PIM-P)DIRECT SCATTERING CRS. |
| 6911 |
30 CALLCRJAB(1,R(1)) |
| 6912 |
40 RETURN |
| 6913 |
END |
| 6914 |
*CMZ : 0.92/03 10/12/92 10.54.57 by Christian Zeitnitz |
| 6915 |
*-- Author : |
| 6916 |
SUBROUTINE ROUT6 |
| 6917 |
C |
| 6918 |
#include "crandm.inc" |
| 6919 |
*KEND. |
| 6920 |
C |
| 6921 |
#include "cbert.inc" |
| 6922 |
*KEND. |
| 6923 |
C |
| 6924 |
IF(I3)10 ,90 ,90 |
| 6925 |
10 XABS=1.0 |
| 6926 |
MED=CLSM |
| 6927 |
KNOT=NOT |
| 6928 |
VALUE1 = RANDC(ISEED) |
| 6929 |
IF(ISW(11))50 ,20 ,50 |
| 6930 |
20 IF(VALUE1-PPMDA)60 ,40 ,40 |
| 6931 |
C PROB. PIM-DEUT ABS. |
| 6932 |
30 RETURN |
| 6933 |
40 I3=1 |
| 6934 |
GO TO 30 |
| 6935 |
50 IF(VALUE1-PPPDA)60 ,40 ,40 |
| 6936 |
C PROB. PIP-DEUT ABS. |
| 6937 |
60 IF(ISW(11))80 ,70 ,80 |
| 6938 |
70 IT=13 |
| 6939 |
ABSEC=PMAC(MED) |
| 6940 |
GO TO 90 |
| 6941 |
80 IT=14 |
| 6942 |
ABSEC=-HVN(MED) |
| 6943 |
90 STRKP=-1.0 |
| 6944 |
I1=0 |
| 6945 |
I2=MED |
| 6946 |
CALL CBBBBB |
| 6947 |
I3=0 |
| 6948 |
GO TO 30 |
| 6949 |
END |
| 6950 |
*CMZ : 0.92/00 02/12/92 16.02.27 by Christian Zeitnitz |
| 6951 |
*-- Author : |
| 6952 |
SUBROUTINE ROUT6A |
| 6953 |
SAVE |
| 6954 |
C |
| 6955 |
#include "cbert.inc" |
| 6956 |
*KEND. |
| 6957 |
C |
| 6958 |
10 I1=0 |
| 6959 |
CALL SPISOM |
| 6960 |
STRKP=-2.0 |
| 6961 |
I1=1 |
| 6962 |
CALL SPISOM |
| 6963 |
STRKP=-1.0 |
| 6964 |
COM=(AWD(MED)-7.0)*2.0*RCPMV |
| 6965 |
IF(COM-E(2))10 ,10 ,20 |
| 6966 |
20 PM(2)=2.0*DNCMS |
| 6967 |
PM(3)=DNCMS |
| 6968 |
E(2)=PM(2)+E(2) |
| 6969 |
RETURN |
| 6970 |
END |
| 6971 |
*CMZ : 0.92/00 02/12/92 16.02.27 by Christian Zeitnitz |
| 6972 |
*-- Author : |
| 6973 |
SUBROUTINE ROUT7 |
| 6974 |
C |
| 6975 |
#include "crandm.inc" |
| 6976 |
*KEND. |
| 6977 |
C |
| 6978 |
#include "cbert.inc" |
| 6979 |
*KEND. |
| 6980 |
SAVE |
| 6981 |
I3=0 |
| 6982 |
IF(CURR(1)-3.0)20 ,50 ,10 |
| 6983 |
10 IF(CURR(1)-5.0)60 ,40 ,20 |
| 6984 |
C PROTON, NEUTRON NOT PERMITTED |
| 6985 |
20 I3=-1 |
| 6986 |
30 RETURN |
| 6987 |
40 IT=7 |
| 6988 |
IFCA=5 |
| 6989 |
C PI MESON - (5) |
| 6990 |
ABSEC=PMAC(MED) |
| 6991 |
C PIM +PP ABS. TYOR=PMAPP(20021) |
| 6992 |
GOTO90 |
| 6993 |
50 IT=10 |
| 6994 |
IFCA=3 |
| 6995 |
C TYOR=PPAN(20004) PIP-NN ABS. ENERGY CORRECTION PIMESON + |
| 6996 |
ABSEC=PPAN(MED) |
| 6997 |
GOTO100 |
| 6998 |
60 VALUE1 = RANDC(ISEED) |
| 6999 |
IF(VALUE1-PPNNA)70 ,80 ,80 |
| 7000 |
70 IT=8 |
| 7001 |
IFCA=4 |
| 7002 |
C PNANN(20015)=TYOR PIN-NN ABS PIMESON 0 |
| 7003 |
ABSEC=-HVN(MED) |
| 7004 |
GOTO100 |
| 7005 |
80 IT=9 |
| 7006 |
IFCA=2 |
| 7007 |
C PNAPP(20011)=TYOR PIN+PP ABS. PIMESON 0 |
| 7008 |
ABSEC=-HVP(MED) |
| 7009 |
90 STRKP=-1.0 |
| 7010 |
E(1)=WKRPN(MED)*RCPMV+PM(1) |
| 7011 |
GOTO110 |
| 7012 |
100 STRKP=-2.0 |
| 7013 |
E(1)=WKRPN(MED+3)*RCPMV+PM(1) |
| 7014 |
110 IF(INC)130,120,130 |
| 7015 |
120 CALLP1CLC |
| 7016 |
GOTO30 |
| 7017 |
130 CALLP1CLI |
| 7018 |
GOTO30 |
| 7019 |
END |
| 7020 |
*CMZ : 0.92/00 02/12/92 16.02.27 by Christian Zeitnitz |
| 7021 |
*-- Author : |
| 7022 |
SUBROUTINE ROUT7A |
| 7023 |
#include "cbert.inc" |
| 7024 |
*KEND. |
| 7025 |
C |
| 7026 |
SAVE |
| 7027 |
10 I1=-1 |
| 7028 |
CALLSPISOM |
| 7029 |
GOTO(20 ,30 ,20 ,20 ,30 ),IFCA |
| 7030 |
20 VALUE1=SPACE(MED+3)-7.0 |
| 7031 |
GOTO40 |
| 7032 |
30 VALUE1=SPACE(MED+9)-7.0 |
| 7033 |
40 IF(VALUE1)50 ,70 ,70 |
| 7034 |
50 I3=2 |
| 7035 |
60 RETURN |
| 7036 |
70 IF((VALUE1*2.0*RCPMV)-E(2))10 ,10 ,80 |
| 7037 |
80 PM(3)=DNCMS |
| 7038 |
PM(2)=2.0*DNCMS |
| 7039 |
E(2)=PM(2)+E(2) |
| 7040 |
VALUE1=EX |
| 7041 |
IF(MED-2)90 ,100,110 |
| 7042 |
90 I3=3 |
| 7043 |
GOTO60 |
| 7044 |
100 I3=4 |
| 7045 |
GOTO60 |
| 7046 |
110 IF(INC)120,170,120 |
| 7047 |
120 IF(ISW(1))140,130,140 |
| 7048 |
130 I3=5 |
| 7049 |
GOTO60 |
| 7050 |
140 IF(ISW(2))150,160,150 |
| 7051 |
150 I3=6 |
| 7052 |
GOTO60 |
| 7053 |
160 I3=9 |
| 7054 |
GOTO60 |
| 7055 |
170 IF(ISW(1))190,180,190 |
| 7056 |
180 I3=7 |
| 7057 |
GOTO60 |
| 7058 |
190 IF(ISW(2))200,210,200 |
| 7059 |
200 I3=1 |
| 7060 |
GOTO60 |
| 7061 |
210 I3=8 |
| 7062 |
GOTO60 |
| 7063 |
END |
| 7064 |
*CMZ : 0.92/00 02/12/92 16.02.27 by Christian Zeitnitz |
| 7065 |
*-- Author : |
| 7066 |
SUBROUTINE ROUT8 |
| 7067 |
C |
| 7068 |
#include "cbert.inc" |
| 7069 |
*KEND. |
| 7070 |
C |
| 7071 |
SAVE |
| 7072 |
I3=1 |
| 7073 |
IF(IV) 20 ,10 ,10 |
| 7074 |
10 IF(VALUE1-VALUE2) 20 ,20 ,110 |
| 7075 |
20 IF(ISW(3)) 80 ,30 ,80 |
| 7076 |
30 IFC=7+IFCC |
| 7077 |
C 7=BG6E(2461) 8=BG6IA(4026) NTNT(21626) BG48X(12762)=19 |
| 7078 |
IF(IN) 40 ,60 ,40 |
| 7079 |
40 I3=2 |
| 7080 |
50 RETURN |
| 7081 |
60 C(3)=D(2) |
| 7082 |
GO TO 70 |
| 7083 |
70 I3=3 |
| 7084 |
GO TO 50 |
| 7085 |
80 IFC=8+IFCC |
| 7086 |
IF(IN)90 ,100,90 |
| 7087 |
90 I3=4 |
| 7088 |
GO TO 50 |
| 7089 |
100 C(3)=D(2)+D(3)+D(4) |
| 7090 |
GO TO 70 |
| 7091 |
110 CALL SIGNEX |
| 7092 |
GOTO 50 |
| 7093 |
END |
| 7094 |
*CMZ : 0.90/00 05/06/92 10.57.24 by Christian Zeitnitz |
| 7095 |
*-- Author : |
| 7096 |
SUBROUTINE SIGNEX |
| 7097 |
#include "cbert.inc" |
| 7098 |
*KEND. |
| 7099 |
SAVE |
| 7100 |
C |
| 7101 |
CALL EXPRN(UNIV) |
| 7102 |
EX=EX+UNIV/SIGN |
| 7103 |
RETURN |
| 7104 |
C EX=DISTANCE IN SAMPLING ROUTINE |
| 7105 |
C EXPONENTIAL RANDOM DIVIDED BY SIGMA CI REGION I |
| 7106 |
END |
| 7107 |
*CMZ : 0.92/00 02/12/92 16.02.27 by Christian Zeitnitz |
| 7108 |
*-- Author : |
| 7109 |
SUBROUTINE SPAC32(I) |
| 7110 |
#include "cbert.inc" |
| 7111 |
*KEND. |
| 7112 |
SAVE |
| 7113 |
C |
| 7114 |
EX=0.0 |
| 7115 |
I4=5 |
| 7116 |
SIGN=9.99999D-1*SPACE(I) |
| 7117 |
IF(I-31)10,20,30 |
| 7118 |
10 I2=18 |
| 7119 |
I3=3 |
| 7120 |
GOTO90 |
| 7121 |
20 I2=22 |
| 7122 |
I3=5 |
| 7123 |
GOTO90 |
| 7124 |
30 IF(I-41)40,50,50 |
| 7125 |
40 I2=26 |
| 7126 |
I3=7 |
| 7127 |
GOTO90 |
| 7128 |
50 I4=3 |
| 7129 |
IF(I-42)60,70,80 |
| 7130 |
60 I2=35 |
| 7131 |
I3=13 |
| 7132 |
GOTO90 |
| 7133 |
70 I2=37 |
| 7134 |
I3=17 |
| 7135 |
GOTO90 |
| 7136 |
80 I2=39 |
| 7137 |
I3=21 |
| 7138 |
90 CALLCABG6B |
| 7139 |
CALLSIGNEX |
| 7140 |
RETURN |
| 7141 |
END |
| 7142 |
*CMZ : 0.92/00 02/12/92 16.02.27 by Christian Zeitnitz |
| 7143 |
*-- Author : |
| 7144 |
SUBROUTINE CASPCN |
| 7145 |
#include "cbert.inc" |
| 7146 |
*KEND. |
| 7147 |
REAL*8 WK |
| 7148 |
SAVE |
| 7149 |
C |
| 7150 |
FMAX(4)=0.0 |
| 7151 |
FMAX(5)=0.0 |
| 7152 |
I6=CURR(1)-1.95 |
| 7153 |
WK=WKRPN(I2) |
| 7154 |
GOTO(10,20,10),I6 |
| 7155 |
10 UNIV=PNMS |
| 7156 |
GOTO30 |
| 7157 |
20 UNIV=POMS |
| 7158 |
30 CALLCBOVER(WK,UNIV,UNIVE) |
| 7159 |
VALUE1=0.0 |
| 7160 |
IF(WK-220.0)40,40,100 |
| 7161 |
40 GOTO(50,80,50),I6 |
| 7162 |
50 FMAX(5)=0.35D-27*UNIVE |
| 7163 |
C (PIP+P)S.P. |
| 7164 |
FMAX(6)=2.3D-27*UNIVE |
| 7165 |
C (PIM+P)S.P. |
| 7166 |
FMAX(1)=0.20D-24*UNIVE |
| 7167 |
C (PIP+P)SC |
| 7168 |
FMAX(3)=.0451D-24*UNIVE |
| 7169 |
C (PIM+P)EX |
| 7170 |
60 FMAX(2)=0.023D-24*UNIVE |
| 7171 |
C (PIM-P)SC |
| 7172 |
70 RETURN |
| 7173 |
80 FMAX(6)=1.35D-27*UNIVE |
| 7174 |
C (PI0+P)S.P. |
| 7175 |
FMAX(1)=89.2D-27*UNIVE |
| 7176 |
C (PI0+P)SC |
| 7177 |
FMAX(2)=.0451D-24*UNIVE |
| 7178 |
C (PI0+P)EX |
| 7179 |
90 FMAX(3)=FMAX(1) |
| 7180 |
C (PI0+N)SC |
| 7181 |
FMAX(4)=FMAX(2) |
| 7182 |
C (PI0+N)EX |
| 7183 |
FMAX(7)=FMAX(6) |
| 7184 |
C (PI0+N)S.P. |
| 7185 |
GOTO70 |
| 7186 |
100 IF(WK-400.0)110,110,140 |
| 7187 |
110 GOTO(120,130,120),I6 |
| 7188 |
120 FMAX(5)=4.5D-27*UNIVE |
| 7189 |
FMAX(6)=20.6D-27*UNIVE |
| 7190 |
FMAX(1)=0.20D-24 |
| 7191 |
FMAX(3)=.0451D-24 |
| 7192 |
GOTO60 |
| 7193 |
130 FMAX(6)=12.5D-27*UNIVE |
| 7194 |
FMAX(1)=89.2D-27 |
| 7195 |
FMAX(2)=.0451D-24 |
| 7196 |
GOTO90 |
| 7197 |
140 IF(WK-500.0)150,150,180 |
| 7198 |
150 GOTO(160,170,160),I6 |
| 7199 |
160 FMAX(1)=.113D-24 |
| 7200 |
FMAX(2)=20.5D-27*UNIVE |
| 7201 |
FMAX(3)=27.7D-27 |
| 7202 |
FMAX(5)=11.7D-27*UNIVE |
| 7203 |
FMAX(6)=21.7D-27*UNIVE |
| 7204 |
GOTO70 |
| 7205 |
170 FMAX(1)=50.8D-27 |
| 7206 |
FMAX(2)=27.7D-27 |
| 7207 |
FMAX(6)=14.6D-27*UNIVE |
| 7208 |
GOTO90 |
| 7209 |
180 VALUE1=1.0 |
| 7210 |
IF(WK-600.0)190,190,220 |
| 7211 |
190 GOTO(200,210,200),I6 |
| 7212 |
200 FMAX(1)=51.0D-27 |
| 7213 |
FMAX(2)=24.7D-27*UNIVE |
| 7214 |
FMAX(3)=15.5D-27*UNIVE |
| 7215 |
FMAX(5)=15.1D-27*UNIVE |
| 7216 |
FMAX(6)=30.4D-27*UNIVE |
| 7217 |
GOTO70 |
| 7218 |
210 FMAX(1)=23.0D-27*UNIVE |
| 7219 |
FMAX(2)=15.5D-27*UNIVE |
| 7220 |
FMAX(6)=22.6D-27*UNIVE |
| 7221 |
GOTO90 |
| 7222 |
220 IF(WK-800.0)230,230,260 |
| 7223 |
230 GOTO(240,250,240),I6 |
| 7224 |
240 FMAX(1)=33.0D-27 |
| 7225 |
FMAX(2)=26.3D-27*UNIVE |
| 7226 |
FMAX(3)=12.0D-27*UNIVE |
| 7227 |
FMAX(5)=20.1D-27*UNIVE |
| 7228 |
FMAX(6)=30.4D-27*UNIVE |
| 7229 |
GOTO70 |
| 7230 |
250 FMAX(1)=16.0D-27*UNIVE |
| 7231 |
FMAX(2)=12.0D-27*UNIVE |
| 7232 |
FMAX(6)=22.6D-27*UNIVE |
| 7233 |
GOTO90 |
| 7234 |
260 GOTO(270,280,270),I6 |
| 7235 |
270 FMAX(1)=19.3D-27*UNIVE |
| 7236 |
FMAX(2)=26.3D-27*UNIVE |
| 7237 |
FMAX(3)=8.2D-27*UNIVE |
| 7238 |
FMAX(5)=23.3D-27*UNIVE |
| 7239 |
FMAX(6)=30.4D-27*UNIVE |
| 7240 |
GOTO70 |
| 7241 |
280 FMAX(1)=16.0D-27*UNIVE |
| 7242 |
FMAX(2)=8.2D-27*UNIVE |
| 7243 |
FMAX(6)=24.9D-27*UNIVE |
| 7244 |
GOTO90 |
| 7245 |
END |
| 7246 |
*CMZ : 0.92/00 02/12/92 16.02.27 by Christian Zeitnitz |
| 7247 |
*-- Author : |
| 7248 |
SUBROUTINE SPISOM |
| 7249 |
#include "cbert.inc" |
| 7250 |
*KEND. |
| 7251 |
SAVE |
| 7252 |
C |
| 7253 |
10 CALL CAISOM |
| 7254 |
IF(I1)20,20,30 |
| 7255 |
20 SPACE(176)=PXYZ(2) |
| 7256 |
SPACE(177)=PXYZ(6) |
| 7257 |
SPACE(178)=PXYZ(10) |
| 7258 |
IF(I1)50,40,40 |
| 7259 |
30 PXYZ(2)=PXYZ(2)+SPACE(176) |
| 7260 |
PXYZ(6)=PXYZ(6)+SPACE(177) |
| 7261 |
PXYZ(10)=PXYZ(10)+SPACE(178) |
| 7262 |
E(2)=(PXYZ(10)*PXYZ(10)+PXYZ(6)*PXYZ(6)+PXYZ(2)*PXYZ(2))/ |
| 7263 |
11.9032D14 |
| 7264 |
40 RETURN |
| 7265 |
50 I1=1 |
| 7266 |
GOTO10 |
| 7267 |
END |
| 7268 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 7269 |
*-- Author : |
| 7270 |
SUBROUTINE CSTORE |
| 7271 |
#include "cbert.inc" |
| 7272 |
*KEND. |
| 7273 |
REAL * 8 SUB1,SUB2 |
| 7274 |
SAVE |
| 7275 |
C |
| 7276 |
CALL CZERO |
| 7277 |
N=I1 |
| 7278 |
IF(I3)200,10,200 |
| 7279 |
10 K=I2+6 |
| 7280 |
L=I2 |
| 7281 |
GOTO(50,50,50,20,50),I5 |
| 7282 |
20 IF(I1-5)30,230,30 |
| 7283 |
30 MM=-6 |
| 7284 |
40 L=K |
| 7285 |
N=N-1 |
| 7286 |
50 DO110 I=1,N,2 |
| 7287 |
ID=I |
| 7288 |
CE(I+1)=FMAX(I)*1.0D30*SPACE(K) |
| 7289 |
CE(I+2)=FMAX(I+1)*1.0D30*SPACE(L) |
| 7290 |
GOTO(110,110,60,60,60),I5 |
| 7291 |
60 M=K |
| 7292 |
K=L |
| 7293 |
GOTO(110,110,100,80,70),I5 |
| 7294 |
70 IF(ID-2)110,110,90 |
| 7295 |
80 K=M+MM |
| 7296 |
MM=-MM |
| 7297 |
L=K |
| 7298 |
GOTO110 |
| 7299 |
90 K=I2 |
| 7300 |
100 L=M |
| 7301 |
110 CONTINUE |
| 7302 |
GOTO(120,120,120,220,120),I5 |
| 7303 |
120 SIGN=0.0 |
| 7304 |
DO130 I=2,8 |
| 7305 |
130 SIGN=SIGN+CE(I) |
| 7306 |
GOTO(140,140,150,250,150),I5 |
| 7307 |
140 SIGN=SIGN*9.99999D-1 |
| 7308 |
RETURN |
| 7309 |
150 IF(I1-4)160,160,140 |
| 7310 |
160 IF(I3)170,170,180 |
| 7311 |
170 SPACE(I2+87)=SIGN |
| 7312 |
GOTO190 |
| 7313 |
180 SPACE(I2+106)=SIGN |
| 7314 |
190 FMAX(5)=0.0 |
| 7315 |
FMAX(6)=0.0 |
| 7316 |
GOTO140 |
| 7317 |
200 K=I2 |
| 7318 |
L=I2+6 |
| 7319 |
GOTO(50,50,50,210,50),I5 |
| 7320 |
210 MM=6 |
| 7321 |
GOTO40 |
| 7322 |
220 CE(8)=FMAX(7)*1.0D30*SPACE(L) |
| 7323 |
GOTO120 |
| 7324 |
230 SUB1=FMAX(1)*1.0D30 |
| 7325 |
SUB2=FMAX(2)*1.0D30 |
| 7326 |
DO240 I=2,N,2 |
| 7327 |
CE(I)=SUB1*SPACE(K) |
| 7328 |
CE(I+1)=SUB2*SPACE(K) |
| 7329 |
K=L |
| 7330 |
240 L=K+6 |
| 7331 |
CE(N+1)=SPACE(K)*1.0D30*FMAX(N) |
| 7332 |
GOTO120 |
| 7333 |
250 IF(I1-5)140,260,140 |
| 7334 |
260 SPACE(I2+68)=SIGN |
| 7335 |
FMAX(6)=0.0 |
| 7336 |
FMAX(7)=0.0 |
| 7337 |
GOTO140 |
| 7338 |
END |
| 7339 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 7340 |
*-- Author : |
| 7341 |
SUBROUTINE CASTPH(W) |
| 7342 |
REAL*8 W(11) |
| 7343 |
#include "cbert.inc" |
| 7344 |
*KEND. |
| 7345 |
SAVE |
| 7346 |
C |
| 7347 |
IF(PGVC(1)-440.0)10,40,40 |
| 7348 |
10 I=PGVC(1)+2.005 |
| 7349 |
J=I+10 |
| 7350 |
C PGVC(1)=NO.OF TIMES VELOCITY GREATER THAN CRITERION ENTERED |
| 7351 |
L=1 |
| 7352 |
DO20 K=I,J |
| 7353 |
PGVC(K)=W(L) |
| 7354 |
20 L=L+1 |
| 7355 |
PGVC(1)=PGVC(1)+11.0 |
| 7356 |
30 RETURN |
| 7357 |
40 I1=1 |
| 7358 |
GOTO30 |
| 7359 |
END |
| 7360 |
*CMZ : 1.01/04 10/06/93 14.43.38 by Christian Zeitnitz |
| 7361 |
*-- Author : |
| 7362 |
SUBROUTINE CASTPL(W) |
| 7363 |
REAL*8 W(12) |
| 7364 |
#include "cbert.inc" |
| 7365 |
*KEND. |
| 7366 |
SAVE |
| 7367 |
C |
| 7368 |
DO10 K=2,950,12 |
| 7369 |
IF(PLVC(K))10,40,10 |
| 7370 |
10 CONTINUE |
| 7371 |
20 I1=1 |
| 7372 |
30 RETURN |
| 7373 |
40 I=K |
| 7374 |
J=I+11 |
| 7375 |
C PLVC(1)=NO. OF TIMES ENTERED FOR STORAGE OF VELOCITY |
| 7376 |
C LESS THAN CRITERION |
| 7377 |
L=1 |
| 7378 |
DO50 K=I,J |
| 7379 |
PLVC(K)=W(L) |
| 7380 |
50 L=L+1 |
| 7381 |
PLVC(1)=PLVC(1)+1.0 |
| 7382 |
GOTO30 |
| 7383 |
END |
| 7384 |
*CMZ : 1.01/04 10/06/93 14.43.39 by Christian Zeitnitz |
| 7385 |
*-- Author : |
| 7386 |
SUBROUTINE CASTPR |
| 7387 |
#include "cbert.inc" |
| 7388 |
*KEND. |
| 7389 |
C |
| 7390 |
SAVE |
| 7391 |
I1=0 |
| 7392 |
MED=CLSM |
| 7393 |
DO90 I=3,39,12 |
| 7394 |
K=I |
| 7395 |
IF(PT(I))10,90,10 |
| 7396 |
10 IF(PT(K-1)-2.0)20,30,20 |
| 7397 |
20 PT(K-2)=PT(K)-SPACE(MED+9) |
| 7398 |
GOTO60 |
| 7399 |
30 PT(K-2)=PT(K)-SPACE(MED+3) |
| 7400 |
40 IF(PT(K-2)-500.0)50,50,80 |
| 7401 |
50 CALLCASTPL(PT(K-2)) |
| 7402 |
C VELOCITY LESS THAN CRITERION |
| 7403 |
IF(I1)100,90,100 |
| 7404 |
60 IF(PT(K-1)-1.0)70,40,70 |
| 7405 |
70 PT(K-2)=(DNCMS*PT(K-2))/PT(K+1) |
| 7406 |
GOTO40 |
| 7407 |
80 CALLCASTPH(PT(K-1)) |
| 7408 |
C VELOCITY GREATER THAN CRITERION |
| 7409 |
IF(I1)100,90,100 |
| 7410 |
90 CONTINUE |
| 7411 |
100 RETURN |
| 7412 |
END |
| 7413 |
*CMZ : 1.01/04 10/06/93 14.43.39 by Christian Zeitnitz |
| 7414 |
*-- Author : |
| 7415 |
SUBROUTINE UNDIS |
| 7416 |
#include "cbert.inc" |
| 7417 |
#include "crandm.inc" |
| 7418 |
#include "cmunpu.inc" |
| 7419 |
#include "crn.inc" |
| 7420 |
#include "cxyinc.inc" |
| 7421 |
*KEND. |
| 7422 |
REAL*8 RAN1,RAN2 |
| 7423 |
SAVE |
| 7424 |
C |
| 7425 |
IF(BEGRU) 110,130,100 |
| 7426 |
10 BEGRU=1.0 |
| 7427 |
DO 20 I = 1,4 |
| 7428 |
20 RANDS(I)=RANDI(I) |
| 7429 |
30 RAN1 = RANDC(ISEED) |
| 7430 |
RAN2 = RANDC(ISEED) |
| 7431 |
RAN1 = 2.D0*RAN1-1.D0 |
| 7432 |
RAN2 = 2.D0*RAN2-1.D0 |
| 7433 |
IF(RAN1**2 + RAN2**2 .GE. 1.D0) GO TO 30 |
| 7434 |
XI(1) = RAN1*OUT(4) |
| 7435 |
XI(2) = RAN2*OUT(4) |
| 7436 |
X = XI(1) |
| 7437 |
Y = XI(2) |
| 7438 |
CURR(4)=XI(1) |
| 7439 |
CURR(5) = XI(2) |
| 7440 |
XI(3)=-OUT(4) |
| 7441 |
DCOS(1)=0.0 |
| 7442 |
DCOS(2)=0.0 |
| 7443 |
DCOS(3)=1.0 |
| 7444 |
MED=4 |
| 7445 |
CURR(6)=XI(3) |
| 7446 |
CURR(7)=0.0 |
| 7447 |
CURR(8)=0.0 |
| 7448 |
CURR(9)=1.0 |
| 7449 |
CURR(10)=MED |
| 7450 |
C X, Y AND Z COORDINATES, ALSO ALPHA, BETA AND GAMMA |
| 7451 |
C DIRECTION COSINES. MED=4, (NO. OF GEOM) |
| 7452 |
40 RETURN |
| 7453 |
50 BEGRU = BEGRU + 1.0 D0 |
| 7454 |
60 BEGRU=BEGRU+1.0 |
| 7455 |
IF(CASESN -BEGRU)80,70,70 |
| 7456 |
70 FRAND = RANDC(ISEED) |
| 7457 |
GO TO 30 |
| 7458 |
80 BEGRU=0.0 |
| 7459 |
DO90 I=1,4 |
| 7460 |
RANDI(I)=RANDS(I) |
| 7461 |
90 ERAND(I)=RANDS(I) |
| 7462 |
GOTO40 |
| 7463 |
C FINAL RANDOM IN ERAND. RUN COMPLETED |
| 7464 |
100 IF(COUNT(6).EQ.0.0) GO TO 130 |
| 7465 |
110 COUNT(6) = 0.0 |
| 7466 |
120 IF(BEGRU) 50,10,60 |
| 7467 |
130 DO 140 I=1,12 |
| 7468 |
PCC(I) = CC(I) |
| 7469 |
140 NIP(I) = IPEC(I) |
| 7470 |
DO 150 I=1,5 |
| 7471 |
150 PPNB(I) = PNBC(I) |
| 7472 |
GO TO 120 |
| 7473 |
C*** WHEN BEGRU = 0, MUNPU COMMON IS ZEROED |
| 7474 |
END |
| 7475 |
*CMZ : 1.01/04 10/06/93 14.43.39 by Christian Zeitnitz |
| 7476 |
*-- Author : |
| 7477 |
SUBROUTINE CALXYI(II,JJ,KK) |
| 7478 |
C |
| 7479 |
#include "cbert.inc" |
| 7480 |
*KEND. |
| 7481 |
C |
| 7482 |
REAL * 8 W1,W2,W3,W4,W5,W6 |
| 7483 |
SAVE |
| 7484 |
C |
| 7485 |
W1=S(II)*1.0D30 |
| 7486 |
W2=S(II+1)*1.0D30 |
| 7487 |
IF(IABS(IV)-1)10,20,10 |
| 7488 |
10 W3=SPACE(JJ)*1.0D30 |
| 7489 |
W4=SPACE(JJ+1)*1.0D30 |
| 7490 |
W5=SPACE(JJ+2)*1.0D30 |
| 7491 |
W6=SPACE(JJ+3)*1.0D30 |
| 7492 |
LL=II+2 |
| 7493 |
IF(IV)40,60,40 |
| 7494 |
20 W3=S(II+2)*1.0D30 |
| 7495 |
W4=S(II+3)*1.0D30 |
| 7496 |
W5=SPACE(JJ)*1.0D30 |
| 7497 |
W6=SPACE(JJ+1)*1.0D30 |
| 7498 |
LL=II+4 |
| 7499 |
IF(IV)50,30,30 |
| 7500 |
30 NM=7 |
| 7501 |
I7=1 |
| 7502 |
40 MM=7 |
| 7503 |
NN=1 |
| 7504 |
GO TO 70 |
| 7505 |
50 NM=1 |
| 7506 |
I7=7 |
| 7507 |
60 MM=1 |
| 7508 |
NN=7 |
| 7509 |
70 DO100 I=1,3 |
| 7510 |
S(LL)=W1*SPACE(MM) |
| 7511 |
S(LL+1)=W2*SPACE(NN) |
| 7512 |
IF(IABS(IV)-1)90,80,90 |
| 7513 |
80 S(LL+2)=W3*SPACE(NM) |
| 7514 |
S(LL+3)=W4*SPACE(I7) |
| 7515 |
LL=LL+2 |
| 7516 |
NM=NM+1 |
| 7517 |
I7=I7+1 |
| 7518 |
90 MM=MM+1 |
| 7519 |
NN=NN+1 |
| 7520 |
100 LL=LL+2 |
| 7521 |
IF(IV)110,120,130 |
| 7522 |
110 NM=7 |
| 7523 |
I7=1 |
| 7524 |
GOTO170 |
| 7525 |
120 MM=1 |
| 7526 |
NN=7 |
| 7527 |
NM=7 |
| 7528 |
I7=7 |
| 7529 |
GOTO 150 |
| 7530 |
130 IF(IV-1)160,160,140 |
| 7531 |
140 MM=7 |
| 7532 |
NN=1 |
| 7533 |
NM=1 |
| 7534 |
I7=7 |
| 7535 |
150 LL=JJ+4 |
| 7536 |
GOTO180 |
| 7537 |
160 NM=1 |
| 7538 |
I7=7 |
| 7539 |
170 LL=JJ |
| 7540 |
180 DO210 I=1,3 |
| 7541 |
SPACE(LL+2)=W5*SPACE(NM) |
| 7542 |
SPACE(LL+3)=W6*SPACE(I7) |
| 7543 |
IF(IABS(IV)-1)190,200,190 |
| 7544 |
190 SPACE(LL)=W3*SPACE(MM) |
| 7545 |
SPACE(LL+1)=W4*SPACE(NN) |
| 7546 |
LL=LL+2 |
| 7547 |
MM=MM+1 |
| 7548 |
NN=NN+1 |
| 7549 |
200 NM=NM+1 |
| 7550 |
I7=I7+1 |
| 7551 |
210 LL=LL+2 |
| 7552 |
LL=KK+2 |
| 7553 |
IF(IABS(IV)-1)220,250,220 |
| 7554 |
220 MM=JJ+4 |
| 7555 |
NN=II+2 |
| 7556 |
DO230 I=KK,LL |
| 7557 |
SPACE(I)=SPACE(MM)+SPACE(MM+1)+SPACE(MM+2)+SPACE(MM+3) +S(NN)+ |
| 7558 |
+ S(NN+1) |
| 7559 |
MM=MM+4 |
| 7560 |
230 NN=NN+2 |
| 7561 |
240 RETURN |
| 7562 |
250 MM=II+4 |
| 7563 |
NN=JJ+2 |
| 7564 |
DO260 I=KK,LL |
| 7565 |
SPACE(I)=SPACE(NN)+SPACE(NN+1)+S(MM)+S(MM+1)+S(MM+2)+S(MM+3) |
| 7566 |
MM=MM+4 |
| 7567 |
260 NN=NN+2 |
| 7568 |
GOTO240 |
| 7569 |
END |
| 7570 |
*CMZ : 0.92/00 02/12/92 16.02.27 by Christian Zeitnitz |
| 7571 |
*-- Author : |
| 7572 |
SUBROUTINE CZERO |
| 7573 |
#include "cbert.inc" |
| 7574 |
*KEND. |
| 7575 |
C |
| 7576 |
DO 10 I = 1,21 |
| 7577 |
10 CE(I) = 0.0 |
| 7578 |
RETURN |
| 7579 |
END |
| 7580 |
*CMZ : 0.92/00 02/12/92 16.02.30 by Christian Zeitnitz |
| 7581 |
*-- Author : |
| 7582 |
FUNCTION CDOST(I,Z) |
| 7583 |
C |
| 7584 |
#include "cevcm.inc" |
| 7585 |
*KEND. |
| 7586 |
C |
| 7587 |
IF(Z-70.0) 30,10,10 |
| 7588 |
10 CDOST = T(I,7) |
| 7589 |
20 RETURN |
| 7590 |
30 IF(Z-10.0) 40,40,50 |
| 7591 |
40 CDOST = T(I,1) |
| 7592 |
GO TO 20 |
| 7593 |
50 N = 0.1 * Z + 1.0 |
| 7594 |
X = 10 * N |
| 7595 |
X = (X-Z) * 0.1 |
| 7596 |
CDOST = X * T(I,N-1) + (1.0-X) * T(I,N) |
| 7597 |
GO TO 20 |
| 7598 |
END |
| 7599 |
*CMZ : 1.05/01 21/02/2000 16.44.49 by Christian Zeitnitz |
| 7600 |
*-- Author : |
| 7601 |
SUBROUTINE CDRES(M2,M3,T1,NPART,EPART,SOCHPE,U,EREC,HEPART) |
| 7602 |
C*****A LA EVAP III(TWA,8-68) |
| 7603 |
C*****COMPATIBLE WITH O5R DRES EXCEPT FOR COMMON/COMON/ |
| 7604 |
C |
| 7605 |
#include "cjoint.inc" |
| 7606 |
#include "crandm.inc" |
| 7607 |
#include "cforcn.inc" |
| 7608 |
#include "cdresc.inc" |
| 7609 |
#include "cevcm.inc" |
| 7610 |
#include "camass.inc" |
| 7611 |
*KEND. |
| 7612 |
LOGICAL INIT |
| 7613 |
C |
| 7614 |
C |
| 7615 |
DIMENSION ZMASS(6),Q(6) , |
| 7616 |
+ FLKCOU(6) ,CCOUL(6) ,THRESH(6) , NPART(6), |
| 7617 |
+ EPART(200,2) ,HEPART(200,4) ,SMALLA(6) , |
| 7618 |
+ R(6) ,S(6) ,SOS(6) ,STRUN(6) ,EYE1(6) ,EYE0(6) , |
| 7619 |
+ SMOM1(6) ,IAI(5) ,IZI(5) ,XX(5) |
| 7620 |
C |
| 7621 |
SAVE |
| 7622 |
DATA INIT/.TRUE./ |
| 7623 |
C |
| 7624 |
CZ DELTAS (A)=(A-1.0)/(1.0+(124.0/A**0.6666667)) |
| 7625 |
IF(.NOT.INIT) GO TO 20 |
| 7626 |
INIT = .FALSE. |
| 7627 |
FKEY=0. |
| 7628 |
C evaporation data read in by CRBERT called by CALINI CZ 19.JUNE 92 |
| 7629 |
DO10 K=1,7 |
| 7630 |
10 T(4,K)=0.0 |
| 7631 |
Y0=1.5 |
| 7632 |
B0=8.0 |
| 7633 |
NBE8 = 0 |
| 7634 |
NRNEEP = 0 |
| 7635 |
ZMASS(1) = XMASS(1)*1.E3 |
| 7636 |
ZMASS(2) = XMASS(0)*1.E3 |
| 7637 |
ZMASS(3) = XMASS(7)*1.E3 |
| 7638 |
ZMASS(4) = XMASS(8)*1.E3 |
| 7639 |
ZMASS(5) = XMASS(9)*1.E3 |
| 7640 |
ZMASS(6) = XMASS(10)*1.E3 |
| 7641 |
EMH = ZMASS(2) |
| 7642 |
EMN = ZMASS(1) |
| 7643 |
C QUESTION:WHAT IS UM? |
| 7644 |
C END OF CHANGE |
| 7645 |
UM = 931.20793 |
| 7646 |
EMHN=EMH-EMN |
| 7647 |
EMNUM=EMN-UM |
| 7648 |
20 CONTINUE |
| 7649 |
DO30 I=1,6 |
| 7650 |
NPART(I)=0 |
| 7651 |
30 SMOM1(I)=0.0 |
| 7652 |
DO40 K=1,6 |
| 7653 |
FLA(K)=IA(K) |
| 7654 |
40 FLZ(K)=IZ(K) |
| 7655 |
50 JA=M2 |
| 7656 |
JZ=M3 |
| 7657 |
U=T1 |
| 7658 |
IF(JA-JZ)60 ,60 ,70 |
| 7659 |
60 CONTINUE |
| 7660 |
RETURN |
| 7661 |
70 A=JA |
| 7662 |
Z=JZ |
| 7663 |
BE=Z*EMHN+A*EMNUM-CENERG(A,Z) |
| 7664 |
RNMASS=Z*EMH+(A-Z)*EMN-BE |
| 7665 |
IF(EREC)80 ,80 ,90 |
| 7666 |
80 VRNSQ=0. |
| 7667 |
VCM=0. |
| 7668 |
GO TO 100 |
| 7669 |
90 VRNSQ=2.0*EREC/RNMASS |
| 7670 |
VCM=SQRT(VRNSQ) |
| 7671 |
100 IF(JA-8)120 ,110 ,120 |
| 7672 |
110 IF(JZ-4)120 ,710 ,120 |
| 7673 |
120 CONTINUE |
| 7674 |
DO150 K=1,6 |
| 7675 |
IF((A-FLA(K)).LE.(Z-FLZ(K)))GO TO 150 |
| 7676 |
IF(A-2.0*FLA(K))150,130,130 |
| 7677 |
130 IF(Z-2.0*FLZ(K))150,140,140 |
| 7678 |
140 Q(K) = CQNRG(A-FLA(K),Z-FLZ(K),A,Z) + EXMASS(K) |
| 7679 |
C 728 Q(K)=CENERG(A-FLA(K),Z-FLZ(K))-CENERG(A,Z)+EXMASS(K) |
| 7680 |
150 CONTINUE |
| 7681 |
FLKCOU(1)=0.0 |
| 7682 |
FLKCOU(2)=CDOST(1,Z-FLZ(2)) |
| 7683 |
FLKCOU(3)=FLKCOU(2)+.06 |
| 7684 |
FLKCOU(4)=FLKCOU(2)+.12 |
| 7685 |
FLKCOU(6)=CDOST(2,Z-FLZ(6)) |
| 7686 |
FLKCOU(5)=FLKCOU(6)-.06 |
| 7687 |
CCOUL(1)=1.0 |
| 7688 |
CCOU2=CDOST(3,Z-FLZ(2)) |
| 7689 |
CCOUL(2)=CCOU2+1.0 |
| 7690 |
CCOUL(3)=CCOU2*1.5+3.0 |
| 7691 |
CCOUL(4)=CCOU2+3.0 |
| 7692 |
CCOUL(6)=CDOST(4,Z-FLZ(6))*2.0+2.0 |
| 7693 |
CCOUL(5)=2.0*CCOUL(6)-1.0 |
| 7694 |
SIGMA=0.0 |
| 7695 |
DO 200 J=1,6 |
| 7696 |
IF(A-2.0*FLA(J))180,160,160 |
| 7697 |
160 IF(Z-2.0*FLZ(J))180,170,170 |
| 7698 |
170 MM=JA-IA(J) |
| 7699 |
ZZ=Z-FLZ(J) |
| 7700 |
AA=A-FLA(J) |
| 7701 |
IF(AA.LE.ZZ)GO TO 180 |
| 7702 |
SMALLA(J)=AA*(1.0+Y0*(AA-2.0*ZZ)**2/AA**2)/B0 |
| 7703 |
THRESH(J)=Q(J)+.88235*FLKCOU(J)*FLZ(J)* ZZ/(RMASS(MM)+RHO(J)) |
| 7704 |
NN=AA-ZZ |
| 7705 |
IZZ=ZZ |
| 7706 |
CORR=CAM4(IZZ)+CAM5(NN) |
| 7707 |
IF(FKEY.EQ.1.) CORR=0. |
| 7708 |
ARG=U-THRESH(J)-CORR |
| 7709 |
IF(ARG)180,190,190 |
| 7710 |
180 R(J)=0.0 |
| 7711 |
S(J)=0.0 |
| 7712 |
SOS(J)=0. |
| 7713 |
GOTO200 |
| 7714 |
190 S(J)=SQRT (SMALLA(J)*ARG)*2.0 |
| 7715 |
SOS(J)=10.0*S(J) |
| 7716 |
200 CONTINUE |
| 7717 |
N1=1 |
| 7718 |
DO210 J=1,6 |
| 7719 |
IF(SOS(J)-1250.0)210 ,220 ,220 |
| 7720 |
210 CONTINUE |
| 7721 |
N1=2 |
| 7722 |
GO TO 230 |
| 7723 |
220 SES=AMAX1(S(1),S(2),S(3),S(4),S(5),S(6)) |
| 7724 |
230 DO390 J=1,6 |
| 7725 |
IF(S(J))240 ,390 ,240 |
| 7726 |
240 JS=SOS(J)+1.0 |
| 7727 |
MM=JA-IA(J) |
| 7728 |
IF(N1-1)250 ,260 ,250 |
| 7729 |
250 IF(JS-1000)290 ,270 ,270 |
| 7730 |
260 SAS=EXP (S(J)-SES) |
| 7731 |
GO TO 280 |
| 7732 |
270 SAS=EXP (S(J)-50.0) |
| 7733 |
280 EYE1(J)=(S(J)**2-3.0*S(J)+3.0)*SAS/(4.0*SMALLA(J)**2) |
| 7734 |
FJS=JS |
| 7735 |
STRUN(J)=FJS-1.0 |
| 7736 |
GO TO 300 |
| 7737 |
290 FJS=JS |
| 7738 |
STRUN(J)=FJS-1.0 |
| 7739 |
EYE1(J)=(P1(JS)+(P1(JS+1)-P1(JS))*(SOS(J)-STRUN(J)))/ SMALLA(J |
| 7740 |
+ )**2 |
| 7741 |
300 IF(J-1)320,320,310 |
| 7742 |
310 R(J)=CCOUL(J)*RMASS(MM)**2*EYE1(J) |
| 7743 |
GOTO380 |
| 7744 |
320 IF(N1-1)330 ,340 ,330 |
| 7745 |
330 IF(JS-1000)350 ,340 ,340 |
| 7746 |
340 EYE0(J)=(S(J)-1.0)*0.5*SAS/SMALLA(J) |
| 7747 |
GO TO 360 |
| 7748 |
350 EYE0(J)=(P0(JS)+(P0(JS+1)-P0(JS))*(SOS(J)-STRUN(J))) / |
| 7749 |
+ SMALLA(J) |
| 7750 |
360 R(J)=RMASS(MM)**2*ALPH(MM)*(EYE1(J)+BET(MM)* EYE0(J)) |
| 7751 |
IF(R(J))370 ,380,380 |
| 7752 |
370 R(J)=0.0 |
| 7753 |
380 SIGMA=SIGMA+R(J) |
| 7754 |
390 CONTINUE |
| 7755 |
NCOUNT = 0 |
| 7756 |
400 IF(SIGMA)410,410,500 |
| 7757 |
410 CONTINUE |
| 7758 |
DO 430 J = 1,6 |
| 7759 |
IF(JA-IA(J))430 ,420 ,430 |
| 7760 |
420 IF(JZ-IZ(J))430 ,440 ,430 |
| 7761 |
430 CONTINUE |
| 7762 |
GO TO 480 |
| 7763 |
440 JEMISS = J |
| 7764 |
C*****STORE,RESIDUAL NUC IS OF EMITTED PARTICLE TYPE |
| 7765 |
EPS = U + EREC |
| 7766 |
NPART(JEMISS) = NPART(JEMISS)+1 |
| 7767 |
NRNEEP = NRNEEP + 1 |
| 7768 |
450 SMOM1(JEMISS) = SMOM1(JEMISS) + EPS |
| 7769 |
IF(JEMISS-2)460 ,460 ,470 |
| 7770 |
460 EPART(NPART(JEMISS),JEMISS)=EPS |
| 7771 |
GO TO 780 |
| 7772 |
470 KEMISS=JEMISS-2 |
| 7773 |
HEPART(NPART(JEMISS),KEMISS)=EPS |
| 7774 |
GO TO 780 |
| 7775 |
480 IF(JA-8)790,490,790 |
| 7776 |
490 IF(JZ-4)790,710,790 |
| 7777 |
500 URAN = RANDC(ISEED) * SIGMA |
| 7778 |
SUM=0.0 |
| 7779 |
DO510 J=1,6 |
| 7780 |
K=J |
| 7781 |
SUM=R(J)+SUM |
| 7782 |
IF(SUM -URAN)510,510,520 |
| 7783 |
510 CONTINUE |
| 7784 |
520 JEMISS=K |
| 7785 |
JS=SOS(JEMISS)+1.0 |
| 7786 |
IF(JS-1000)540 ,530 ,530 |
| 7787 |
530 RATIO2=(S(JEMISS)**3-6.0*S(JEMISS)**2+15.0* |
| 7788 |
+S(JEMISS)-15.0)/((2.0*S(JEMISS)**2-6.0*S(JEMISS)+6.0)*SMALLA |
| 7789 |
+(JEMISS)) |
| 7790 |
GO TO 550 |
| 7791 |
540 RATIO2=(P22(JS)+(P22(JS+1)-P22(JS))* |
| 7792 |
+(SOS(JEMISS)-STRUN(JEMISS)))/SMALLA(JEMISS) |
| 7793 |
550 EPSAV=RATIO2*2.0 |
| 7794 |
IF(JEMISS-1)560,560,580 |
| 7795 |
560 MM=JA-IA(J) |
| 7796 |
570 EPSAV=(EPSAV+BET(MM))/(1.0+BET(MM)*EYE0(JEMISS) |
| 7797 |
+/EYE1(JEMISS)) |
| 7798 |
580 E1=EXPRNF(V)/2.0 |
| 7799 |
E2=EXPRNF(V)/2.0 |
| 7800 |
EPS=(E1+E2)*EPSAV+THRESH(JEMISS)-Q(JEMISS) |
| 7801 |
COSCM = RANDC(ISEED) |
| 7802 |
PLORMI = RANDC(ISEED) |
| 7803 |
IF(PLORMI-0.5)590,590,600 |
| 7804 |
590 COSCM=-COSCM |
| 7805 |
600 AR=A-FLOAT (IA(JEMISS)) |
| 7806 |
ZR=Z-FLOAT (IZ(JEMISS)) |
| 7807 |
BE=ZR*EMHN+AR*EMNUM-CENERG(AR,ZR) |
| 7808 |
RNMASS=ZR*EMH+(AR-ZR)*EMN-BE |
| 7809 |
VCMEPS = 2.0*EPS/(ZMASS(JEMISS)*(1.+ZMASS(JEMISS)/RNMASS)) |
| 7810 |
VCMEVP=SQRT(VCMEPS) |
| 7811 |
VRNSQ=VCMEPS*ZMASS(JEMISS)*ZMASS(JEMISS)/(RNMASS*RNMASS) |
| 7812 |
++VCM*VCM+2.0*ZMASS(JEMISS)/RNMASS*VCMEVP*VCM*COSCM |
| 7813 |
VLBEPS=VCMEPS+VCM*VCM-2.*VCMEVP*VCM*COSCM |
| 7814 |
EPS=0.5*ZMASS(JEMISS)*VLBEPS |
| 7815 |
610 UNEW=U-0.5*VCMEPS*(ZMASS(JEMISS)*ZMASS(JEMISS)/RNMASS+ZMASS(JEMISS |
| 7816 |
+))-Q(JEMISS) |
| 7817 |
IF(UNEW)630 ,620 ,620 |
| 7818 |
620 U = UNEW |
| 7819 |
VCM=SQRT(VRNSQ) |
| 7820 |
EREC=0.5*RNMASS*VRNSQ |
| 7821 |
NPART(JEMISS)=NPART(JEMISS)+1 |
| 7822 |
GO TO 650 |
| 7823 |
630 NCOUNT = NCOUNT + 1 |
| 7824 |
IF(NCOUNT-10) 580,580,640 |
| 7825 |
640 SIGMA = SIGMA - R(JEMISS) |
| 7826 |
R(JEMISS) = 0.0 |
| 7827 |
NCOUNT = 0 |
| 7828 |
GO TO 400 |
| 7829 |
650 JAT=JA-IA(JEMISS) |
| 7830 |
JZT=JZ-IZ(JEMISS) |
| 7831 |
IF(JAT-JZT)410,410,660 |
| 7832 |
660 JA=JAT |
| 7833 |
JZ=JZT |
| 7834 |
C*****STORE,END OF NORMAL CYCLE |
| 7835 |
SMOM1(JEMISS)=SMOM1(JEMISS)+EPS |
| 7836 |
IF(NPART(JEMISS).LE.0)CALL CERROR('CDRES1$') |
| 7837 |
IF(JEMISS-2)670 ,670 ,680 |
| 7838 |
670 EPART(NPART(JEMISS),JEMISS)=EPS |
| 7839 |
GO TO 690 |
| 7840 |
680 KEMISS=JEMISS-2 |
| 7841 |
HEPART(NPART(JEMISS),KEMISS)=EPS |
| 7842 |
690 IF(JA-8)70,700 ,70 |
| 7843 |
700 IF(JZ-4)70,710 ,70 |
| 7844 |
710 IF(U)720 ,720 ,730 |
| 7845 |
720 EPS=0. |
| 7846 |
GO TO 740 |
| 7847 |
730 EPS=0.5*(U+.093) |
| 7848 |
740 NBE8=NBE8+1 |
| 7849 |
COSCM = RANDC(ISEED) |
| 7850 |
VCMEPS=2.0*EPS/ZMASS(6) |
| 7851 |
VCMEVP=SQRT(VCMEPS) |
| 7852 |
VLBEPS=VCMEPS+VRNSQ+2.0*VCMEVP*VCM*COSCM |
| 7853 |
NOP=0 |
| 7854 |
750 EPS=0.5*ZMASS(6)*VLBEPS |
| 7855 |
C*****STORE,BE 8 BREAKUP |
| 7856 |
SMOM1(6)=SMOM1(6)+EPS |
| 7857 |
NPART(6)=NPART(6)+1 |
| 7858 |
HEPART(NPART(6),4)=EPS |
| 7859 |
IF(NOP)760,760,770 |
| 7860 |
760 VLBEPS=VCMEPS+VRNSQ-2.0*VCMEVP*VCM*COSCM |
| 7861 |
NOP=1 |
| 7862 |
GO TO 750 |
| 7863 |
770 CONTINUE |
| 7864 |
780 EREC=0. |
| 7865 |
U = 0.0 |
| 7866 |
790 SOCHPE=SMOM1(3)+SMOM1(5)+SMOM1(6)+SMOM1(4) |
| 7867 |
800 CONTINUE |
| 7868 |
RETURN |
| 7869 |
END |
| 7870 |
*CMZ : 1.01/04 10/06/93 14.43.43 by Christian Zeitnitz |
| 7871 |
*-- Author : |
| 7872 |
FUNCTION CENERG(A,Z) |
| 7873 |
C |
| 7874 |
#include "cevcm.inc" |
| 7875 |
*KEND. |
| 7876 |
C |
| 7877 |
DELTAS (A)=(A-1.0)/(1.0+(124.0/A**0.6666667)) |
| 7878 |
CAM (A,Z)=8.367*A-0.783*Z |
| 7879 |
+ -17.0354*A*(1.0-1.84619*(A-2.0*Z)**2/A**2) |
| 7880 |
+ +25.8357*A**0.6666667*(1.0-1.71219*(A-2.0*Z)**2/A**2) |
| 7881 |
+ *(1.0-0.62025/A**0.6666667)**2 |
| 7882 |
+ +0.779*Z*(Z-1.0)*(1.0-1.5849/A**0.6666667+1.2273/A |
| 7883 |
+ +1.5772/A**1.3333333)/A**0.3333333 |
| 7884 |
+ -0.4323*Z**1.3333333*(1.0-0.57811/A**0.3333333 |
| 7885 |
+ -0.14518/A**0.6666667+0.49597/A)/A**0.3333333 |
| 7886 |
I=A |
| 7887 |
KZ=Z |
| 7888 |
N=A-Z |
| 7889 |
IF(I.EQ.0) THEN |
| 7890 |
CENERG=0.0 |
| 7891 |
RETURN |
| 7892 |
ENDIF |
| 7893 |
IF(N.LT.0)CALL CERROR('CENERG A<Z $') |
| 7894 |
JPRIME=DELTAS (A) |
| 7895 |
J=I-2*KZ-JPRIME+10 |
| 7896 |
IF(J-20)10,10,40 |
| 7897 |
10 IF(J)40,40,20 |
| 7898 |
20 IF(WAPS(I,J))30,40,30 |
| 7899 |
30 CENERG=WAPS(I,J) |
| 7900 |
RETURN |
| 7901 |
40 CENERG=CAM (A,Z)+CAM2(KZ)+CAM3(N) |
| 7902 |
RETURN |
| 7903 |
END |
| 7904 |
*CMZ : 1.01/09 29/06/93 19.03.31 by Christian Zeitnitz |
| 7905 |
*-- Author : |
| 7906 |
SUBROUTINE CERUP |
| 7907 |
C*****MODIFIED TO OBTAIN APR,ZPR AFTER CAS + EVAP (8-68,T.W.A.) |
| 7908 |
#include "chevap.inc" |
| 7909 |
#include "ccomon.inc" |
| 7910 |
#include "ccomn3.inc" |
| 7911 |
#include "ccomn2.inc" |
| 7912 |
#include "cforcn.inc" |
| 7913 |
#include "cinout.inc" |
| 7914 |
#include "caz.inc" |
| 7915 |
*KEND. |
| 7916 |
DIMENSION FPART(6) |
| 7917 |
SAVE |
| 7918 |
C |
| 7919 |
IF(EX) 10 ,20 ,50 |
| 7920 |
10 NEGEX =NEGEX +1 |
| 7921 |
20 DO 30 I=1,6 |
| 7922 |
30 NPART(I)=0 |
| 7923 |
HEVSUM = 0.0 |
| 7924 |
UU = 0.0 |
| 7925 |
RETURN |
| 7926 |
40 LOWAZ=LOWAZ+1 |
| 7927 |
GO TO 20 |
| 7928 |
50 IF(APR.LE.4.)GO TO 40 |
| 7929 |
IF(ZPR.LE.2.)GO TO 40 |
| 7930 |
IF(APR.LE.ZPR)GO TO 40 |
| 7931 |
M2= APR |
| 7932 |
M3= ZPR |
| 7933 |
CALL CDRES(M2,M3,EX,NPART,EPART,HEVSUM,UU,EREC,HEPART) |
| 7934 |
DO 60 I=1,6 |
| 7935 |
60 IF(NPART(I).GT.0) GOTO 70 |
| 7936 |
FKEY =1. |
| 7937 |
CALL CDRES(M2,M3,EX,NPART,EPART,HEVSUM,UU,EREC,HEPART) |
| 7938 |
FKEY=0. |
| 7939 |
70 CONTINUE |
| 7940 |
80 DO 90 I=1,6 |
| 7941 |
IF(NPART(I).GT.200) THEN |
| 7942 |
CALL CERROR(' CERUP : N_EVAP > 200 $') |
| 7943 |
WRITE(IO,10000) I,NPART(I) |
| 7944 |
10000 FORMAT(' CERUP: I=',I5,' NPART=',I5) |
| 7945 |
NPART(I)=200 |
| 7946 |
ENDIF |
| 7947 |
FPART(I)=NPART(I) |
| 7948 |
90 CONTINUE |
| 7949 |
ZPR=ZPR-FPART(2)-FPART(3)-2.*(FPART(5)+FPART(6)) -FPART(4) |
| 7950 |
APR=APR-FPART(1)-FPART(2)-2.*FPART(3)-3.*(FPART(4)+FPART(5)) |
| 7951 |
+ -4.*FPART(6) |
| 7952 |
C CHANGED JAN.1,1986 |
| 7953 |
NPART1=NPART(1) |
| 7954 |
NPART2=NPART(2) |
| 7955 |
IF(NPART1.LE.0)GO TO 110 |
| 7956 |
DO 100 I=1,NPART1 |
| 7957 |
KINDI(I)=2 |
| 7958 |
IBBARR(I)=1 |
| 7959 |
100 CONTINUE |
| 7960 |
110 IF(NPART2.LE.0) RETURN |
| 7961 |
DO 120 I=1,NPART2 |
| 7962 |
KINDI(I)=1 |
| 7963 |
IBBARR(I)=1 |
| 7964 |
120 CONTINUE |
| 7965 |
C END OF CHANGE |
| 7966 |
RETURN |
| 7967 |
END |
| 7968 |
*CMZ : 0.92/00 02/12/92 16.02.30 by Christian Zeitnitz |
| 7969 |
*-- Author : |
| 7970 |
SUBROUTINE GTISO(U,V,W) |
| 7971 |
C |
| 7972 |
#include "crandm.inc" |
| 7973 |
*KEND. |
| 7974 |
C |
| 7975 |
10 Z = RANDC(ISEED) |
| 7976 |
X = 0.687368 * SFLRAF(X) |
| 7977 |
Y = 0.687368 * SFLRAF(X) |
| 7978 |
XSQ = X * X |
| 7979 |
YSQ = Y * Y |
| 7980 |
ZSQ = Z * Z |
| 7981 |
D = XSQ + YSQ + ZSQ |
| 7982 |
IF(D*D-Z) 20 ,20 ,10 |
| 7983 |
20 U = 2.0*X*Z/D |
| 7984 |
V = 2.0*Y*Z/D |
| 7985 |
W = (ZSQ-XSQ-YSQ)/D |
| 7986 |
RETURN |
| 7987 |
END |
| 7988 |
*CMZ : 1.01/09 29/06/93 16.14.56 by Christian Zeitnitz |
| 7989 |
*-- Author : |
| 7990 |
SUBROUTINE RECOIL |
| 7991 |
C |
| 7992 |
#include "cinout.inc" |
| 7993 |
#include "ccomon.inc" |
| 7994 |
#include "camass.inc" |
| 7995 |
*KEND. |
| 7996 |
SAVE |
| 7997 |
C |
| 7998 |
IF(APR.LE.4.) THEN |
| 7999 |
EREC = 0.0 |
| 8000 |
ELSE |
| 8001 |
PX=0. |
| 8002 |
PY=0. |
| 8003 |
PZ=0. |
| 8004 |
IF(NOPART.NE.0) THEN |
| 8005 |
DO 10 I=1,NOPART |
| 8006 |
TM = XMASS(KIND(I))*1000. |
| 8007 |
PI = EP(I)*SQRT (1.+2.*TM/EP(I)) |
| 8008 |
PX = PI*ALPHA(I) +PX |
| 8009 |
PY = PI*BETA(I) +PY |
| 8010 |
PZ = PI*GAM(I) +PZ |
| 8011 |
10 CONTINUE |
| 8012 |
ENDIF |
| 8013 |
KT= TIP(NO) |
| 8014 |
TM = XMASS(KT)*1000. |
| 8015 |
PZ = EC(NO)*SQRT (1.+2.*TM/EC(NO)) - PZ |
| 8016 |
AA = APR * 931.49432 |
| 8017 |
EREC = SQRT (AA**2 +PX**2 +PY**2 +PZ**2)-AA |
| 8018 |
ENDIF |
| 8019 |
RETURN |
| 8020 |
END |
| 8021 |
*CMZ : 0.92/00 02/12/92 16.02.30 by Christian Zeitnitz |
| 8022 |
*-- Author : |
| 8023 |
FUNCTION CQNRG(A1,Z1,A2,Z2) |
| 8024 |
C |
| 8025 |
#include "cevcm.inc" |
| 8026 |
*KEND. |
| 8027 |
C |
| 8028 |
DELTAS (A)=(A-1.0)/(1.0+(124.0/A**0.6666667)) |
| 8029 |
CAM (A,Z)=8.367*A-0.783*Z |
| 8030 |
1-17.0354*A*(1.0-1.84619*(A-2.0*Z)**2/A**2) |
| 8031 |
2+25.8357*A**0.6666667*(1.0-1.71219*(A-2.0*Z)**2/A**2) |
| 8032 |
3*(1.0-0.62025/A**0.6666667)**2 |
| 8033 |
4+0.779*Z*(Z-1.0)*(1.0-1.5849/A**0.6666667+1.2273/A |
| 8034 |
5+1.5772/A**1.3333333)/A**0.3333333 |
| 8035 |
6-0.4323*Z**1.3333333*(1.0-0.57811/A**0.3333333 |
| 8036 |
7-0.14518/A**0.6666667+0.49597/A)/A**0.3333333 |
| 8037 |
I1 = A1 |
| 8038 |
I2 = A2 |
| 8039 |
KZ1 = Z1 |
| 8040 |
KZ2 = Z2 |
| 8041 |
N1 = A1 - Z1 |
| 8042 |
N2 = A2 - Z2 |
| 8043 |
IF(N1.LE.0) CALL CERROR('CQNRG1$') |
| 8044 |
IF(N2.LE.0) CALL CERROR('CQNRG2$') |
| 8045 |
JP1 = DELTAS(A1) |
| 8046 |
JP2 = DELTAS(A2) |
| 8047 |
J1 = I1 - 2*KZ1 - JP1 + 10 |
| 8048 |
J2 = I2 - 2*KZ2 - JP2 + 10 |
| 8049 |
IF(J1.LT.1.OR.J1.GT.20) GO TO 10 |
| 8050 |
IF(J2.LT.1.OR.J2.GT.20) GO TO 10 |
| 8051 |
ENRG1 = WAPS(I1,J1) |
| 8052 |
ENRG2 = WAPS(I2,J2) |
| 8053 |
IF(ENRG1.EQ.0.) GO TO 10 |
| 8054 |
IF(ENRG2.EQ.0.) GO TO 10 |
| 8055 |
GO TO 20 |
| 8056 |
10 ENRG1 = CAM(A1,Z1) + CAM2(KZ1) + CAM3(N1) |
| 8057 |
ENRG2 = CAM(A2,Z2) + CAM2(KZ2) + CAM3(N2) |
| 8058 |
20 CQNRG = ENRG1 - ENRG2 |
| 8059 |
RETURN |
| 8060 |
END |
| 8061 |
*CMZ : 1.04/10 07/10/97 09.28.00 by Christian Zeitnitz |
| 8062 |
*-- Author : Christian Zeitnitz 06/06/92 |
| 8063 |
SUBROUTINE CALSIG |
| 8064 |
C************************************************************ |
| 8065 |
C CALOR-Cross-Section |
| 8066 |
C |
| 8067 |
C INPUT : material constants and particle type |
| 8068 |
C OUTPUT : distance to next hadronic interaction |
| 8069 |
C |
| 8070 |
C Author : Christian Zeitnitz (U of Arizona) |
| 8071 |
C Date : 6-6-92 |
| 8072 |
C************************************************************ |
| 8073 |
C |
| 8074 |
C GEANT Commons |
| 8075 |
#include "gckine.inc" |
| 8076 |
#include "gctrak.inc" |
| 8077 |
#include "gcmate.inc" |
| 8078 |
#include "gcjloc.inc" |
| 8079 |
#include "gcbank.inc" |
| 8080 |
#include "gconsp.inc" |
| 8081 |
#include "gcphys.inc" |
| 8082 |
*KEND. |
| 8083 |
C |
| 8084 |
C CALOR common |
| 8085 |
#include "calgea.inc" |
| 8086 |
*KEND. |
| 8087 |
C |
| 8088 |
C Avogadro number multiplied by 1.E-24 |
| 8089 |
PARAMETER(XNAVO = 0.60221367) |
| 8090 |
CC |
| 8091 |
LOGICAL INIT,GOFLUK,DOSKAL,SKALEF |
| 8092 |
C |
| 8093 |
DATA INIT/.TRUE./ |
| 8094 |
C |
| 8095 |
IF(INIT) THEN |
| 8096 |
C |
| 8097 |
C Initialize CALOR at first call |
| 8098 |
INIT = .FALSE. |
| 8099 |
CALL CALINI |
| 8100 |
ENDIF |
| 8101 |
C |
| 8102 |
DOSKAL = .FALSE. |
| 8103 |
IF(Z+0.5.GE.1.0 ) THEN |
| 8104 |
IPINC = -1 |
| 8105 |
IF(IPART .LE. 48) IPINC = IGECAL(IPART) |
| 8106 |
C |
| 8107 |
C ------------- check if FLUKA have to be called --------- |
| 8108 |
C ------------------------------------------------- Goto FLUKA ? |
| 8109 |
C |
| 8110 |
C particle type not implemented in CALOR |
| 8111 |
GOFLUK = IPINC .EQ. -1 .OR. GEKIN .GE. ESKALE |
| 8112 |
DOSKAL = (IPINC.EQ.0 .OR. IPINC.EQ.1) .AND. GEKIN.GT.EMAXP |
| 8113 |
DOSKAL = DOSKAL .OR. (GEKIN .GT. EMAXPI .AND. (IPINC .GT. 1)) |
| 8114 |
DOSKAL = DOSKAL .AND. .NOT.GOFLUK |
| 8115 |
GOFLUK = GOFLUK .OR. (DOSKAL.AND.SKALEF(IPINC,GEKIN,ESKALE)) |
| 8116 |
C |
| 8117 |
IF(GOFLUK) THEN |
| 8118 |
ICPROC = 3 |
| 8119 |
CALL FLDIST |
| 8120 |
RETURN |
| 8121 |
ENDIF |
| 8122 |
C |
| 8123 |
C --------- material information for CALOR -------------------------- |
| 8124 |
C |
| 8125 |
EINC = GEKIN * 1000.0 |
| 8126 |
IF(IPINC .EQ. 1 .AND. EINC .LT. 20.0 ) THEN |
| 8127 |
C MICAP needs only the GEANT material number ! |
| 8128 |
NCEL = NMAT |
| 8129 |
ELSE |
| 8130 |
NCEL = 1 |
| 8131 |
AMED(1) = A |
| 8132 |
ZMED(1) = Z |
| 8133 |
DMED(1) = DENS/A*XNAVO |
| 8134 |
IF(A.GT.1.0 .AND. A.LT.1.1) THEN |
| 8135 |
HDEN = DMED(1) |
| 8136 |
ELSE |
| 8137 |
HDEN = 0.0 |
| 8138 |
ENDIF |
| 8139 |
C ------- get material parameter for a mixture--------------------- |
| 8140 |
KK=MIN(Q(JMA+11),100.) |
| 8141 |
NCEL = 1 |
| 8142 |
IF(KK.GT.1) THEN |
| 8143 |
NCEL = 0 |
| 8144 |
HDEN = 0.0 |
| 8145 |
AMOL = Q(LQ(JMIXT-1)+2) |
| 8146 |
DO 10 K=1,KK |
| 8147 |
IF(NINT(Q(JMIXT+K)).EQ.1) THEN |
| 8148 |
XMOLCM = DENS/AMOL*XNAVO |
| 8149 |
WI = Q(JMIXT+K+2*KK)*AMOL/Q(JMIXT+K) |
| 8150 |
HDEN = HDEN + XMOLCM*WI |
| 8151 |
ELSE |
| 8152 |
NCEL = NCEL + 1 |
| 8153 |
AMED(NCEL)= Q(JMIXT+K) |
| 8154 |
ZMED(NCEL) = Q(JMIXT+K+KK) |
| 8155 |
XMOLCM = DENS/AMOL*XNAVO |
| 8156 |
WI = Q(JMIXT+K+2*KK)*AMOL/AMED(NCEL) |
| 8157 |
DMED(NCEL) = XMOLCM*WI |
| 8158 |
ENDIF |
| 8159 |
10 CONTINUE |
| 8160 |
ENDIF |
| 8161 |
ENDIF |
| 8162 |
C |
| 8163 |
CALL GETXSC |
| 8164 |
IF( SIG .GT. 0.0) THEN |
| 8165 |
SHADR = ZINTHA/SIG |
| 8166 |
ELSE |
| 8167 |
SHADR = BIG |
| 8168 |
ENDIF |
| 8169 |
ELSE |
| 8170 |
SHADR = BIG |
| 8171 |
ENDIF |
| 8172 |
IF(DOSKAL) ICPROC = 2 |
| 8173 |
RETURN |
| 8174 |
END |
| 8175 |
*CMZ : 1.01/04 10/06/93 14.43.44 by Christian Zeitnitz |
| 8176 |
*-- Author : Christian Zeitnitz 06/06/92 |
| 8177 |
SUBROUTINE GETXSC |
| 8178 |
C*************************************************** |
| 8179 |
C Get x-section for hadronic interaction |
| 8180 |
C |
| 8181 |
C INPUT: material and particle parameters |
| 8182 |
C OUTPUT: SIG = x-section |
| 8183 |
C Author: C.Zeitnitz |
| 8184 |
C |
| 8185 |
C************************************************** |
| 8186 |
C GEANT-CALOR interface common |
| 8187 |
#include "calgea.inc" |
| 8188 |
*KEND. |
| 8189 |
C HETC-COMMON |
| 8190 |
#include "ccomon.inc" |
| 8191 |
*KEND. |
| 8192 |
C |
| 8193 |
C MICAP or HETC ? |
| 8194 |
IF(IPINC.EQ.1.AND.EINC.LT.20.0) THEN |
| 8195 |
C set MICAP parameter |
| 8196 |
EK = EINC * 1.0E6 |
| 8197 |
SIG = SIGMOR(EK,NCEL) |
| 8198 |
ICPROC = 1 |
| 8199 |
ELSE |
| 8200 |
C copy parameter to HETC common |
| 8201 |
NO = 1 |
| 8202 |
ITYP = IPINC + 1 |
| 8203 |
TIP(1) = FLOAT(IPINC) |
| 8204 |
EC(1) = EINC |
| 8205 |
IF(IPINC.LE.1.AND.EINC.GT.EMAXP) EC(1) = EMAXP*1000. |
| 8206 |
IF(IPINC.GT.1.AND.EINC.GT.EMAXPI) EC(1) = EMAXPI*1000. |
| 8207 |
MAT = 1 |
| 8208 |
MXMAT = 1 |
| 8209 |
NEL(1) = NCEL |
| 8210 |
C copy material data to HETC |
| 8211 |
DO 10 I=1,NCEL |
| 8212 |
DEN(I,1) = DMED(I) |
| 8213 |
ZZ(I,1) = ZMED(I) |
| 8214 |
A(I,1) = AMED(I) |
| 8215 |
DENH(1) = HDEN |
| 8216 |
10 CONTINUE |
| 8217 |
C calcutlate x-section for particle type IPINC and material |
| 8218 |
CALL CALCXS |
| 8219 |
SIG = SIGMX(ITYP,MAT) |
| 8220 |
ICPROC = 0 |
| 8221 |
ENDIF |
| 8222 |
RETURN |
| 8223 |
END |
| 8224 |
*CMZ : 1.01/04 10/06/93 14.43.44 by Christian Zeitnitz |
| 8225 |
*-- Author : Christian Zeitnitz 06/06/92 |
| 8226 |
SUBROUTINE CALCXS |
| 8227 |
C*********************************************** |
| 8228 |
C |
| 8229 |
C calculate cross section for given material |
| 8230 |
C |
| 8231 |
C*********************************************** |
| 8232 |
#include "ccomon.inc" |
| 8233 |
#include "cgeos.inc" |
| 8234 |
#include "cxpd.inc" |
| 8235 |
*KEND. |
| 8236 |
C |
| 8237 |
M=1 |
| 8238 |
DO 10 I=1,7 |
| 8239 |
SIGMX(I,M) = 0.0 |
| 8240 |
10 CONTINUE |
| 8241 |
TOT = 0.0 |
| 8242 |
DO 20 L=1,NEL(MAT) |
| 8243 |
EION(L,M) = CZFOI(ZZ(L,M))*1.0E-6 |
| 8244 |
NA = INT(A(L,M)+0.5) |
| 8245 |
SIGG(L,M) = DEN(L,M)*GEOSIG(NA) |
| 8246 |
TOT = TOT + SIGG(L,M) |
| 8247 |
20 CONTINUE |
| 8248 |
DO 30 IT=1,5 |
| 8249 |
HSIGG(IT,M) = DENH(M) * HSIGMX(IT) * 1.E24 |
| 8250 |
30 CONTINUE |
| 8251 |
SIGMX(1,M) = TOT + HSIGG(1,M) |
| 8252 |
SIGMX(2,M) = TOT + HSIGG(2,M) |
| 8253 |
SIGMX(3,M) = TOT + SGPIMX + HSIGG(3,M) |
| 8254 |
SIGMX(4,M) = 0. |
| 8255 |
SIGMX(5,M) = TOT + SGPIMX + HSIGG(5,M) |
| 8256 |
SIGMX(6,M) = SGMUMX |
| 8257 |
SIGMX(7,M) = SGMUMX |
| 8258 |
C |
| 8259 |
MT =MXMAT +1 |
| 8260 |
SIGMX(1,MT)= SGPIMX |
| 8261 |
SIGMX(2,MT)= SGPIMX |
| 8262 |
SIGMX(3,MT)= SGPIMX |
| 8263 |
SIGMX(4,MT)= 0. |
| 8264 |
SIGMX(5,MT)= SGPIMX |
| 8265 |
SIGMX(6,MT)= SGMUMX |
| 8266 |
SIGMX(7,MT)= SGMUMX |
| 8267 |
CZ CALL RANGE |
| 8268 |
K =1 |
| 8269 |
SUMARG = DENH(K)* 21.132 |
| 8270 |
III = NEL(K) |
| 8271 |
DO 40 I=1,III |
| 8272 |
SUMARG = DEN(I,K)*ZZ(I,K)*(ZZ(I,K)+1.)* (10.566-.333* |
| 8273 |
+ ALOG(ZZ(I,K)* A(I,K))) +SUMARG |
| 8274 |
40 CONTINUE |
| 8275 |
ARG(K) = SQRT (.498*SUMARG) |
| 8276 |
RETURN |
| 8277 |
END |
| 8278 |
*CMZ : 1.05/03 27/06/2001 18.17.08 by Christian Zeitnitz |
| 8279 |
*-- Author : Christian Zeitnitz 30/07/92 |
| 8280 |
FUNCTION SIGMOR(EK,NMED) |
| 8281 |
C*************************************************** |
| 8282 |
C Get x-section for low energetic neutrons |
| 8283 |
C Ek < 20 MeV (Ek is given in eV) |
| 8284 |
C INPUT: material and neutron energy |
| 8285 |
C OUTPUT: SIG = x-section |
| 8286 |
C |
| 8287 |
C************************************************** |
| 8288 |
C MICAP common |
| 8289 |
#include "mmicap.inc" |
| 8290 |
#include "mpoint.inc" |
| 8291 |
*KEND. |
| 8292 |
C |
| 8293 |
CALL NSIGTA(EK,NMED,TSIG,D,LD(LFP32),LD(LFP33)) |
| 8294 |
SIGMOR = TSIG |
| 8295 |
RETURN |
| 8296 |
END |
| 8297 |
*CMZ : 1.01/04 10/06/93 14.43.45 by Christian Zeitnitz |
| 8298 |
*-- Author : |
| 8299 |
SUBROUTINE ANGCDF(D,LD,LZ) |
| 8300 |
C THIS ROUTINE READS THE INPUT ANGULAR DISTRIBUTION FILES |
| 8301 |
C AND CONVERTS THEM TO A NORMALIZED CDF |
| 8302 |
DIMENSION D(*),LD(*) |
| 8303 |
IPP=1 |
| 8304 |
NR=LD(IPP) |
| 8305 |
NE=LD(IPP+1) |
| 8306 |
NR2=2*NR |
| 8307 |
II=2+NR2 |
| 8308 |
10 CONTINUE |
| 8309 |
E=D(II+1) |
| 8310 |
NP=LD(II+2) |
| 8311 |
A1=-1.0 |
| 8312 |
PL=D(II+4) |
| 8313 |
D(II+4)=0.0 |
| 8314 |
PROB=0.0 |
| 8315 |
DO 20 I=2,NP |
| 8316 |
N=II+2*I+2 |
| 8317 |
A2=D(N-1) |
| 8318 |
PH=D(N) |
| 8319 |
PROB=PROB+(PH+PL)*(A2-A1)/2.0 |
| 8320 |
PL=PH |
| 8321 |
D(N)=PROB |
| 8322 |
A1=A2 |
| 8323 |
20 CONTINUE |
| 8324 |
DO 30 I=1,NP |
| 8325 |
N=II+2*I+2 |
| 8326 |
D(N)=D(N)/PROB |
| 8327 |
30 CONTINUE |
| 8328 |
II=II+2*NP+2 |
| 8329 |
IF(II.GE.LZ)GO TO 40 |
| 8330 |
GO TO 10 |
| 8331 |
40 RETURN |
| 8332 |
END |
| 8333 |
*CMZ : 0.92/00 02/12/92 16.02.31 by Christian Zeitnitz |
| 8334 |
*-- Author : |
| 8335 |
SUBROUTINE BANKR(D,LD,NBNKID) |
| 8336 |
C THIS IS A DUMMY ROUTINE USUALLY SUPPLIED BY THE USER TO |
| 8337 |
C OBTAIN FURTHER ANALYSIS OF THE PROBLEM DEPENDING ON THE |
| 8338 |
C VALUE ASSIGNED TO NBNKID. |
| 8339 |
#include "minput.inc" |
| 8340 |
#include "mconst.inc" |
| 8341 |
#include "mpoint.inc" |
| 8342 |
#include "mapoll.inc" |
| 8343 |
#include "mrecoi.inc" |
| 8344 |
#include "mgamma.inc" |
| 8345 |
#include "mmass.inc" |
| 8346 |
*KEND. |
| 8347 |
DIMENSION D(*),LD(*) |
| 8348 |
NBNK=NBNKID |
| 8349 |
10 GO TO (20,30,40,50,60,70,80,90,100,110,120,130,140),NBNKID |
| 8350 |
C SOURCES GENERATED |
| 8351 |
20 RETURN |
| 8352 |
C SPLITTINGS OCCURRING |
| 8353 |
30 RETURN |
| 8354 |
C FISSIONS OCCURRING |
| 8355 |
40 RETURN |
| 8356 |
C GAMMA RAYS GENERATED |
| 8357 |
50 RETURN |
| 8358 |
C REAL COLLISIONS |
| 8359 |
60 RETURN |
| 8360 |
C ALBEDO SCATTERINGS |
| 8361 |
70 RETURN |
| 8362 |
80 RETURN |
| 8363 |
90 RETURN |
| 8364 |
C ENERGY CUTOFFS |
| 8365 |
100 RETURN |
| 8366 |
C TIME CUTOFFS |
| 8367 |
110 RETURN |
| 8368 |
C RUSSIAN ROULETTE KILLS |
| 8369 |
120 RETURN |
| 8370 |
C RUSSIAN ROULETTE SURVIVORS |
| 8371 |
130 RETURN |
| 8372 |
C GAMMA RAYS NOT STORED BECAUSE BANK WAS FULL |
| 8373 |
140 RETURN |
| 8374 |
END |
| 8375 |
*CMZ : 1.01/16 26/10/93 09.45.57 by Christian Zeitnitz |
| 8376 |
*-- Author : |
| 8377 |
SUBROUTINE BARIER(KZ1,KZ2,A1,A2,CB) |
| 8378 |
C THIS ROUTINE CALCULATES THE COULOMB BARRIER FOR A |
| 8379 |
C COLLISION INVOLVING CHARGED PARTICLE EMISSION |
| 8380 |
IFLG=0 |
| 8381 |
C CALCULATE THE RADIUS OF THE NUCLEUS AND CHARGED PARTICLE |
| 8382 |
A=A1 |
| 8383 |
10 IF(A.LT.5.5)R=1.20E-13 |
| 8384 |
IF((A.GE.5.5).AND.(A.LT.6.5))R=2.02E-13 |
| 8385 |
IF((A.GE.6.5).AND.(A.LT.7.5))R=2.43E-13 |
| 8386 |
IF((A.GE.7.5).AND.(A.LT.8.5))R=2.84E-13 |
| 8387 |
IF((A.GE.8.5).AND.(A.LT.9.5))R=3.25E-13 |
| 8388 |
IF(A.GE.9.5)R=(A**(1.0/3.0))*1.70E-13 |
| 8389 |
IF(IFLG.EQ.0)R1=R |
| 8390 |
IF(IFLG.EQ.1)GO TO 20 |
| 8391 |
IFLG=1 |
| 8392 |
A=A2 |
| 8393 |
GO TO 10 |
| 8394 |
20 R2=R |
| 8395 |
C CALCULATE THE COULOMB BARRIER (UNITS=MEV) |
| 8396 |
C THE FACTOR 0.75 IS ARBITRARYLY SET TO ACCOUNT FOR CHARGED |
| 8397 |
C PARTICLE EMISSION BELOW THE COULOMB BARRIER |
| 8398 |
CB=((KZ1*KZ2*1.44E-13)/(R1+R2))*0.75 |
| 8399 |
IF(CB.LT.0.0) CB = 0.0 |
| 8400 |
RETURN |
| 8401 |
END |
| 8402 |
*CMZ : 0.90/00 20/07/92 14.28.01 by Christian Zeitnitz |
| 8403 |
*-- Author : |
| 8404 |
FUNCTION CADIG(E) |
| 8405 |
C THIS FUNCTION ADDS A TOLERANCE TO THE ARGUMENT |
| 8406 |
ARG=ALOG10(E) |
| 8407 |
ITR=5-IFIX(ARG) |
| 8408 |
EPS=10.**ITR |
| 8409 |
CADIG=1./EPS |
| 8410 |
RETURN |
| 8411 |
END |
| 8412 |
*CMZ : 1.01/04 10/06/93 14.43.45 by Christian Zeitnitz |
| 8413 |
*-- Author : |
| 8414 |
SUBROUTINE CANGLE(D,LD,E,FM,LEN) |
| 8415 |
C THIS ROUTINE SELECTS THE SCATTERING ANGLE AT A COLLISION |
| 8416 |
DIMENSION D(*),LD(*) |
| 8417 |
SAVE |
| 8418 |
I=0 |
| 8419 |
IPP=1 |
| 8420 |
NR=LD(IPP) |
| 8421 |
NE=LD(IPP+1) |
| 8422 |
NR2=2*NR |
| 8423 |
IP=2+NR2 |
| 8424 |
INT=LD(IP) |
| 8425 |
10 IP=IP+1 |
| 8426 |
I=I+1 |
| 8427 |
EINCD=D(IP) |
| 8428 |
IF(E.LE.EINCD)GO TO 30 |
| 8429 |
IP1=IP |
| 8430 |
IP=IP+1 |
| 8431 |
NP=LD(IP) |
| 8432 |
IP=IP+2*NP |
| 8433 |
IF(IP.GE.LEN)GO TO 20 |
| 8434 |
GO TO 10 |
| 8435 |
C E IS GREATER THAN THE LAST INCIDENT ENERGY |
| 8436 |
C USE THE LAST DISTRIBUTION |
| 8437 |
20 IP=IP-2*NP-1 |
| 8438 |
GO TO 70 |
| 8439 |
30 IF(I.EQ.1)GO TO 60 |
| 8440 |
C CHOOSE WHICH DISTRIBUTION TO SAMPLE FROM |
| 8441 |
C THE INTERPOLATION SCHEME IS ASSUMED LINEAR-LINEAR IF IT |
| 8442 |
C IS NOT EQUAL TO THREE (LINEAR-LOG). THIS IS GENERALLY TRUE |
| 8443 |
IF(INT.NE.3)GO TO 40 |
| 8444 |
PROB=ALOG(EINCD/E)/ALOG(EINCD/D(IP1)) |
| 8445 |
40 PROB=(EINCD-E)/(EINCD-D(IP1)) |
| 8446 |
R=FLTRNF(0) |
| 8447 |
IF(R.LE.PROB)GO TO 50 |
| 8448 |
C SELECT FROM THE SECOND DISTRIBUTION |
| 8449 |
NP=LD(IP+1) |
| 8450 |
GO TO 70 |
| 8451 |
C SELECT FROM THE FIRST DISTRIBUTION |
| 8452 |
50 IP=IP1 |
| 8453 |
GO TO 70 |
| 8454 |
C E IS LESS THAN THE FIRST INCIDENT ENERGY |
| 8455 |
C USE THE FIRST DISTRIBUTION |
| 8456 |
60 NP=LD(IP+1) |
| 8457 |
70 CONTINUE |
| 8458 |
PROB1=0.0 |
| 8459 |
R=FLTRNF(0) |
| 8460 |
DO 80 I=2,NP |
| 8461 |
N=IP+2*I+1 |
| 8462 |
A1=D(N-3) |
| 8463 |
IF(R.LE.D(N))GO TO 90 |
| 8464 |
PROB1=D(N) |
| 8465 |
80 CONTINUE |
| 8466 |
FM=1.0 |
| 8467 |
RETURN |
| 8468 |
90 FM=A1+(R-PROB1)*(D(N-1)-A1)/(D(N)-PROB1) |
| 8469 |
IF(ABS(FM).GT.1.) FM = 1.0 |
| 8470 |
RETURN |
| 8471 |
END |
| 8472 |
*CMZ : 1.04/00 02/02/95 09.20.58 by Christian Zeitnitz |
| 8473 |
*-- Author : |
| 8474 |
SUBROUTINE CEVAP(E,Q,ATAR,CB,EX) |
| 8475 |
C THIS ROUTINE SAMPLES AN EXIT ENERGY FROM AN |
| 8476 |
C EVAPORATION SPECTRUM |
| 8477 |
#include "minput.inc" |
| 8478 |
*KEND. |
| 8479 |
SAVE |
| 8480 |
C CONVERT THE COULOMB BARRIER (CB) TO UNITS OF EV |
| 8481 |
CB=CB*1.00E+06 |
| 8482 |
C CALCULATE THE MAXIMUM ENERGY AVAILABLE |
| 8483 |
CBI=CB |
| 8484 |
EMAX=E+Q-CB |
| 8485 |
IF(EMAX.GT.0.0)GO TO 10 |
| 8486 |
CB=0.5*CB |
| 8487 |
EMAX=E+Q-CB |
| 8488 |
IF(EMAX.GT.0.0)GO TO 10 |
| 8489 |
CB=0.0 |
| 8490 |
EMAX=E+Q-CB |
| 8491 |
IF(EMAX.GT.0.0)GO TO 10 |
| 8492 |
WRITE(IOUT,10000)E,EMAX,Q,CBI |
| 8493 |
10000 FORMAT(' MICAP: NEGATIVE MAXIMUM ENERGY CALCULATED IN ROUTINE ', |
| 8494 |
1'EVAP --- INDICATING PROBABLE CROSS SECTION ERROR ALLOWING ', |
| 8495 |
2'THE REACTION TO OCCUR',/,10X,'E,EMAX,Q,CB=',4E13.5) |
| 8496 |
WRITE(6,*) ' CALOR: Fatal ERROR in EVAP ====> STOP ' |
| 8497 |
STOP |
| 8498 |
C CALCULATE THE NUCLEAR TEMPERATURE (THETA) |
| 8499 |
10 THETA=4.0161E+03*(SQRT(E+Q-CB)/(ATAR**0.8333333)) |
| 8500 |
C SELECT THE EXIT ENERGY FROM AN EVAPORATION SPECTRUM |
| 8501 |
20 R1=FLTRNF(0) |
| 8502 |
R2=FLTRNF(0) |
| 8503 |
W=-ALOG(R1*R2) |
| 8504 |
EX=THETA*W |
| 8505 |
IF(EX.LT.0.0) EX = 0.0 |
| 8506 |
IF(EX.LE.EMAX)RETURN |
| 8507 |
C RESAMPLE 75% OF THE TIME IF EX IS GREATER THAN EMAX |
| 8508 |
R=FLTRNF(0) |
| 8509 |
IF(R.LE.0.75)GO TO 20 |
| 8510 |
EX=EMAX |
| 8511 |
RETURN |
| 8512 |
END |
| 8513 |
*CMZ : 0.92/00 02/12/92 16.02.32 by Christian Zeitnitz |
| 8514 |
*-- Author : |
| 8515 |
SUBROUTINE CEVAP1(EOLD,E,Q,ATAR,CB,EX) |
| 8516 |
C THIS ROUTINE SAMPLES AN EXIT ENERGY FROM AN |
| 8517 |
C EVAPORATION SPECTRUM FOR AN (N,N-PRIME X) REACTION |
| 8518 |
#include "minput.inc" |
| 8519 |
*KEND. |
| 8520 |
SAVE |
| 8521 |
C CONVERT THE COULOMB BARRIER (CB) TO UNITS OF EV |
| 8522 |
CB=CB*1.00E+06 |
| 8523 |
C CALCULATE THE MAXIMUM ENERGY AVAILABLE |
| 8524 |
CBI=CB |
| 8525 |
EMAX=EOLD+Q-CB-E |
| 8526 |
IF(EMAX.GT.0.0)GO TO 10 |
| 8527 |
CB=0.5*CB |
| 8528 |
EMAX=EOLD+Q-CB-E |
| 8529 |
IF(EMAX.GT.0.0)GO TO 10 |
| 8530 |
CB=0.0 |
| 8531 |
EMAX=EOLD+Q-CB-E |
| 8532 |
IF(EMAX.LE.0.0)EMAX=1.0E+00 |
| 8533 |
C CALCULATE THE NUCLEAR TEMPERATURE (THETA) |
| 8534 |
10 THETA=4.0161E+03*(SQRT(EMAX)/(ATAR**0.8333333)) |
| 8535 |
C SELECT THE EXIT ENERGY FROM AN EVAPORATION SPECTRUM |
| 8536 |
ITRY = 0 |
| 8537 |
20 R1=FLTRNF(0) |
| 8538 |
R2=FLTRNF(0) |
| 8539 |
W=-ALOG(R1*R2) |
| 8540 |
EX=THETA*W |
| 8541 |
IF(EX.LE.EMAX)RETURN |
| 8542 |
C RESAMPLE 75% OF THE TIME IF EX IS GREATER THAN EMAX |
| 8543 |
R=FLTRNF(0) |
| 8544 |
ITRY = ITRY + 1 |
| 8545 |
IF(R.LE.0.75.AND.ITRY.LT.5)GO TO 20 |
| 8546 |
EX=EMAX |
| 8547 |
RETURN |
| 8548 |
END |
| 8549 |
*CMZ : 1.01/04 10/06/93 14.43.45 by Christian Zeitnitz |
| 8550 |
*-- Author : Christian Zeitnitz 27/04/93 |
| 8551 |
SUBROUTINE CHKZEB(NW,IX) |
| 8552 |
C |
| 8553 |
C Check if NW words are available in ZEBRA division IX |
| 8554 |
C |
| 8555 |
C ZEBRA user communication common |
| 8556 |
COMMON/ QUEST / IQUEST(100) |
| 8557 |
C |
| 8558 |
CALL MZNEED(IX,NW,'G') |
| 8559 |
IF(IQUEST(11).LT.0) THEN |
| 8560 |
PRINT *,'******************************************' |
| 8561 |
PRINT *,'* G C A L O R *' |
| 8562 |
PRINT *,'* NOT enough space available in ZEBRA *' |
| 8563 |
PRINT '('' * division '',I3,'' to store '',I8, ' |
| 8564 |
+ //' '' words *'')',IX,NW |
| 8565 |
PRINT *,'* *' |
| 8566 |
PRINT *,'* INCREASE ZEBRA COMMON SIZE AND RERUN *' |
| 8567 |
PRINT *,'* *' |
| 8568 |
PRINT *,'* RUN TERMINATED *' |
| 8569 |
PRINT *,'******************************************' |
| 8570 |
STOP |
| 8571 |
ENDIF |
| 8572 |
RETURN |
| 8573 |
END |
| 8574 |
*CMZ : 0.93/05 12/02/93 19.04.36 by Christian Zeitnitz |
| 8575 |
*-- Author : |
| 8576 |
SUBROUTINE CLEAR(L,L1,L2) |
| 8577 |
C THIS ROUTINE ZEROS ARRAY L FROM |
| 8578 |
C STARTING POINT L1 TO ENDING POINT L2 |
| 8579 |
DIMENSION L(*) |
| 8580 |
IF(L2-L1.LT.0)GO TO 20 |
| 8581 |
DO 10 I=L1,L2 |
| 8582 |
10 L(I)=0 |
| 8583 |
20 RETURN |
| 8584 |
END |
| 8585 |
*CMZ : 1.01/04 10/06/93 14.43.45 by Christian Zeitnitz |
| 8586 |
*-- Author : |
| 8587 |
SUBROUTINE CMLABE(D,LD,AWR,KZ,ID,FM,Q,IFLG) |
| 8588 |
C THIS ROUTINE CONVERTS THE EXIT NEUTRON SCATTERING ANGLE |
| 8589 |
C FROM THE CENTER OF MASS COORDINATE SYSTEM TO THE LABORATORY |
| 8590 |
C COORDINATE SYSTEM FOR AN ELASTIC SCATTERING REACTION. IT |
| 8591 |
C ALSO CALCULATES THE EXIT ENERGIES AND DIRECTIONAL COSINES |
| 8592 |
C FOR THE NEUTRON AND RECOIL NUCLEUS AS WELL AS SETTING ALL |
| 8593 |
C EXIT PARAMETERS FOR THE RECOIL NUCLEUS. |
| 8594 |
#include "minput.inc" |
| 8595 |
#include "mconst.inc" |
| 8596 |
#include "mnutrn.inc" |
| 8597 |
#include "mrecoi.inc" |
| 8598 |
#include "mapoll.inc" |
| 8599 |
#include "mmass.inc" |
| 8600 |
#include "mupsca.inc" |
| 8601 |
#include "mpstor.inc" |
| 8602 |
*KEND. |
| 8603 |
DIMENSION D(*),LD(*) |
| 8604 |
SAVE |
| 8605 |
MT=0 |
| 8606 |
IF(ID.EQ.2)MT=2 |
| 8607 |
C IFLG EQUAL TO ONE IMPLIES LABORATORY COORDINATE SYSTEM |
| 8608 |
IF(IFLG.EQ.1)GO TO 10 |
| 8609 |
IF(IFLG.EQ.2)GO TO 50 |
| 8610 |
ALPHA=((AWR-1.0)/(AWR+1.0))**2 |
| 8611 |
C E EQUALS THE EXIT ENERGY IN THE LAB SYSTEM |
| 8612 |
E=0.5*EOLD*((1.0-ALPHA)*FM+1.0+ALPHA) |
| 8613 |
C CALCULATE COSINE OF SCATTERING ANGLE (FM) IN LAB SYSTEM |
| 8614 |
FM=(1.0+AWR*FM)/SQRT(1.0+AWR**2+2.0*AWR*FM) |
| 8615 |
C CALCULATE THE NEUTRON EXIT DIRECTIONAL COSINES |
| 8616 |
10 SINPSI=SQRT(1.0-FM**2) |
| 8617 |
CALL AZIRN(SINETA,COSETA) |
| 8618 |
STHETA=1.0-UOLD**2 |
| 8619 |
IF(STHETA)30,30,20 |
| 8620 |
20 STHETA=SQRT(STHETA) |
| 8621 |
COSPHI=VOLD/STHETA |
| 8622 |
SINPHI=WOLD/STHETA |
| 8623 |
GO TO 40 |
| 8624 |
30 COSPHI=1.0 |
| 8625 |
SINPHI=0.0 |
| 8626 |
STHETA=0.0 |
| 8627 |
40 U=UOLD*FM-COSETA*SINPSI*STHETA |
| 8628 |
V=VOLD*FM+UOLD*COSPHI*COSETA*SINPSI-SINPHI*SINPSI*SINETA |
| 8629 |
W=WOLD*FM+UOLD*SINPHI*COSETA*SINPSI+COSPHI*SINPSI*SINETA |
| 8630 |
S=1.0/SQRT(U**2+V**2+W**2) |
| 8631 |
U=U*S |
| 8632 |
V=V*S |
| 8633 |
W=W*S |
| 8634 |
C CALCULATE AND SET THE RECOIL NUCLEUS EXIT PARAMETERS |
| 8635 |
50 ER=EOLD-E |
| 8636 |
C PERFORM ENERGY BALANCE CONSIDERING TARGET NUCLEUS ENERGY |
| 8637 |
IF(IFLG.EQ.2)ER=ERFGM+EOLD-E |
| 8638 |
XR=X |
| 8639 |
YR=Y |
| 8640 |
ZR=Z |
| 8641 |
WATER=WTBC |
| 8642 |
NZR=KZ |
| 8643 |
AGER=AGE |
| 8644 |
NCOLR=NCOL |
| 8645 |
MTNR=MT |
| 8646 |
AR=AWR*AN |
| 8647 |
ENIR=EOLD |
| 8648 |
UNIR=UOLD |
| 8649 |
VNIR=VOLD |
| 8650 |
WNIR=WOLD |
| 8651 |
ENOR=E |
| 8652 |
UNOR=U |
| 8653 |
VNOR=V |
| 8654 |
WNOR=W |
| 8655 |
WTNR=WATE |
| 8656 |
QR=Q |
| 8657 |
C CALCULATE THE NEUTRON MOMENTUM BEFORE AND AFTER COLLISION |
| 8658 |
C NEUTRON MOMENTUM BEFORE COLLISION (PI) EQUALS TOTAL MOMENTUM |
| 8659 |
PI=SQRT(2.0*ZN*EOLD) |
| 8660 |
PO=SQRT(2.0*ZN*E) |
| 8661 |
C CALCULATE THE DIRECTIONAL MOMENTUM OF THE RECOIL NUCLEUS |
| 8662 |
PRX=PI*UOLD-PO*U |
| 8663 |
PRY=PI*VOLD-PO*V |
| 8664 |
PRZ=PI*WOLD-PO*W |
| 8665 |
C CALCULATE THE TOTAL MOMENTUM OF THE RECOIL NUCLEUS |
| 8666 |
PR=SQRT(PRX**2+PRY**2+PRZ**2) |
| 8667 |
C CALCULATE THE RECOIL NUCLEUS DIRECTIONAL COSINES |
| 8668 |
IF(PR.GT.0.0) THEN |
| 8669 |
UR=PRX/PR |
| 8670 |
VR=PRY/PR |
| 8671 |
WR=PRZ/PR |
| 8672 |
ELSE |
| 8673 |
UR=0.0 |
| 8674 |
VR=0.0 |
| 8675 |
WR=0.0 |
| 8676 |
ENDIF |
| 8677 |
C STORE THE RECOIL HEAVY ION IN THE RECOIL BANK |
| 8678 |
EP = ER |
| 8679 |
UP = UR |
| 8680 |
VP = VR |
| 8681 |
WP = WR |
| 8682 |
AGEP = AGE |
| 8683 |
MTP = MT |
| 8684 |
AMP = AR |
| 8685 |
ZMP = FLOAT(NZR) |
| 8686 |
CALL STOPAR(IDHEVY,NHEVY) |
| 8687 |
RETURN |
| 8688 |
END |
| 8689 |
*CMZ : 1.01/04 10/06/93 14.43.45 by Christian Zeitnitz |
| 8690 |
*-- Author : |
| 8691 |
SUBROUTINE CMLABI(D,LD,AWR,KZ,ID,FM,Q,IFLG,LIFLAG,LRI) |
| 8692 |
C THIS ROUTINE CONVERTS THE EXIT NEUTRON SCATTERING ANGLE |
| 8693 |
C FROM THE CENTER OF MASS COORDINATE SYSTEM TO THE LABORATORY |
| 8694 |
C COORDINATE SYSTEM FOR AN INELASTIC SCATTERING REACTION. IT |
| 8695 |
C ALSO CALCULATES THE EXIT ENERGIES AND DIRECTIONAL COSINES |
| 8696 |
C FOR THE NEUTRON AND RECOIL NUCLEUS AS WELL AS SETTING ALL |
| 8697 |
C EXIT PARAMETERS FOR THE RECOIL NUCLEUS. |
| 8698 |
#include "minput.inc" |
| 8699 |
#include "mconst.inc" |
| 8700 |
#include "mnutrn.inc" |
| 8701 |
#include "mrecoi.inc" |
| 8702 |
#include "mapoll.inc" |
| 8703 |
#include "mmass.inc" |
| 8704 |
#include "mpstor.inc" |
| 8705 |
*KEND. |
| 8706 |
DIMENSION D(*),LD(*) |
| 8707 |
SAVE |
| 8708 |
MT=0 |
| 8709 |
IF((ID.GE.14).AND.(ID.LE.54))MT=51 |
| 8710 |
IF(MT.NE.51)GO TO 10 |
| 8711 |
IMT=ID-14 |
| 8712 |
MT=MT+IMT |
| 8713 |
10 IF(ID.EQ.11)MT=22 |
| 8714 |
IF(ID.EQ.13)MT=28 |
| 8715 |
C IFLG EQUAL TO ONE IMPLIES LABORATORY COORDINATE SYSTEM |
| 8716 |
IF(LIFLAG.EQ.1)GO TO 60 |
| 8717 |
IF(IFLG.EQ.1)GO TO 20 |
| 8718 |
C E1 EQUALS THE EXIT ENERGY IN THE COM SYSTEM |
| 8719 |
E1=((AWR/(AWR+1.0))**2)*EOLD+Q*(AWR/(AWR+1.0)) |
| 8720 |
C re-sample in COLISN E1<0.0 (Q-value = -EOLD) !!! |
| 8721 |
IF(E1.LT.0.0) THEN |
| 8722 |
IFLG = -1 |
| 8723 |
RETURN |
| 8724 |
ENDIF |
| 8725 |
C E2 EQUALS THE EXIT ENERGY IN THE LAB SYSTEM |
| 8726 |
E2=E1+(EOLD+2.0*FM*(AWR+1.0)*SQRT(EOLD*E1))/((AWR+1.0)**2) |
| 8727 |
C CALCULATE COSINE OF SCATTERING ANGLE FM IN LAB SYSTEM |
| 8728 |
FM=(SQRT(E1/E2))*FM+(SQRT(EOLD/E2))*(1.0/(AWR+1.0)) |
| 8729 |
E=E2 |
| 8730 |
C CALCULATE THE NEUTRON EXIT DIRECTIONAL COSINES |
| 8731 |
20 SINPSI=SQRT(1.0-FM**2) |
| 8732 |
CALL AZIRN(SINETA,COSETA) |
| 8733 |
STHETA=1.0-UOLD**2 |
| 8734 |
IF(STHETA)40,40,30 |
| 8735 |
30 STHETA=SQRT(STHETA) |
| 8736 |
COSPHI=VOLD/STHETA |
| 8737 |
SINPHI=WOLD/STHETA |
| 8738 |
GO TO 50 |
| 8739 |
40 COSPHI=1.0 |
| 8740 |
SINPHI=0.0 |
| 8741 |
STHETA=0.0 |
| 8742 |
50 U=UOLD*FM-COSETA*SINPSI*STHETA |
| 8743 |
V=VOLD*FM+UOLD*COSPHI*COSETA*SINPSI-SINPHI*SINPSI*SINETA |
| 8744 |
W=WOLD*FM+UOLD*SINPHI*COSETA*SINPSI+COSPHI*SINPSI*SINETA |
| 8745 |
S=1.0/SQRT(U**2+V**2+W**2) |
| 8746 |
U=U*S |
| 8747 |
V=V*S |
| 8748 |
W=W*S |
| 8749 |
IF(MT.EQ.91)LIFLAG=1 |
| 8750 |
IF(MT.EQ.22)LIFLAG=1 |
| 8751 |
IF(MT.EQ.28)LIFLAG=1 |
| 8752 |
IF(LIFLAG.EQ.1)GO TO 60 |
| 8753 |
C CALCULATE AND SET THE RECOIL NUCLEUS EXIT PARAMETERS |
| 8754 |
ER=EOLD-E+Q |
| 8755 |
60 XR=X |
| 8756 |
YR=Y |
| 8757 |
ZR=Z |
| 8758 |
WATER=WTBC |
| 8759 |
NZR=KZ |
| 8760 |
AGER=AGE |
| 8761 |
NCOLR=NCOL |
| 8762 |
MTNR=MT |
| 8763 |
AR=AWR*AN |
| 8764 |
ENIR=EOLD |
| 8765 |
UNIR=UOLD |
| 8766 |
VNIR=VOLD |
| 8767 |
WNIR=WOLD |
| 8768 |
ENOR=E |
| 8769 |
UNOR=U |
| 8770 |
VNOR=V |
| 8771 |
WNOR=W |
| 8772 |
WTNR=WATE |
| 8773 |
QR=Q |
| 8774 |
C CALCULATE THE NEUTRON MOMENTUM BEFORE AND AFTER COLLISION |
| 8775 |
C NEUTRON MOMENTUM BEFORE COLLISION (PI) EQUALS TOTAL MOMENTUM |
| 8776 |
PI=SQRT(2.0*ZN*EOLD) |
| 8777 |
PO=SQRT(2.0*ZN*E) |
| 8778 |
C CALCULATE THE DIRECTIONAL MOMENTUM OF THE RECOIL NUCLEUS |
| 8779 |
PRX=PI*UOLD-PO*U |
| 8780 |
PRY=PI*VOLD-PO*V |
| 8781 |
PRZ=PI*WOLD-PO*W |
| 8782 |
C CALCULATE THE TOTAL MOMENTUM OF THE RECOIL NUCLEUS |
| 8783 |
PR=SQRT(PRX**2+PRY**2+PRZ**2) |
| 8784 |
C CALCULATE THE RECOIL NUCLEUS DIRECTIONAL COSINES |
| 8785 |
UR=PRX/PR |
| 8786 |
VR=PRY/PR |
| 8787 |
WR=PRZ/PR |
| 8788 |
C CALCULATE THE RECOIL HEAVY ION ENERGY FOR MT-91 |
| 8789 |
IF(LIFLAG.EQ.0)GO TO 70 |
| 8790 |
XM = AR*931.075E6 |
| 8791 |
ER= SQRT(PR**2 + XM**2) - XM |
| 8792 |
70 CONTINUE |
| 8793 |
C IF LR-FLAG IS USED, DO NOT STORE RECOIL ION AT THIS TIME |
| 8794 |
IF(LRI.EQ.22)RETURN |
| 8795 |
IF(LRI.EQ.23)RETURN |
| 8796 |
IF(LRI.EQ.28)RETURN |
| 8797 |
C STORE THE RECOIL HEAVY ION IN THE RECOIL BANK |
| 8798 |
EP = ER |
| 8799 |
UP = UR |
| 8800 |
VP = VR |
| 8801 |
WP = WR |
| 8802 |
AGEP = AGE |
| 8803 |
MTP = MT |
| 8804 |
AMP = AR |
| 8805 |
ZMP = FLOAT(NZR) |
| 8806 |
CALL STOPAR(IDHEVY,NHEVY) |
| 8807 |
RETURN |
| 8808 |
END |
| 8809 |
*CMZ : 1.05/03 27/06/2001 18.32.27 by Christian Zeitnitz |
| 8810 |
*-- Author : |
| 8811 |
SUBROUTINE COLISN(D,LD,IGAMS,LGAM,INABS,LNAB,XTHRMS,ITHRMS,LTHRM, |
| 8812 |
+ IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR,Q,NSEI,NAEI,NMT2,NMT4, |
| 8813 |
+ NMT16,NMT17,NMT18,NMT22,NMT23,NMT24,NMT28,NMT51,NMT91, |
| 8814 |
+ NMT102,NMT103,NMT104,NMT105,NMT106,NMT107,NMT108,NMT109, |
| 8815 |
+ NMT111,NMT112,NMT113,NMT114,IGCBS2,LGCB2,KZ,LR,QLR, |
| 8816 |
+ IIN,IIM) |
| 8817 |
C THIS ROUTINE IS CALLED AT EACH COLLISION TO |
| 8818 |
C DETERMINE THE POST COLLISION PARAMETERS |
| 8819 |
#include "minput.inc" |
| 8820 |
#include "mconst.inc" |
| 8821 |
#include "mnutrn.inc" |
| 8822 |
#include "mapoll.inc" |
| 8823 |
#include "mcross.inc" |
| 8824 |
#include "mmass.inc" |
| 8825 |
#include "mupsca.inc" |
| 8826 |
#include "mpstor.inc" |
| 8827 |
#include "mmicab.inc" |
| 8828 |
*KEND. |
| 8829 |
DIMENSION D(*),LD(*),IGAMS(*),LGAM(*),INABS(*),LNAB(*), |
| 8830 |
+ XTHRMS(*),ITHRMS(*),LTHRM(*),IDICTS(NNR,NNUC),LDICT(NNR,NNUC), |
| 8831 |
+ NTX(*), |
| 8832 |
+ NTS(*),IGCBS(NGR,NNUC),LGCB(NGR,NNUC),AWR(*),Q(NQ,NNUC), |
| 8833 |
+ NSEI(*),NAEI(*),NMT2(*),NMT4(*),NMT16(1),NMT17(*),NMT18(*), |
| 8834 |
+ NMT22(*),NMT23(*),NMT24(*),NMT28(*),NMT51(*),NMT91(*), |
| 8835 |
+ NMT102(*),NMT103(*),NMT104(*),NMT105(*),NMT106(*),NMT107(*), |
| 8836 |
+ NMT108(*),NMT109(*),NMT111(*),NMT112(*),NMT113(*),NMT114(*), |
| 8837 |
+ IGCBS2(NGR,NNUC),LGCB2(NGR,NNUC),KZ(*),LR(NQ,NNUC),QLR(NQ,NNUC), |
| 8838 |
+ FM(MAXNEU) |
| 8839 |
C |
| 8840 |
CHARACTER*80 COMM |
| 8841 |
C |
| 8842 |
DATA QBE8/-7.3686E+06/ |
| 8843 |
SAVE |
| 8844 |
CALL GTMED(NMED,MED) |
| 8845 |
C INITIALIZE THE COUNTERS AND FLAGS |
| 8846 |
C ITRY ALLOWS FOR MULTIPLE ATTEMPTS IF THE ENDF/B PARTIAL |
| 8847 |
C CROSS SECTIONS DO NOT EXACTLY SUM TO THE TOTAL |
| 8848 |
10 ISTOP=0 |
| 8849 |
ITRY=0 |
| 8850 |
NCOL=NCOL+1 |
| 8851 |
SIGREC=0.0 |
| 8852 |
SUMREC=0.0 |
| 8853 |
FSUMS = 1.0 |
| 8854 |
FSUMIS = 1.0 |
| 8855 |
FSUMA = 1.0 |
| 8856 |
20 ID=0 |
| 8857 |
MT=0 |
| 8858 |
QI=0.0 |
| 8859 |
LRI=0 |
| 8860 |
QLRI=0.0 |
| 8861 |
DO 30 I=1,MAXNEU |
| 8862 |
FM(I)=1.0 |
| 8863 |
30 CONTINUE |
| 8864 |
DO 40 I=1,MAXNEU |
| 8865 |
ENE(I)=0.0 |
| 8866 |
40 CONTINUE |
| 8867 |
INEU = 0 |
| 8868 |
U1=0.0 |
| 8869 |
V1=0.0 |
| 8870 |
W1=0.0 |
| 8871 |
ERFGM=0.0 |
| 8872 |
IFLG=0 |
| 8873 |
LIFLAG=0 |
| 8874 |
AWRI=AWR(IIN) |
| 8875 |
KZI=KZ(IIM) |
| 8876 |
C INITIALIZE THE CROSS SECTION VARIABLES |
| 8877 |
SIGT=0.0 |
| 8878 |
SIGTNS=0.0 |
| 8879 |
SIGTNA=0.0 |
| 8880 |
SIGNES=0.0 |
| 8881 |
SIGNIS=0.0 |
| 8882 |
SGNISD=0.0 |
| 8883 |
SGNISC=0.0 |
| 8884 |
SIGN2N=0.0 |
| 8885 |
SIGN3N=0.0 |
| 8886 |
SIGNNA=0.0 |
| 8887 |
SGNN3A=0.0 |
| 8888 |
SGN2NA=0.0 |
| 8889 |
SIGNNP=0.0 |
| 8890 |
SIGNF=0.0 |
| 8891 |
SIGNG=0.0 |
| 8892 |
SIGNP=0.0 |
| 8893 |
SIGND=0.0 |
| 8894 |
SIGNT=0.0 |
| 8895 |
SGN3HE=0.0 |
| 8896 |
SIGNA=0.0 |
| 8897 |
SIGN2A=0.0 |
| 8898 |
SIGN3A=0.0 |
| 8899 |
SIGN2P=0.0 |
| 8900 |
SIGNPA=0.0 |
| 8901 |
SGNT2A=0.0 |
| 8902 |
SGND2A=0.0 |
| 8903 |
SUMIS=0.0 |
| 8904 |
SUMS=0.0 |
| 8905 |
SUMA=0.0 |
| 8906 |
C DETERMINE THE TOTAL CROSS SECTION (MT-1) |
| 8907 |
L1=LDICT(1,IIN) |
| 8908 |
IF(L1.EQ.0)GO TO 50 |
| 8909 |
LS1=IDICTS(1,IIN) + LMOX2 |
| 8910 |
LEN=L1/2 |
| 8911 |
CALL TBSPLT(D(LS1),E,LEN,SIGT) |
| 8912 |
GO TO 60 |
| 8913 |
50 CONTINUE |
| 8914 |
COMM=' COLISN: TOTAL CROSS SECTION LENGTH IS ZERO' |
| 8915 |
SIGREC = 0.0 |
| 8916 |
SUMREC = 0.0 |
| 8917 |
GOTO 980 |
| 8918 |
60 CONTINUE |
| 8919 |
C DETERMINE THE TOTAL NEUTRON DISAPPEARANCE (MT-102 TO MT-114 |
| 8920 |
C AND MT-18) |
| 8921 |
L1=LNAB(IIN) |
| 8922 |
IF(L1.EQ.0)GO TO 70 |
| 8923 |
LS1=INABS(IIN)+LMOX2 |
| 8924 |
LEN=L1/2 |
| 8925 |
CALL TBSPLT(D(LS1),E,LEN,SIGTNA) |
| 8926 |
GO TO 80 |
| 8927 |
70 SIGTNA=0.0 |
| 8928 |
80 CONTINUE |
| 8929 |
C DETERMINE THE NON-ABSORPTION PROBABILITY |
| 8930 |
PNAB=1.0-SIGTNA/SIGT |
| 8931 |
C DETERMINE THE COLLISION TYPE (ABSORPTION OR SCATTERING) |
| 8932 |
R=FLTRNF(0) |
| 8933 |
IF(R.GT.PNAB)GO TO 570 |
| 8934 |
C THE REACTION TYPE IS A SCATTER |
| 8935 |
NSEI(IIN)=NSEI(IIN)+1 |
| 8936 |
SIGTNS=SIGT-SIGTNA |
| 8937 |
R=FLTRNF(0) |
| 8938 |
C DETERMINE (N,N) CROSS SECTION (MT-2) |
| 8939 |
ID=2 |
| 8940 |
L1=LDICT(ID,IIN) |
| 8941 |
IF(L1.EQ.0)GO TO 110 |
| 8942 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 8943 |
LEN=L1/2 |
| 8944 |
CALL TBSPLT(D(LS1),E,LEN,SIGNES) |
| 8945 |
SUMS=SIGNES/SIGTNS*FSUMS |
| 8946 |
IF(R.GT.SUMS)GO TO 120 |
| 8947 |
C REACTION TYPE IS (N,N) |
| 8948 |
NMT2(MED)=NMT2(MED)+1 |
| 8949 |
C DETERMINE IF SCATTERING OCCURS IN THE THERMAL ENERGY RANGE |
| 8950 |
ETHERM = 500.*8.617E-5*TEMP/AWRI |
| 8951 |
IF(E.LE.ETHERM) THEN |
| 8952 |
C Reaction is a thermal scatter |
| 8953 |
CALL THRMSC(D,LD,XTHRMS,ITHRMS,LTHRM,E,U,V,W,TEMP,FM,AWR,IIN, |
| 8954 |
+ IFLG,IOUT) |
| 8955 |
QI=Q(ID,IIN) |
| 8956 |
CALL CMLABE(D,LD,AWRI,KZI,ID,FM,QI,IFLG) |
| 8957 |
EP = E |
| 8958 |
VP = V |
| 8959 |
UP = U |
| 8960 |
WP = W |
| 8961 |
AGEP = AGE |
| 8962 |
MTP = 2 |
| 8963 |
CALL STOPAR(IDNEU,NNEU) |
| 8964 |
RETURN |
| 8965 |
ENDIF |
| 8966 |
C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE |
| 8967 |
C CENTER OF MASS COORDINATE SYSTEM |
| 8968 |
L1=LDICT(67,IIN) |
| 8969 |
IF(L1.EQ.0)GO TO 90 |
| 8970 |
LS1=IDICTS(67,IIN)+LMOX2 |
| 8971 |
LEN=L1 |
| 8972 |
CALL CANGLE(D(LS1),LD(LS1),E,FM(1),LEN) |
| 8973 |
GO TO 100 |
| 8974 |
C ASSUME ISOTROPIC IN THE CENTER OF MASS COORDINATE SYSTEM |
| 8975 |
90 R=FLTRNF(0) |
| 8976 |
FM(1)=2.0*R-1.0 |
| 8977 |
C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY |
| 8978 |
C COORDINATE SYSTEM |
| 8979 |
100 CONTINUE |
| 8980 |
QI=Q(ID,IIN) |
| 8981 |
CALL CMLABE(D,LD,AWRI,KZI,ID,FM(1),QI,IFLG) |
| 8982 |
EP = E |
| 8983 |
VP = V |
| 8984 |
UP = U |
| 8985 |
WP = W |
| 8986 |
AGEP = AGE |
| 8987 |
MTP = 2 |
| 8988 |
CALL STOPAR(IDNEU,NNEU) |
| 8989 |
RETURN |
| 8990 |
110 SIGNES=0.0 |
| 8991 |
120 CONTINUE |
| 8992 |
C DETERMINE (N,N") CROSS SECTION (MT-4) |
| 8993 |
ID=3 |
| 8994 |
L1=LDICT(ID,IIN) |
| 8995 |
IF(L1.EQ.0)GO TO 240 |
| 8996 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 8997 |
LEN=L1/2 |
| 8998 |
CALL TBSPLT(D(LS1),E,LEN,SIGNIS) |
| 8999 |
SUMS=SUMS+SIGNIS/SIGTNS*FSUMS |
| 9000 |
IF(R.GT.SUMS)GO TO 250 |
| 9001 |
C REACTION TYPE IS (N,N") |
| 9002 |
NMT4(MED)=NMT4(MED)+1 |
| 9003 |
C DETERMINE (N,N"-DISCRETE) CROSS SECTION (MT-51 TO MT-90) |
| 9004 |
R=FLTRNF(0) |
| 9005 |
DO 130 I=14,53 |
| 9006 |
L1=LDICT(I,IIN) |
| 9007 |
IF(L1.EQ.0)GO TO 170 |
| 9008 |
LS1=IDICTS(I,IIN)+LMOX2 |
| 9009 |
LEN=L1/2 |
| 9010 |
CALL XSECNU(D,LEN,E,SGNISD,LS1,L1) |
| 9011 |
SUMIS=SUMIS+SGNISD/SIGNIS*FSUMIS |
| 9012 |
IF(R.LE.SUMIS)GO TO 140 |
| 9013 |
130 CONTINUE |
| 9014 |
GO TO 180 |
| 9015 |
140 CONTINUE |
| 9016 |
C REACTION TYPE IS (N,N") DISCRETE |
| 9017 |
NMT51(MED)=NMT51(MED)+1 |
| 9018 |
I=I+68 |
| 9019 |
C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE |
| 9020 |
C CENTER OF MASS COORDINATE SYSTEM |
| 9021 |
L1=LDICT(I,IIN) |
| 9022 |
IF(L1.EQ.0)GO TO 150 |
| 9023 |
LS1=IDICTS(I,IIN)+LMOX2 |
| 9024 |
LEN=L1 |
| 9025 |
CALL CANGLE(D(LS1),LD(LS1),E,FM(1),LEN) |
| 9026 |
GO TO 160 |
| 9027 |
C ASSUME ISOTROPIC IN THE CENTER OF MASS COORDINATE SYSTEM |
| 9028 |
150 R=FLTRNF(0) |
| 9029 |
FM(1)=2.0*R-1.0 |
| 9030 |
C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY |
| 9031 |
C COORDINATE SYSTEM |
| 9032 |
160 ID=I-68 |
| 9033 |
QI=Q(ID,IIN) |
| 9034 |
LRI=LR(ID,IIN) |
| 9035 |
QLRI=QLR(ID,IIN) |
| 9036 |
CALL CMLABI(D,LD,AWRI,KZI,ID,FM(1),QI,IFLG,LIFLAG,LRI) |
| 9037 |
C Re-sample if no energy determined in CMLABI |
| 9038 |
IF(IFLG.EQ.-1) GOTO 10 |
| 9039 |
EP = E |
| 9040 |
VP = V |
| 9041 |
UP = U |
| 9042 |
WP = W |
| 9043 |
AGEP = AGE |
| 9044 |
MTP = 51 |
| 9045 |
CALL STOPAR(IDNEU,NNEU) |
| 9046 |
IF(LRI.EQ.22)GO TO 520 |
| 9047 |
IF(LRI.EQ.23)GO TO 530 |
| 9048 |
IF(LRI.EQ.28)GO TO 540 |
| 9049 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9050 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGNISD) |
| 9051 |
RETURN |
| 9052 |
170 SGNISD=0.0 |
| 9053 |
180 CONTINUE |
| 9054 |
C DISCRETE INELASTIC SCATTERING LEVEL WAS NOT CHOSEN |
| 9055 |
C DETERMINE (N,N"-CONTINUUM) CROSS SECTION (MT-91) |
| 9056 |
ID=54 |
| 9057 |
L1=LDICT(ID,IIN) |
| 9058 |
IF(L1.EQ.0)GO TO 210 |
| 9059 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9060 |
LEN=L1/2 |
| 9061 |
CALL TBSPLT(D(LS1),E,LEN,SGNISC) |
| 9062 |
SUMIS=SUMIS+SGNISC/SIGNIS*FSUMIS |
| 9063 |
IF(R.GT.SUMIS)GO TO 220 |
| 9064 |
C REACTION TYPE IS (N,N") CONTINUUM |
| 9065 |
NMT91(MED)=NMT91(MED)+1 |
| 9066 |
C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE |
| 9067 |
C LABORATORY COORDINATE SYSTEM |
| 9068 |
L1=LDICT(122,IIN) |
| 9069 |
IF(L1.EQ.0)GO TO 190 |
| 9070 |
LS1=IDICTS(122,IIN)+LMOX2 |
| 9071 |
LEN=L1 |
| 9072 |
CALL CANGLE(D(LS1),LD(LS1),E,FM(1),LEN) |
| 9073 |
GO TO 200 |
| 9074 |
C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM |
| 9075 |
190 CALL GTISO(U1,V1,W1) |
| 9076 |
U=U1 |
| 9077 |
V=V1 |
| 9078 |
W=W1 |
| 9079 |
LIFLAG=1 |
| 9080 |
C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY |
| 9081 |
C COORDINATE SYSTEM |
| 9082 |
200 L1=LDICT(133,IIN) |
| 9083 |
IF(L1.EQ.0)GO TO 230 |
| 9084 |
LS1=IDICTS(133,IIN)+LMOX2 |
| 9085 |
CALL SECEGY(EX,D(LS1),E,LD(LS1)) |
| 9086 |
E=EX |
| 9087 |
IFLG=1 |
| 9088 |
C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY |
| 9089 |
C COORDINATE SYSTEM |
| 9090 |
QI=Q(ID,IIN) |
| 9091 |
LRI=LR(ID,IIN) |
| 9092 |
QLRI=QLR(ID,IIN) |
| 9093 |
CALL CMLABI(D,LD,AWRI,KZI,ID,FM(1),QI,IFLG,LIFLAG,LRI) |
| 9094 |
C Re-sample if no energy determined in CMLABI |
| 9095 |
IF(IFLG.EQ.-1) GOTO 10 |
| 9096 |
EP = E |
| 9097 |
VP = V |
| 9098 |
UP = U |
| 9099 |
WP = W |
| 9100 |
AGEP = AGE |
| 9101 |
MTP = 91 |
| 9102 |
CALL STOPAR(IDNEU,NNEU) |
| 9103 |
IF(LRI.EQ.22)GO TO 520 |
| 9104 |
IF(LRI.EQ.23)GO TO 530 |
| 9105 |
IF(LRI.EQ.28)GO TO 540 |
| 9106 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9107 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGNISC) |
| 9108 |
RETURN |
| 9109 |
210 SGNISC=0.0 |
| 9110 |
220 CONTINUE |
| 9111 |
COMM= ' COLISN: INELASTIC SCATTERING CROSS SECTION WAS NOT CHOSEN' |
| 9112 |
NMT4(MED)=NMT4(MED)-1 |
| 9113 |
FSUMIS = 1./SUMIS |
| 9114 |
GO TO 550 |
| 9115 |
230 CONTINUE |
| 9116 |
COMM=' COLISN: NO SECONDARY ENERGY DISTRIBUTION WAS FOUND MT-91' |
| 9117 |
ISTOP=1 |
| 9118 |
GO TO 560 |
| 9119 |
240 SIGNIS=0.0 |
| 9120 |
250 CONTINUE |
| 9121 |
C DETERMINE (N,2N) CROSS SECTION (MT-16) |
| 9122 |
ID=8 |
| 9123 |
L1=LDICT(ID,IIN) |
| 9124 |
IF(L1.EQ.0)GO TO 290 |
| 9125 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9126 |
LEN=L1/2 |
| 9127 |
CALL TBSPLT(D(LS1),E,LEN,SIGN2N) |
| 9128 |
SUMS=SUMS+SIGN2N/SIGTNS*FSUMS |
| 9129 |
IF(R.GT.SUMS)GO TO 300 |
| 9130 |
C REACTION TYPE IS (N,2N) |
| 9131 |
NMT16(MED)=NMT16(MED)+1 |
| 9132 |
C USE THE ONE NEUTRON EMISSION MODEL AND MULTIPLY THE |
| 9133 |
C WEIGHT BY TWO |
| 9134 |
C changed to 2 neutron production CZ July 30, 1992 |
| 9135 |
CZ WATE=2.0*WATE |
| 9136 |
C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE |
| 9137 |
C LABORATORY COORDINATE SYSTEM |
| 9138 |
L1=LDICT(72,IIN) |
| 9139 |
IF(L1.EQ.0)GO TO 260 |
| 9140 |
LS1=IDICTS(72,IIN)+LMOX2 |
| 9141 |
LEN=L1 |
| 9142 |
C get scattering angle for 1. neutron |
| 9143 |
CALL CANGLE(D(LS1),LD(LS1),E,FM(1),LEN) |
| 9144 |
C get scattering angle for 2. neutron |
| 9145 |
CALL CANGLE(D(LS1),LD(LS1),E,FM(2),LEN) |
| 9146 |
GO TO 270 |
| 9147 |
C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM |
| 9148 |
260 CONTINUE |
| 9149 |
IFLG=1 |
| 9150 |
C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY |
| 9151 |
C COORDINATE SYSTEM |
| 9152 |
270 INEU = 2 |
| 9153 |
L1=LDICT(123,IIN) |
| 9154 |
IF(L1.EQ.0)GO TO 280 |
| 9155 |
LS1=IDICTS(123,IIN)+LMOX2 |
| 9156 |
CALL GETENE(E,D(LS1),LD(LS1),INEU) |
| 9157 |
C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY |
| 9158 |
C COORDINATE SYSTEM |
| 9159 |
QI=Q(ID,IIN) |
| 9160 |
CALL N2NN3N(D,LD,AWRI,KZI,ID,FM,QI,IFLG) |
| 9161 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9162 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGN2N) |
| 9163 |
RETURN |
| 9164 |
280 CONTINUE |
| 9165 |
COMM=' COLISN: NO SECONDARY ENERGY DISTRIBUTION WAS FOUND MT-16' |
| 9166 |
ISTOP=1 |
| 9167 |
GO TO 560 |
| 9168 |
290 SIGN2N=0.0 |
| 9169 |
300 CONTINUE |
| 9170 |
C DETERMINE (N,3N) CROSS SECTION (MT-17) |
| 9171 |
ID=9 |
| 9172 |
L1=LDICT(ID,IIN) |
| 9173 |
IF(L1.EQ.0)GO TO 350 |
| 9174 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9175 |
LEN=L1/2 |
| 9176 |
CALL TBSPLT(D(LS1),E,LEN,SIGN3N) |
| 9177 |
SUMS=SUMS+SIGN3N/SIGTNS*FSUMS |
| 9178 |
IF(R.GT.SUMS)GO TO 360 |
| 9179 |
C REACTION TYPE IS (N,3N) |
| 9180 |
NMT17(MED)=NMT17(MED)+1 |
| 9181 |
C USE THE ONE NEUTRON EMISSION MODEL AND MULTIPLY THE |
| 9182 |
C WEIGHT BY THREE |
| 9183 |
C changed to 3 neutron production CZ July 30,1992 |
| 9184 |
CZ WATE=3.0*WATE |
| 9185 |
C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE |
| 9186 |
C LABORATORY COORDINATE SYSTEM |
| 9187 |
L1=LDICT(73,IIN) |
| 9188 |
IF(L1.EQ.0)GO TO 320 |
| 9189 |
LS1=IDICTS(73,IIN)+LMOX2 |
| 9190 |
LEN=L1 |
| 9191 |
DO 310 KN=1,3 |
| 9192 |
CALL CANGLE(D(LS1),LD(LS1),E,FM(KN),LEN) |
| 9193 |
310 CONTINUE |
| 9194 |
GO TO 330 |
| 9195 |
C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM |
| 9196 |
320 CONTINUE |
| 9197 |
IFLG=1 |
| 9198 |
C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY |
| 9199 |
C COORDINATE SYSTEM |
| 9200 |
330 L1=LDICT(124,IIN) |
| 9201 |
IF(L1.EQ.0)GO TO 340 |
| 9202 |
LS1=IDICTS(124,IIN)+LMOX2 |
| 9203 |
INEU = 3 |
| 9204 |
CALL GETENE(E,D(LS1),LD(LS1),INEU) |
| 9205 |
C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY |
| 9206 |
C COORDINATE SYSTEM |
| 9207 |
QI=Q(ID,IIN) |
| 9208 |
CALL N2NN3N(D,LD,AWRI,KZI,ID,FM,QI,IFLG) |
| 9209 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9210 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGN3N) |
| 9211 |
RETURN |
| 9212 |
340 CONTINUE |
| 9213 |
COMM= ' COLISN; NO SECONDARY ENERGY DISTRIBUTION WAS FOUND MT-17' |
| 9214 |
ISTOP=1 |
| 9215 |
GO TO 560 |
| 9216 |
350 SIGN3N=0.0 |
| 9217 |
360 CONTINUE |
| 9218 |
C DETERMINE (N,N"A) CROSS SECTION (MT-22) |
| 9219 |
ID=11 |
| 9220 |
L1=LDICT(ID,IIN) |
| 9221 |
IF(L1.EQ.0)GO TO 400 |
| 9222 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9223 |
LEN=L1/2 |
| 9224 |
CALL TBSPLT(D(LS1),E,LEN,SIGNNA) |
| 9225 |
SUMS=SUMS+SIGNNA/SIGTNS*FSUMS |
| 9226 |
IF(R.GT.SUMS)GO TO 410 |
| 9227 |
C REACTION TYPE IS (N,N"A) |
| 9228 |
NMT22(MED)=NMT22(MED)+1 |
| 9229 |
C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE |
| 9230 |
C LABORATORY COORDINATE SYSTEM |
| 9231 |
L1=LDICT(75,IIN) |
| 9232 |
IF(L1.EQ.0)GO TO 370 |
| 9233 |
LS1=IDICTS(75,IIN)+LMOX2 |
| 9234 |
LEN=L1 |
| 9235 |
CALL CANGLE(D(LS1),LD(LS1),E,FM(1),LEN) |
| 9236 |
GO TO 380 |
| 9237 |
C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM |
| 9238 |
370 CALL GTISO(U1,V1,W1) |
| 9239 |
U=U1 |
| 9240 |
V=V1 |
| 9241 |
W=W1 |
| 9242 |
LIFLAG=1 |
| 9243 |
C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY |
| 9244 |
C COORDINATE SYSTEM |
| 9245 |
380 L1=LDICT(126,IIN) |
| 9246 |
IF(L1.EQ.0)GO TO 390 |
| 9247 |
LS1=IDICTS(126,IIN)+LMOX2 |
| 9248 |
CALL SECEGY(EX,D(LS1),E,LD(LS1)) |
| 9249 |
E=EX |
| 9250 |
IFLG=1 |
| 9251 |
C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY |
| 9252 |
C COORDINATE SYSTEM |
| 9253 |
QI=Q(ID,IIN) |
| 9254 |
LRI=22 |
| 9255 |
CALL CMLABI(D,LD,AWRI,KZI,ID,FM(1),QI,IFLG,LIFLAG,LRI) |
| 9256 |
C Re-sample if no energy determined in CMLABI |
| 9257 |
IF(IFLG.EQ.-1) GOTO 10 |
| 9258 |
UP = U |
| 9259 |
VP = V |
| 9260 |
WP = W |
| 9261 |
EP = E |
| 9262 |
AGEP = AGE |
| 9263 |
MTP = 22 |
| 9264 |
CALL STOPAR(IDNEU,NNEU) |
| 9265 |
KZ1=2 |
| 9266 |
KZ2=KZI-KZ1 |
| 9267 |
ATAR=AWRI*AN |
| 9268 |
A1=AA |
| 9269 |
A2=ATAR-AA |
| 9270 |
Z1=ZA |
| 9271 |
Z2=A2*9.31075E+08 |
| 9272 |
MT=22 |
| 9273 |
CALL NN2BOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9274 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9275 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNNA) |
| 9276 |
RETURN |
| 9277 |
390 CONTINUE |
| 9278 |
COMM=' COLISN; NO SECONDARY ENERGY DISTRIBUTION WAS FOUND MT-22' |
| 9279 |
ISTOP=1 |
| 9280 |
GO TO 560 |
| 9281 |
400 SIGNNA=0.0 |
| 9282 |
410 CONTINUE |
| 9283 |
C DETERMINE (N,2NA) CROSS SECTION (MT-24) |
| 9284 |
ID=12 |
| 9285 |
L1=LDICT(ID,IIN) |
| 9286 |
IF(L1.EQ.0)GO TO 450 |
| 9287 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9288 |
LEN=L1/2 |
| 9289 |
CALL TBSPLT(D(LS1),E,LEN,SGN2NA) |
| 9290 |
SUMS=SUMS+SGN2NA/SIGTNS*FSUMS |
| 9291 |
IF(R.GT.SUMS)GO TO 460 |
| 9292 |
C REACTION TYPE IS (N,2NA) |
| 9293 |
NMT24(MED)=NMT24(MED)+1 |
| 9294 |
C USE THE ONE NEUTRON EMISSION MODEL AND MULTIPLY THE |
| 9295 |
C WEIGHT BY TWO |
| 9296 |
C changed to 2 neutron production CZ July 30,1992 |
| 9297 |
CZ WATE=2.0*WATE |
| 9298 |
C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE |
| 9299 |
C LABORATORY COORDINATE SYSTEM |
| 9300 |
L1=LDICT(76,IIN) |
| 9301 |
IF(L1.EQ.0)GO TO 420 |
| 9302 |
LS1=IDICTS(76,IIN)+LMOX2 |
| 9303 |
LEN=L1 |
| 9304 |
CALL CANGLE(D(LS1),LD(LS1),E,FM(1),LEN) |
| 9305 |
CALL CANGLE(D(LS1),LD(LS1),E,FM(2),LEN) |
| 9306 |
GO TO 430 |
| 9307 |
C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM |
| 9308 |
420 CONTINUE |
| 9309 |
IFLG=1 |
| 9310 |
C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY |
| 9311 |
C COORDINATE SYSTEM |
| 9312 |
430 L1=LDICT(127,IIN) |
| 9313 |
IF(L1.EQ.0)GO TO 440 |
| 9314 |
LS1=IDICTS(127,IIN)+LMOX2 |
| 9315 |
INEU=2 |
| 9316 |
CALL GETENE(E,D(LS1),LD(LS1),INEU) |
| 9317 |
C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY |
| 9318 |
C COORDINATE SYSTEM |
| 9319 |
QI=Q(ID,IIN) |
| 9320 |
CALL N2NN3N(D,LD,AWRI,KZI,ID,FM,QI,IFLG) |
| 9321 |
KZ1=2 |
| 9322 |
KZ2=KZI-KZ1 |
| 9323 |
ATAR=AWRI*AN |
| 9324 |
A1=AA |
| 9325 |
A2=ATAR-AN-AA |
| 9326 |
Z1=ZA |
| 9327 |
Z2=A2*9.31075E+08 |
| 9328 |
MT=24 |
| 9329 |
CALL NN2BOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9330 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9331 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGN2NA) |
| 9332 |
RETURN |
| 9333 |
440 CONTINUE |
| 9334 |
COMM=' COLISN; NO SECONDARY ENERGY DISTRIBUTION WAS FOUND MT-24' |
| 9335 |
ISTOP=1 |
| 9336 |
GO TO 560 |
| 9337 |
450 SGN2NA=0.0 |
| 9338 |
460 CONTINUE |
| 9339 |
C DETERMINE (N,N"P) CROSS SECTION (MT-28) |
| 9340 |
ID=13 |
| 9341 |
L1=LDICT(ID,IIN) |
| 9342 |
IF(L1.EQ.0)GO TO 500 |
| 9343 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9344 |
LEN=L1/2 |
| 9345 |
CALL TBSPLT(D(LS1),E,LEN,SIGNNP) |
| 9346 |
SUMS=SUMS+SIGNNP/SIGTNS*FSUMS |
| 9347 |
IF(R.GT.SUMS)GO TO 510 |
| 9348 |
C REACTION TYPE IS (N,N"P) |
| 9349 |
NMT28(MED)=NMT28(MED)+1 |
| 9350 |
C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE |
| 9351 |
C LABORATORY COORDINATE SYSTEM |
| 9352 |
L1=LDICT(77,IIN) |
| 9353 |
IF(L1.EQ.0)GO TO 470 |
| 9354 |
LS1=IDICTS(77,IIN)+LMOX2 |
| 9355 |
LEN=L1 |
| 9356 |
CALL CANGLE(D(LS1),LD(LS1),E,FM(1),LEN) |
| 9357 |
GO TO 480 |
| 9358 |
C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM |
| 9359 |
470 CALL GTISO(U1,V1,W1) |
| 9360 |
U=U1 |
| 9361 |
V=V1 |
| 9362 |
W=W1 |
| 9363 |
LIFLAG=1 |
| 9364 |
C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY |
| 9365 |
C COORDINATE SYSTEM |
| 9366 |
480 L1=LDICT(128,IIN) |
| 9367 |
IF(L1.EQ.0)GO TO 490 |
| 9368 |
LS1=IDICTS(128,IIN)+LMOX2 |
| 9369 |
CALL SECEGY(EX,D(LS1),E,LD(LS1)) |
| 9370 |
E=EX |
| 9371 |
IFLG=1 |
| 9372 |
C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY |
| 9373 |
C COORDINATE SYSTEM |
| 9374 |
QI=Q(ID,IIN) |
| 9375 |
LRI=28 |
| 9376 |
CALL CMLABI(D,LD,AWRI,KZI,ID,FM(1),QI,IFLG,LIFLAG,LRI) |
| 9377 |
C Re-sample if no energy determined in CMLABI |
| 9378 |
IF(IFLG.EQ.-1) GOTO 10 |
| 9379 |
EP = E |
| 9380 |
UP = U |
| 9381 |
VP = V |
| 9382 |
WP = W |
| 9383 |
AGEP = AGE |
| 9384 |
MTP = 28 |
| 9385 |
CALL STOPAR(IDNEU,NNEU) |
| 9386 |
KZ1=1 |
| 9387 |
KZ2=KZI-KZ1 |
| 9388 |
ATAR=AWRI*AN |
| 9389 |
A1=AP |
| 9390 |
A2=ATAR-AP |
| 9391 |
Z1=ZP |
| 9392 |
Z2=A2*9.31075E+08 |
| 9393 |
MT=28 |
| 9394 |
CALL NN2BOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9395 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9396 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNNP) |
| 9397 |
RETURN |
| 9398 |
490 CONTINUE |
| 9399 |
COMM=' COLISN; NO SECONDARY ENERGY DISTRIBUTION FOUND FOR MT-28' |
| 9400 |
SIGREC=SIGTNS |
| 9401 |
SUMREC=SUMS |
| 9402 |
ISTOP=1 |
| 9403 |
GO TO 560 |
| 9404 |
500 SIGNNP=0.0 |
| 9405 |
510 CONTINUE |
| 9406 |
FSUMS = 1./SUMS |
| 9407 |
GO TO 550 |
| 9408 |
520 CONTINUE |
| 9409 |
C REACTION TYPE IS (N,N"A) USING LR FLAG |
| 9410 |
NMT22(MED)=NMT22(MED)+1 |
| 9411 |
SIGNNA=SGNISD |
| 9412 |
IF(ID.EQ.54)SIGNNA=SGNISC |
| 9413 |
KZ1=2 |
| 9414 |
KZ2=KZI-KZ1 |
| 9415 |
ATAR=AWRI*AN |
| 9416 |
A1=AA |
| 9417 |
A2=ATAR-AA |
| 9418 |
Z1=ZA |
| 9419 |
Z2=A2*9.31075E+08 |
| 9420 |
MT=22 |
| 9421 |
CALL LR2BOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,QLRI,ID,MT) |
| 9422 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9423 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNNA) |
| 9424 |
RETURN |
| 9425 |
530 CONTINUE |
| 9426 |
C REACTION TYPE IS (N,N"3A) USING LR FLAG |
| 9427 |
C CARBON-12 IS CURRENTLY THE ONLY ELEMENT CONTAINING MT-23 |
| 9428 |
NMT23(MED)=NMT23(MED)+1 |
| 9429 |
SGNN3A=SGNISD |
| 9430 |
IF(ID.EQ.54)SGNN3A=SGNISC |
| 9431 |
KZ1=2 |
| 9432 |
KZ2=KZI-KZ1 |
| 9433 |
ATAR=AWRI*AN |
| 9434 |
A1=AA |
| 9435 |
A2=ATAR-AA |
| 9436 |
Z1=ZA |
| 9437 |
Z2=A2*9.31075E+08 |
| 9438 |
C QBE8 IS THE MASS DIFFERENCE FOR A CARBON-ALPHA EMISSION |
| 9439 |
MT=23 |
| 9440 |
CALL LR2BOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,QBE8,ID,MT) |
| 9441 |
KZ1=2 |
| 9442 |
KZ2=KZ2-KZ1 |
| 9443 |
ATAR=AWRI*AN |
| 9444 |
A1=AA |
| 9445 |
A2=A2-AA |
| 9446 |
Z1=ZA |
| 9447 |
Z2=A2*9.31075E+08 |
| 9448 |
MT=23 |
| 9449 |
CALL LR2BOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QBE8,QLRI,ID,MT) |
| 9450 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9451 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGNN3A) |
| 9452 |
RETURN |
| 9453 |
540 CONTINUE |
| 9454 |
C REACTION TYPE IS (N,N"P) USING LR FLAG |
| 9455 |
NMT28(MED)=NMT28(MED)+1 |
| 9456 |
SIGNNP=SGNISD |
| 9457 |
IF(ID.EQ.54)SIGNNP=SGNISC |
| 9458 |
KZ1=1 |
| 9459 |
KZ2=KZI-KZ1 |
| 9460 |
ATAR=AWRI*AN |
| 9461 |
A1=AP |
| 9462 |
A2=ATAR-AP |
| 9463 |
Z1=ZP |
| 9464 |
Z2=A2*9.31075E+08 |
| 9465 |
MT=28 |
| 9466 |
CALL LR2BOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,QLRI,ID,MT) |
| 9467 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9468 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNNP) |
| 9469 |
RETURN |
| 9470 |
550 ITRY=ITRY+1 |
| 9471 |
NSEI(IIN)=NSEI(IIN)-1 |
| 9472 |
ISTOP = 1 |
| 9473 |
IF((FSUMS.GT.0.1.AND.FSUMS.LE.10.0).AND. |
| 9474 |
+ (FSUMIS.GT.0.1.AND.FSUMIS.LE.10.0)) ISTOP = 0 |
| 9475 |
IF(ISTOP.EQ.0.AND.ITRY.LE.5) GOTO 20 |
| 9476 |
C A SCATTERING REACTION WAS NOT CHOSEN |
| 9477 |
COMM=' COLISN: A SCATTERING REACTION TYPE WAS NOT CHOSEN ' |
| 9478 |
SIGREC=SIGTNS |
| 9479 |
SUMREC=SUMS |
| 9480 |
GOTO 980 |
| 9481 |
560 CONTINUE |
| 9482 |
IF(ISTOP.EQ.1)GO TO 980 |
| 9483 |
ITRY=0 |
| 9484 |
GO TO 20 |
| 9485 |
C THE REACTION TYPE IS AN ABSORPTION |
| 9486 |
570 NAEI(IIN)=NAEI(IIN)+1 |
| 9487 |
R=FLTRNF(0) |
| 9488 |
C DETERMINE THE FISSION CROSS SECTION (MT-18) |
| 9489 |
C THE TREATMENT OF THE FISSION REACTION ASSUMES THE FISSION |
| 9490 |
C CROSS SECTION IS STORED AS NUBAR*SIGF |
| 9491 |
ID=10 |
| 9492 |
L1=LDICT(ID,IIN) |
| 9493 |
IF(L1.EQ.0)GO TO 640 |
| 9494 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9495 |
LEN=L1/2 |
| 9496 |
CALL TBSPLT(D(LS1),E,LEN,SIGNF) |
| 9497 |
C DETERMINE THE AVERAGE NUMBER OF NEUTRONS EMITTED PER FISSION |
| 9498 |
C EVENT (NUBAR) |
| 9499 |
L1=LDICT(134,IIN) |
| 9500 |
IF(L1.EQ.0)GO TO 630 |
| 9501 |
LS1=IDICTS(134,IIN)+LMOX2 |
| 9502 |
LEN=L1 |
| 9503 |
CALL GETNU(D(LS1),LD(LS1),EOLD,LEN,XNU) |
| 9504 |
C EXTRACT THE FISSION CROSS SECTION FROM THE NUBAR*SIGF CROSS |
| 9505 |
C SECTION STORED IN POSITION 10 OF THE DICTIONARY |
| 9506 |
SIGNF=SIGNF/XNU |
| 9507 |
SUMA=SIGNF/SIGTNA*FSUMA |
| 9508 |
IF(R.GT.SUMA)GO TO 650 |
| 9509 |
C THE REACTION TYPE IS (N,F) |
| 9510 |
NMT18(MED)=NMT18(MED)+1 |
| 9511 |
WATE = 0.0 |
| 9512 |
C DETERMINE THE COSINE OF THE NEUTRON SCATTERING ANGLE IN THE |
| 9513 |
C LABORATORY COORDINATE SYSTEM |
| 9514 |
C changed in order to get N fission neutron CZ July 30,1992 |
| 9515 |
C INEU is poisson distributed with mean XNU |
| 9516 |
580 CALL GPOISS(XNU,INEU,1) |
| 9517 |
IF(INEU.GT.INT(4.*XNU)) GOTO 580 |
| 9518 |
C check for maximum number of neutrons emitted |
| 9519 |
IF(INEU.GT.INT(AWRI)-KZ(MED)) INEU = INT(AWRI) - KZ(MED) |
| 9520 |
IF(INEU.GT.MAXNEU) INEU = MAXNEU |
| 9521 |
L1=LDICT(74,IIN) |
| 9522 |
IF(L1.EQ.0)GO TO 600 |
| 9523 |
LS1=IDICTS(74,IIN)+LMOX2 |
| 9524 |
LEN=L1 |
| 9525 |
DO 590 KN=1,INEU |
| 9526 |
CALL CANGLE(D(LS1),LD(LS1),E,FM(KN),LEN) |
| 9527 |
590 CONTINUE |
| 9528 |
GO TO 610 |
| 9529 |
C ASSUME ISOTROPIC IN THE LABORATORY COORDINATE SYSTEM |
| 9530 |
600 CONTINUE |
| 9531 |
LIFLAG=1 |
| 9532 |
C DETERMINE THE EXIT NEUTRON ENERGY IN THE LABORATORY |
| 9533 |
C COORDINATE SYSTEM |
| 9534 |
610 L1=LDICT(125,IIN) |
| 9535 |
IF(L1.EQ.0)GO TO 620 |
| 9536 |
LS1=IDICTS(125,IIN)+LMOX2 |
| 9537 |
IF(INEU.GT.0) CALL GETENE(E,D(LS1),LD(LS1),INEU) |
| 9538 |
C DETERMINE THE EXIT NEUTRON WEIGHT FROM THE AVERAGE NUMBER |
| 9539 |
C OF NEUTRONS EMITTED PER FISSION REACTION (NU) |
| 9540 |
C changed CZ July 30,1992 |
| 9541 |
CZ WATE=WATE*XNU |
| 9542 |
C DETERMINE THE EXIT COLLISION PARAMETERS IN THE LABORATORY |
| 9543 |
C COORDINATE SYSTEM |
| 9544 |
QI=Q(ID,IIN) |
| 9545 |
IF(INEU.GT.0) CALL LABNF(D,LD,FM,AWRI,KZI,QI,LIFLAG) |
| 9546 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9547 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNF) |
| 9548 |
NPSCL(3)=NPSCL(3)+1 |
| 9549 |
CALL BANKR(D,LD,3) |
| 9550 |
RETURN |
| 9551 |
620 CONTINUE |
| 9552 |
COMM=' COLISN: NO SECONDARY ENERGY DISTRIBUTION FOUND FOR MT-18' |
| 9553 |
SIGREC=SIGNF |
| 9554 |
SUMREC=SUMA |
| 9555 |
ISTOP=1 |
| 9556 |
GO TO 970 |
| 9557 |
630 CONTINUE |
| 9558 |
COMM=' COLISN: NO NUMBER OF FISSION NEUTRON FOUND FOR MT-18' |
| 9559 |
SIGREC=SIGNF |
| 9560 |
SUMREC=SUMA |
| 9561 |
ISTOP=1 |
| 9562 |
GO TO 970 |
| 9563 |
640 SIGNF=0.0 |
| 9564 |
650 CONTINUE |
| 9565 |
C DETERMINE (N,G) CROSS SECTION (MT-102) |
| 9566 |
ID=55 |
| 9567 |
L1=LDICT(ID,IIN) |
| 9568 |
IF(L1.EQ.0)GO TO 660 |
| 9569 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9570 |
LEN=L1/2 |
| 9571 |
CALL TBSPLT(D(LS1),E,LEN,SIGNG) |
| 9572 |
SUMA=SUMA+SIGNG/SIGTNA*FSUMA |
| 9573 |
IF(R.GT.SUMA)GO TO 670 |
| 9574 |
C THE REACTION TYPE IS (N,G) |
| 9575 |
NMT102(MED)=NMT102(MED)+1 |
| 9576 |
QI=Q(ID,IIN) |
| 9577 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9578 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNG) |
| 9579 |
MT=102 |
| 9580 |
CALL NGHEVY(D,LD,KZI,AWRI,QI,MT) |
| 9581 |
WATE=0.0 |
| 9582 |
RETURN |
| 9583 |
660 SIGNG=0.0 |
| 9584 |
670 CONTINUE |
| 9585 |
C DETERMINE (N,P) CROSS SECTION (MT-103) |
| 9586 |
ID=56 |
| 9587 |
L1=LDICT(ID,IIN) |
| 9588 |
IF(L1.EQ.0)GO TO 690 |
| 9589 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9590 |
LEN=L1/2 |
| 9591 |
CALL TBSPLT(D(LS1),E,LEN,SIGNP) |
| 9592 |
SUMA=SUMA+SIGNP/SIGTNA*FSUMA |
| 9593 |
IF(R.GT.SUMA)GO TO 700 |
| 9594 |
C THE REACTION TYPE IS (N,P) |
| 9595 |
NMT103(MED)=NMT103(MED)+1 |
| 9596 |
QI=Q(ID,IIN) |
| 9597 |
KZ1=1 |
| 9598 |
KZ2=KZI-KZ1 |
| 9599 |
ATAR=AWRI*AN |
| 9600 |
A1=AP |
| 9601 |
A2=ATAR+AN-AP |
| 9602 |
Z1=ZP |
| 9603 |
Z2=A2*9.31075E+08 |
| 9604 |
MT=103 |
| 9605 |
IF(KZI.EQ.6)GO TO 680 |
| 9606 |
CALL TWOBOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9607 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9608 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNP) |
| 9609 |
WATE=0.0 |
| 9610 |
RETURN |
| 9611 |
680 CALL GRNDST(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9612 |
WATE=0.0 |
| 9613 |
RETURN |
| 9614 |
690 SIGNP=0.0 |
| 9615 |
700 CONTINUE |
| 9616 |
C DETERMINE (N,D) CROSS SECTION (MT-104) |
| 9617 |
ID=57 |
| 9618 |
L1=LDICT(ID,IIN) |
| 9619 |
IF(L1.EQ.0)GO TO 720 |
| 9620 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9621 |
LEN=L1/2 |
| 9622 |
CALL TBSPLT(D(LS1),E,LEN,SIGND) |
| 9623 |
SUMA=SUMA+SIGND/SIGTNA*FSUMA |
| 9624 |
IF(R.GT.SUMA)GO TO 730 |
| 9625 |
C THE REACTION TYPE IS (N,D) |
| 9626 |
NMT104(MED)=NMT104(MED)+1 |
| 9627 |
QI=Q(ID,IIN) |
| 9628 |
KZ1=1 |
| 9629 |
KZ2=KZI-KZ1 |
| 9630 |
ATAR=AWRI*AN |
| 9631 |
A1=AD |
| 9632 |
A2=ATAR+AN-AD |
| 9633 |
Z1=ZD |
| 9634 |
Z2=A2*9.31075E+08 |
| 9635 |
MT=104 |
| 9636 |
IF((KZI.EQ.5).OR.(KZI.EQ.6))GO TO 710 |
| 9637 |
IF((KZI.EQ.8).OR.(KZI.EQ.13))GO TO 710 |
| 9638 |
IF((KZI.EQ.14).OR.(KZI.EQ.20))GO TO 710 |
| 9639 |
CALL TWOBOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9640 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9641 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGND) |
| 9642 |
WATE=0.0 |
| 9643 |
RETURN |
| 9644 |
710 CALL GRNDST(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9645 |
WATE=0.0 |
| 9646 |
RETURN |
| 9647 |
720 SIGND=0.0 |
| 9648 |
730 CONTINUE |
| 9649 |
C DETERMINE (N,T) CROSS SECTION (MT-105) |
| 9650 |
ID=58 |
| 9651 |
L1=LDICT(ID,IIN) |
| 9652 |
IF(L1.EQ.0)GO TO 750 |
| 9653 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9654 |
LEN=L1/2 |
| 9655 |
CALL TBSPLT(D(LS1),E,LEN,SIGNT) |
| 9656 |
SUMA=SUMA+SIGNT/SIGTNA*FSUMA |
| 9657 |
IF(R.GT.SUMA)GO TO 760 |
| 9658 |
C THE REACTION TYPE IS (N,T) |
| 9659 |
NMT105(MED)=NMT105(MED)+1 |
| 9660 |
QI=Q(ID,IIN) |
| 9661 |
KZ1=1 |
| 9662 |
KZ2=KZI-KZ1 |
| 9663 |
ATAR=AWRI*AN |
| 9664 |
A1=AT |
| 9665 |
A2=ATAR+AN-AT |
| 9666 |
Z1=ZT |
| 9667 |
Z2=A2*9.31075E+08 |
| 9668 |
MT=105 |
| 9669 |
IF((KZI.EQ.5).OR.(KZI.EQ.13))GO TO 740 |
| 9670 |
IF(KZI.EQ.20)GO TO 740 |
| 9671 |
CALL TWOBOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9672 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9673 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNT) |
| 9674 |
WATE=0.0 |
| 9675 |
RETURN |
| 9676 |
740 CALL GRNDST(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9677 |
WATE=0.0 |
| 9678 |
RETURN |
| 9679 |
750 SIGNT=0.0 |
| 9680 |
760 CONTINUE |
| 9681 |
C DETERMINE (N,3HE) CROSS SECTION (MT-106) |
| 9682 |
ID=59 |
| 9683 |
L1=LDICT(ID,IIN) |
| 9684 |
IF(L1.EQ.0)GO TO 780 |
| 9685 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9686 |
LEN=L1/2 |
| 9687 |
CALL TBSPLT(D(LS1),E,LEN,SGN3HE) |
| 9688 |
SUMA=SUMA+SGN3HE/SIGTNA*FSUMA |
| 9689 |
IF(R.GT.SUMA)GO TO 790 |
| 9690 |
C THE REACTION TYPE IS (N,3HE) |
| 9691 |
NMT106(MED)=NMT106(MED)+1 |
| 9692 |
QI=Q(ID,IIN) |
| 9693 |
KZ1=2 |
| 9694 |
KZ2=KZI-KZ1 |
| 9695 |
ATAR=AWRI*AN |
| 9696 |
A1=AHE3 |
| 9697 |
A2=ATAR+AN-AHE3 |
| 9698 |
Z1=ZHE3 |
| 9699 |
Z2=A2*9.31075E+08 |
| 9700 |
MT=106 |
| 9701 |
IF(KZI.EQ.20)GO TO 770 |
| 9702 |
CALL TWOBOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9703 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9704 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGN3HE) |
| 9705 |
WATE=0.0 |
| 9706 |
RETURN |
| 9707 |
770 CALL GRNDST(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9708 |
WATE=0.0 |
| 9709 |
RETURN |
| 9710 |
780 SGN3HE=0.0 |
| 9711 |
790 CONTINUE |
| 9712 |
C DETERMINE (N,A) CROSS SECTION (MT-107) |
| 9713 |
ID=60 |
| 9714 |
L1=LDICT(ID,IIN) |
| 9715 |
IF(L1.EQ.0)GO TO 810 |
| 9716 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9717 |
LEN=L1/2 |
| 9718 |
CALL TBSPLT(D(LS1),E,LEN,SIGNA) |
| 9719 |
SUMA=SUMA+SIGNA/SIGTNA*FSUMA |
| 9720 |
IF(R.GT.SUMA)GO TO 820 |
| 9721 |
C THE REACTION TYPE IS (N,A) |
| 9722 |
NMT107(MED)=NMT107(MED)+1 |
| 9723 |
QI=Q(ID,IIN) |
| 9724 |
KZ1=2 |
| 9725 |
KZ2=KZI-KZ1 |
| 9726 |
ATAR=AWRI*AN |
| 9727 |
A1=AA |
| 9728 |
A2=ATAR+AN-AA |
| 9729 |
Z1=ZA |
| 9730 |
Z2=A2*9.31075E+08 |
| 9731 |
MT=107 |
| 9732 |
IF((KZI.EQ.6).OR.(KZI.EQ.13))GO TO 800 |
| 9733 |
CALL TWOBOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9734 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9735 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNA) |
| 9736 |
WATE=0.0 |
| 9737 |
RETURN |
| 9738 |
800 CALL GRNDST(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9739 |
WATE=0.0 |
| 9740 |
RETURN |
| 9741 |
810 SIGNA=0.0 |
| 9742 |
820 CONTINUE |
| 9743 |
C DETERMINE (N,2A) CROSS SECTION (MT-108) |
| 9744 |
ID=61 |
| 9745 |
L1=LDICT(ID,IIN) |
| 9746 |
IF(L1.EQ.0)GO TO 840 |
| 9747 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9748 |
LEN=L1/2 |
| 9749 |
CALL TBSPLT(D(LS1),E,LEN,SIGN2A) |
| 9750 |
SUMA=SUMA+SIGN2A/SIGTNA*FSUMA |
| 9751 |
IF(R.GT.SUMA)GO TO 850 |
| 9752 |
C THE REACTION TYPE IS (N,2A) |
| 9753 |
NMT108(MED)=NMT108(MED)+1 |
| 9754 |
QI=Q(ID,IIN) |
| 9755 |
KZ1=2 |
| 9756 |
KZ2=KZI-2*KZ1 |
| 9757 |
ATAR=AWRI*AN |
| 9758 |
A1=AA |
| 9759 |
A2=ATAR+AN-AA |
| 9760 |
Z1=ZA |
| 9761 |
Z2=A2*9.31075E+08 |
| 9762 |
MT=108 |
| 9763 |
C USE THE ONE PARTICLE EMISSION MODEL AND MULTIPLY THE |
| 9764 |
C WEIGHT BY TWO |
| 9765 |
IF((KZI.EQ.7).OR.(KZI.EQ.20))GO TO 830 |
| 9766 |
CALL TWOBOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9767 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9768 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGN2A) |
| 9769 |
WATE=0.0 |
| 9770 |
RETURN |
| 9771 |
830 CALL GRNDST(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9772 |
WATE=0.0 |
| 9773 |
RETURN |
| 9774 |
840 SIGN2A=0.0 |
| 9775 |
850 CONTINUE |
| 9776 |
C DETERMINE (N,3A) CROSS SECTION (MT-109) |
| 9777 |
ID=62 |
| 9778 |
L1=LDICT(ID,IIN) |
| 9779 |
IF(L1.EQ.0)GO TO 860 |
| 9780 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9781 |
LEN=L1/2 |
| 9782 |
CALL TBSPLT(D(LS1),E,LEN,SIGN3A) |
| 9783 |
SUMA=SUMA+SIGN3A/SIGTNA*FSUMA |
| 9784 |
IF(R.GT.SUMA)GO TO 870 |
| 9785 |
C THE REACTION TYPE IS (N,3A) |
| 9786 |
NMT109(MED)=NMT109(MED)+1 |
| 9787 |
QI=Q(ID,IIN) |
| 9788 |
KZ1=2 |
| 9789 |
KZ2=KZI-3*KZ1 |
| 9790 |
ATAR=AWRI*AN |
| 9791 |
A1=AA |
| 9792 |
A2=ATAR+AN-AA |
| 9793 |
Z1=ZA |
| 9794 |
Z2=A2*9.31075E+08 |
| 9795 |
MT=109 |
| 9796 |
C USE THE ONE PARTICLE EMISSION MODEL AND MULTIPLY THE |
| 9797 |
C WEIGHT BY THREE |
| 9798 |
CALL TWOBOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9799 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9800 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGN3A) |
| 9801 |
WATE=0.0 |
| 9802 |
RETURN |
| 9803 |
860 SIGN3A=0.0 |
| 9804 |
870 CONTINUE |
| 9805 |
C DETERMINE (N,2P) CROSS SECTION (MT-111) |
| 9806 |
ID=63 |
| 9807 |
L1=LDICT(ID,IIN) |
| 9808 |
IF(L1.EQ.0)GO TO 890 |
| 9809 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9810 |
LEN=L1/2 |
| 9811 |
CALL TBSPLT(D(LS1),E,LEN,SIGN2P) |
| 9812 |
SUMA=SUMA+SIGN2P/SIGTNA*FSUMA |
| 9813 |
IF(R.GT.SUMA)GO TO 900 |
| 9814 |
C THE REACTION TYPE IS (N,2P) |
| 9815 |
NMT111(MED)=NMT111(MED)+1 |
| 9816 |
QI=Q(ID,IIN) |
| 9817 |
KZ1=1 |
| 9818 |
KZ2=KZI-2*KZ1 |
| 9819 |
ATAR=AWRI*AN |
| 9820 |
A1=AP |
| 9821 |
A2=ATAR+AN-AP |
| 9822 |
Z1=ZP |
| 9823 |
Z2=A2*9.31075E+08 |
| 9824 |
MT=111 |
| 9825 |
C USE THE ONE PARTICLE EMISSION MODEL AND MULTIPLY THE |
| 9826 |
C WEIGHT BY TWO |
| 9827 |
IF(KZI.EQ.20)GO TO 880 |
| 9828 |
CALL TWOBOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9829 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9830 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGN2P) |
| 9831 |
WATE=0.0 |
| 9832 |
RETURN |
| 9833 |
880 CALL GRNDST(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,QI,MT) |
| 9834 |
WATE=0.0 |
| 9835 |
RETURN |
| 9836 |
890 SIGN2P=0.0 |
| 9837 |
900 CONTINUE |
| 9838 |
C DETERMINE (N,PA) CROSS SECTION (MT-112) |
| 9839 |
ID=64 |
| 9840 |
L1=LDICT(ID,IIN) |
| 9841 |
IF(L1.EQ.0)GO TO 910 |
| 9842 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9843 |
LEN=L1/2 |
| 9844 |
CALL TBSPLT(D(LS1),E,LEN,SIGNPA) |
| 9845 |
SUMA=SUMA+SIGNPA/SIGTNA*FSUMA |
| 9846 |
IF(R.GT.SUMA)GO TO 920 |
| 9847 |
C THE REACTION TYPE IS (N,PA) |
| 9848 |
NMT112(MED)=NMT112(MED)+1 |
| 9849 |
QI=Q(ID,IIN) |
| 9850 |
KZ1=1 |
| 9851 |
KZ2=2 |
| 9852 |
KZ3=KZI-KZ1-KZ2 |
| 9853 |
ATAR=AWRI*AN |
| 9854 |
A1=AP |
| 9855 |
A2=AA |
| 9856 |
A3=ATAR+AN-A1 |
| 9857 |
Z1=ZP |
| 9858 |
Z2=ZA |
| 9859 |
Z3=A3*9.31075E+08 |
| 9860 |
MT=112 |
| 9861 |
CZ July 30,1992 Three-Body process added ---- |
| 9862 |
CALL TREBOD(D,LD,KZ1,KZ2,KZ3,A1,A2,A3,Z1,Z2,Z3,ATAR,QI,MT) |
| 9863 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9864 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGNPA) |
| 9865 |
WATE=0.0 |
| 9866 |
RETURN |
| 9867 |
910 SIGNPA=0.0 |
| 9868 |
920 CONTINUE |
| 9869 |
C DETERMINE (N,T2A) CROSS SECTION (MT-113) |
| 9870 |
ID=65 |
| 9871 |
L1=LDICT(ID,IIN) |
| 9872 |
IF(L1.EQ.0)GO TO 930 |
| 9873 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9874 |
LEN=L1/2 |
| 9875 |
CALL TBSPLT(D(LS1),E,LEN,SGNT2A) |
| 9876 |
SUMA=SUMA+SGNT2A/SIGTNA*FSUMA |
| 9877 |
IF(R.GT.SUMA)GO TO 940 |
| 9878 |
C THE REACTION TYPE IS (N,T2A) |
| 9879 |
NMT113(MED)=NMT113(MED)+1 |
| 9880 |
QI=Q(ID,IIN) |
| 9881 |
KZ1=1 |
| 9882 |
KZ2=2 |
| 9883 |
KZ3=KZI-KZ1-2*KZ2 |
| 9884 |
ATAR=AWRI*AN |
| 9885 |
A1=AT |
| 9886 |
A2=AA |
| 9887 |
A3=ATAR+AN-A1 |
| 9888 |
Z1=ZT |
| 9889 |
Z2=ZA |
| 9890 |
Z3=A3*9.31075E+08 |
| 9891 |
MT=113 |
| 9892 |
CZ July 30,1992 Three-Body process added ---- |
| 9893 |
CALL TREBOD(D,LD,KZ1,KZ2,KZ3,A1,A2,A3,Z1,Z2,Z3,ATAR,QI,MT) |
| 9894 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9895 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGNT2A) |
| 9896 |
WATE=0.0 |
| 9897 |
RETURN |
| 9898 |
930 SGNT2A=0.0 |
| 9899 |
940 CONTINUE |
| 9900 |
C DETERMINE (N,D2A) CROSS SECTION (MT-114) |
| 9901 |
ID=66 |
| 9902 |
L1=LDICT(ID,IIN) |
| 9903 |
IF(L1.EQ.0)GO TO 950 |
| 9904 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 9905 |
LEN=L1/2 |
| 9906 |
CALL TBSPLT(D(LS1),E,LEN,SGND2A) |
| 9907 |
SUMA=SUMA+SGND2A/SIGTNA*FSUMA |
| 9908 |
IF(R.GT.SUMA)GO TO 960 |
| 9909 |
C THE REACTION TYPE IS (N,D2A) |
| 9910 |
NMT114(MED)=NMT114(MED)+1 |
| 9911 |
QI=Q(ID,IIN) |
| 9912 |
KZ1=1 |
| 9913 |
KZ2=2 |
| 9914 |
KZ3=KZI-KZ1-2*KZ2 |
| 9915 |
ATAR=AWRI*AN |
| 9916 |
A1=AD |
| 9917 |
A2=AA |
| 9918 |
A3=ATAR+AN-A1 |
| 9919 |
Z1=ZD |
| 9920 |
Z2=ZA |
| 9921 |
Z3=A3*9.31075E+08 |
| 9922 |
MT=114 |
| 9923 |
CZ July 30,1992 Three-Body process added ---- |
| 9924 |
CALL TREBOD(D,LD,KZ1,KZ2,KZ3,A1,A2,A3,Z1,Z2,Z3,ATAR,QI,MT) |
| 9925 |
CALL PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR, |
| 9926 |
+IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SGND2A) |
| 9927 |
WATE=0.0 |
| 9928 |
RETURN |
| 9929 |
950 SGND2A=0.0 |
| 9930 |
960 CONTINUE |
| 9931 |
FSUMA = 1./SUMA |
| 9932 |
ITRY=ITRY+1 |
| 9933 |
ISTOP=1 |
| 9934 |
IF(FSUMA.GT.0.1.AND.FSUMA.LE.10.0) ISTOP=0 |
| 9935 |
NAEI(IIN)=NAEI(IIN)-1 |
| 9936 |
IF(ISTOP.EQ.0.AND.ITRY.LE.5)GO TO 20 |
| 9937 |
C AN ABSORPTION REACTION WAS NOT CHOSEN |
| 9938 |
COMM=' COLISN:AN ABSORPTION REACTION TYPE WAS NOT CHOSEN ' |
| 9939 |
SIGREC = SIGTNA |
| 9940 |
SUMREC = SUMA |
| 9941 |
GOTO 980 |
| 9942 |
970 CONTINUE |
| 9943 |
IF(ISTOP.EQ.1)GO TO 980 |
| 9944 |
ITRY=0 |
| 9945 |
GO TO 20 |
| 9946 |
980 CONTINUE |
| 9947 |
WRITE(IOUT,'(A80,/,I5,F7.1,I4,/,G18.7,I5,3G10.4)') COMM, |
| 9948 |
+ NMED,AWR(IIN),KZ(IIM), |
| 9949 |
+ E,MT, |
| 9950 |
+ SIGT,SIGREC,SUMREC |
| 9951 |
RETURN |
| 9952 |
END |
| 9953 |
*CMZ : 0.90/00 20/07/92 14.28.14 by Christian Zeitnitz |
| 9954 |
*-- Author : |
| 9955 |
SUBROUTINE CTERP(X1,X2,X,Y1,Y2,Y) |
| 9956 |
C THIS ROUTINE PERFORMS LINEAR INTERPOLATION |
| 9957 |
Y=Y2-(X2-X)*(Y2-Y1)/(X2-X1) |
| 9958 |
RETURN |
| 9959 |
END |
| 9960 |
*CMZ : 1.04/00 02/02/95 09.21.40 by Christian Zeitnitz |
| 9961 |
*-- Author : |
| 9962 |
SUBROUTINE EVAPLR(E,Q,SQ,ATAR,CB,EX) |
| 9963 |
C THIS ROUTINE SAMPLES AN EXIT ENERGY FROM AN |
| 9964 |
C EVAPORATION SPECTRUM FOR AN LR-FLAG (N,N-PRIME X) REACTION |
| 9965 |
#include "minput.inc" |
| 9966 |
*KEND. |
| 9967 |
SAVE |
| 9968 |
C CONVERT THE COULOMB BARRIER (CB) TO UNITS OF EV |
| 9969 |
CB=CB*1.00E+06 |
| 9970 |
C SET THE EXCITATION ENERGY (Q) TO ITS ABSOLUTE VALUE |
| 9971 |
QA=ABS(Q) |
| 9972 |
C CALCULATE THE MAXIMUM ENERGY AVAILABLE |
| 9973 |
CBI=CB |
| 9974 |
EMAX=QA+SQ-CB |
| 9975 |
IF(EMAX.GT.0.0)GO TO 10 |
| 9976 |
CB=0.5*CB |
| 9977 |
EMAX=QA+SQ-CB |
| 9978 |
IF(EMAX.GT.0.0)GO TO 10 |
| 9979 |
CB=0.0 |
| 9980 |
EMAX=QA+SQ-CB |
| 9981 |
IF(EMAX.GT.0.0)GO TO 10 |
| 9982 |
WRITE(IOUT,10000)E,EMAX,QA,SQ,CBI |
| 9983 |
10000 FORMAT(' MICAP: NEGATIVE MAXIMUM ENERGY CALCULATED IN ROUTINE ', |
| 9984 |
1'EVAPLR --- INDICATING PROBABLE CROSS SECTION ERROR ALLOWING ', |
| 9985 |
2'THE REACTION TO OCCUR',/,10X,'E,EMAX,QA,SQ,CB=',1P5E13.5) |
| 9986 |
WRITE(6,*) ' CALOR: ERROR in EVAPLR ====> STOP ' |
| 9987 |
STOP |
| 9988 |
C CALCULATE THE NUCLEAR TEMPERATURE (THETA) |
| 9989 |
10 THETA=4.0161E+03*(SQRT(QA+SQ-CB)/(ATAR**0.8333333)) |
| 9990 |
C SELECT THE EXIT ENERGY FROM AN EVAPORATION SPECTRUM |
| 9991 |
20 R1=FLTRNF(0) |
| 9992 |
R2=FLTRNF(0) |
| 9993 |
W=-ALOG(R1*R2) |
| 9994 |
EX=THETA*W |
| 9995 |
IF(EX.LE.EMAX)RETURN |
| 9996 |
C RESAMPLE 75% OF THE TIME IF EX IS GREATER THAN EMAX |
| 9997 |
R=FLTRNF(0) |
| 9998 |
IF(R.LE.0.75)GO TO 20 |
| 9999 |
EX=EMAX |
| 10000 |
RETURN |
| 10001 |
END |
| 10002 |
*CMZ : 0.90/09 03/11/92 15.18.49 by Christian Zeitnitz |
| 10003 |
*-- Author : |
| 10004 |
C********************************************************************* |
| 10005 |
FUNCTION FISRNF(A,B) |
| 10006 |
C********************************************************************* |
| 10007 |
C Sample secondary fission neutron energy from Watt spectrum |
| 10008 |
C taken from ORNL/TM-7631 |
| 10009 |
C CZ 3/11/92 |
| 10010 |
DIMENSION RNDM(3) |
| 10011 |
C |
| 10012 |
CALL GRNDM(RNDM,3) |
| 10013 |
Z=SQRT(-ALOG(RNDM(1))) |
| 10014 |
S=6.28319*RNDM(2) |
| 10015 |
ALOGR3=ALOG(RNDM(3)) |
| 10016 |
X=SQRT(A*B)/2. |
| 10017 |
E1=A*((Z*COS(S)+X)**2-ALOGR3) |
| 10018 |
C-- E2=A*((Z*SIN(S)+X)**2-ALOGR3) |
| 10019 |
C distribution of E1 and E2 are identical |
| 10020 |
FISRNF = E1 |
| 10021 |
RETURN |
| 10022 |
END |
| 10023 |
*CMZ : 1.05/03 27/06/2001 17.54.33 by Christian Zeitnitz |
| 10024 |
*-- Author : |
| 10025 |
C********************************************************************* |
| 10026 |
FUNCTION FLTRNF(IX) |
| 10027 |
C********************************************************************* |
| 10028 |
#include "crandm.inc" |
| 10029 |
*KEND. |
| 10030 |
FLTRNF = RANDC(ISEED) |
| 10031 |
RETURN |
| 10032 |
END |
| 10033 |
*CMZ : 1.05/03 27/06/2001 17.56.54 by Christian Zeitnitz |
| 10034 |
*-- Author : Christian Zeitnitz 23/10/92 |
| 10035 |
SUBROUTINE GETENE(EN,D1,LD2,N) |
| 10036 |
C sample N times secondary energy distribution and |
| 10037 |
C store in ENE(*) |
| 10038 |
#include "mconst.inc" |
| 10039 |
#include "mnutrn.inc" |
| 10040 |
*KEND. |
| 10041 |
C |
| 10042 |
DIMENSION D1(*),LD2(*) |
| 10043 |
C |
| 10044 |
DO 10 I=1,N |
| 10045 |
CALL SECEGY(EX,D1,EN,LD2) |
| 10046 |
ENE(I) = EX |
| 10047 |
10 CONTINUE |
| 10048 |
RETURN |
| 10049 |
END |
| 10050 |
|
| 10051 |
*CMZ : 1.01/04 10/06/93 14.43.47 by Christian Zeitnitz |
| 10052 |
*-- Author : |
| 10053 |
SUBROUTINE GETNU(D,LD,E,LEN,XNU) |
| 10054 |
C THIS ROUTINE SELECTS THE AVERAGE NUMBER OF NEUTRONS |
| 10055 |
C BORN FROM A FISSION REACTION (I.E. NU-BAR) |
| 10056 |
#include "minput.inc" |
| 10057 |
*KEND. |
| 10058 |
DIMENSION D(*),LD(*),C(4) |
| 10059 |
SAVE |
| 10060 |
IP=1 |
| 10061 |
XNU=0.0 |
| 10062 |
LNU=LD(IP) |
| 10063 |
IP=IP+1 |
| 10064 |
IF(LNU.NE.1)GO TO 30 |
| 10065 |
C POLYNOMIAL REPRESENTATION USED TO SPECIFY NU-BAR |
| 10066 |
C INITIALIZE THE POLYNOMIAL COEFFICIENTS TO ZERO |
| 10067 |
DO 10 I=1,4 |
| 10068 |
C(I)=0.0 |
| 10069 |
10 CONTINUE |
| 10070 |
NC=LD(IP) |
| 10071 |
DO 20 I=1,NC |
| 10072 |
C(I)=D(IP+I) |
| 10073 |
20 CONTINUE |
| 10074 |
C CALCULATE NU-BAR USING POLYNOMIAL COEFFICIENTS |
| 10075 |
XNU=C(1)+C(2)*E+C(3)*(E**2)+C(4)*(E**3) |
| 10076 |
RETURN |
| 10077 |
C TABULATED DATA USED TO SPECIFY NU-BAR |
| 10078 |
C CURRENT ENDF/B DATA (VERSION V) ALLOWS ONLY ONE |
| 10079 |
C INTERPOLATION RANGE (NR) AND ONLY LINEAR-LINEAR |
| 10080 |
C INTERPOLABLE DATA (INT=2) |
| 10081 |
30 IF(LNU.NE.2)GO TO 40 |
| 10082 |
NR=LD(IP) |
| 10083 |
NP=LD(IP+1) |
| 10084 |
IP=IP+2*NR+2 |
| 10085 |
C SELECT NU-BAR FROM THE TABULATED DATA |
| 10086 |
C LINEAR-LINEAR INTERPOLATION IS ASSUMED AT THIS POINT |
| 10087 |
CALL TBSPLT(D(IP),E,NP,XNU) |
| 10088 |
RETURN |
| 10089 |
40 WRITE(IOUT,10000)LNU |
| 10090 |
10000 FORMAT(' MICAP: ERROR IN ROUTINE GETNU; LNU=',I3) |
| 10091 |
WRITE(6,*) ' CALOR: ERROR in GETNU ====> STOP' |
| 10092 |
STOP |
| 10093 |
END |
| 10094 |
*CMZ : 1.01/04 10/06/93 14.43.48 by Christian Zeitnitz |
| 10095 |
*-- Author : Christian Zeitnitz 03/08/92 |
| 10096 |
SUBROUTINE GETPAR(ID,N,IERR) |
| 10097 |
C retrieve particle from MPSTOR common |
| 10098 |
#include "mconst.inc" |
| 10099 |
#include "mpstor.inc" |
| 10100 |
#include "minput.inc" |
| 10101 |
*KEND. |
| 10102 |
IERR = 0 |
| 10103 |
NN = 0 |
| 10104 |
NS = 1 |
| 10105 |
10 CONTINUE |
| 10106 |
IF(IDN(NS).EQ.ID) NN = NN + 1 |
| 10107 |
IF(N.EQ.NN) GOTO 20 |
| 10108 |
NS = NS + 1 |
| 10109 |
IF(NS.GT.NPSTOR) THEN |
| 10110 |
WRITE(IOUT,'('' MICAP: Cant retrieve particle no. '',I3, ' |
| 10111 |
+ //' '' of type '',I3,''; End of data '')') N,ID |
| 10112 |
IERR = 1 |
| 10113 |
RETURN |
| 10114 |
ENDIF |
| 10115 |
GOTO 10 |
| 10116 |
20 CONTINUE |
| 10117 |
EP = EN(NS) |
| 10118 |
UP = UN(NS) |
| 10119 |
VP = VN(NS) |
| 10120 |
WP = WN(NS) |
| 10121 |
AMP = AMN(NS) |
| 10122 |
ZMP = ZMN(NS) |
| 10123 |
AGEP = AGEN(NS) |
| 10124 |
MTP = MTN(NS) |
| 10125 |
RETURN |
| 10126 |
END |
| 10127 |
*CMZ : 1.01/16 18/11/93 09.19.55 by Christian Zeitnitz |
| 10128 |
*-- Author : |
| 10129 |
SUBROUTINE GRNDST(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,Q,MT) |
| 10130 |
C THIS ROUTINE CALCULATES THE EXIT ENERGIES AND DIRECTIONAL |
| 10131 |
C COSINES FOR THE CHARGED PARTICLE AND RECOIL NUCLEUS FOR |
| 10132 |
C A GROUND STATE TWO-BODY REACTION USING CLASSICAL KINEMATICS |
| 10133 |
C AND A MOMEMTUM BALANCE. IT ALSO SETS ALL EXIT PARAMETERS FOR |
| 10134 |
C THE COLLISION PRODUCTS AND STORES THEM IN THE RECOIL BANK. |
| 10135 |
#include "minput.inc" |
| 10136 |
#include "mconst.inc" |
| 10137 |
#include "mnutrn.inc" |
| 10138 |
#include "mrecoi.inc" |
| 10139 |
#include "mapoll.inc" |
| 10140 |
#include "mmass.inc" |
| 10141 |
#include "mpstor.inc" |
| 10142 |
*KEND. |
| 10143 |
DIMENSION D(*),LD(*) |
| 10144 |
SAVE |
| 10145 |
NPN = 1 |
| 10146 |
IF(MT.EQ.108) NPN = 2 |
| 10147 |
IF(MT.EQ.109) NPN = 3 |
| 10148 |
IF(MT.EQ.111) NPN = 2 |
| 10149 |
C CALCULATE THE CONSTANTS USED IN THE KINEMATIIC EQUATIONS |
| 10150 |
ZATAR=ATAR*9.31075E+08 |
| 10151 |
PXO = 0.0 |
| 10152 |
PYO = 0.0 |
| 10153 |
PZO = 0.0 |
| 10154 |
C loop over emmited particles |
| 10155 |
DO 40 NP=1,NPN |
| 10156 |
C ASSUME ISOTROPIC CHARGED PARTICLE EMISSION IN THE CENTER |
| 10157 |
C OF MASS COORDINATE SYSTEM |
| 10158 |
R=FLTRNF(0) |
| 10159 |
FM=2.0*R-1.0 |
| 10160 |
C FOR A GROUND STATE REACTION THE RECOIL MASS IS KNOWN EXACTLY |
| 10161 |
Z2=ZN+ZATAR-FLOAT(NP)*Z1-Q |
| 10162 |
A2=Z2/9.31075E+08 |
| 10163 |
DENOM=(AN+ATAR)*(A1*FLOAT(NP)+A2) |
| 10164 |
ERATIO=EOLD/(EOLD+Q) |
| 10165 |
AC=((AN*A2)/DENOM)*ERATIO |
| 10166 |
BC=((AN*A1)/DENOM)*ERATIO |
| 10167 |
CC=((ATAR*A1)/DENOM)*(1.0+(AN*Q)/(ATAR*(EOLD+Q))) |
| 10168 |
DC=((ATAR*A2)/DENOM)*(1.0+(AN*Q)/(ATAR*(EOLD+Q))) |
| 10169 |
C CALCULATE THE CHARGED PARTICLE AND RECOIL NUCLEUS IN THE |
| 10170 |
C LABORATORY COORDINATE SYSTEM |
| 10171 |
E1=(EOLD+Q)*(BC+DC+(2.0*SQRT(AC*CC))*FM) |
| 10172 |
E2=(EOLD+Q)*(AC+CC-(2.0*SQRT(AC*CC))*FM) |
| 10173 |
C CALCULATE THE CHARGED PARTICLE ENERGY AND VELOCITY IN THE |
| 10174 |
C CENTER OF MASS COORDINATE SYSTEM |
| 10175 |
E1CM=(Z2/(Z1+Z2))*((ZATAR/(ZN+ZATAR))*EOLD+Q) |
| 10176 |
V1CM=SQRT((2.0*E1CM)/Z1) |
| 10177 |
C CALCULATE THE VELOCITY OF THE CENTER OF MASS |
| 10178 |
VCM=SQRT(2.0*ZN*EOLD)/(ZN+ZATAR) |
| 10179 |
C CONVERT THE COSINE OF THE SCATTERING ANGLE IN THE CENTER OF |
| 10180 |
C MASS COORDINATE SYSTEM TO THE LABORATORY COORDINATE SYSTEM |
| 10181 |
FM=(V1CM*FM+VCM)/(SQRT(((V1CM*FM+VCM)**2)+ ((V1CM*(1.0-FM**2)) |
| 10182 |
+ **2))) |
| 10183 |
C CALCULATE THE CHARGED PARTICLE EXIT DIRECTIONAL COSINES |
| 10184 |
SINPSI=SQRT(1.0-FM**2) |
| 10185 |
CALL AZIRN(SINETA,COSETA) |
| 10186 |
STHETA=1.0-UOLD**2 |
| 10187 |
IF(STHETA)20,20,10 |
| 10188 |
10 STHETA=SQRT(STHETA) |
| 10189 |
COSPHI=VOLD/STHETA |
| 10190 |
SINPHI=WOLD/STHETA |
| 10191 |
GO TO 30 |
| 10192 |
20 COSPHI=1.0 |
| 10193 |
SINPHI=0.0 |
| 10194 |
STHETA=0.0 |
| 10195 |
30 U1=UOLD*FM-COSETA*SINPSI*STHETA |
| 10196 |
V1=VOLD*FM+UOLD*COSPHI*COSETA*SINPSI-SINPHI*SINPSI*SINETA |
| 10197 |
W1=WOLD*FM+UOLD*SINPHI*COSETA*SINPSI+COSPHI*SINPSI*SINETA |
| 10198 |
S=1.0/SQRT(U1**2+V1**2+W1**2) |
| 10199 |
U1=U1*S |
| 10200 |
V1=V1*S |
| 10201 |
W1=W1*S |
| 10202 |
PPO = SQRT(2.0*Z1*E1) |
| 10203 |
PXO = PXO + U1*PPO |
| 10204 |
PYO = PYO + V1*PPO |
| 10205 |
PZO = PZO + W1*PPO |
| 10206 |
C CALCULATE AND SET THE CHARGED PARTICLE EXIT PARAMETERS |
| 10207 |
XR=X |
| 10208 |
YR=Y |
| 10209 |
ZR=Z |
| 10210 |
WATER=WTBC |
| 10211 |
NZR=KZ1 |
| 10212 |
AGER=AGE |
| 10213 |
NCOLR=NCOL |
| 10214 |
MTNR=MT |
| 10215 |
AR=A1 |
| 10216 |
ENIR=EOLD |
| 10217 |
UNIR=UOLD |
| 10218 |
VNIR=VOLD |
| 10219 |
WNIR=WOLD |
| 10220 |
ENOR=0.0 |
| 10221 |
UNOR=0.0 |
| 10222 |
VNOR=0.0 |
| 10223 |
WNOR=0.0 |
| 10224 |
WTNR=0.0 |
| 10225 |
QR=Q |
| 10226 |
UR=U1 |
| 10227 |
VR=V1 |
| 10228 |
WR=W1 |
| 10229 |
ER=E1 |
| 10230 |
C STORE THE CHARGED PARTICLE IN THE RECOIL BANK |
| 10231 |
EP = ER |
| 10232 |
UP = UR |
| 10233 |
VP = VR |
| 10234 |
WP = WR |
| 10235 |
AMP = AR |
| 10236 |
ZMP = FLOAT(NZR) |
| 10237 |
AGEP = AGE |
| 10238 |
MTP = MT |
| 10239 |
CALL STOPAR(IDHEVY,NHEVY) |
| 10240 |
40 CONTINUE |
| 10241 |
C CALCULATE THE TOTAL MOMENTUM BEFORE THE COLLISION |
| 10242 |
C NEUTRON MOMENTUM BEFORE COLLISION (PI) EQUALS TOTAL MOMENTUM |
| 10243 |
PI=SQRT(2.0*ZN*EOLD) |
| 10244 |
C CALCULATE THE DIRECTIONAL MOMENTUM OF THE RECOIL NUCLEUS |
| 10245 |
PRX=PI*UOLD-PXO |
| 10246 |
PRY=PI*VOLD-PYO |
| 10247 |
PRZ=PI*WOLD-PZO |
| 10248 |
C CALCULATE THE TOTAL MOMENTUM OF THE RECOIL NUCLEUS |
| 10249 |
PR=SQRT(PRX**2+PRY**2+PRZ**2) |
| 10250 |
C CALCULATE THE RECOIL NUCLEUS DIRECTIONAL COSINES |
| 10251 |
U2=PRX/PR |
| 10252 |
V2=PRY/PR |
| 10253 |
W2=PRZ/PR |
| 10254 |
C CALCULATE THE RECOIL NUCLEUS EXIT ENERGY |
| 10255 |
XM = A2 * 931.075E6 |
| 10256 |
E2 = SQRT(PR**2+XM**2) - XM |
| 10257 |
C CALCULATE AND SET THE CHARGED PARTICLE EXIT PARAMETERS |
| 10258 |
XR=X |
| 10259 |
YR=Y |
| 10260 |
ZR=Z |
| 10261 |
WATER=WTBC |
| 10262 |
NZR=KZ2 |
| 10263 |
AGER=AGE |
| 10264 |
NCOLR=NCOL |
| 10265 |
MTNR=MT |
| 10266 |
AR=A2 |
| 10267 |
ENIR=EOLD |
| 10268 |
UNIR=UOLD |
| 10269 |
VNIR=VOLD |
| 10270 |
WNIR=WOLD |
| 10271 |
ENOR=0.0 |
| 10272 |
UNOR=0.0 |
| 10273 |
VNOR=0.0 |
| 10274 |
WNOR=0.0 |
| 10275 |
WTNR=0.0 |
| 10276 |
QR=Q |
| 10277 |
UR=U2 |
| 10278 |
VR=V2 |
| 10279 |
WR=W2 |
| 10280 |
ER=E2 |
| 10281 |
C STORE THE RECOIL HEAVY ION IN THE RECOIL BANK |
| 10282 |
EP = ER |
| 10283 |
UP = UR |
| 10284 |
VP = VR |
| 10285 |
WP = WR |
| 10286 |
AMP = AR |
| 10287 |
ZMP = FLOAT(NZR) |
| 10288 |
AGEP = AGE |
| 10289 |
MTP = MT |
| 10290 |
CALL STOPAR(IDHEVY,NHEVY) |
| 10291 |
RETURN |
| 10292 |
END |
| 10293 |
*CMZ : 1.04/05 16/08/95 15.27.07 by Christian Zeitnitz |
| 10294 |
*-- Author : Christian Zeitnitz 28/07/92 |
| 10295 |
SUBROUTINE GTMED(MEDGEA,MEDMOR) |
| 10296 |
#include "mmicap.inc" |
| 10297 |
#include "minput.inc" |
| 10298 |
*KEND. |
| 10299 |
C get MICAP material number |
| 10300 |
DO 10 I=1,MEDIA |
| 10301 |
IF(LD(LGE2MO+I).EQ.MEDGEA) THEN |
| 10302 |
MEDMOR = I |
| 10303 |
GOTO 20 |
| 10304 |
ENDIF |
| 10305 |
10 CONTINUE |
| 10306 |
WRITE(IOUT,'('' MICAP GTMED: GEANT Medium '',I5, ' |
| 10307 |
+ //' '' not found ==> STOP'')') MEDGEA |
| 10308 |
STOP |
| 10309 |
20 RETURN |
| 10310 |
END |
| 10311 |
*CMZ : 0.92/00 02/12/92 16.02.32 by Christian Zeitnitz |
| 10312 |
*-- Author : |
| 10313 |
SUBROUTINE INTERP(X,Y,X1,Y1,X2,Y2,INT) |
| 10314 |
C THIS ROUTINE PERFORMS THE INTERPOLATION ACCORDING |
| 10315 |
C TO THE ENDF/B INTERPOLATION SCHEME INT |
| 10316 |
#include "minput.inc" |
| 10317 |
*KEND. |
| 10318 |
SAVE |
| 10319 |
IF(INT.LT.1.OR.INT.GT.5)GO TO 60 |
| 10320 |
IF(X2.EQ.X1)GO TO 10 |
| 10321 |
GO TO (10,20,30,40,50),INT |
| 10322 |
10 Y=Y1 |
| 10323 |
RETURN |
| 10324 |
20 Y=Y1+(X-X1)*(Y2-Y1)/(X2-X1) |
| 10325 |
RETURN |
| 10326 |
30 IF(X1.EQ.0.0.OR.X2.EQ.0.0)GO TO 20 |
| 10327 |
Y=Y1+ALOG(X/X1)*(Y2-Y1)/ALOG(X2/X1) |
| 10328 |
RETURN |
| 10329 |
40 IF(Y1.EQ.0.0.OR.Y2.EQ.0.0)GO TO 20 |
| 10330 |
Y=Y1*EXP((X-X1)*ALOG(Y2/Y1)/(X2-X1)) |
| 10331 |
RETURN |
| 10332 |
50 IF(Y1.EQ.0.0.OR.Y2.EQ.0.0)GO TO 30 |
| 10333 |
IF(X1.EQ.0.0.OR.X2.EQ.0.0)GO TO 40 |
| 10334 |
Y=Y1*EXP(ALOG(X/X1)*ALOG(Y2/Y1)/ALOG(X2/X1)) |
| 10335 |
RETURN |
| 10336 |
60 WRITE(IOUT,10000)INT |
| 10337 |
10000 FORMAT(' MICAP: INTERP-INVALID INTERPOLATION SCHEME',I11) |
| 10338 |
WRITE(6,*) ' CALOR: ERROR in INTERP ====> STOP ' |
| 10339 |
STOP |
| 10340 |
END |
| 10341 |
*CMZ : 1.01/04 10/06/93 14.43.48 by Christian Zeitnitz |
| 10342 |
*-- Author : |
| 10343 |
SUBROUTINE INTSCH(IFSE,I,IS,NR) |
| 10344 |
C THIS ROUTINE DETERMINES THE INTERPOLATION SCHEME |
| 10345 |
C ACCORDING TO ENDF/B-V FORMATTED DATA FILES |
| 10346 |
DIMENSION IFSE(*) |
| 10347 |
DO 10 J=1,NR |
| 10348 |
J1=3+2*(J-1) |
| 10349 |
NPTS=IFSE(J1) |
| 10350 |
IF(I.LE.NPTS)GO TO 20 |
| 10351 |
10 CONTINUE |
| 10352 |
20 IS=IFSE(J1+1) |
| 10353 |
RETURN |
| 10354 |
END |
| 10355 |
*CMZ : 1.04/00 02/02/95 09.26.26 by Christian Zeitnitz |
| 10356 |
*-- Author : |
| 10357 |
SUBROUTINE ISOTPE(D,LD,KM,RHO,IN,IDICTS,LDICT,E,TSIG,NMED, |
| 10358 |
+ IIN,IIM) |
| 10359 |
C THIS ROUTINE DETERMINES WHICH ISOTOPE HAS BEEN STRUCK |
| 10360 |
C IN MEDIA NMED |
| 10361 |
#include "minput.inc" |
| 10362 |
#include "mconst.inc" |
| 10363 |
#include "mmicab.inc" |
| 10364 |
*KEND. |
| 10365 |
C |
| 10366 |
DIMENSION D(*),LD(*),KM(*),RHO(*),IN(*),IDICTS(NNR,NNUC), |
| 10367 |
+ LDICT(NNR,NNUC) |
| 10368 |
SAVE |
| 10369 |
C |
| 10370 |
R=FLTRNF(0) |
| 10371 |
NOA=0 |
| 10372 |
SUM=0. |
| 10373 |
20 DO 30 K=1,NMIX |
| 10374 |
IF(KM(K).NE.NMED)GO TO 30 |
| 10375 |
C DETERMINE ISOTOPE NUMBER |
| 10376 |
K1=IN(K) |
| 10377 |
K2=K |
| 10378 |
C DETERMINE TOTAL CROSS SECTION FOR THIS ISOTOPE |
| 10379 |
LS1=IDICTS(1,K1)+LMOX2 |
| 10380 |
L1=LDICT(1,K1) |
| 10381 |
LEN=L1/2 |
| 10382 |
CALL TBSPLT(D(LS1),E,LEN,X) |
| 10383 |
SUM=SUM+X*RHO(K) |
| 10384 |
C CHECK TO SEE IF THIS ISOTOPE WAS HIT |
| 10385 |
IF(R.LE.SUM/TSIG)GO TO 40 |
| 10386 |
30 CONTINUE |
| 10387 |
C AN ISOTOPE WAS NOT CHOSEN, TRY AGAIN |
| 10388 |
NOA=NOA+1 |
| 10389 |
IF(NOA.GT.5)GO TO 50 |
| 10390 |
SUM=0.0 |
| 10391 |
R=FLTRNF(0) |
| 10392 |
GO TO 20 |
| 10393 |
40 IIN=K1 |
| 10394 |
IIM=K2 |
| 10395 |
RETURN |
| 10396 |
50 WRITE(IOUT,10000)NMED,TSIG |
| 10397 |
10000 FORMAT(' MICAP: AN ISOTOPE WAS NOT CHOSEN IN 5 ATTEMPTS IN ', |
| 10398 |
+'ROUTINE ISOTPE',/,3X,'MEDIUM=',I5,5X,'MACROSCOPIC XSEC=', |
| 10399 |
+1PE12.4) |
| 10400 |
WRITE(IOUT,10100)R,SUM,TSIG,X,E,RHO(K2),NMED,K1,K2 |
| 10401 |
10100 FORMAT('0',1X,1P6E12.4,3I10) |
| 10402 |
WRITE(6,*) ' CALOR: ERROR in ISOTPE =====> STOP ' |
| 10403 |
STOP |
| 10404 |
END |
| 10405 |
*CMZ : 1.01/04 10/06/93 14.43.48 by Christian Zeitnitz |
| 10406 |
*-- Author : |
| 10407 |
SUBROUTINE LABNF(D,LD,FM,AWR,KZ,Q,LIFLAG) |
| 10408 |
C THIS ROUTINE CALCULATES THE DIRECTIONAL COSINES FOR THE |
| 10409 |
C NEUTRON BORN FROM THE FISSION REACTION. THIS VERSION OF |
| 10410 |
C THE PROGRAM WILL TREAT A FISSION REACTION AS A SCATTERING |
| 10411 |
C EVENT WITH THE NEUTRON EMERGING WITH A MODIFIED WEIGHT OF |
| 10412 |
C WATE*NU-BAR. NO PROVISIONS ARE MADE AT THIS TIME TO |
| 10413 |
C CALCULATE THE FISSION FRAGMENTS PARAMETERS, HOWEVER A HEAVY |
| 10414 |
C RECOIL ION WILL BE STORED (FOR ANALYSIS PURPOSES) WITH |
| 10415 |
C ENERGY AND DIRECTION COSINES EQUAL TO ZERO. |
| 10416 |
#include "minput.inc" |
| 10417 |
#include "mconst.inc" |
| 10418 |
#include "mnutrn.inc" |
| 10419 |
#include "mrecoi.inc" |
| 10420 |
#include "mapoll.inc" |
| 10421 |
#include "mmass.inc" |
| 10422 |
#include "mpstor.inc" |
| 10423 |
*KEND. |
| 10424 |
DIMENSION D(*),LD(*),FM(*) |
| 10425 |
SAVE |
| 10426 |
MT=18 |
| 10427 |
C CALCULATE THE NEUTRON EXIT DIRECTIONAL COSINES |
| 10428 |
POX = 0.0 |
| 10429 |
POY = 0.0 |
| 10430 |
POZ = 0.0 |
| 10431 |
DO 40 KN=1,INEU |
| 10432 |
IF(LIFLAG.EQ.1) THEN |
| 10433 |
CALL GTISO(UP,VP,WP) |
| 10434 |
ELSE |
| 10435 |
SINPSI=SQRT(1.0-FM(KN)**2) |
| 10436 |
CALL AZIRN(SINETA,COSETA) |
| 10437 |
STHETA=1.0-UOLD**2 |
| 10438 |
IF(STHETA)20,20,10 |
| 10439 |
10 STHETA=SQRT(STHETA) |
| 10440 |
COSPHI=VOLD/STHETA |
| 10441 |
SINPHI=WOLD/STHETA |
| 10442 |
GO TO 30 |
| 10443 |
20 COSPHI=1.0 |
| 10444 |
SINPHI=0.0 |
| 10445 |
STHETA=0.0 |
| 10446 |
30 UP=UOLD*FM(KN)-COSETA*SINPSI*STHETA |
| 10447 |
VP=VOLD*FM(KN)+UOLD*COSPHI*COSETA*SINPSI-SINPHI* SINPSI* |
| 10448 |
+ SINETA |
| 10449 |
WP=WOLD*FM(KN)+UOLD*SINPHI*COSETA*SINPSI+COSPHI* SINPSI* |
| 10450 |
+ SINETA |
| 10451 |
S=1.0/SQRT(UP**2+VP**2+WP**2) |
| 10452 |
UP=UP*S |
| 10453 |
VP=VP*S |
| 10454 |
WP=WP*S |
| 10455 |
ENDIF |
| 10456 |
AGEP = AGE |
| 10457 |
EP = ENE(KN) |
| 10458 |
C use only first neutron for recoil calculation in order to ensure |
| 10459 |
C correct recoil nucleus energy spectrum |
| 10460 |
IF(KN.EQ.1) THEN |
| 10461 |
PP = SQRT(EP**2 + 2.0*EP*ZN) |
| 10462 |
POX = POX + PP*UP |
| 10463 |
POY = POY + PP*VP |
| 10464 |
POZ = POZ + PP*WP |
| 10465 |
ENDIF |
| 10466 |
MTP = MT |
| 10467 |
CALL STOPAR(IDNEU,NNEU) |
| 10468 |
40 CONTINUE |
| 10469 |
C SET THE HEAVY RECOIL ION PARAMETERS FOR ANALYSIS TAPE |
| 10470 |
50 PI=SQRT(2.0*ZN*EOLD) |
| 10471 |
PIX=PI*UOLD |
| 10472 |
PIY=PI*VOLD |
| 10473 |
PIZ=PI*WOLD |
| 10474 |
PRX=PIX-POX |
| 10475 |
PRY=PIY-POY |
| 10476 |
PRZ=PIZ-POZ |
| 10477 |
PR=SQRT(PRX**2+PRY**2+PRZ**2) |
| 10478 |
UR=PRX/PR |
| 10479 |
VR=PRY/PR |
| 10480 |
WR=PRZ/PR |
| 10481 |
AR=AWR*AN+AN-INEU*AN |
| 10482 |
XM=AR*931.075E6 |
| 10483 |
ER=SQRT(PR**2+XM**2)-XM |
| 10484 |
EP = ER |
| 10485 |
UP = UR |
| 10486 |
VP = VR |
| 10487 |
WP = WR |
| 10488 |
AGEP = AGE |
| 10489 |
MTP = MT |
| 10490 |
XR=X |
| 10491 |
YR=Y |
| 10492 |
ZR=Z |
| 10493 |
WATER=WTBC |
| 10494 |
NZR=KZ |
| 10495 |
AGER=AGE |
| 10496 |
NCOLR=NCOL |
| 10497 |
MTNR=MT |
| 10498 |
AMP = AR |
| 10499 |
ZMP = FLOAT(KZ) |
| 10500 |
ENIR=EOLD |
| 10501 |
UNIR=UOLD |
| 10502 |
VNIR=VOLD |
| 10503 |
WNIR=WOLD |
| 10504 |
ENOR=E |
| 10505 |
UNOR=U |
| 10506 |
VNOR=V |
| 10507 |
WNOR=W |
| 10508 |
WTNR=WATE |
| 10509 |
QR=Q |
| 10510 |
C STORE THE RECOIL HEAVY ION IN THE RECOIL BANK |
| 10511 |
CALL STOPAR(IDHEVY,NHEVY) |
| 10512 |
RETURN |
| 10513 |
END |
| 10514 |
*CMZ : 0.92/00 02/12/92 16.02.32 by Christian Zeitnitz |
| 10515 |
*-- Author : |
| 10516 |
SUBROUTINE LR2BOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,Q,SQ,ID,MT) |
| 10517 |
C THIS ROUTINE CALCULATES THE EXIT ENERGIES AND DIRECTIONAL |
| 10518 |
C COSINES FOR THE CHARGED PARTICLE AND RECOIL NUCLEUS FOR |
| 10519 |
C A TWO-BODY REACTION USING AN EVAPORATION SPECTRUM AND |
| 10520 |
C MOMEMTUM BALANCE. IT ALSO SETS ALL EXIT PARAMETERS FOR |
| 10521 |
C THE COLLISION PRODUCTS AND STORES THEM IN THE RECOIL BANK. |
| 10522 |
C THE TWO BODY REACTION RESULTS FROM THE BREAK-UP OF A NUCLEUS |
| 10523 |
C LEFT IN AN EXCITED STATE BY AN INELASTIC COLLISION |
| 10524 |
C DESIGNATED BY A LR-FLAG IN THE INELASTIC RESOLVED DATA |
| 10525 |
#include "minput.inc" |
| 10526 |
#include "mconst.inc" |
| 10527 |
#include "mnutrn.inc" |
| 10528 |
#include "mrecoi.inc" |
| 10529 |
#include "mapoll.inc" |
| 10530 |
#include "mmass.inc" |
| 10531 |
#include "mpstor.inc" |
| 10532 |
*KEND. |
| 10533 |
DIMENSION D(*),LD(*) |
| 10534 |
SAVE |
| 10535 |
C CALCULATE THE CONSTANTS USED IN THE KINEMATIIC EQUATIONS |
| 10536 |
ZATAR=ATAR*9.31075E+08 |
| 10537 |
C FOR A CARBON-ALPHA EMISSION THE RECOIL MASS IS KNOWN EXACTLY |
| 10538 |
IF(KZ1+KZ2.EQ.6)Z2=ZATAR-Z1-SQ |
| 10539 |
IF(KZ1+KZ2.EQ.6)A2=Z2/9.31075E+08 |
| 10540 |
C TRANSFER THE RECOILING COMPOUND NUCLEUS PARAMETERS OUT OF |
| 10541 |
C COMMON RECOIL FOR USE IN THE MOMENTUM BALANCE EQUATIONS |
| 10542 |
ERCN=ER |
| 10543 |
URCN=UR |
| 10544 |
VRCN=VR |
| 10545 |
WRCN=WR |
| 10546 |
ARCN=AR |
| 10547 |
NZRCN=NZR |
| 10548 |
ZARCN=ARCN*9.31075E+08 |
| 10549 |
IF(MT.EQ.23)GO TO 10 |
| 10550 |
C CALCULATE THE COULOMB BARRIER (CB) |
| 10551 |
CALL BARIER(KZ1,KZ2,A1,A2,CB) |
| 10552 |
C CALCULATE THE ENERGY AVAILABLE IN THE CENTER OF MASS (EAV) |
| 10553 |
CALL EVAPLR(E,Q,SQ,ATAR,CB,EX) |
| 10554 |
EAV=EX+CB |
| 10555 |
GO TO 30 |
| 10556 |
10 IF((ID.EQ.54).AND.(KZ1+KZ2.EQ.6))GO TO 20 |
| 10557 |
EAV=ABS(Q)+SQ |
| 10558 |
GO TO 30 |
| 10559 |
20 Q=EOLD-E-ERCN |
| 10560 |
IF(Q.LE.ABS(SQ))Q=7.65300E+06 |
| 10561 |
EAV=Q+SQ |
| 10562 |
30 CONTINUE |
| 10563 |
C CALCULATE THE CHARGED PARTICLE ENERGY USING CONSERVATION |
| 10564 |
C OF MOMENTUM (CENTER OF MASS SYSTEM) |
| 10565 |
E1CM=(A2/(A1+A2))*EAV |
| 10566 |
C ASSUME ISOTROPIC CHARGED PARTICLE EMISSION IN THE CENTER |
| 10567 |
C OF MASS COORDINATE SYSTEM |
| 10568 |
R=FLTRNF(0) |
| 10569 |
FM=2.0*R-1.0 |
| 10570 |
C CALCULATE THE VELOCITY OF THE CENTER OF MASS AND THE |
| 10571 |
C CHARGED PARTICLE IN THE CENTER OF MASS SYSTEM |
| 10572 |
VCM=SQRT((2.0*ERCN)/ZARCN) |
| 10573 |
V1CM=SQRT((2.0*E1CM)/Z1) |
| 10574 |
C CALCULATE THE CHARGED PARTICLE ENERGY IN THE LABORATORY |
| 10575 |
C COORDINATE SYSTEM |
| 10576 |
E1=0.5*Z1*(VCM**2+V1CM**2+VCM*V1CM*FM) |
| 10577 |
C CONVERT THE COSINE OF THE SCATTERING ANGLE IN THE CENTER OF |
| 10578 |
C MASS COORDINATE SYSTEM TO THE LABORATORY COORDINATE SYSTEM |
| 10579 |
FM=(V1CM*FM+VCM)/(SQRT(((V1CM*FM+VCM)**2)+((V1CM*(1.0-FM**2)) |
| 10580 |
1**2))) |
| 10581 |
C CALCULATE THE CHARGED PARTICLE EXIT DIRECTIONAL COSINES |
| 10582 |
SINPSI=SQRT(1.0-FM**2) |
| 10583 |
CALL AZIRN(SINETA,COSETA) |
| 10584 |
STHETA=1.0-URCN**2 |
| 10585 |
IF(STHETA)50,50,40 |
| 10586 |
40 STHETA=SQRT(STHETA) |
| 10587 |
COSPHI=VRCN/STHETA |
| 10588 |
SINPHI=WRCN/STHETA |
| 10589 |
GO TO 60 |
| 10590 |
50 COSPHI=1.0 |
| 10591 |
SINPHI=0.0 |
| 10592 |
STHETA=0.0 |
| 10593 |
60 U1=URCN*FM-COSETA*SINPSI*STHETA |
| 10594 |
V1=VRCN*FM+URCN*COSPHI*COSETA*SINPSI-SINPHI*SINPSI*SINETA |
| 10595 |
W1=WRCN*FM+URCN*SINPHI*COSETA*SINPSI+COSPHI*SINPSI*SINETA |
| 10596 |
S=1.0/SQRT(U1**2+V1**2+W1**2) |
| 10597 |
U1=U1*S |
| 10598 |
V1=V1*S |
| 10599 |
W1=W1*S |
| 10600 |
C CALCULATE AND SET THE CHARGED PARTICLE EXIT PARAMETERS |
| 10601 |
XR=X |
| 10602 |
YR=Y |
| 10603 |
ZR=Z |
| 10604 |
WATER=WTBC |
| 10605 |
NZR=KZ1 |
| 10606 |
AGER=AGE |
| 10607 |
NCOLR=NCOL |
| 10608 |
MTNR=MT |
| 10609 |
AR=A1 |
| 10610 |
ENIR=EOLD |
| 10611 |
UNIR=UOLD |
| 10612 |
VNIR=VOLD |
| 10613 |
WNIR=WOLD |
| 10614 |
ENOR=E |
| 10615 |
UNOR=U |
| 10616 |
VNOR=V |
| 10617 |
WNOR=W |
| 10618 |
WTNR=WATE |
| 10619 |
QR=Q |
| 10620 |
UR=U1 |
| 10621 |
VR=V1 |
| 10622 |
WR=W1 |
| 10623 |
ER=E1 |
| 10624 |
C STORE THE CHARGED PARTICLE IN THE RECOIL BANK |
| 10625 |
EP = ER |
| 10626 |
UP = UR |
| 10627 |
VP = VR |
| 10628 |
WP = WR |
| 10629 |
AGEP = AGE |
| 10630 |
MTP = MT |
| 10631 |
AMP = AR |
| 10632 |
ZMP = FLOAT(NZR) |
| 10633 |
CALL STOPAR(IDHEVY,NHEVY) |
| 10634 |
C CALCULATE THE TOTAL MOMENTUM BEFORE THE COLLISION |
| 10635 |
C COMPOUND NUCLEUS MOMENTUM BEFORE THE COLLISION (PI) EQUALS |
| 10636 |
C THE TOTAL MOMENTUM |
| 10637 |
PI=SQRT(2.0*ZARCN*ERCN) |
| 10638 |
C CALCULATE THE TOTAL MOMEMTUM OF THE EXIT CHARGED PARTICLE |
| 10639 |
PO=SQRT(2.0*Z1*E1) |
| 10640 |
C CALCULATE THE DIRECTIONAL MOMENTUM OF THE RECOIL NUCLEUS |
| 10641 |
PRX=PI*URCN-PO*U1 |
| 10642 |
PRY=PI*VRCN-PO*V1 |
| 10643 |
PRZ=PI*WRCN-PO*W1 |
| 10644 |
C CALCULATE THE TOTAL MOMENTUM OF THE RECOIL NUCLEUS |
| 10645 |
PR=SQRT(PRX**2+PRY**2+PRZ**2) |
| 10646 |
C CALCULATE THE RECOIL NUCLEUS DIRECTIONAL COSINES |
| 10647 |
U2=PRX/PR |
| 10648 |
V2=PRY/PR |
| 10649 |
W2=PRZ/PR |
| 10650 |
C CALCULATE THE RECOIL NUCLEUS EXIT ENERGY |
| 10651 |
XM = A2*931.075E6 |
| 10652 |
E2 = SQRT(PR**2+XM**2) - XM |
| 10653 |
C CALCULATE AND SET THE CHARGED PARTICLE EXIT PARAMETERS |
| 10654 |
XR=X |
| 10655 |
YR=Y |
| 10656 |
ZR=Z |
| 10657 |
WATER=WTBC |
| 10658 |
NZR=KZ2 |
| 10659 |
AGER=AGE |
| 10660 |
NCOLR=NCOL |
| 10661 |
MTNR=MT |
| 10662 |
AR=A2 |
| 10663 |
ENIR=EOLD |
| 10664 |
UNIR=UOLD |
| 10665 |
VNIR=VOLD |
| 10666 |
WNIR=WOLD |
| 10667 |
ENOR=E |
| 10668 |
UNOR=U |
| 10669 |
VNOR=V |
| 10670 |
WNOR=W |
| 10671 |
WTNR=WATE |
| 10672 |
QR=Q |
| 10673 |
UR=U2 |
| 10674 |
VR=V2 |
| 10675 |
WR=W2 |
| 10676 |
ER=E2 |
| 10677 |
IF((KZ2.EQ.4).AND.(MT.EQ.23))RETURN |
| 10678 |
C STORE THE RECOIL HEAVY ION IN THE RECOIL BANK |
| 10679 |
EP = ER |
| 10680 |
UP = UR |
| 10681 |
VP = VR |
| 10682 |
WP = WR |
| 10683 |
AGEP = AGE |
| 10684 |
MTP = MT |
| 10685 |
AMP = AR |
| 10686 |
ZMP = FLOAT(NZR) |
| 10687 |
CALL STOPAR(IDHEVY,NHEVY) |
| 10688 |
RETURN |
| 10689 |
END |
| 10690 |
*CMZ : 1.01/04 10/06/93 14.43.48 by Christian Zeitnitz |
| 10691 |
*-- Author : |
| 10692 |
SUBROUTINE LRNORM(D,LD,IDICTS,LDICT,LR,EOLD,MT,IIN,XSLR) |
| 10693 |
C THIS ROUTINE IS DESIGNED TO ADJUST THE NEUTRON CROSS SECTION |
| 10694 |
C USED TO CALCULATE THE PHOTON MULTIPLICITY WHEN THE |
| 10695 |
C INELASTIC RESOLVED DATA CONTAINS LR-FLAGS DESIGNATING |
| 10696 |
C CHARGED PARTICLE EMISSION |
| 10697 |
#include "minput.inc" |
| 10698 |
#include "mconst.inc" |
| 10699 |
#include "mcross.inc" |
| 10700 |
#include "mmicab.inc" |
| 10701 |
*KEND. |
| 10702 |
DIMENSION D(*),LD(*),IDICTS(NNR,NNUC),LDICT(NNR,NNUC), |
| 10703 |
+LR(NQ,NNUC) |
| 10704 |
SAVE |
| 10705 |
C INITIALIZE VARIABLES USED IN THE CALCULATION |
| 10706 |
SUM=0.0 |
| 10707 |
SUM4=SIGNIS |
| 10708 |
C DETERMINE (N,N") CROSS SECTION AND LR-FLAG |
| 10709 |
DO 10 I=14,54 |
| 10710 |
L1=LDICT(I,IIN) |
| 10711 |
IF(L1.EQ.0)GO TO 10 |
| 10712 |
LS1=IDICTS(I,IIN)+LMOX2 |
| 10713 |
LEN=L1/2 |
| 10714 |
CALL XSECNU(D,LEN,EOLD,SIG,LS1,L1) |
| 10715 |
LRI=LR(I,IIN) |
| 10716 |
IF(LRI.EQ.MT)SUM=SUM+SIG |
| 10717 |
IF(LRI.EQ.22)SUM4=SUM4-SIG |
| 10718 |
IF(LRI.EQ.23)SUM4=SUM4-SIG |
| 10719 |
IF(LRI.EQ.28)SUM4=SUM4-SIG |
| 10720 |
10 CONTINUE |
| 10721 |
XSLR=SUM |
| 10722 |
IF(MT.EQ.4)XSLR=SUM4 |
| 10723 |
RETURN |
| 10724 |
END |
| 10725 |
*CMZ : 1.04/05 16/08/95 14.52.27 by Christian Zeitnitz |
| 10726 |
*-- Author : Christian Zeitnitz 25/05/94 |
| 10727 |
SUBROUTINE MATISO(IZ,IA,NI,IDISO,FSINGL,NUNIT) |
| 10728 |
C |
| 10729 |
C Search array MATIDS for the isotopes which have to be taken |
| 10730 |
C into account for the element described by IZ and IA |
| 10731 |
C |
| 10732 |
#include "mmicap.inc" |
| 10733 |
#include "minput.inc" |
| 10734 |
*KEND. |
| 10735 |
C |
| 10736 |
DIMENSION IDISO(20,2) |
| 10737 |
LOGICAL FSINGL |
| 10738 |
C |
| 10739 |
IF(IZ.GT.0.AND.IZ.LE.100.and.MATIDS(IZ,1,1).GT.0) THEN |
| 10740 |
ID = IZ*1000+IA |
| 10741 |
IF = 0 |
| 10742 |
IC = 0 |
| 10743 |
IDIFF = 1000000 |
| 10744 |
C |
| 10745 |
C check first if selected isotope available |
| 10746 |
DO 10 I=2,MATIDS(IZ,1,1)+1 |
| 10747 |
IF( MATIDS(IZ,I,1).EQ.ID .AND. |
| 10748 |
+ (MATIDS(IZ,I,2).EQ.100 .OR. FSINGL)) IF = I |
| 10749 |
IF( IABS(MATIDS(IZ,I,1)-ID).LT.IDIFF) THEN |
| 10750 |
IDIFF = IABS(MATIDS(IZ,I,1)-ID) |
| 10751 |
IC = I |
| 10752 |
ENDIF |
| 10753 |
IDISO(I-1,1) = MATIDS(IZ,I,1) |
| 10754 |
IDISO(I-1,2) = MATIDS(IZ,I,2) |
| 10755 |
10 CONTINUE |
| 10756 |
NI = 1 |
| 10757 |
C the unit number on which the x-section is stored |
| 10758 |
NUNIT = MATIDS(IZ,1,2) |
| 10759 |
IF(.NOT. FSINGL) THEN |
| 10760 |
IF(IF .EQ. 0) THEN |
| 10761 |
C no matching isotope found. Look for closest one |
| 10762 |
IF(MATIDS(IZ,2,2).NE.100) NI = MATIDS(IZ,1,1) |
| 10763 |
ELSE |
| 10764 |
C matching isotope found |
| 10765 |
IDISO(1,1) = MATIDS(IZ,IF,1) |
| 10766 |
IDISO(1,2) = 100 |
| 10767 |
ENDIF |
| 10768 |
ELSE |
| 10769 |
IDISO(1,1) = MATIDS(IZ,IC,1) |
| 10770 |
IDISO(1,2) = 100 |
| 10771 |
ENDIF |
| 10772 |
ELSE |
| 10773 |
WRITE(IOUT,'('' MATISO: Error in neutron x-section '', ' |
| 10774 |
+ //' ''file detected - Z = '',I4)') IZ |
| 10775 |
WRITE(6,'('' MICAP : Error in x-section file '', ' |
| 10776 |
+ //' '' detected -> STOP '')') |
| 10777 |
STOP |
| 10778 |
ENDIF |
| 10779 |
RETURN |
| 10780 |
END |
| 10781 |
*CMZ : 1.05/03 27/06/2001 18.31.28 by Christian Zeitnitz |
| 10782 |
*-- Author : |
| 10783 |
SUBROUTINE MICAP |
| 10784 |
C |
| 10785 |
C CALOR-GEANT interface COMMON |
| 10786 |
#include "calgea.inc" |
| 10787 |
*KEND. |
| 10788 |
C MICAP commons |
| 10789 |
#include "mmicap.inc" |
| 10790 |
#include "minput.inc" |
| 10791 |
#include "mconst.inc" |
| 10792 |
#include "mnutrn.inc" |
| 10793 |
#include "mapoll.inc" |
| 10794 |
#include "mpoint.inc" |
| 10795 |
#include "mrecoi.inc" |
| 10796 |
#include "mmass.inc" |
| 10797 |
#include "mpstor.inc" |
| 10798 |
#include "cmagic.inc" |
| 10799 |
*KEND. |
| 10800 |
C |
| 10801 |
C convert Z,A of recoil to CALOR particle code |
| 10802 |
C only p = 0, D = 7, T = 8, He3 = 9, alpha=10 |
| 10803 |
DIMENSION NPART(4,0:2) |
| 10804 |
DATA ((NPART(I,J),I=1,4),J=0,2)/1 ,-1 ,-1 , -1, |
| 10805 |
+ 0 , 7 , 8 , -1, |
| 10806 |
+ -1 ,-1 , 9 , 10/ |
| 10807 |
LOGICAL NOP |
| 10808 |
SAVE |
| 10809 |
C first check, if ZEBRA still in order |
| 10810 |
IF(LD(LMAG1).NE.NMAGIC.OR.LD(LMAG2).NE.NMAGIC) THEN |
| 10811 |
WRITE(6,*) ' CALOR: ZEBRA banks screwed up --> STOP' |
| 10812 |
WRITE(IOUT,'('' MICAP: Magic number '',I12,'' not found: '', ' |
| 10813 |
+ //' 2I12)') NMAGIC,LD(LMAG1),LD(LMAG2) |
| 10814 |
STOP |
| 10815 |
ENDIF |
| 10816 |
C THIS ROUTINE PERFORMS THE RANDOM WALK FOR ALL PARTICLES |
| 10817 |
10 CONTINUE |
| 10818 |
C get material and particle information |
| 10819 |
U = UINC(1) |
| 10820 |
V = UINC(2) |
| 10821 |
W = UINC(3) |
| 10822 |
X = 0.0 |
| 10823 |
Y = 0.0 |
| 10824 |
Z = 0.0 |
| 10825 |
BLZNT = 1 |
| 10826 |
WATE = 1.0 |
| 10827 |
AGE = 0.0 |
| 10828 |
NREG = 1 |
| 10829 |
WTBC = 1.0 |
| 10830 |
C Energy MeV -> eV |
| 10831 |
E = EINC * 1.E6 |
| 10832 |
C Material number a la GEANT |
| 10833 |
NMED = NCEL |
| 10834 |
NMEM=1 |
| 10835 |
C reset counter of heavy/charged and gamma bank |
| 10836 |
NMEMR = 0 |
| 10837 |
NMEMG = 0 |
| 10838 |
INALB=0 |
| 10839 |
EOLD=E |
| 10840 |
UOLD=U |
| 10841 |
VOLD=V |
| 10842 |
WOLD=W |
| 10843 |
OLDWT=WATE |
| 10844 |
XOLD=X |
| 10845 |
YOLD=Y |
| 10846 |
ZOLD=Z |
| 10847 |
BLZON=BLZNT |
| 10848 |
MEDOLD=NMED |
| 10849 |
OLDAGE=AGE |
| 10850 |
I=1 |
| 10851 |
CALL GTMED(NMED,IMED) |
| 10852 |
C get total cross-section |
| 10853 |
CALL NSIGTA(E,NMED,TSIG,D,LD(LFP32),LD(LFP33)) |
| 10854 |
C DETERMINE WHICH ISOTOPE HAS BEEN HIT |
| 10855 |
CALL ISOTPE(D,LD,LD(LFP10),D(LFP12),LD(LFP16),LD(LFP26),LD(LFP27), |
| 10856 |
+ E,TSIG,IMED,IIN,IIM) |
| 10857 |
C THE PARAMETER (IIN) IS THE POINTER FOR ARRAYS DIMENSIONED BY |
| 10858 |
C (NNUC) AND THE PARAMETER (IIM) IS THE POINTER FOR ARRAYS |
| 10859 |
C DIMENSIONED BY (NMIX) |
| 10860 |
LD(LFP42+IMED-1)=LD(LFP42+IMED-1)+1 |
| 10861 |
INEU = 0 |
| 10862 |
NNEU = 0 |
| 10863 |
NHEVY = 0 |
| 10864 |
NGAMA = 0 |
| 10865 |
NPSTOR = 0 |
| 10866 |
ATARGT = D(LFP34+IIN-1)*1.008665 |
| 10867 |
ZTARGT = FLOAT(LD(LFP13+IIM-1)) |
| 10868 |
CALL COLISN(D,LD,LD(LFP20),LD(LFP21),LD(LFP22),LD(LFP23), |
| 10869 |
+ D(LFP24),LD(LFP24), |
| 10870 |
+ LD(LFP25),LD(LFP26),LD(LFP27),LD(LFP28),LD(LFP29),LD(LFP30), |
| 10871 |
+ LD(LFP31),D(LFP34),D(LFP35),LD(LFP41),LD(LFP41+NNUC), |
| 10872 |
+ LD(LFP42),LD(LFP42+MEDIA),LD(LFP42+2*MEDIA),LD(LFP42+3*MEDIA), |
| 10873 |
+ LD(LFP42+4*MEDIA),LD(LFP42+5*MEDIA),LD(LFP42+6*MEDIA), |
| 10874 |
+ LD(LFP42+7*MEDIA),LD(LFP42+8*MEDIA),LD(LFP42+9*MEDIA), |
| 10875 |
+ LD(LFP42+10*MEDIA),LD(LFP42+11*MEDIA),LD(LFP42+12*MEDIA), |
| 10876 |
+ LD(LFP42+13*MEDIA),LD(LFP42+14*MEDIA),LD(LFP42+15*MEDIA), |
| 10877 |
+ LD(LFP42+16*MEDIA),LD(LFP42+17*MEDIA),LD(LFP42+18*MEDIA), |
| 10878 |
+ LD(LFP42+19*MEDIA),LD(LFP42+20*MEDIA),LD(LFP42+21*MEDIA), |
| 10879 |
+ LD(LFP42+22*MEDIA),LD(LFP45),LD(LFP46),LD(LFP13), |
| 10880 |
+ LD(LFP35+NQ*NNUC),D(LFP35+2*NQ*NNUC),IIN,IIM) |
| 10881 |
CALL BANKR(D,LD,5) |
| 10882 |
C -------- fill return arrays with generated particles --------------- |
| 10883 |
C first heavy/charged particles |
| 10884 |
20 NPHETC = 0 |
| 10885 |
NRECOL = 0 |
| 10886 |
ERMED(1) = 0.0 |
| 10887 |
EETOT = 0.0 |
| 10888 |
C -------- store neutrons ------------------------------------- |
| 10889 |
INTCAL = 0 |
| 10890 |
C |
| 10891 |
DO 30 N=1,NNEU |
| 10892 |
CALL GETPAR(IDNEU,N,IERR) |
| 10893 |
IF(IERR.EQ.0) THEN |
| 10894 |
NPHETC = NPHETC + 1 |
| 10895 |
IF(NPHETC.GT.MXCP) NPHETC=MXCP |
| 10896 |
IPCAL(NPHETC) = 1 |
| 10897 |
C kinetic energy in MeV |
| 10898 |
EKINET(NPHETC) = EP * 1.E-6 |
| 10899 |
UCAL(NPHETC,1) = UP |
| 10900 |
UCAL(NPHETC,2) = VP |
| 10901 |
UCAL(NPHETC,3) = WP |
| 10902 |
CALTIM(NPHETC) = AGEP |
| 10903 |
ENDIF |
| 10904 |
30 CONTINUE |
| 10905 |
C -------- store heavy recoil products ------------------------ |
| 10906 |
DO 40 N=1,NHEVY |
| 10907 |
CALL GETPAR(IDHEVY,N,IERR) |
| 10908 |
IF(IERR.EQ.0) THEN |
| 10909 |
C check particle type |
| 10910 |
MA = NINT(AMP) |
| 10911 |
MZ = NINT(ZMP) |
| 10912 |
NOP = .TRUE. |
| 10913 |
IF(MA.LE.4.AND.MZ.LE.2) THEN |
| 10914 |
IF(NPART(MA,MZ).GT.-1) NOP = .FALSE. |
| 10915 |
ENDIF |
| 10916 |
IF(NOP) THEN |
| 10917 |
C get heavy recoil nucleus |
| 10918 |
NRECOL = NRECOL + 1 |
| 10919 |
AMED(NRECOL) = AMP |
| 10920 |
ZMED(NRECOL) = ZMP |
| 10921 |
ERMED(NRECOL)= EP * 1.E-6 |
| 10922 |
GOTO 40 |
| 10923 |
ENDIF |
| 10924 |
C store particle type |
| 10925 |
NPHETC = NPHETC + 1 |
| 10926 |
IF(NPHETC.GT.MXCP) NPHETC=MXCP |
| 10927 |
IPCAL(NPHETC) = NPART(MA,MZ) |
| 10928 |
C kinetic energy in MeV |
| 10929 |
EKINET(NPHETC) = EP * 1.E-6 |
| 10930 |
UCAL(NPHETC,1) = UP |
| 10931 |
UCAL(NPHETC,2) = VP |
| 10932 |
UCAL(NPHETC,3) = WP |
| 10933 |
CALTIM(NPHETC) = AGEP |
| 10934 |
ENDIF |
| 10935 |
40 CONTINUE |
| 10936 |
C |
| 10937 |
C----------- get generated gammas -------------------- |
| 10938 |
DO 50 N=1,NGAMA |
| 10939 |
CALL GETPAR(IDGAMA,N,IERR) |
| 10940 |
IF(IERR.EQ.0) THEN |
| 10941 |
NG = NG + 1 |
| 10942 |
NPHETC = NPHETC + 1 |
| 10943 |
IF(NPHETC.GT.MXCP) NPHETC=MXCP |
| 10944 |
IPCAL(NPHETC) = 11 |
| 10945 |
EKINET(NPHETC) = EP*1.E-6 |
| 10946 |
UCAL(NPHETC,1) = UP |
| 10947 |
UCAL(NPHETC,2) = VP |
| 10948 |
UCAL(NPHETC,3) = WP |
| 10949 |
CALTIM(NPHETC) = AGEP |
| 10950 |
C nucleus is in ground state ! |
| 10951 |
EXMED = 0.0 |
| 10952 |
ENDIF |
| 10953 |
50 CONTINUE |
| 10954 |
IF (MTP .EQ. 2) THEN |
| 10955 |
INTCAL = 13 |
| 10956 |
ELSEIF (MTP .EQ. 18) THEN |
| 10957 |
IF (NHEVY.GT.0) INTCAL = 15 |
| 10958 |
ELSEIF (MTP .LT. 100) THEN |
| 10959 |
IF (NNEU .GT.0) INTCAL = 20 |
| 10960 |
ELSEIF (MTP .EQ. 102) THEN |
| 10961 |
INTCAL = 18 |
| 10962 |
ELSEIF (MTP .GE. 100) THEN |
| 10963 |
IF (NHEVY+NGAMA.GT.0) INTCAL = 16 |
| 10964 |
ENDIF |
| 10965 |
IF(NNEU+NHEVY+NGAMA.GT.0.AND.INTCAL.EQ.0) INTCAL=12 |
| 10966 |
RETURN |
| 10967 |
END |
| 10968 |
*CMZ : 1.05/03 29/08/2001 14.35.16 by Christian Zeitnitz |
| 10969 |
*-- Author : Christian Zeitnitz 21/07/92 |
| 10970 |
SUBROUTINE MORINI |
| 10971 |
C************************************************************** |
| 10972 |
C Initialize MICAP |
| 10973 |
C ================ |
| 10974 |
C Called by : CALINI |
| 10975 |
C |
| 10976 |
C Purpose : setup cross-section tables and initialize pointer |
| 10977 |
C print flags etc. |
| 10978 |
C |
| 10979 |
C Author : C.Zeitnitz |
| 10980 |
C |
| 10981 |
C last modification: Changed in order to read new x-section file |
| 10982 |
C |
| 10983 |
C |
| 10984 |
C for details see MICAP manual ORNL/TM-10340 |
| 10985 |
C************************************************************* |
| 10986 |
C MICAP commons |
| 10987 |
#include "mmicap.inc" |
| 10988 |
#include "mpoint.inc" |
| 10989 |
#include "minput.inc" |
| 10990 |
#include "mmass.inc" |
| 10991 |
#include "mconst.inc" |
| 10992 |
#include "cmagic.inc" |
| 10993 |
#include "cerrcm.inc" |
| 10994 |
#include "camass.inc" |
| 10995 |
*KEND. |
| 10996 |
C GEANT common |
| 10997 |
#include "gccuts.inc" |
| 10998 |
#include "gcflag.inc" |
| 10999 |
*KEND. |
| 11000 |
C pointer to material/mixture bank (NMATE,JMATE) |
| 11001 |
#include "gcnum.inc" |
| 11002 |
*KEND. |
| 11003 |
C |
| 11004 |
COMMON / QUEST / IQUEST(100) |
| 11005 |
C |
| 11006 |
C Avogadro number multiplied by 1.E-24 |
| 11007 |
PARAMETER(XNAVO = 0.60221367) |
| 11008 |
C |
| 11009 |
DIMENSION A(100),AGEA(100),Z(100),DEN(100),MID(100,2),IDI(20,2) |
| 11010 |
CHARACTER*100 XSFILE |
| 11011 |
CHARACTER*4 CNAME |
| 11012 |
CHARACTER*70 CCOMM |
| 11013 |
CHARACTER*100 CHROOT |
| 11014 |
LOGICAL OPENED,EXISTS,IFOUND,FMIST,FSINGL,FMIFL |
| 11015 |
C |
| 11016 |
C set GEANT initialization flag |
| 11017 |
IFINIT(7) = 1 |
| 11018 |
C |
| 11019 |
C neutron energy cut (eV) |
| 11020 |
ECUT = CUTNEU * 1.E9 |
| 11021 |
C get time cut off from GEANT |
| 11022 |
TCUT = TOFMAX |
| 11023 |
C temperature for thermal neutron xsection (Kelvin) |
| 11024 |
C only temporary constant !!! |
| 11025 |
TEMP = 300.0 |
| 11026 |
C xsection file unit |
| 11027 |
MICROS = 31 |
| 11028 |
C open MICAP I/O units |
| 11029 |
INQUIRE(UNIT=MICROS,OPENED=OPENED) |
| 11030 |
IF(OPENED) THEN |
| 11031 |
REWIND MICROS |
| 11032 |
ELSE |
| 11033 |
XSFILE = 'xsneut.dat' |
| 11034 |
INQUIRE(FILE=XSFILE,EXIST=EXISTS) |
| 11035 |
IF(.NOT.EXISTS) THEN |
| 11036 |
CHROOT=' ' |
| 11037 |
CALL GETENV('CERN_ROOT',CHROOT) |
| 11038 |
LNROOT = LNBLNK(CHROOT) |
| 11039 |
IF(LNROOT.GT.0)XSFILE = CHROOT(1:LNROOT)//'/lib/xsneut.dat' |
| 11040 |
ENDIF |
| 11041 |
INQUIRE(FILE=XSFILE,EXIST=EXISTS) |
| 11042 |
IF(.NOT.EXISTS) THEN |
| 11043 |
PRINT*,'**********************************' |
| 11044 |
PRINT*,'* G C A L O R *' |
| 11045 |
PRINT*,'* ----------- *' |
| 11046 |
PRINT*,'* File XSNEUT.DAT not found *' |
| 11047 |
PRINT*,'* Program STOP *' |
| 11048 |
PRINT*,'**********************************' |
| 11049 |
STOP |
| 11050 |
ENDIF |
| 11051 |
OPEN(UNIT=MICROS,FILE=XSFILE,STATUS='OLD') |
| 11052 |
ENDIF |
| 11053 |
C setup the link areas needed for x-section banks |
| 11054 |
CALL MZLINK(IXCONS,'MICTMP',LTEMP,LTEMP,LTEMP) |
| 11055 |
CALL MZLINK(IXCONS,'MMICAP',LMAG2,LMOX4,LMAG2) |
| 11056 |
CALL MZLINK(IXCONS,'MPOINT',LMAG1,LFP210,LMAG1) |
| 11057 |
C |
| 11058 |
LSUP = 0 |
| 11059 |
LCSUP = 0 |
| 11060 |
NUNIT = MICROS |
| 11061 |
C pointers into TEMP bank |
| 11062 |
NTUNIT = 1 |
| 11063 |
NTNAME = NTUNIT + 1 |
| 11064 |
NTMPNI = NTNAME + 1 + 80/4 |
| 11065 |
NTCOMM = NTMPNI + 1 |
| 11066 |
NTDATS = NTCOMM + 1 + 80/4 |
| 11067 |
NTLIST = NTDATS + 1 + 24/4 |
| 11068 |
10 CONTINUE |
| 11069 |
C read comment and date of xsection file |
| 11070 |
READ(NUNIT,'(A80,/,A24)') COMMEN,DATSTR |
| 11071 |
C read in material definition array |
| 11072 |
READ(NUNIT,'(I10)') NISO |
| 11073 |
NWW = NISO * 3 + 12 + NTLIST |
| 11074 |
C get temporary buffer |
| 11075 |
CALL CHKZEB(NWW,IXCONS) |
| 11076 |
IF(LSUP.EQ.0) Then |
| 11077 |
C create a top level bank for the list of isotopes |
| 11078 |
CALL MZBOOK(IXCONS,LTEMP,LSUP,1,'TEMP',3,0,NWW,0,-1) |
| 11079 |
LT = LTEMP |
| 11080 |
ELSE |
| 11081 |
C create an additional bank in the linear structure TEMP |
| 11082 |
CALL MZBOOK(IXCONS,LT,LSUP,0,'TEMP',3,0,NWW,0,-1) |
| 11083 |
LSUP = LT |
| 11084 |
ENDIF |
| 11085 |
NREC = NISO * 3 / 12 |
| 11086 |
NN = 0 |
| 11087 |
C store the unit number of the file in bank TEMP |
| 11088 |
IQ(LT + NTUNIT) = NUNIT |
| 11089 |
C store the file name in bank TEMP |
| 11090 |
CALL UCTOH(XSFILE,IQ(LT+NTNAME+1),4,LNBLNK(XSFILE)) |
| 11091 |
IQ(LT + NTNAME) = LNBLNK(XSFILE) |
| 11092 |
C store the comment and date string in bank TEMP |
| 11093 |
IQ(LT + NTCOMM) = LNBLNK(COMMEN) |
| 11094 |
CALL UCTOH(COMMEN,IQ(LT+NTCOMM+1),4,LNBLNK(COMMEN)) |
| 11095 |
IQ(LT + NTDATS) = LNBLNK(DATSTR) |
| 11096 |
CALL UCTOH(DATSTR,IQ(LT+NTDATS+1),4,LNBLNK(DATSTR)) |
| 11097 |
DO 20 I=1,NREC |
| 11098 |
LL = (I-1)*12 + LT + NTLIST |
| 11099 |
READ(NUNIT,'(12I6)') (IQ(L),L=LL,LL+11) |
| 11100 |
20 CONTINUE |
| 11101 |
C |
| 11102 |
C get number of comment lines for different isotopes |
| 11103 |
READ(NUNIT,'(I10)') NCOM |
| 11104 |
NWW = NCOM * 80 + 2 |
| 11105 |
C get CISO bank |
| 11106 |
CALL CHKZEB(NWW,IXCONS) |
| 11107 |
IF(LCSUP.EQ.0) Then |
| 11108 |
C create a top level bank for the isotope comments |
| 11109 |
CALL MZBOOK(IXCONS,LCISO,LCSUP,1,'CISO',3,0,NWW,0,-1) |
| 11110 |
LC = LCISO |
| 11111 |
ELSE |
| 11112 |
C create an additional bank in the linear structure CISO |
| 11113 |
CALL MZBOOK(IXCONS,LC,LCSUP,0,'CISO',3,0,NWW,0,-1) |
| 11114 |
LCSUP = LC |
| 11115 |
ENDIF |
| 11116 |
IQ(LC+1) = NCOM |
| 11117 |
DO 30 I=1,NCOM |
| 11118 |
J = (I-1)*81 + 2 |
| 11119 |
READ(NUNIT,'(I4,I4,A70)') IQ(LC+J),IQ(LC+J+1), |
| 11120 |
+ CCOMM |
| 11121 |
CALL UCTOH(CCOMM,IQ(LC+J+2),4,70) |
| 11122 |
30 CONTINUE |
| 11123 |
C |
| 11124 |
C--------------------------------------------------------------------- |
| 11125 |
C check the existence of secondary x-section files stored in bank MIFL |
| 11126 |
C real messy code !!! But its fortran after all !!! CZ Jan 95 |
| 11127 |
XSFILE = ' ' |
| 11128 |
IF(NUNIT.EQ.MICROS) THEN |
| 11129 |
FMIFL = .FALSE. |
| 11130 |
CALL MZINQD(IXCONS) |
| 11131 |
IF(LMIFIL.GE.IQUEST(3) .AND. LMIFIL.LE.IQUEST(4)) THEN |
| 11132 |
CALL UHTOC(IQ(LMIFIL-4),4,CNAME,4) |
| 11133 |
IF(CNAME.EQ.'MIFL') FMIFL = .TRUE. |
| 11134 |
ENDIF |
| 11135 |
IXSF=LMIFIL |
| 11136 |
ENDIF |
| 11137 |
IF(FMIFL) THEN |
| 11138 |
40 CONTINUE |
| 11139 |
C get the file name |
| 11140 |
CALL UHTOC(IQ(IXSF+2),4,XSFILE,IQ(IXSF+1)) |
| 11141 |
IXSF = IXSF + 101 |
| 11142 |
C last name in the list ? |
| 11143 |
IF(IXSF-LMIFIL .GE. IQ(LMIFIL-1) ) FMIFL = .FALSE. |
| 11144 |
C |
| 11145 |
INQUIRE(FILE=XSFILE,EXIST=EXISTS) |
| 11146 |
IF(.NOT.EXISTS) THEN |
| 11147 |
PRINT '(70(''*''))' |
| 11148 |
PRINT '('' * MICAP : x-section file not found '')' |
| 11149 |
PRINT '('' * '',A77)', XSFILE |
| 11150 |
PRINT '(70(''*''))' |
| 11151 |
IF(FMIFL) GOTO 40 |
| 11152 |
ELSE |
| 11153 |
C find a free unit number (greater 31), and use it |
| 11154 |
DO 50 I=NUNIT+1,99 |
| 11155 |
INQUIRE(UNIT=I,OPENED=OPENED) |
| 11156 |
IF(.NOT.OPENED) THEN |
| 11157 |
NUNIT = I |
| 11158 |
OPEN(UNIT=I,FILE=XSFILE,STATUS='OLD') |
| 11159 |
GOTO 10 |
| 11160 |
ENDIF |
| 11161 |
50 CONTINUE |
| 11162 |
PRINT '(70(''*''))' |
| 11163 |
PRINT *,'* MICAP : No more free units available !' |
| 11164 |
PRINT '(70(''*''))' |
| 11165 |
ENDIF |
| 11166 |
ENDIF |
| 11167 |
C--------------------------------------------------------------------- |
| 11168 |
CALL VZERO(MATIDS,4000) |
| 11169 |
LT = LTEMP |
| 11170 |
60 CONTINUE |
| 11171 |
NUNIT = IQ(LT + NTUNIT) |
| 11172 |
KK = LT + NTLIST |
| 11173 |
DO 90 I=1,100 |
| 11174 |
NIS = IQ(KK) |
| 11175 |
KK = KK + 1 |
| 11176 |
IF(NIS.EQ.0) GOTO 100 |
| 11177 |
IF(MATIDS(I,1,1).EQ.0) THEN |
| 11178 |
MATIDS(I,1,1) = NIS |
| 11179 |
MATIDS(I,1,2) = NUNIT |
| 11180 |
C is the Z of the element correct? |
| 11181 |
ELSE IF(IQ(KK)/1000.EQ.I) THEN |
| 11182 |
C overwrite existing element with the one stored in new file |
| 11183 |
DO 70 J=2,MATIDS(I,1,1)+1 |
| 11184 |
MATIDS(I,J,1) = 0 |
| 11185 |
MATIDS(I,J,2) = 0 |
| 11186 |
70 CONTINUE |
| 11187 |
MATIDS(I,1,1) = NIS |
| 11188 |
MATIDS(I,1,2) = NUNIT |
| 11189 |
ELSE |
| 11190 |
C no action |
| 11191 |
KK = KK + 2 * NIS |
| 11192 |
GOTO 90 |
| 11193 |
ENDIF |
| 11194 |
C maximal 20 isotopes per element |
| 11195 |
NIS = MIN(NIS,19) |
| 11196 |
DO 80 J=2,NIS+1 |
| 11197 |
MATIDS(I,J,1) = IQ(KK) |
| 11198 |
MATIDS(I,J,2) = IQ(KK+1) |
| 11199 |
KK = KK + 2 |
| 11200 |
80 CONTINUE |
| 11201 |
90 CONTINUE |
| 11202 |
100 CONTINUE |
| 11203 |
LT = LQ(LT) |
| 11204 |
IF(LT.GT.0) GOTO 60 |
| 11205 |
C |
| 11206 |
C DEFINE CROSS SECTION DIMENSIONING VARIABLES |
| 11207 |
C NNR EQUALS THE NUMBER OF NEUTRON RECORDS |
| 11208 |
C NQ EQUALS THE NUMBER OF Q VALUES |
| 11209 |
C NGR EQUALS THE NUMBER OF GAMMA RECORDS |
| 11210 |
C SET THE DEFAULT VALUES FOR THE CURRENT CROSS SECTION DATA |
| 11211 |
NNR=134 |
| 11212 |
NQ=66 |
| 11213 |
NGR=60 |
| 11214 |
C |
| 11215 |
C SET THE DEFAULT VALUES FOR THE NEUTRON, PROTON, DEUTERON, |
| 11216 |
C TRITON, HELIUM-3, AND ALPHA PARTICLE MASSES (IN EV) |
| 11217 |
ZN=XMASS(1)*1.E9 |
| 11218 |
ZP=XMASS(0)*1.E9 |
| 11219 |
ZD=XMASS(7)*1.E9 |
| 11220 |
ZT=XMASS(8)*1.E9 |
| 11221 |
ZHE3=XMASS(9)*1.E9 |
| 11222 |
ZA=XMASS(10)*1.E9 |
| 11223 |
C SET THE DEFAULT VALUES FOR THE NEUTRON, PROTON, DEUTERON, |
| 11224 |
C TRITON, HELIUM-3, AND ALPHA PARTICLE MASSES (IN AMU) |
| 11225 |
XAMU=0.93149432*1.E9 |
| 11226 |
AN=ZN/XAMU |
| 11227 |
AP=ZP/XAMU |
| 11228 |
AD=ZD/XAMU |
| 11229 |
AT=ZT/XAMU |
| 11230 |
AHE3=ZHE3/XAMU |
| 11231 |
AA=ZA/XAMU |
| 11232 |
C now preprocess all materials xs |
| 11233 |
MEDIA = 0 |
| 11234 |
NMIX = 0 |
| 11235 |
NMAT = 0 |
| 11236 |
C Check if material option bank MIST exists |
| 11237 |
FMIST = .FALSE. |
| 11238 |
CALL MZINQD(IXCONS) |
| 11239 |
IF(LMIST.GE.IQUEST(3) .AND. LMIST.LE.IQUEST(4)) THEN |
| 11240 |
CALL UHTOC(IQ(LMIST-4),4,CNAME,4) |
| 11241 |
IF(CNAME.EQ.'MIST') FMIST = .TRUE. |
| 11242 |
ENDIF |
| 11243 |
C 1. loop over tracking media -> get NMIX,MEDIA |
| 11244 |
DO 140 I=1,NTMED |
| 11245 |
JTM = LQ(JTMED - I) |
| 11246 |
IF(JTM.LE.0) GOTO 140 |
| 11247 |
C valid tracking medium found get material number |
| 11248 |
C and get corresponding material parameters from JMATE structure |
| 11249 |
IMA = INT(Q(JTM+6)) |
| 11250 |
IF(IMA.LE.0 .OR. IMA.GT.NMATE) GOTO 140 |
| 11251 |
C count number of elements and number of mixing operations |
| 11252 |
JMA = LQ(JMATE-IMA) |
| 11253 |
IF(JMA.LE.0) GOTO 140 |
| 11254 |
IF(Q(JMA+6) .LE. 1.0 .OR. Q(JMA+6) .GE. 240.) GOTO 140 |
| 11255 |
C Check if for material IMA single isotopes are selected |
| 11256 |
FSINGL = .FALSE. |
| 11257 |
IF(FMIST) THEN |
| 11258 |
DO 110 KIM=1,IQ(LMIST-1),2 |
| 11259 |
IF(IMA.EQ.IQ(LMIST+KIM).AND.IQ(LMIST+KIM+1).EQ.0) THEN |
| 11260 |
FSINGL = .TRUE. |
| 11261 |
GOTO 120 |
| 11262 |
ENDIF |
| 11263 |
110 CONTINUE |
| 11264 |
120 CONTINUE |
| 11265 |
ENDIF |
| 11266 |
C get number of elements in material max = 100 |
| 11267 |
KK = MIN(ABS(Q(JMA+11)),100.) |
| 11268 |
C relation between MICAP and GEANT material number |
| 11269 |
MEDIA = MEDIA + 1 |
| 11270 |
C mixture ? |
| 11271 |
KK1 = KK |
| 11272 |
IF(KK.GT.1) THEN |
| 11273 |
JMIXT = LQ(JMA - 5) |
| 11274 |
C |
| 11275 |
C check if more than one isotope has to taken into account for all |
| 11276 |
C elements in the mixture |
| 11277 |
DO 130 K=1,KK |
| 11278 |
IA = NINT(Q(JMIXT+K)) |
| 11279 |
IZ = NINT(Q(JMIXT+K+KK)) |
| 11280 |
CALL MATISO(IZ,IA,NNI,IDI,FSINGL,NUNIT) |
| 11281 |
KK1 = KK1 + NNI - 1 |
| 11282 |
130 CONTINUE |
| 11283 |
ELSE |
| 11284 |
IA = NINT(Q(JMA+6)) |
| 11285 |
IZ = NINT(Q(JMA+7)) |
| 11286 |
CALL MATISO(IZ,IA,NNI,IDI,FSINGL,NUNIT) |
| 11287 |
KK1 = KK1 + NNI - 1 |
| 11288 |
ENDIF |
| 11289 |
NMIX = NMIX + KK1 |
| 11290 |
140 CONTINUE |
| 11291 |
C allocate ZEBRA bank for material information |
| 11292 |
NW = 9 * NMIX + MEDIA + 10 |
| 11293 |
C define link area for MICAP banks in GCBANK |
| 11294 |
CALL CHKZEB(NW,IXCONS) |
| 11295 |
CALL MZBOOK(IXCONS,LMOMA,0,2,'MOME',0,0,NW,0,-1) |
| 11296 |
LMAG1 = LMOMA + 1 |
| 11297 |
IQ(LMAG1) = NMAGIC |
| 11298 |
LGE2MO = LMAG1 + 1 |
| 11299 |
LFP10 = LGE2MO + MEDIA + 1 |
| 11300 |
LFP11 = LFP10 + NMIX |
| 11301 |
LFP12 = LFP11 + NMIX |
| 11302 |
LFP13 = LFP12 + NMIX |
| 11303 |
LFP14 = LFP13 + NMIX |
| 11304 |
LFP140 = LFP14 + NMIX |
| 11305 |
LFP16 = LFP140 + NMIX |
| 11306 |
LFP17 = LFP16 + NMIX |
| 11307 |
C 2. loop over tracking media |
| 11308 |
MEDIA1 = 0 |
| 11309 |
NMIX1 = 0 |
| 11310 |
DO 230 I=1,NTMED |
| 11311 |
JTM = LQ(JTMED - I) |
| 11312 |
IF(JTM.LE.0) GOTO 230 |
| 11313 |
C valid tracking medium found get material number |
| 11314 |
C and get corresponding material parameters from JMATE structure |
| 11315 |
IMA = INT(Q(JTM+6)) |
| 11316 |
IF(IMA.LE.0 .OR. IMA.GT.NMATE) GOTO 230 |
| 11317 |
C count number of elements and number of mixing operations |
| 11318 |
JMA = LQ(JMATE-IMA) |
| 11319 |
IF(JMA.LE.0) GOTO 230 |
| 11320 |
IF(Q(JMA+6) .LE. 1.0 .OR. Q(JMA+6) .GE. 240.) GOTO 230 |
| 11321 |
C Check if for material IMA single isotopes are selected |
| 11322 |
FSINGL = .FALSE. |
| 11323 |
IF(FMIST) THEN |
| 11324 |
DO 150 KIM=1,IQ(LMIST-1),2 |
| 11325 |
IF(IMA.EQ.IQ(LMIST+KIM).AND.IQ(LMIST+KIM+1).EQ.0) THEN |
| 11326 |
FSINGL = .TRUE. |
| 11327 |
GOTO 160 |
| 11328 |
ENDIF |
| 11329 |
150 CONTINUE |
| 11330 |
160 CONTINUE |
| 11331 |
ENDIF |
| 11332 |
NMAT = NMAT + 1 |
| 11333 |
C get number of elements in material max = 100 |
| 11334 |
RHO1 = Q(JMA+8) |
| 11335 |
KK = MIN1(ABS(Q(JMA+11)),100.) |
| 11336 |
C relation between MICAP and GEANT material number |
| 11337 |
C check if medium IMA already stored (multiple tracking media) |
| 11338 |
DO K=1,100 |
| 11339 |
AGEA(K) = 0.0 |
| 11340 |
ENDDO |
| 11341 |
DO 180 KMI=1,MEDIA1 |
| 11342 |
IF(IQ(LGE2MO+KMI).EQ.IMA) THEN |
| 11343 |
IF(KK.EQ.1) THEN |
| 11344 |
IA = NINT(Q(JMA+6)) |
| 11345 |
IZ = NINT(Q(JMA+7)) |
| 11346 |
CALL MATISO(IZ,IA,NNI,IDI,FSINGL,NUNIT) |
| 11347 |
NMIX = NMIX - NNI |
| 11348 |
ELSE |
| 11349 |
JMIXT = LQ(JMA - 5) |
| 11350 |
DO 170 K=1,KK |
| 11351 |
IA = NINT(Q(JMIXT+K)) |
| 11352 |
IZ = NINT(Q(JMIXT+K+KK)) |
| 11353 |
CALL MATISO(IZ,IA,NNI,IDI,FSINGL,NUNIT) |
| 11354 |
NMIX = NMIX - NNI |
| 11355 |
170 CONTINUE |
| 11356 |
ENDIF |
| 11357 |
MEDIA = MEDIA - 1 |
| 11358 |
GOTO 230 |
| 11359 |
ENDIF |
| 11360 |
180 CONTINUE |
| 11361 |
MEDIA1 = MEDIA1 + 1 |
| 11362 |
IQ(LGE2MO+MEDIA1) = IMA |
| 11363 |
C mixture ? |
| 11364 |
KK2 = KK |
| 11365 |
IF(KK.GT.1) THEN |
| 11366 |
JMIXT = LQ(JMA - 5) |
| 11367 |
KPOS = 1 |
| 11368 |
DO 200 K=1,KK |
| 11369 |
AMOL = Q(LQ(JMIXT-1) + 2) |
| 11370 |
XMOLCM = RHO1/AMOL*XNAVO |
| 11371 |
IA = NINT(Q(JMIXT+K)) |
| 11372 |
IZ = NINT(Q(JMIXT+K+KK)) |
| 11373 |
CALL MATISO(IZ,IA,NNI,IDI,FSINGL,NUNIT) |
| 11374 |
KK2 = KK2 + NNI - 1 |
| 11375 |
DO 190 KJ=1,NNI |
| 11376 |
KKPOS = KPOS + KJ - 1 |
| 11377 |
IF(KJ.EQ.1) THEN |
| 11378 |
AGEA(KKPOS) = Q(JMIXT+K) |
| 11379 |
ELSE |
| 11380 |
AGEA(KKPOS) = 0. |
| 11381 |
ENDIF |
| 11382 |
MID(KKPOS,1) = IDI(KJ,1) |
| 11383 |
MID(KKPOS,2) = NUNIT |
| 11384 |
IIZ = IDI(KJ,1)/1000 |
| 11385 |
IIA = IDI(KJ,1) - IIZ * 1000 |
| 11386 |
IF(IIA.NE.0 .AND. NNI.GT.1.) THEN |
| 11387 |
A(KKPOS) = FLOAT(IIA) |
| 11388 |
ELSE |
| 11389 |
A(KKPOS) = Q(JMIXT+K) |
| 11390 |
ENDIF |
| 11391 |
Z(KKPOS) = Q(JMIXT+K+KK) |
| 11392 |
WISO = FLOAT(IDI(KJ,2))/100. |
| 11393 |
WI = Q(JMIXT+K+2*KK)*AMOL/A(KKPOS)*WISO |
| 11394 |
DEN(KKPOS) = XMOLCM * WI |
| 11395 |
190 CONTINUE |
| 11396 |
KPOS = KPOS + NNI |
| 11397 |
200 CONTINUE |
| 11398 |
C element or compound |
| 11399 |
ELSE |
| 11400 |
IA = NINT(Q(JMA+6)) |
| 11401 |
IZ = NINT(Q(JMA+7)) |
| 11402 |
CALL MATISO(IZ,IA,NNI,IDI,FSINGL,NUNIT) |
| 11403 |
KK2 = KK2 + NNI - 1 |
| 11404 |
DO 210 KJ=1,NNI |
| 11405 |
IF(KJ.EQ.1) THEN |
| 11406 |
AGEA(KJ) = Q(JMA+6) |
| 11407 |
ELSE |
| 11408 |
AGEA(KJ) = 0. |
| 11409 |
ENDIF |
| 11410 |
MID(KJ,1) = IDI(KJ,1) |
| 11411 |
MID(KJ,2) = NUNIT |
| 11412 |
IIZ = IDI(KJ,1)/1000 |
| 11413 |
IIA = IDI(KJ,1) - IIZ * 1000 |
| 11414 |
IF(IIA.NE.0 .AND. NNI.GT.1.) THEN |
| 11415 |
A(KJ) = FLOAT(IIA) |
| 11416 |
ELSE |
| 11417 |
A(KJ) = Q(JMA+6) |
| 11418 |
ENDIF |
| 11419 |
Z(KJ) = Q(JMA+7) |
| 11420 |
WISO = FLOAT(IDI(KJ,2))/100. |
| 11421 |
DEN(KJ) = RHO1/A(KJ) * WISO *XNAVO |
| 11422 |
210 CONTINUE |
| 11423 |
ENDIF |
| 11424 |
C |
| 11425 |
C fill MICAP material arrays |
| 11426 |
C actual number of isotopes given by KK2 |
| 11427 |
C |
| 11428 |
DO 220 J = NMIX1 + 1, NMIX1 + KK2 |
| 11429 |
IQ(LFP10+J-1) = MEDIA1 |
| 11430 |
IQ(LFP11+J-1) = MID(J-NMIX1,1) |
| 11431 |
C check if bound hydrogen has been selected |
| 11432 |
IF(MID(J-NMIX1,1).eq.1001.AND.KK.GT.1) IQ(LFP11+J-1) = 1000 |
| 11433 |
Q(LFP12+J-1) = DEN(J-NMIX1) |
| 11434 |
IQ(LFP13+J-1) = NINT(Z(J-NMIX1)) |
| 11435 |
Q(LFP14+J-1) = A(J-NMIX1) |
| 11436 |
Q(LFP140+J-1) = AGEA(J-NMIX1) |
| 11437 |
220 CONTINUE |
| 11438 |
NMIX1 = NMIX1 + KK2 |
| 11439 |
230 CONTINUE |
| 11440 |
IF(NMIX.LE.0) THEN |
| 11441 |
PRINT *,' GCALOR: NO tracking media found ===> STOP ' |
| 11442 |
STOP |
| 11443 |
ENDIF |
| 11444 |
C read cross-sections and perform mixing and thinning |
| 11445 |
CALL MOXSEC |
| 11446 |
C close MICAP cross-section file(s) |
| 11447 |
LT = LTEMP |
| 11448 |
240 CONTINUE |
| 11449 |
CLOSE(UNIT=IQ(LT+NTUNIT)) |
| 11450 |
LT = LQ(LT) |
| 11451 |
IF(LT.GT.0) GOTO 240 |
| 11452 |
C Drop temporary linear structures |
| 11453 |
CALL MZDROP(IXCONS,LTEMP,'L') |
| 11454 |
CALL MZDROP(IXCONS,LCISO,'L') |
| 11455 |
RETURN |
| 11456 |
END |
| 11457 |
*CMZ : 1.05/04 25/02/2005 14.27.38 by Christian Zeitnitz |
| 11458 |
*-- Author : Christian Zeitnitz 22/07/92 |
| 11459 |
SUBROUTINE MOXSEC |
| 11460 |
C************************************************************ |
| 11461 |
C |
| 11462 |
C setup cross-section tables for MICAP |
| 11463 |
C |
| 11464 |
C Called by: MORINI |
| 11465 |
C |
| 11466 |
C INPUT: MICAP element IDs in KE = LD(LFP11) |
| 11467 |
C element densities in RHO = D (LFP12) |
| 11468 |
C |
| 11469 |
C Author : C.Zeitnitz |
| 11470 |
C |
| 11471 |
C See USER's GUIDE TO MICAP ORNL/TM-10340 |
| 11472 |
C for details and pointer description (MPOINT) |
| 11473 |
C |
| 11474 |
C************************************************************ |
| 11475 |
#include "mmicap.inc" |
| 11476 |
#include "minput.inc" |
| 11477 |
#include "mpoint.inc" |
| 11478 |
#include "mconst.inc" |
| 11479 |
#include "cmagic.inc" |
| 11480 |
*KEND. |
| 11481 |
C |
| 11482 |
CHARACTER*80 XSFILE |
| 11483 |
CHARACTER*70 CCOMM |
| 11484 |
CHARACTER*11 CGEANT |
| 11485 |
CHARACTER*4 MARK |
| 11486 |
CHARACTER*20 MATNAM |
| 11487 |
INTEGER INEL(134) |
| 11488 |
LOGICAL NOHED,XSTOP |
| 11489 |
C |
| 11490 |
C CALCULATE THE NUMBER OF ELEMENTS (NNUC) |
| 11491 |
C AND GENERATE THE ISOTOPE NUMBER ARRAY (IN(NMIX)) |
| 11492 |
NWTOT = 0 |
| 11493 |
DO 10 I=1,NMIX |
| 11494 |
LD(LFP17+I-1)=0 |
| 11495 |
LD(LFP16+I-1)=0 |
| 11496 |
10 CONTINUE |
| 11497 |
C INITIALIZE THE NUMBER OF ELEMENTS (NNUC) |
| 11498 |
NNUC=0 |
| 11499 |
DO 30 I=1,NMIX |
| 11500 |
IF(LD(LFP16+I-1).GT.0)GO TO 30 |
| 11501 |
NNUC=NNUC+1 |
| 11502 |
LD(LFP16+I-1)=NNUC |
| 11503 |
DO 20 J=I+1,NMIX |
| 11504 |
IF(LD(LFP11+I-1).NE.LD(LFP11+J-1))GO TO 20 |
| 11505 |
LD(LFP16+J-1)=NNUC |
| 11506 |
20 CONTINUE |
| 11507 |
30 CONTINUE |
| 11508 |
C get number of isoptopes from xsection file(s) |
| 11509 |
LT = LTEMP |
| 11510 |
NII = 0 |
| 11511 |
40 CONTINUE |
| 11512 |
NUNIT = IQ(LT+NTUNIT) |
| 11513 |
READ(NUNIT,'(I10)') NIS |
| 11514 |
NII = NII + NIS |
| 11515 |
IQ(LT+NTMPNI) = NIS |
| 11516 |
LT = LQ(LT) |
| 11517 |
IF(LT.GT.0) GOTO 40 |
| 11518 |
C allocate needed memory for x-section |
| 11519 |
NW = 2*NII+13*NNUC+2*NNR*NNUC+4*NGR*NNUC+3*NQ*NNUC+26*MEDIA + 2 |
| 11520 |
NI = NII |
| 11521 |
NWTOT = NWTOT + NW |
| 11522 |
CALL CHKZEB(NW,IXCONS) |
| 11523 |
CALL MZBOOK(IXCONS,LMOX1,0,2,'MOX1',0,0,NW,0,-1) |
| 11524 |
C SET UP THE B CONTROL BLOCK LOCATION NUMBER ARRAY ICOM(NNUC) |
| 11525 |
C LFP170 points to length of x-section data |
| 11526 |
LFP170 = LMOX1 + 2 |
| 11527 |
LFP18=LFP170+NNUC |
| 11528 |
LFP18A=LFP18+NII |
| 11529 |
LFP19=LFP18A+NII |
| 11530 |
LFP20=LFP19+NMIX |
| 11531 |
C SET UP THE ARRAY (IREC(NII)) |
| 11532 |
CALL XSECN1(NII,LD(LFP11),LD(LFP16),LD(LFP17), |
| 11533 |
+ LD(LFP18),LD(LFP18A),LD(LFP170),LD(LFP19), |
| 11534 |
+ D(LFP20),LD(LFP20),INEL) |
| 11535 |
C check if all isotopes have been found in the x-section file(s) |
| 11536 |
XSTOP = .FALSE. |
| 11537 |
DO 50 I=1,NMIX |
| 11538 |
IF(LD(LFP19+I-1).EQ.0) THEN |
| 11539 |
WRITE(IOUT,10100)LD(LFP19+I-1) |
| 11540 |
10000 FORMAT(' MICAP: Could not find x-section of element ',I8) |
| 11541 |
XSTOP = .TRUE. |
| 11542 |
ENDIF |
| 11543 |
50 CONTINUE |
| 11544 |
IF(XSTOP) THEN |
| 11545 |
PRINT '('' CALOR : Neutron x-section not found ===> STOP '')' |
| 11546 |
STOP |
| 11547 |
ENDIF |
| 11548 |
LFP21=LFP20+NNUC |
| 11549 |
C store xs accuracy at LFP210 (used for thinning in XSECN3) |
| 11550 |
LFP210 = LFP21 + NNUC |
| 11551 |
LFP22=LFP210+NNUC |
| 11552 |
LFP23=LFP22+NNUC |
| 11553 |
LFP24=LFP23+NNUC |
| 11554 |
LFP25=LFP24+NNUC |
| 11555 |
LFP26=LFP25+NNUC |
| 11556 |
LFP27=LFP26+NNR*NNUC |
| 11557 |
LFP28=LFP27+NNR*NNUC |
| 11558 |
LFP29=LFP28+NNUC |
| 11559 |
LFP30=LFP29+NNUC |
| 11560 |
LFP31=LFP30+NGR*NNUC |
| 11561 |
LFP32=LFP31+NGR*NNUC |
| 11562 |
LFP33=LFP32+MEDIA |
| 11563 |
LFP34=LFP33+MEDIA |
| 11564 |
LFP35=LFP34+NNUC |
| 11565 |
LFP36=LFP35+3*NQ*NNUC |
| 11566 |
C CLEAR THE STORAGE LOCATIONS FOR THE DICTIONARIES, ETC. |
| 11567 |
CALL CLEAR(LD,LFP20,LFP36-1) |
| 11568 |
C ESTABLISH THE RANDOM WALK STORAGE LOCATIONS |
| 11569 |
LFP41=LFP36 |
| 11570 |
LFP42=LFP41+2*NNUC |
| 11571 |
LFP45=LFP42+24*MEDIA |
| 11572 |
LFP46=LFP45+NGR*NNUC |
| 11573 |
NW = 0 |
| 11574 |
DO 60 INUC=1,NNUC |
| 11575 |
NW = NW + LD(LFP170+INUC-1) |
| 11576 |
60 CONTINUE |
| 11577 |
NW = NW + 2 |
| 11578 |
NWTOT = NWTOT + NW |
| 11579 |
CALL CHKZEB(NW,IXCONS) |
| 11580 |
CALL MZBOOK(IXCONS,LMOX2,0,2,'MOX2',0,0,NW,0,-1) |
| 11581 |
LFP43 = LMOX2 + 2 |
| 11582 |
LAST = LFP43 - 1 |
| 11583 |
MAXD = LMOX2 + NW |
| 11584 |
C PLACE THE MICROSCOPIC CROSS SECTION DATA INTO THE CORE |
| 11585 |
CALL XSECN2(LD(LFP17),LD(LFP18),LD(LFP18A), |
| 11586 |
+ LD(LFP20),LD(LFP21),D(LFP210),LD(LFP22),LD(LFP23), |
| 11587 |
+ LD(LFP24),LD(LFP25),LD(LFP26),LD(LFP27),LD(LFP28), |
| 11588 |
+ LD(LFP29),LD(LFP30),LD(LFP31),D(LFP34),D(LFP35), |
| 11589 |
+ LD(LFP35+NQ*NNUC),D(LFP35+2*NQ*NNUC), |
| 11590 |
+ D(LFP43),LD(LFP43),MAXD,LAST,INEL) |
| 11591 |
C determine length needed for macroscopic xs and mixing |
| 11592 |
C the bank has to store: |
| 11593 |
C - the xs of each isotope in the mixture |
| 11594 |
C - the mixed xs (defined by sum of diff. energy points) |
| 11595 |
NW = 0 |
| 11596 |
DO 90 IM=1,MEDIA |
| 11597 |
NM = 0 |
| 11598 |
LZ = 0 |
| 11599 |
DO 70 IN=1,NMIX |
| 11600 |
IF(LD(LFP10+IN-1).NE.IM) GOTO 70 |
| 11601 |
NM = NM+1 |
| 11602 |
II = LD(LFP16+IN-1) |
| 11603 |
LZ = LD(LFP27+NNR*(II-1))+LZ |
| 11604 |
C LZ = MAX0(LD(LFP27+NNR*(II-1)),LZ) |
| 11605 |
C LZ = MAX0(LDICT(1,II),LZ) |
| 11606 |
70 CONTINUE |
| 11607 |
C IF(NM.GT.1) LZ = 6*LZ |
| 11608 |
NW = NW + 2.*LZ |
| 11609 |
90 CONTINUE |
| 11610 |
NW = NW + 2 |
| 11611 |
NWTOT = NWTOT + NW |
| 11612 |
CALL CHKZEB(NW,IXCONS) |
| 11613 |
CALL MZBOOK(IXCONS,LMOX3,0,2,'MOX3',0,0,NW,0,-1) |
| 11614 |
LAST = LMOX3 + 1 |
| 11615 |
LFP44=LAST+1 |
| 11616 |
MAXD = LMOX3+NW |
| 11617 |
C SET, MIX AND THIN THE TOTAL CROSS SECTIONS |
| 11618 |
C ACCORDING TO THE MIXING TABLE |
| 11619 |
CALL XSECN3(LD(LFP10),LD(LFP11),D(LFP12),LD(LFP16),LD(LFP26), |
| 11620 |
+ LD(LFP27),LD(LFP32),LD(LFP33),D(LFP44),LD(LFP44), |
| 11621 |
+ D,MAXD,LAST) |
| 11622 |
C ESTABLISH THE PHOTON TOTAL CROSS SECTION DATA DICTIONARY |
| 11623 |
C STORAGE LOCATIONS |
| 11624 |
C determine number of words needed for photon production xs |
| 11625 |
NW = 0 |
| 11626 |
DO 110 I=1,NNUC |
| 11627 |
DO 100 J=1,LD(LFP28+I-1) |
| 11628 |
LZ = LD(LFP31 + 2*J - 1 + NGR*(I-1)) |
| 11629 |
C LZ = LGCB(2*J,I) |
| 11630 |
NW = NW + LZ |
| 11631 |
100 CONTINUE |
| 11632 |
110 CONTINUE |
| 11633 |
NW = NW + 2*NGR*NNUC+2 |
| 11634 |
NWTOT = NWTOT + NW + 1 |
| 11635 |
CALL CHKZEB(NW,IXCONS) |
| 11636 |
CALL MZBOOK(IXCONS,LMOX4,0,2,'MOX4',0,0,NW,0,-1) |
| 11637 |
LMAG2 = LMOX4 + 1 |
| 11638 |
LD(LMAG2) = NMAGIC |
| 11639 |
LFP45 = LMAG2 + 1 |
| 11640 |
LFP46 = LFP45 + NGR*NNUC |
| 11641 |
LFP47 = LFP46 + NGR*NNUC |
| 11642 |
LAST = LFP47 - 1 |
| 11643 |
MAXD = LMOX4 + NW |
| 11644 |
C CLEAR THE STORAGE LOCATIONS FOR THE PHOTON DICTIONARIES |
| 11645 |
C OF THE TOTAL PHOTON PRODUCTION CROSS SECTIONS |
| 11646 |
CALL CLEAR(LD,LFP45,LFP47-1) |
| 11647 |
C SUM THE PHOTON PARTIAL DISTRIBUTIONS OF THE ENDF/B-V |
| 11648 |
C FILE 12 AND FILE 13 DATA (BY MT NUMBER) AND PLACE THESE |
| 11649 |
C MICROSCOPIC MULTIPLICITIES TIMES CROSS SECTIONS IN CORE |
| 11650 |
CALL XSECN5(LD(LFP28),LD(LFP30),LD(LFP31),LD(LFP45),LD(LFP46), |
| 11651 |
+ D(LFP47),LD(LFP47),D,LD,MAXD,LAST) |
| 11652 |
C |
| 11653 |
C print out media to print unit IOUT |
| 11654 |
C WRITE(IOUT,10000) |
| 11655 |
10100 FORMAT(23X,'MICAP Material Parameters',/, |
| 11656 |
+ 23X,'-------------------------',/) |
| 11657 |
WRITE(IOUT,10200) |
| 11658 |
10200 FORMAT(8X,'GEANT Material Parameters',10X, |
| 11659 |
+ 6X,'MICAP Material Parameters',/, |
| 11660 |
+ 8X,25('-'),10X,6X,25('-')) |
| 11661 |
WRITE(IOUT,10300) |
| 11662 |
10300 FORMAT(1X,'Material',16X,'No/Iso',4X,'A',5X,'Z',2X,'|', |
| 11663 |
+ 4X,'A',5X,'Z',3X,'Density', |
| 11664 |
+ 3X,'Coll.Len',/,44('-'),'+',33('-')) |
| 11665 |
MFLAG = 0 |
| 11666 |
KMED = 0 |
| 11667 |
NISO = 1 |
| 11668 |
DO 130 I=0,NMIX-1 |
| 11669 |
C get GEANT name of material |
| 11670 |
MARK = '/ ' |
| 11671 |
IF(LD(LFP11+I)/1000.NE.LD(LFP13+I).OR. |
| 11672 |
+ (I.LT.NMIX-1.AND.D(LFP140+I).NE.0..AND.D(LFP140+I+1).NE.0. |
| 11673 |
+ .AND.NINT(D(LFP34+LD(LFP16+I)-1)*1.008665) |
| 11674 |
+ .NE.NINT(D(LFP140+I)))) THEN |
| 11675 |
MARK = '/ *' |
| 11676 |
MFLAG=1 |
| 11677 |
ENDIF |
| 11678 |
K1 = LD(LFP16+I)-1 |
| 11679 |
LS1 = LD(LFP26+NNR*K1)+LMOX2 |
| 11680 |
LEN = LD(LFP27+NNR*K1)/2 |
| 11681 |
EN = 1.E6 |
| 11682 |
CALL TBSPLT(D(LS1),EN,LEN,XSEC) |
| 11683 |
XSEC = 1./XSEC/D(LFP12+I) |
| 11684 |
IF(D(LFP140+I).NE.0.) THEN |
| 11685 |
WRITE(CGEANT,'(F6.1,I5)') D(LFP140+I),LD(LFP13+I) |
| 11686 |
ELSE |
| 11687 |
WRITE(CGEANT,'(A11)') ' - -' |
| 11688 |
ENDIF |
| 11689 |
IF(KMED.NE.LD(LFP10+I)) THEN |
| 11690 |
NISO = 1 |
| 11691 |
CALL GFMATE(LD(LGE2MO+LD(LFP10+I)),MATNAM,AA,ZZ,DENS, |
| 11692 |
+ RADL,ABSL,UB,NW) |
| 11693 |
NBLK = LNBLNK(MATNAM) |
| 11694 |
DO 120 JC=NBLK+1,20 |
| 11695 |
WRITE(MATNAM(JC:JC),'(A1)') '.' |
| 11696 |
120 CONTINUE |
| 11697 |
WRITE(MARK(2:3),'(I2)') NISO |
| 11698 |
WRITE(IOUT,10400) MATNAM,LD(LGE2MO+LD(LFP10+I)),MARK, |
| 11699 |
+ CGEANT, |
| 11700 |
+ D(LFP34+LD(LFP16+I)-1)*1.008665, |
| 11701 |
+ LD(LFP11+I)/1000,D(LFP12+I),XSEC |
| 11702 |
KMED = LD(LFP10+I) |
| 11703 |
ELSE |
| 11704 |
WRITE(MARK(2:3),'(I2)') NISO |
| 11705 |
WRITE(IOUT,10500) LD(LGE2MO+LD(LFP10+I)),MARK,CGEANT, |
| 11706 |
+ D(LFP34+LD(LFP16+I)-1)*1.008665, |
| 11707 |
+ LD(LFP11+I)/1000,D(LFP12+I),XSEC |
| 11708 |
ENDIF |
| 11709 |
10400 FORMAT(1X,A20,I6,A4,A11,' |',F6.1,I5,1X,E11.4,1X,E9.3) |
| 11710 |
10500 FORMAT(1X,20X,I6,A4,A11,' |',F6.1,I5,1X,E11.4,1X,E9.3) |
| 11711 |
LD(LFP13+I) = LD(LFP11+I)/1000 |
| 11712 |
NISO = NISO + 1 |
| 11713 |
130 CONTINUE |
| 11714 |
WRITE(IOUT,'(78(''-''),/,48X,''Density in (Atoms/barn/cm)'')') |
| 11715 |
WRITE(IOUT,'(36X, ' |
| 11716 |
+ //' ''Collision Length for 1 MeV neutron in (cm)'',/)') |
| 11717 |
IF(MFLAG.EQ.1) WRITE(IOUT,'(/, ' |
| 11718 |
+ //'15X,''*******************************************'',/, ' |
| 11719 |
+ //'15X,''* W A R N I N G *'',/, ' |
| 11720 |
+ //'15X,''* Marked isotopes (*) not found in the *'',/, ' |
| 11721 |
+ //'15X,''* cross-section file(s) *'',/, ' |
| 11722 |
+ //'15X,''* Cross-sections of the isotope with *'',/, ' |
| 11723 |
+ //'15X,''* the closest Z will be used instead *'',/, ' |
| 11724 |
+ //'15X,''*******************************************'',/)') |
| 11725 |
C which x-section files have been used? |
| 11726 |
LT = LTEMP |
| 11727 |
LCI = LCISO |
| 11728 |
LC = 0 |
| 11729 |
NOHED=.TRUE. |
| 11730 |
140 CONTINUE |
| 11731 |
C first check if x-section file has been used! |
| 11732 |
NUNIT = IQ(LT+NTUNIT) |
| 11733 |
DO 150 I=0,NMIX-1 |
| 11734 |
KISO = LD(LFP16+I) |
| 11735 |
MISO = LD(LFP17+KISO-1) |
| 11736 |
IF(NUNIT.EQ.LD(LFP18A+MISO-1)) GOTO 160 |
| 11737 |
150 CONTINUE |
| 11738 |
C unit never used ! |
| 11739 |
GOTO 190 |
| 11740 |
160 CONTINUE |
| 11741 |
C search for comments for selected isotopes |
| 11742 |
NCOM = IQ(LCI+1) |
| 11743 |
DO 180 J=1,NCOM |
| 11744 |
K = (J-1)*81 + 2 |
| 11745 |
JZ = IQ(LCI+K) |
| 11746 |
JA = IQ(LCI+K+1) |
| 11747 |
CCOMM = ' ' |
| 11748 |
CALL UHTOC(IQ(LCI+K+2),4,CCOMM,70) |
| 11749 |
DO 170 I=0,NMIX-1 |
| 11750 |
KISO = LD(LFP16+I) |
| 11751 |
IA = NINT(D(LFP34+KISO-1)*1.008665) |
| 11752 |
IZ = LD(LFP11+I)/1000 |
| 11753 |
MISO = LD(LFP17+KISO-1) |
| 11754 |
C print the comment, if the isotope is correct and has been read from |
| 11755 |
C the current x-section file |
| 11756 |
IF(IA.EQ.JA .AND. IZ.EQ.JZ .AND. |
| 11757 |
+ NUNIT.EQ.LD(LFP18A+MISO-1)) THEN |
| 11758 |
IF(NOHED) THEN |
| 11759 |
WRITE(IOUT,'(/,23X,''COMMENTS ABOUT ISOTOPE DATA'')') |
| 11760 |
WRITE(IOUT,'( 23X,''---------------------------'',/)') |
| 11761 |
NOHED = .FALSE. |
| 11762 |
ENDIF |
| 11763 |
LC = LC + 1 |
| 11764 |
WRITE(IOUT,'(I4,'') '',A70)') LC,CCOMM |
| 11765 |
GOTO 180 |
| 11766 |
ENDIF |
| 11767 |
170 CONTINUE |
| 11768 |
180 CONTINUE |
| 11769 |
190 LT = LQ(LT) |
| 11770 |
LCI = LQ(LCI) |
| 11771 |
IF(LT.GT.0.AND.LCI.GT.0) GOTO 140 |
| 11772 |
C print the x-section file names and comments |
| 11773 |
WRITE(IOUT,'(/,20X,''USED NEUTRON CROSS-SECTION FILES'')') |
| 11774 |
WRITE(IOUT,'( 20X,''--------------------------------'',/)') |
| 11775 |
LT = LTEMP |
| 11776 |
200 CONTINUE |
| 11777 |
C first check if x-section file has been used! |
| 11778 |
NUNIT = IQ(LT+NTUNIT) |
| 11779 |
DO 210 I=0,NMIX-1 |
| 11780 |
KISO = LD(LFP16+I) |
| 11781 |
MISO = LD(LFP17+KISO-1) |
| 11782 |
IF(NUNIT.EQ.LD(LFP18A+MISO-1)) GOTO 220 |
| 11783 |
210 CONTINUE |
| 11784 |
C unit never used ! |
| 11785 |
GOTO 230 |
| 11786 |
220 CONTINUE |
| 11787 |
C get file name of x-section file |
| 11788 |
XSFILE = ' ' |
| 11789 |
COMMEN = ' ' |
| 11790 |
DATSTR = ' ' |
| 11791 |
CALL UHTOC(IQ(LT+NTNAME+1),4,XSFILE,IQ(LT+NTNAME)) |
| 11792 |
CALL UHTOC(IQ(LT+NTCOMM+1),4,COMMEN,IQ(LT+NTCOMM)) |
| 11793 |
CALL UHTOC(IQ(LT+NTDATS+1),4,DATSTR,IQ(LT+NTDATS)) |
| 11794 |
WRITE(IOUT,'('' File : '',A66)') XSFILE |
| 11795 |
WRITE(IOUT,'('' Generated : '',A24,/, ' |
| 11796 |
+ //' '' Comment : '',A66,/)') DATSTR,COMMEN |
| 11797 |
230 LT = LQ(LT) |
| 11798 |
IF(LT.GT.0) GOTO 200 |
| 11799 |
WRITE(IOUT,'(/,'' MICAP :'',I10, ' |
| 11800 |
+ //' '' words used in GCBANK for neutron x-section tables''/)') |
| 11801 |
+ NWTOT |
| 11802 |
RETURN |
| 11803 |
END |
| 11804 |
*CMZ : 1.01/04 10/06/93 14.43.48 by Christian Zeitnitz |
| 11805 |
*-- Author : |
| 11806 |
SUBROUTINE N2NN3N(D,LD,AWR,KZ,ID,FM,Q,IFLG) |
| 11807 |
C THIS ROUTINE CALCULATES THE DIRECTIONAL COSINES FOR THE |
| 11808 |
C NEUTRON AND RECOIL NUCLEUS FOR AN N2N OR N3N REACTION |
| 11809 |
C USING THE ONE NEUTRON EMMISION MODEL. IT ALSO SETS ALL |
| 11810 |
C EXIT PARAMETRS FOR THE RECOIL NUCLEUS. |
| 11811 |
#include "minput.inc" |
| 11812 |
#include "mconst.inc" |
| 11813 |
#include "mnutrn.inc" |
| 11814 |
#include "mrecoi.inc" |
| 11815 |
#include "mapoll.inc" |
| 11816 |
#include "mmass.inc" |
| 11817 |
#include "mpstor.inc" |
| 11818 |
*KEND. |
| 11819 |
DIMENSION D(*),LD(*),FM(*) |
| 11820 |
SAVE |
| 11821 |
MT=0 |
| 11822 |
IF(ID.EQ.8)MT=16 |
| 11823 |
IF(ID.EQ.9)MT=17 |
| 11824 |
IF(ID.EQ.12)MT=24 |
| 11825 |
C IFLG EQUAL TO ONE IMPLIES THE DIRECTION COSINES WERE |
| 11826 |
C SELECTED ISOTROPICALLY IN THE LABORATORY COORDINATE SYSTEM |
| 11827 |
C CALCULATE THE NEUTRON EXIT DIRECTIONAL COSINES |
| 11828 |
POX = 0.0 |
| 11829 |
POY = 0.0 |
| 11830 |
POZ = 0.0 |
| 11831 |
DO 40 KN=1,INEU |
| 11832 |
IF(IFLG.EQ.1) THEN |
| 11833 |
CALL GTISO(UP,VP,WP) |
| 11834 |
ELSE |
| 11835 |
SINPSI=SQRT(1.0-FM(KN)**2) |
| 11836 |
CALL AZIRN(SINETA,COSETA) |
| 11837 |
STHETA=1.0-UOLD**2 |
| 11838 |
IF(STHETA)20,20,10 |
| 11839 |
10 STHETA=SQRT(STHETA) |
| 11840 |
COSPHI=VOLD/STHETA |
| 11841 |
SINPHI=WOLD/STHETA |
| 11842 |
GO TO 30 |
| 11843 |
20 COSPHI=1.0 |
| 11844 |
SINPHI=0.0 |
| 11845 |
STHETA=0.0 |
| 11846 |
30 UP = UOLD*FM(KN)-COSETA*SINPSI*STHETA |
| 11847 |
VP = VOLD*FM(KN)+UOLD*COSPHI*COSETA*SINPSI-SINPHI* SINPSI* |
| 11848 |
+ SINETA |
| 11849 |
WP = WOLD*FM(KN)+UOLD*SINPHI*COSETA*SINPSI+COSPHI* SINPSI* |
| 11850 |
+ SINETA |
| 11851 |
S=1.0/SQRT(UP*UP+VP*VP+WP*WP) |
| 11852 |
UP=UP*S |
| 11853 |
VP=VP*S |
| 11854 |
WP=WP*S |
| 11855 |
ENDIF |
| 11856 |
EP = ENE(KN) |
| 11857 |
C use ONLY first neutron for recoil calculation in order the ensure |
| 11858 |
C correct energy spectrum of recoil nucleus |
| 11859 |
IF(KN.EQ.1) THEN |
| 11860 |
PP = SQRT(EP**2 + 2.0*EP*ZN) |
| 11861 |
POX = POX + PP*UP |
| 11862 |
POY = POY + PP*VP |
| 11863 |
POZ = POZ + PP*WP |
| 11864 |
ENDIF |
| 11865 |
AGEP = AGE |
| 11866 |
MTP = MT |
| 11867 |
CALL STOPAR(IDNEU,NNEU) |
| 11868 |
40 CONTINUE |
| 11869 |
C CALCULATE AND SET THE RECOIL NUCLEUS EXIT PARAMETERS |
| 11870 |
50 XR=X |
| 11871 |
YR=Y |
| 11872 |
ZR=Z |
| 11873 |
WATER=WTBC |
| 11874 |
NZR=KZ |
| 11875 |
ZMP = FLOAT(KZ) |
| 11876 |
AGER=AGE |
| 11877 |
AGEP = AGE |
| 11878 |
NCOLR=NCOL |
| 11879 |
MTNR=MT |
| 11880 |
MTP = MT |
| 11881 |
AR = (AWR*AN) - FLOAT(INEU-1)*AN |
| 11882 |
AMP = AR |
| 11883 |
ENIR=EOLD |
| 11884 |
UNIR=UOLD |
| 11885 |
VNIR=VOLD |
| 11886 |
WNIR=WOLD |
| 11887 |
ENOR=E |
| 11888 |
UNOR=U |
| 11889 |
VNOR=V |
| 11890 |
WNOR=W |
| 11891 |
WTNR=WATE |
| 11892 |
QR=Q |
| 11893 |
C CALCULATE THE NEUTRON MOMENTUM BEFORE AND AFTER COLLISION |
| 11894 |
C NEUTRON MOMENTUM BEFORE COLLISION (PI) EQUALS TOTAL MOMENTUM |
| 11895 |
PI=SQRT(2.0*ZN*EOLD) |
| 11896 |
C CALCULATE THE DIRECTIONAL MOMENTUM OF THE RECOIL NUCLEUS |
| 11897 |
PIX=PI*UOLD |
| 11898 |
PIY=PI*VOLD |
| 11899 |
PIZ=PI*WOLD |
| 11900 |
PRX = PIX - POX |
| 11901 |
PRY = PIY - POY |
| 11902 |
PRZ = PIZ - POZ |
| 11903 |
C CALCULATE THE TOTAL MOMENTUM OF THE RECOIL NUCLEUS |
| 11904 |
PR=SQRT(PRX**2+PRY**2+PRZ**2) |
| 11905 |
C CALCULATE THE RECOIL NUCLEUS DIRECTIONAL COSINES |
| 11906 |
UR=PRX/PR |
| 11907 |
VR=PRY/PR |
| 11908 |
WR=PRZ/PR |
| 11909 |
UP = UR |
| 11910 |
VP = VR |
| 11911 |
WP = WR |
| 11912 |
C CALCULATE THE RECOIL NUCLEUS EXIT ENERGY |
| 11913 |
XM = AR*931.075E6 |
| 11914 |
ER= SQRT(PR**2 + XM**2) - XM |
| 11915 |
EP = ER |
| 11916 |
MTP = MT |
| 11917 |
C IF MT=24, DO NOT STORE THE RECOIL HEAVY ION IN THE BANK |
| 11918 |
IF(MT.EQ.24)RETURN |
| 11919 |
C STORE THE RECOIL HEAVY ION IN THE RECOIL BANK |
| 11920 |
CALL STOPAR(IDHEVY,NHEVY) |
| 11921 |
RETURN |
| 11922 |
END |
| 11923 |
*CMZ : 1.01/00 01/06/93 09.05.16 by Christian Zeitnitz |
| 11924 |
*-- Author : |
| 11925 |
SUBROUTINE NGHEVY(D,LD,KZ,AWR,Q,MT) |
| 11926 |
C THIS ROUTINE CALCULATES THE EXIT ENERGY AND DIRECTIONAL |
| 11927 |
C COSINES FOR THE RECOIL NUCLEUS RESULTING FROM THE (N,G) |
| 11928 |
C REACTION MT-102, AND STORES THE RECOIL NUCLEUS IN THE |
| 11929 |
C HEAVY ION BANK. THE ENERGY AND DIRECTIONAL COSINES ARE |
| 11930 |
C DETERMINED BY A MOMENTUM BALANCE IN THE LABORATORY SYSTEM |
| 11931 |
C WITH THE PHOTONS MOMENTUM EQUAL TO ITS ENERGY. |
| 11932 |
#include "minput.inc" |
| 11933 |
#include "mconst.inc" |
| 11934 |
#include "mnutrn.inc" |
| 11935 |
#include "mrecoi.inc" |
| 11936 |
#include "mapoll.inc" |
| 11937 |
#include "mmass.inc" |
| 11938 |
#include "mpstor.inc" |
| 11939 |
#include "mgamma.inc" |
| 11940 |
*KEND. |
| 11941 |
DIMENSION D(*),LD(*) |
| 11942 |
SAVE |
| 11943 |
AR=AWR*AN+AN |
| 11944 |
C CALCULATE THE TOTAL MOMENTUM BEFORE THE COLLISION |
| 11945 |
C NEUTRON MOMENTUM BEFORE COLLISION (PI) EQUALS TOTAL MOMENTUM |
| 11946 |
PI=SQRT(2.0*ZN*EOLD) |
| 11947 |
C CALCULATE THE TOTAL MOMEMTUM OF THE EXIT PHOTON |
| 11948 |
PO=EG*1.00E+06 |
| 11949 |
C CALCULATE THE DIRECTIONAL MOMENTUM OF THE RECOIL NUCLEUS |
| 11950 |
PRX=PI*UOLD-PO*UG |
| 11951 |
PRY=PI*VOLD-PO*VG |
| 11952 |
PRZ=PI*WOLD-PO*WG |
| 11953 |
C CALCULATE THE TOTAL MOMENTUM OF THE RECOIL NUCLEUS |
| 11954 |
PR=SQRT(PRX**2+PRY**2+PRZ**2) |
| 11955 |
C CALCULATE THE RECOIL NUCLEUS DIRECTIONAL COSINES |
| 11956 |
UR=PRX/PR |
| 11957 |
VR=PRY/PR |
| 11958 |
WR=PRZ/PR |
| 11959 |
C CALCULATE THE RECOIL NUCLEUS EXIT ENERGY |
| 11960 |
ER=PR**2/(2*AR*9.31075E+08) |
| 11961 |
C CALCULATE AND SET THE CHARGED PARTICLE EXIT PARAMETERS |
| 11962 |
XR=X |
| 11963 |
YR=Y |
| 11964 |
ZR=Z |
| 11965 |
WATER=WTBC |
| 11966 |
NZR=KZ |
| 11967 |
AGER=AGE |
| 11968 |
NCOLR=NCOL |
| 11969 |
MTNR=MT |
| 11970 |
ENIR=EOLD |
| 11971 |
UNIR=UOLD |
| 11972 |
VNIR=VOLD |
| 11973 |
WNIR=WOLD |
| 11974 |
ENOR=0.0 |
| 11975 |
UNOR=0.0 |
| 11976 |
VNOR=0.0 |
| 11977 |
WNOR=0.0 |
| 11978 |
WTNR=0.0 |
| 11979 |
QR=Q |
| 11980 |
C STORE THE RECOIL HEAVY ION IN THE RECOIL BANK |
| 11981 |
EP = ER |
| 11982 |
UP = UR |
| 11983 |
VP = VR |
| 11984 |
WP = WR |
| 11985 |
AMP = AR |
| 11986 |
ZMP = FLOAT(NZR) |
| 11987 |
AGEP = AGE |
| 11988 |
MTP = MT |
| 11989 |
CALL STOPAR(IDHEVY,NHEVY) |
| 11990 |
RETURN |
| 11991 |
END |
| 11992 |
*CMZ : 0.90/00 03/08/92 17.58.51 by Christian Zeitnitz |
| 11993 |
*-- Author : |
| 11994 |
SUBROUTINE NN2BOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,Q,MT) |
| 11995 |
C THIS ROUTINE CALCULATES THE EXIT ENERGIES AND DIRECTIONAL |
| 11996 |
C COSINES FOR THE CHARGED PARTICLE AND RECOIL NUCLEUS FOR |
| 11997 |
C A TWO-BODY REACTION USING AN EVAPORATION SPECTRUM AND |
| 11998 |
C MOMEMTUM BALANCE. IT ALSO SETS ALL EXIT PARAMETERS FOR |
| 11999 |
C THE COLLISION PRODUCTS AND STORES THEM IN THE RECOIL BANK. |
| 12000 |
C THE TWO BODY REACTION RESULTS FROM THE BREAK-UP OF A NUCLEUS |
| 12001 |
C LEFT IN AN EXCITED STATE BY AN INELASTIC COLLISION OR A |
| 12002 |
C N,2N REACTION (I.E. MT-24). |
| 12003 |
#include "minput.inc" |
| 12004 |
#include "mconst.inc" |
| 12005 |
#include "mrecoi.inc" |
| 12006 |
#include "mapoll.inc" |
| 12007 |
#include "mmass.inc" |
| 12008 |
#include "mpstor.inc" |
| 12009 |
#include "mnutrn.inc" |
| 12010 |
*KEND. |
| 12011 |
DIMENSION D(*),LD(*) |
| 12012 |
SAVE |
| 12013 |
C TRANSFER THE RECOILING COMPOUND NUCLEUS PARAMETERS OUT OF |
| 12014 |
C COMMON RECOIL FOR USE IN THE MOMENTUM BALANCE EQUATIONS |
| 12015 |
ERCN=ER |
| 12016 |
URCN=UR |
| 12017 |
VRCN=VR |
| 12018 |
WRCN=WR |
| 12019 |
ARCN=AR |
| 12020 |
NZRCN=NZR |
| 12021 |
ZARCN=ARCN*9.31075E+08 |
| 12022 |
C CALCULATE THE COULOMB BARRIER (CB) |
| 12023 |
CALL BARIER(KZ1,KZ2,A1,A2,CB) |
| 12024 |
C CALCULATE THE CHARGED PARTICLE EXIT ENERGY (EX) |
| 12025 |
CALL CEVAP1(EOLD,E,Q,ATAR,CB,EX) |
| 12026 |
E1=EX+CB |
| 12027 |
C ASSUME ISOTROPIC CHARGED PARTICLE EMISSION IN THE LABORATORY |
| 12028 |
CALL GTISO(U1,V1,W1) |
| 12029 |
C CALCULATE AND SET THE CHARGED PARTICLE EXIT PARAMETERS |
| 12030 |
XR=X |
| 12031 |
YR=Y |
| 12032 |
ZR=Z |
| 12033 |
WATER=WTBC |
| 12034 |
NZR=KZ1 |
| 12035 |
AGER=AGE |
| 12036 |
NCOLR=NCOL |
| 12037 |
MTNR=MT |
| 12038 |
AR=A1 |
| 12039 |
ENIR=EOLD |
| 12040 |
UNIR=UOLD |
| 12041 |
VNIR=VOLD |
| 12042 |
WNIR=WOLD |
| 12043 |
ENOR=E |
| 12044 |
UNOR=U |
| 12045 |
VNOR=V |
| 12046 |
WNOR=W |
| 12047 |
WTNR=WATE |
| 12048 |
QR=Q |
| 12049 |
UR=U1 |
| 12050 |
VR=V1 |
| 12051 |
WR=W1 |
| 12052 |
ER=E1 |
| 12053 |
C STORE THE CHARGED PARTICLE IN THE RECOIL BANK |
| 12054 |
EP = ER |
| 12055 |
UP = UR |
| 12056 |
VP = VR |
| 12057 |
WP = WR |
| 12058 |
AGEP = AGE |
| 12059 |
MTP = MT |
| 12060 |
AMP = AR |
| 12061 |
ZMP = FLOAT(NZR) |
| 12062 |
CALL STOPAR(IDHEVY,NHEVY) |
| 12063 |
C CALCULATE THE TOTAL MOMENTUM BEFORE THE COLLISION |
| 12064 |
C COMPOUND NUCLEUS MOMENTUM BEFORE THE COLLISION (PI) EQUALS |
| 12065 |
C THE TOTAL MOMENTUM |
| 12066 |
PI=SQRT(2.0*ZARCN*ERCN) |
| 12067 |
C CALCULATE THE TOTAL MOMEMTUM OF THE EXIT CHARGED PARTICLE |
| 12068 |
PO=SQRT(2.0*Z1*E1) |
| 12069 |
C CALCULATE THE DIRECTIONAL MOMENTUM OF THE RECOIL NUCLEUS |
| 12070 |
PRX=PI*URCN-PO*U1 |
| 12071 |
PRY=PI*VRCN-PO*V1 |
| 12072 |
PRZ=PI*WRCN-PO*W1 |
| 12073 |
C CALCULATE THE TOTAL MOMENTUM OF THE RECOIL NUCLEUS |
| 12074 |
PR=SQRT(PRX**2+PRY**2+PRZ**2) |
| 12075 |
C CALCULATE THE RECOIL NUCLEUS DIRECTIONAL COSINES |
| 12076 |
U2=PRX/PR |
| 12077 |
V2=PRY/PR |
| 12078 |
W2=PRZ/PR |
| 12079 |
C CALCULATE THE RECOIL NUCLEUS EXIT ENERGY |
| 12080 |
XM = A2 * 931.075E6 |
| 12081 |
E2 = SQRT(PR**2 + XM**2) - XM |
| 12082 |
C CALCULATE AND SET THE CHARGED PARTICLE EXIT PARAMETERS |
| 12083 |
XR=X |
| 12084 |
YR=Y |
| 12085 |
ZR=Z |
| 12086 |
WATER=WTBC |
| 12087 |
NZR=KZ2 |
| 12088 |
AGER=AGE |
| 12089 |
NCOLR=NCOL |
| 12090 |
MTNR=MT |
| 12091 |
AR=A2 |
| 12092 |
ENIR=EOLD |
| 12093 |
UNIR=UOLD |
| 12094 |
VNIR=VOLD |
| 12095 |
WNIR=WOLD |
| 12096 |
ENOR=E |
| 12097 |
UNOR=U |
| 12098 |
VNOR=V |
| 12099 |
WNOR=W |
| 12100 |
WTNR=WATE |
| 12101 |
QR=Q |
| 12102 |
UR=U2 |
| 12103 |
VR=V2 |
| 12104 |
WR=W2 |
| 12105 |
ER=E2 |
| 12106 |
C STORE THE RECOIL HEAVY ION IN THE RECOIL BANK |
| 12107 |
EP = ER |
| 12108 |
UP = UR |
| 12109 |
VP = VR |
| 12110 |
WP = WR |
| 12111 |
AGEP = AGE |
| 12112 |
MTP = MT |
| 12113 |
AMP = AR |
| 12114 |
ZMP = FLOAT(NZR) |
| 12115 |
CALL STOPAR(IDHEVY,NHEVY) |
| 12116 |
RETURN |
| 12117 |
END |
| 12118 |
*CMZ : 0.94/04 18/03/93 22.56.07 by Christian Zeitnitz |
| 12119 |
*-- Author : |
| 12120 |
SUBROUTINE NSIGTA(E,JMED,TSIG,D,ISIGTS,LSIGT) |
| 12121 |
C THIS ROUTINE DETERMINES THE MACROSCOPIC TOTAL |
| 12122 |
C CROSS SECTION FOR MEDIA MED |
| 12123 |
#include "mmicab.inc" |
| 12124 |
*KEND. |
| 12125 |
DIMENSION D(*),ISIGTS(*),LSIGT(*) |
| 12126 |
CALL GTMED(JMED,MED) |
| 12127 |
TSIG=0.0 |
| 12128 |
L1=LSIGT(MED) |
| 12129 |
LS1=ISIGTS(MED)+LMOX3 |
| 12130 |
LEN=L1/2 |
| 12131 |
CALL TBSPLT(D(LS1),E,LEN,TSIG) |
| 12132 |
RETURN |
| 12133 |
END |
| 12134 |
*CMZ : 1.01/04 10/06/93 14.43.48 by Christian Zeitnitz |
| 12135 |
*-- Author : |
| 12136 |
SUBROUTINE PARTXS(D,LD,E,SIGTOT,EP) |
| 12137 |
C THIS ROUTINE SAMPLES FROM THE FILE 12 OR 13 PHOTON |
| 12138 |
C PRODUCTION PARTIAL DISTRIBUTIONS TO OBTAIN THE EXIT |
| 12139 |
C PHOTON ENERGY FROM A NEUTRON REACTION |
| 12140 |
#include "minput.inc" |
| 12141 |
*KEND. |
| 12142 |
DIMENSION D(*),LD(*) |
| 12143 |
SAVE |
| 12144 |
C INITIALIZE THE VALUES USED IN THE SELECTION PROCESS |
| 12145 |
C THE VALUE (II) IS A POINTER |
| 12146 |
ITRY1=0 |
| 12147 |
10 R=FLTRNF(0) |
| 12148 |
SUM=0.0 |
| 12149 |
NH=0 |
| 12150 |
NL=0 |
| 12151 |
II=0 |
| 12152 |
C SET THE NUMBER OF PARTIAL DISTRIBUTIONS (NK) AND THE NUMBER |
| 12153 |
C OF POINTS PER PARTIAL DISTRIBUTION (NP) |
| 12154 |
NK=LD(II+1) |
| 12155 |
NP=LD(II+2) |
| 12156 |
II=II+2 |
| 12157 |
C DETERMINE WHICH POINTS (NL) AND (NH) BOUND THE INCIDENT |
| 12158 |
C NEUTRON ENERGY |
| 12159 |
DO 20 N=1,NP |
| 12160 |
IF(E.LE.D(II+N))GO TO 40 |
| 12161 |
20 CONTINUE |
| 12162 |
C THE INCIDENT NEUTRON ENERGY IS GREATER THAN THE LAST ENERGY |
| 12163 |
C POINT OF THE PARTIAL DISTRIBUTIONS, THEREFORE USE THE LAST |
| 12164 |
C ENERGY POINT OF THE PARTIAL DISTRIBUTION TO SAMPLE FROM |
| 12165 |
NH=NP |
| 12166 |
II=II+NP |
| 12167 |
DO 30 K=1,NK |
| 12168 |
EP=D(II+1) |
| 12169 |
LP=LD(II+2) |
| 12170 |
A=D(II+3) |
| 12171 |
LF=LD(II+4) |
| 12172 |
IF(LP.EQ.2)EP=EP+(A/(A+1))*E |
| 12173 |
II=II+4 |
| 12174 |
SIG=D(II+NH) |
| 12175 |
SUM=SUM+SIG/SIGTOT |
| 12176 |
IF(EP.EQ.0.0)GO TO 100 |
| 12177 |
IF(R.LE.SUM)GO TO 100 |
| 12178 |
II=II+NP |
| 12179 |
30 CONTINUE |
| 12180 |
GO TO 80 |
| 12181 |
40 IF(N.EQ.1)GO TO 60 |
| 12182 |
C THE INCIDENT NEUTRON ENERGY IS BOUNDED BY THE ENEGY POINTS |
| 12183 |
C (NL) AND (NH) OF THE PARTIAL DISTRIBUTIONS, THEREFORE USE |
| 12184 |
C LINEAR INTERPOLATION |
| 12185 |
NH=N |
| 12186 |
NL=N-1 |
| 12187 |
EH=D(II+NH) |
| 12188 |
EL=D(II+NL) |
| 12189 |
II=II+NP |
| 12190 |
DO 50 K=1,NK |
| 12191 |
EP=D(II+1) |
| 12192 |
LP=LD(II+2) |
| 12193 |
A=D(II+3) |
| 12194 |
LF=LD(II+4) |
| 12195 |
IF(LP.EQ.2)EP=EP+(A/(A+1))*E |
| 12196 |
II=II+4 |
| 12197 |
SIG=D(II+NL)+(E-EL)*(D(II+NH)-D(II+NL))/(EH-EL) |
| 12198 |
SUM=SUM+SIG/SIGTOT |
| 12199 |
IF(EP.EQ.0.0)GO TO 100 |
| 12200 |
IF(R.LE.SUM)GO TO 100 |
| 12201 |
II=II+NP |
| 12202 |
50 CONTINUE |
| 12203 |
GO TO 80 |
| 12204 |
C THE INCIDENT NEUTRON ENERGY IS LESS THAN THE FIRST ENERGY |
| 12205 |
C POINT OF THE PARTIAL DISTRIBUTIONS, THEREFORE USE THE FIRST |
| 12206 |
C ENERGY POINT OF THE PARTIAL DISTRIBUTION TO SAMPLE FROM |
| 12207 |
60 NL=N |
| 12208 |
II=II+NP |
| 12209 |
DO 70 K=1,NK |
| 12210 |
EP=D(II+1) |
| 12211 |
LP=LD(II+2) |
| 12212 |
A=D(II+3) |
| 12213 |
LF=LD(II+4) |
| 12214 |
IF(LP.EQ.2)EP=EP+(A/(A+1))*E |
| 12215 |
II=II+4 |
| 12216 |
SIG=D(II+NL) |
| 12217 |
SUM=SUM+SIG/SIGTOT |
| 12218 |
IF(EP.EQ.0.0)GO TO 100 |
| 12219 |
IF(R.LE.SUM)GO TO 100 |
| 12220 |
II=II+NP |
| 12221 |
70 CONTINUE |
| 12222 |
C retry with new R if SUM != 0 |
| 12223 |
80 IF(SUM.EQ.0.0) GOTO 90 |
| 12224 |
ITRY1 = ITRY1 + 1 |
| 12225 |
IF(ITRY1.LE.2) GOTO 10 |
| 12226 |
C no success set EP = 0 |
| 12227 |
90 EP = 0.0 |
| 12228 |
100 RETURN |
| 12229 |
END |
| 12230 |
*CMZ : 1.05/03 27/06/2001 18.21.00 by Christian Zeitnitz |
| 12231 |
*-- Author : |
| 12232 |
SUBROUTINE PHOTON(D,LD,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB, |
| 12233 |
+ AWR,IGCBS2,LGCB2,LR,IGAMS,LGAM,QI,ID,IIN,LRI,SIGN) |
| 12234 |
C THIS ROUTINE CONTROLS THE GENERATION AND STORAGE OF ALL |
| 12235 |
C PHOTONS PRODUCED BY THE NEUTRON INTERACTIONS. WHERE DATA |
| 12236 |
C PERMITS, THE PHOTON PRODUCED IS DIRECTLY COUPLED TO THE |
| 12237 |
C NEUTRON REACTION OCCURING. |
| 12238 |
#include "minput.inc" |
| 12239 |
#include "mconst.inc" |
| 12240 |
#include "mnutrn.inc" |
| 12241 |
#include "mapoll.inc" |
| 12242 |
#include "mcross.inc" |
| 12243 |
#include "mpstor.inc" |
| 12244 |
#include "mmicab.inc" |
| 12245 |
*KEND. |
| 12246 |
DIMENSION IDICTS(NNR,NNUC),LDICT(NNR,NNUC),NTX(*),NTS(*), |
| 12247 |
+ IGCBS(NGR,NNUC),LGCB(NGR,NNUC),AWR(*),IGCBS2(NGR,NNUC), |
| 12248 |
+ LGCB2(NGR,NNUC),LR(NQ,NNUC),IGAMS(*),LGAM(*),D(*),LD(*) |
| 12249 |
SAVE |
| 12250 |
C flag to mark call to SECEGY = 1 or PARTXS = 2 for EP CZ 13/8/92 |
| 12251 |
IEP = 0 |
| 12252 |
C INITIALIZE THE PHOTON ENERGY TO ZERO IN CASE NO PHOTON IS |
| 12253 |
C CHOSEN (THIS IS NECESSARY BECAUSE OF ENDF INCONSISTENCY) |
| 12254 |
EG=0.0 |
| 12255 |
C INITIALIZE THE PARAMETERS USED IN THE SELECTION PROCESS |
| 12256 |
MT=0 |
| 12257 |
IMT=0 |
| 12258 |
NUMBG=0 |
| 12259 |
XSIG2=0.0 |
| 12260 |
XSIG=0.0 |
| 12261 |
SIGMT3=0.0 |
| 12262 |
SIGP=0.0 |
| 12263 |
AWRI=AWR(IIN) |
| 12264 |
NNTX=NTX(IIN) |
| 12265 |
NNTS=NTS(IIN) |
| 12266 |
L=2*NNTX+2*NNTS |
| 12267 |
C NO PHOTON DATA PRESENT (IF L=0) |
| 12268 |
IF(L.EQ.0)GO TO 360 |
| 12269 |
LX=2*NNTX |
| 12270 |
LS=LX+1 |
| 12271 |
C DETERMINE THE NEUTRON REACTION MT NUMBER |
| 12272 |
IF(ID.EQ.8)MT=16 |
| 12273 |
IF(ID.EQ.9)MT=17 |
| 12274 |
IF(ID.EQ.10)MT=18 |
| 12275 |
IF(ID.EQ.11)MT=22 |
| 12276 |
IF(ID.EQ.12)MT=24 |
| 12277 |
IF(ID.EQ.13)MT=28 |
| 12278 |
IF((ID.GE.14).AND.(ID.LE.54))MT=51 |
| 12279 |
IF(ID.EQ.55)MT=102 |
| 12280 |
IF(ID.EQ.56)MT=103 |
| 12281 |
IF(ID.EQ.57)MT=104 |
| 12282 |
IF(ID.EQ.58)MT=105 |
| 12283 |
IF(ID.EQ.59)MT=106 |
| 12284 |
IF(ID.EQ.60)MT=107 |
| 12285 |
IF(ID.EQ.61)MT=108 |
| 12286 |
IF(ID.EQ.62)MT=109 |
| 12287 |
IF(ID.EQ.63)MT=111 |
| 12288 |
IF(ID.EQ.64)MT=112 |
| 12289 |
IF(ID.EQ.65)MT=113 |
| 12290 |
IF(ID.EQ.66)MT=114 |
| 12291 |
C DETERMINE WHICH DISCRETE INELASTIC SCATTERING LEVEL OCCURRED |
| 12292 |
IF(MT.NE.51)GO TO 130 |
| 12293 |
IMT=ID-14 |
| 12294 |
MT=MT+IMT |
| 12295 |
C RESET THE MT NUMBER IF AN LR-FLAG IS INVOLKED |
| 12296 |
IF(LRI.EQ.22)MT=22 |
| 12297 |
IF(LRI.EQ.23)MT=23 |
| 12298 |
IF(LRI.EQ.28)MT=28 |
| 12299 |
C CHECK PHOTON PRODUCTION DICTIONARY TO SEE IF THERE IS PHOTON |
| 12300 |
C DATA CORRESPONDING TO THE NEUTRON MT REACTION THAT OCCURRED |
| 12301 |
DO 10 IX=1,NNTX |
| 12302 |
MTG=LGCB(2*IX-1,IIN) |
| 12303 |
IF(MTG.EQ.MT)GO TO 30 |
| 12304 |
10 CONTINUE |
| 12305 |
20 IF(LRI.EQ.22)GO TO 190 |
| 12306 |
IF(LRI.EQ.23)GO TO 190 |
| 12307 |
IF(LRI.EQ.28)GO TO 190 |
| 12308 |
GO TO 70 |
| 12309 |
C PHOTON DATA FOUND CORRESPONDING TO NEUTRON MT REACTION |
| 12310 |
30 L1=LGCB2(2*IX,IIN) |
| 12311 |
IF(L1.EQ.0)GO TO 370 |
| 12312 |
LS1=IGCBS2(2*IX,IIN)+LMOX4 |
| 12313 |
LEN=L1/2 |
| 12314 |
CALL TBSPLT(D(LS1),EOLD,LEN,SIGP) |
| 12315 |
IF(SIGP.EQ.0.0)GO TO 190 |
| 12316 |
LS2=IGCBS(2*IX,IIN)+LMOX2 |
| 12317 |
C DETERMINE EXIT PHOTON ENERGY (EP) |
| 12318 |
CALL PARTXS(D(LS2),LD(LS2),EOLD,SIGP,EP) |
| 12319 |
IEP = 2 |
| 12320 |
IF(EP.GT.0.0)GO TO 60 |
| 12321 |
C DISCRETE PHOTON ENERGY WAS NOT SELECTED (EP=0.0) |
| 12322 |
C CHECK SECONDARY PHOTON DISTRIBUTION (FILE 15) FOR EP |
| 12323 |
DO 40 IS=1,NNTS |
| 12324 |
MTGS=LGCB(LX+2*IS-1,IIN) |
| 12325 |
IF(MTGS.EQ.MT)GO TO 50 |
| 12326 |
40 CONTINUE |
| 12327 |
C no file 15 found and EP=0 in PARTXS -> try MT=4 etc |
| 12328 |
GO TO 20 |
| 12329 |
50 L1=LGCB(LX+2*IS,IIN) |
| 12330 |
IF(L1.EQ.0)GO TO 380 |
| 12331 |
LS3=IGCBS(LX+2*IS,IIN)+LMOX2 |
| 12332 |
C DETERMINE EXIT PHOTON ENERGY (EP) |
| 12333 |
CALL SECEGY(EP,D(LS3),EOLD,LD(LS3)) |
| 12334 |
IEP = 1 |
| 12335 |
C DETERMINE THE PHOTON MULTIPLICITY (YP) |
| 12336 |
C RECALCULATE THE DENOMINATOR USED IN CALCULATING THE |
| 12337 |
C PHOTON MULTIPLICITY TO ACCOUNT FOR THE LR-FLAGS |
| 12338 |
60 IF(LRI.EQ.22)CALL LRNORM(D,LD,IDICTS,LDICT,LR,EOLD,MT,IIN,SIGN) |
| 12339 |
IF(LRI.EQ.23)CALL LRNORM(D,LD,IDICTS,LDICT,LR,EOLD,MT,IIN,SIGN) |
| 12340 |
IF(LRI.EQ.28)CALL LRNORM(D,LD,IDICTS,LDICT,LR,EOLD,MT,IIN,SIGN) |
| 12341 |
YP=SIGP/SIGN |
| 12342 |
GO TO 330 |
| 12343 |
C THE DISCRETE INELASTIC LEVEL PHOTON DATA WAS NOT FOUND |
| 12344 |
C CHECK THE PHOTON PRODUCTION DICTIONARY TO SEE IF THERE IS |
| 12345 |
C PHOTON DATA CORRESPONDING TO MT=4 |
| 12346 |
70 DO 80 IX=1,NNTX |
| 12347 |
MTG=LGCB(2*IX-1,IIN) |
| 12348 |
IF(MTG.EQ.4)GO TO 90 |
| 12349 |
80 CONTINUE |
| 12350 |
GO TO 190 |
| 12351 |
C PHOTON DATA FOUND CORRESPONDING TO MT=4 |
| 12352 |
90 L1=LGCB2(2*IX,IIN) |
| 12353 |
IF(L1.EQ.0)GO TO 370 |
| 12354 |
LS1=IGCBS2(2*IX,IIN)+LMOX4 |
| 12355 |
LEN=L1/2 |
| 12356 |
CALL TBSPLT(D(LS1),EOLD,LEN,SIGP) |
| 12357 |
IF(SIGP.EQ.0.0)GO TO 190 |
| 12358 |
LS2=IGCBS(2*IX,IIN)+LMOX2 |
| 12359 |
C DETERMINE EXIT PHOTON ENERGY (EP) |
| 12360 |
CALL PARTXS(D(LS2),LD(LS2),EOLD,SIGP,EP) |
| 12361 |
IEP = 2 |
| 12362 |
IF(EP.GT.0.0)GO TO 120 |
| 12363 |
C DISCRETE PHOTON ENERGY WAS NOT SELECTED (EP=0.0) |
| 12364 |
C CHECK SECONDARY PHOTON DISTRIBUTION (FILE 15) FOR EP |
| 12365 |
DO 100 IS=1,NNTS |
| 12366 |
MTGS=LGCB(LX+2*IS-1,IIN) |
| 12367 |
IF(MTGS.EQ.4)GO TO 110 |
| 12368 |
100 CONTINUE |
| 12369 |
GO TO 380 |
| 12370 |
110 L1=LGCB(LX+2*IS,IIN) |
| 12371 |
IF(L1.EQ.0)GO TO 380 |
| 12372 |
LS3=IGCBS(LX+2*IS,IIN)+LMOX2 |
| 12373 |
C DETERMINE EXIT PHOTON ENERGY (EP) |
| 12374 |
CALL SECEGY(EP,D(LS3),EOLD,LD(LS3)) |
| 12375 |
IEP = 1 |
| 12376 |
C DETERMINE THE PHOTON MULTIPLICITY (YP) |
| 12377 |
C RECALCULATE THE DENOMINATOR USED IN CALCULATING THE |
| 12378 |
C PHOTON MULTIPLICITY TO ACCOUNT FOR THE LR-FLAGS |
| 12379 |
120 MT=4 |
| 12380 |
CALL LRNORM(D,LD,IDICTS,LDICT,LR,EOLD,MT,IIN,SIGNIS) |
| 12381 |
YP=SIGP/SIGNIS |
| 12382 |
GO TO 330 |
| 12383 |
C CHECK PHOTON PRODUCTION DICTIONARY TO SEE IF THERE IS PHOTON |
| 12384 |
C DATA CORRESPONDING TO THE NEUTRON MT REACTION THAT OCCURRED |
| 12385 |
130 DO 140 IX=1,NNTX |
| 12386 |
MTG=LGCB(2*IX-1,IIN) |
| 12387 |
IF(MTG.EQ.MT)GO TO 150 |
| 12388 |
140 CONTINUE |
| 12389 |
GO TO 190 |
| 12390 |
C PHOTON DATA FOUND CORRESPONDING TO NEUTRON MT REACTION |
| 12391 |
150 L1=LGCB2(2*IX,IIN) |
| 12392 |
IF(L1.EQ.0)GO TO 370 |
| 12393 |
LS1=IGCBS2(2*IX,IIN)+LMOX4 |
| 12394 |
LEN=L1/2 |
| 12395 |
CALL TBSPLT(D(LS1),EOLD,LEN,SIGP) |
| 12396 |
IF(SIGP.EQ.0.0)GO TO 190 |
| 12397 |
LS2=IGCBS(2*IX,IIN)+LMOX2 |
| 12398 |
C DETERMINE EXIT PHOTON ENERGY (EP) |
| 12399 |
CALL PARTXS(D(LS2),LD(LS2),EOLD,SIGP,EP) |
| 12400 |
IEP = 2 |
| 12401 |
IF(EP.GT.0.0)GO TO 180 |
| 12402 |
C DISCRETE PHOTON ENERGY WAS NOT SELECTED (EP=0.0) |
| 12403 |
C CHECK SECONDARY PHOTON DISTRIBUTION (FILE 15) FOR EP |
| 12404 |
DO 160 IS=1,NNTS |
| 12405 |
MTGS=LGCB(LX+2*IS-1,IIN) |
| 12406 |
IF(MTGS.EQ.MT)GO TO 170 |
| 12407 |
160 CONTINUE |
| 12408 |
GO TO 380 |
| 12409 |
170 L1=LGCB(LX+2*IS,IIN) |
| 12410 |
IF(L1.EQ.0)GO TO 380 |
| 12411 |
LS3=IGCBS(LX+2*IS,IIN)+LMOX2 |
| 12412 |
C DETERMINE EXIT PHOTON ENERGY (EP) |
| 12413 |
CALL SECEGY(EP,D(LS3),EOLD,LD(LS3)) |
| 12414 |
IEP = 1 |
| 12415 |
C DETERMINE THE PHOTON MULTIPLICITY (YP) |
| 12416 |
180 YP=SIGP/SIGN |
| 12417 |
GO TO 330 |
| 12418 |
C NO PHOTON DATA WAS FOUND FOR THE PARTICULAR NEUTRON MT |
| 12419 |
C REACTION OR FOR NEUTRON MT=4, THEREFORE CHECK THE PHOTON |
| 12420 |
C PRODUCTION DICTIONARY TO SEE IF THERE IS PHOTON DATA |
| 12421 |
C CORRESPONDING TO MT=3 (THE CATCH-ALL MT) |
| 12422 |
190 DO 200 IX=1,NNTX |
| 12423 |
MTG=LGCB(2*IX-1,IIN) |
| 12424 |
IF(MTG.EQ.3)GO TO 210 |
| 12425 |
200 CONTINUE |
| 12426 |
GO TO 360 |
| 12427 |
C PHOTON DATA FOUND CORRESPONDING TO MT=3 |
| 12428 |
210 L1=LGCB2(2*IX,IIN) |
| 12429 |
IF(L1.EQ.0)GO TO 370 |
| 12430 |
LS1=IGCBS2(2*IX,IIN)+LMOX4 |
| 12431 |
LEN=L1/2 |
| 12432 |
CALL TBSPLT(D(LS1),EOLD,LEN,SIGP) |
| 12433 |
IF(SIGP.EQ.0.0)GO TO 360 |
| 12434 |
LS2=IGCBS(2*IX,IIN)+LMOX2 |
| 12435 |
C DETERMINE EXIT PHOTON ENERGY (EP) |
| 12436 |
CALL PARTXS(D(LS2),LD(LS2),EOLD,SIGP,EP) |
| 12437 |
IEP = 2 |
| 12438 |
IF(EP.GT.0.0)GO TO 240 |
| 12439 |
C DISCRETE PHOTON ENERGY WAS NOT SELECTED (EP=0.0) |
| 12440 |
C CHECK SECONDARY PHOTON DISTRIBUTION (FILE 15) FOR EP |
| 12441 |
DO 220 IS=1,NNTS |
| 12442 |
MTGS=LGCB(LX+2*IS-1,IIN) |
| 12443 |
IF(MTGS.EQ.3)GO TO 230 |
| 12444 |
220 CONTINUE |
| 12445 |
GO TO 380 |
| 12446 |
230 L1=LGCB(LX+2*IS,IIN) |
| 12447 |
IF(L1.EQ.0)GO TO 380 |
| 12448 |
LS3=IGCBS(LX+2*IS,IIN)+LMOX2 |
| 12449 |
C DETERMINE EXIT PHOTON ENERGY (EP) |
| 12450 |
CALL SECEGY(EP,D(LS3),EOLD,LD(LS3)) |
| 12451 |
IEP = 1 |
| 12452 |
C THE PHOTON WAS SELECTED FROM PHOTON DATA FOR MT=3 |
| 12453 |
C TO OBTAIN THE CORRECT MULTIPLICITY, THE NEUTRON CROSS |
| 12454 |
C SECTION FOR MT=3 MUST BE ADJUSTED TO REPRESENT THE SAME |
| 12455 |
C DATA AS MT=3 DOES IN THE PHOTON DATA |
| 12456 |
240 ID=2 |
| 12457 |
C OBTAIN NEUTRON ELASTIC SCATTERING CROSS SECTION |
| 12458 |
L1=LDICT(ID,IIN) |
| 12459 |
IF(L1.EQ.0)GO TO 250 |
| 12460 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 12461 |
LEN=L1/2 |
| 12462 |
CALL TBSPLT(D(LS1),EOLD,LEN,XSIG2) |
| 12463 |
C SUBTRACT THE ELASTIC SCATTERING CROSS SECTION FROM THE TOTAL |
| 12464 |
C CROSS SECTION TO OBTAIN BASE NEUTRON MT=3 REACTION |
| 12465 |
SIGMT3=SIGT-XSIG2 |
| 12466 |
GO TO 260 |
| 12467 |
250 SIGMT3=SIGT |
| 12468 |
260 CONTINUE |
| 12469 |
C SCAN THE PHOTON PRODUCTION DICTIONARY FOR ALL MT NUMBERS |
| 12470 |
C NOT EQUAL TO MT=3 |
| 12471 |
DO 300 IX=1,NNTX |
| 12472 |
MTG=LGCB(2*IX-1,IIN) |
| 12473 |
IF(MTG.EQ.3)GO TO 300 |
| 12474 |
L1=LGCB2(2*IX,IIN) |
| 12475 |
IF(L1.EQ.0)GO TO 370 |
| 12476 |
LS1=IGCBS2(2*IX,IIN)+LMOX4 |
| 12477 |
LEN=L1/2 |
| 12478 |
CALL TBSPLT(D(LS1),EOLD,LEN,SIGEX) |
| 12479 |
C IF THE TOTAL PHOTON PRODUCTION CROSS SECTION IS ZERO AT |
| 12480 |
C THE NEUTRON ENERGY, THEN THE NEUTRON CROSS SECTION SHOULD |
| 12481 |
C NOT BE SUBTRACTED FROM MT3 TO MAINTAIN PROPER NORMALIZATION |
| 12482 |
IF(SIGEX.EQ.0.0)GO TO 300 |
| 12483 |
C SET THE NEUTRON DICTIONARY ID NUMBER CORRESPONDING TO MTG |
| 12484 |
IF((MTG.LT.51).OR.(MTG.GT.91))GO TO 270 |
| 12485 |
ID=14 |
| 12486 |
IMT3=MTG-51 |
| 12487 |
ID=ID+IMT3 |
| 12488 |
270 IF(MTG.EQ.4)ID=3 |
| 12489 |
IF(MTG.EQ.16)ID=8 |
| 12490 |
IF(MTG.EQ.17)ID=9 |
| 12491 |
IF(MTG.EQ.18)ID=10 |
| 12492 |
IF(MTG.EQ.22)ID=11 |
| 12493 |
IF(MTG.EQ.24)ID=12 |
| 12494 |
IF(MTG.EQ.28)ID=13 |
| 12495 |
IF(MTG.EQ.102)ID=55 |
| 12496 |
IF(MTG.EQ.103)ID=56 |
| 12497 |
IF(MTG.EQ.104)ID=57 |
| 12498 |
IF(MTG.EQ.105)ID=58 |
| 12499 |
IF(MTG.EQ.106)ID=59 |
| 12500 |
IF(MTG.EQ.107)ID=60 |
| 12501 |
IF(MTG.EQ.108)ID=61 |
| 12502 |
IF(MTG.EQ.109)ID=62 |
| 12503 |
IF(MTG.EQ.111)ID=63 |
| 12504 |
IF(MTG.EQ.112)ID=64 |
| 12505 |
IF(MTG.EQ.113)ID=65 |
| 12506 |
IF(MTG.EQ.114)ID=66 |
| 12507 |
C OBTAIN THE NEUTRON CROSS SECTION CORRESPONDING TO MTG AND |
| 12508 |
C SUBTRACT IT OFF OF THE BASE NEUTRON MT=3 CROSS SECTION |
| 12509 |
L1=LDICT(ID,IIN) |
| 12510 |
IF(L1.EQ.0)GO TO 280 |
| 12511 |
LS1=IDICTS(ID,IIN)+LMOX2 |
| 12512 |
LEN=L1/2 |
| 12513 |
CALL TBSPLT(D(LS1),EOLD,LEN,XSIG) |
| 12514 |
GO TO 290 |
| 12515 |
280 XSIG=0.0 |
| 12516 |
290 SIGMT3=SIGMT3-XSIG |
| 12517 |
IF(SIGMT3.LE.0.0)GO TO 310 |
| 12518 |
300 CONTINUE |
| 12519 |
C DETERMINE THE PHOTON MULTIPLICITY (YP) |
| 12520 |
YP=SIGP/SIGMT3 |
| 12521 |
IF(YP.GE.100.0)GO TO 310 |
| 12522 |
GO TO 330 |
| 12523 |
310 CONTINUE |
| 12524 |
C THIS SECTION OF CODING IS INCLUDED TO ACCOUNT FOR ANY |
| 12525 |
C ENDF/B DATA INCONSISTENCY WHICH COULD YIELD A PHOTON OF |
| 12526 |
C CONSIDERABLE WEIGHT. THE FOLLOWING CODING WILL SAMPLE THE |
| 12527 |
C PHOTON WEIGHT FROM THE GENERAL PHOTON YIELD ARRAY AND |
| 12528 |
C ADJUST THE WEIGHT TO PHOTONS PER NON-ELASTIC COLLISION. |
| 12529 |
L1=LGAM(IIN) |
| 12530 |
IF(L1.EQ.0)GO TO 320 |
| 12531 |
LS1=IGAMS(IIN)+LMOX2 |
| 12532 |
LEN=L1/2 |
| 12533 |
CALL TBSPLT(D(LS1),EOLD,LEN,YP) |
| 12534 |
YP=(YP*SIGT)/(SIGT-XSIG2) |
| 12535 |
GO TO 330 |
| 12536 |
320 YP=1.00 |
| 12537 |
C THE FOLLOWING SECTION OF CODING IS INCLUDED TO DISTRIBUTE |
| 12538 |
C THE WEIGHT ENDF/B-V DATA MAY GIVE A PARTICULAR PHOTON. |
| 12539 |
C FOR EXAMPLE, ENDF/B-V DATA MAY ASSIGN A MULITPLICITY OF |
| 12540 |
C 75 TO A PARTICULAR PHOTON. BECAUSE SUCH A PHOTON COULD |
| 12541 |
C CONSIDERABLY MODIFY THE RESULTS OF A DETECTOR RESPONSE, THE |
| 12542 |
C MULTIPLICITY (PHOTON WEIGHT) IS DISTRIBUTED TO SEVERAL |
| 12543 |
C PHOTONS (SPLITTING OF SORTS) WITH BOTH WEIGHT AND ENERGY |
| 12544 |
C BEING CONSERVED. THIS RARELY OCCURS BUT IS NECESSARY. |
| 12545 |
330 CONTINUE |
| 12546 |
MGPAR = INT(FLOAT(MAXPAR)*0.7) |
| 12547 |
C |
| 12548 |
C for a photon multiplicity > 1.01 a poisson distribution is sampled |
| 12549 |
C for the actually generated multiplicity (with mean YP) |
| 12550 |
C |
| 12551 |
IF(YP.GT.1.01) THEN |
| 12552 |
C |
| 12553 |
C use poisson distribution |
| 12554 |
C |
| 12555 |
340 CALL GPOISS(YP,NUMBG,1) |
| 12556 |
IGTRY=IGTRY+1 |
| 12557 |
IF(NUMBG.GT.INT(4.*YP).OR. |
| 12558 |
+ NUMBG.GT.MGPAR.AND.IGTRY.LT.5) GOTO 340 |
| 12559 |
ELSE |
| 12560 |
C YP <= 1.01 |
| 12561 |
C number of photons generated = INT(YP) |
| 12562 |
C plus an additional photon if YP-INT(YP) > random number |
| 12563 |
C CZ 21.8.95 |
| 12564 |
NUMBG = INT(YP) |
| 12565 |
IF((YP-FLOAT(NUMBG)).GT.FLTRNF(0)) NUMBG = NUMBG + 1 |
| 12566 |
ENDIF |
| 12567 |
NUMBG=MIN(NUMBG,MGPAR) |
| 12568 |
C Allow 0 Photons to be generated |
| 12569 |
IF(NUMBG.EQ.0) RETURN |
| 12570 |
EPTOT = YP*EP |
| 12571 |
EPSUM = 0.0 |
| 12572 |
DO 350 I=1,NUMBG |
| 12573 |
C ASSUME ISOTROPIC PHOTON EMISSION IN THE LABORATORY SYSTEM |
| 12574 |
CALL GTISO(U1,V1,W1) |
| 12575 |
C SET THE PHOTON EXIT PARAMETERS |
| 12576 |
UP=U1 |
| 12577 |
VP=V1 |
| 12578 |
WP=W1 |
| 12579 |
AGEP=AGE |
| 12580 |
MTP=MT |
| 12581 |
C re-sample photon energy depending on model used CZ 13.8.92 |
| 12582 |
IF(IEP.EQ.2) THEN |
| 12583 |
CALL PARTXS(D(LS2),LD(LS2),EOLD,SIGP,EP1) |
| 12584 |
IF(EP1.GT.0.0) EP=EP1 |
| 12585 |
ENDIF |
| 12586 |
IF(IEP.EQ.1) THEN |
| 12587 |
CALL SECEGY(EP1,D(LS3),EOLD,LD(LS3)) |
| 12588 |
IF(EP1.GT.0.0) EP=EP1 |
| 12589 |
ENDIF |
| 12590 |
EPSUM = EPSUM+EP |
| 12591 |
C check for energy conservation |
| 12592 |
IF(EPSUM.GT.EPTOT.OR.I.EQ.NUMBG) EP = EPTOT-EPSUM+EP |
| 12593 |
C STORE THE PHOTON |
| 12594 |
CALL STOPAR(IDGAMA,NGAMA) |
| 12595 |
C end photon production when energy is used up CZ 13.8.92 |
| 12596 |
IF(EPSUM.GT.EPTOT) GOTO 360 |
| 12597 |
350 CONTINUE |
| 12598 |
360 RETURN |
| 12599 |
370 WRITE(IOUT,10000) |
| 12600 |
10000 FORMAT(' PHOTON: THE PHOTON PRODUCTION ', |
| 12601 |
+ 'CROSS SECTION DATA WAS NOT FOUND (L1=0)') |
| 12602 |
GOTO 390 |
| 12603 |
380 WRITE(IOUT,10100) |
| 12604 |
10100 FORMAT(' PHOTON: NO SECONDARY ENERGY ', |
| 12605 |
+ 'DISTRIBUTION WAS FOUND FOR THE CONTINUUM REACTION CHOSEN') |
| 12606 |
390 WRITE(6,*) ' CALOR: ERROR in PHOTON ===> STOP ' |
| 12607 |
STOP |
| 12608 |
END |
| 12609 |
*CMZ : 1.05/03 27/06/2001 17.54.25 by Christian Zeitnitz |
| 12610 |
*-- Author : |
| 12611 |
C********************************************************************* |
| 12612 |
FUNCTION RNMAXF(T) |
| 12613 |
C T := most probable value of distribution |
| 12614 |
C********************************************************************* |
| 12615 |
DATA FF/0./ |
| 12616 |
SAVE FF,R1SQ,W,U |
| 12617 |
U=EXPRNF(U) |
| 12618 |
IF(FF) 30 ,10 ,30 |
| 12619 |
10 R1=FLTRNF(0) |
| 12620 |
R2=FLTRNF(0) |
| 12621 |
R1SQ=R1*R1 |
| 12622 |
R2SQ=R2*R2 |
| 12623 |
RSQ=R1SQ+R2SQ |
| 12624 |
IF(RSQ-1.) 20 ,20 ,10 |
| 12625 |
20 W=EXPRNF(W)/RSQ |
| 12626 |
FF=1. |
| 12627 |
RNMAXF=(R2SQ*W+U)*T |
| 12628 |
GO TO 40 |
| 12629 |
30 FF=0. |
| 12630 |
RNMAXF=(R1SQ*W+U)*T |
| 12631 |
40 RETURN |
| 12632 |
END |
| 12633 |
*CMZ : 1.04/00 02/02/95 09.26.27 by Christian Zeitnitz |
| 12634 |
*-- Author : |
| 12635 |
SUBROUTINE SECEGY(EX,FSE,E,IFSE) |
| 12636 |
C THIS ROUTINE SELECTS A PARTIAL ENERGY DISTRIBUTION |
| 12637 |
C TO SAMPLE THE EXIT ENERGY FROM |
| 12638 |
#include "minput.inc" |
| 12639 |
*KEND. |
| 12640 |
DIMENSION FSE(*),IFSE(*) |
| 12641 |
SAVE |
| 12642 |
EX = 0.0 |
| 12643 |
IPP=1 |
| 12644 |
N=1 |
| 12645 |
IP=1 |
| 12646 |
R=FLTRNF(0) |
| 12647 |
NK=IFSE(IP) |
| 12648 |
PROB=0. |
| 12649 |
10 IP=IP+1 |
| 12650 |
LF=IFSE(IP) |
| 12651 |
IP=IP+1 |
| 12652 |
C TEMP FIX UP |
| 12653 |
U=FSE(IP) |
| 12654 |
IF(LF.EQ.11)U=FLOAT(IFSE(IP)) |
| 12655 |
IP=IP+1 |
| 12656 |
NR=IFSE(IP) |
| 12657 |
IPR=IP |
| 12658 |
IP=IP+1 |
| 12659 |
NP=IFSE(IP) |
| 12660 |
IP=IP+2*NR |
| 12661 |
20 CONTINUE |
| 12662 |
DO 30 I=1,NP |
| 12663 |
IP=IP+2 |
| 12664 |
C IF E IS LESS THAN THE LOWEST ENERGY OF THE MESH, THEN THE |
| 12665 |
C PROBABILITY WILL EQUAL ZERO FOR SELECTING THAT DISTRIBUTION |
| 12666 |
IF(E.LT.FSE(IP-1))GO TO 50 |
| 12667 |
30 CONTINUE |
| 12668 |
C TRY THE NEXT PARTIAL DISTRIBUTION |
| 12669 |
40 N=N+1 |
| 12670 |
IF(N.GT.NK)GO TO 170 |
| 12671 |
IF(LF.EQ.1)GO TO 100 |
| 12672 |
IF(LF.EQ.5)GO TO 120 |
| 12673 |
IF((LF.EQ.7).OR.(LF.EQ.9))GO TO 130 |
| 12674 |
GO TO 140 |
| 12675 |
50 IF(I.NE.1)GO TO 70 |
| 12676 |
IF(E+CADIG(E).LT.FSE(IP-1))GO TO 60 |
| 12677 |
E=E+CADIG(E) |
| 12678 |
IP=IP-2 |
| 12679 |
GO TO 20 |
| 12680 |
60 CONTINUE |
| 12681 |
IP=IP+(NP-1)*2 |
| 12682 |
GO TO 40 |
| 12683 |
C DETERMINE THE INTERPOLATING SCHEME |
| 12684 |
70 CONTINUE |
| 12685 |
DO 80 J=1,NR |
| 12686 |
J1=IPR+2*J |
| 12687 |
IF(I.LE.IFSE(J1))GO TO 90 |
| 12688 |
80 CONTINUE |
| 12689 |
90 IS=IFSE(J1+1) |
| 12690 |
CALL INTERP(E,P,FSE(IP-3),FSE(IP-2),FSE(IP-1),FSE(IP),IS) |
| 12691 |
PROB=PROB+P |
| 12692 |
IF(R.LE.PROB)GO TO 150 |
| 12693 |
IP=IP+2*(NP-I) |
| 12694 |
GO TO 40 |
| 12695 |
C SKIP THE DATA FOR LF EQUAL ONE |
| 12696 |
100 IP=IP+1 |
| 12697 |
NR=IFSE(IP) |
| 12698 |
NE=IFSE(IP+1) |
| 12699 |
IP=IP+2*NR+1 |
| 12700 |
DO 110 I=1,NE |
| 12701 |
IP=IP+2 |
| 12702 |
NR=IFSE(IP) |
| 12703 |
IP=IP+1 |
| 12704 |
NP=IFSE(IP) |
| 12705 |
IP=IP+2*NR+2*NP |
| 12706 |
110 CONTINUE |
| 12707 |
GO TO 10 |
| 12708 |
C SKIP THE DATA FOR LF EQUAL FIVE |
| 12709 |
120 IP=IP+1 |
| 12710 |
NR=IFSE(IP) |
| 12711 |
NE=IFSE(IP+1) |
| 12712 |
IP=IP+2*NR+1 |
| 12713 |
IP=IP+2*NE |
| 12714 |
IP=IP+1 |
| 12715 |
NR=IFSE(IP) |
| 12716 |
NF=IFSE(IP+1) |
| 12717 |
IP=IP+2*NF+2*NR+1 |
| 12718 |
GO TO 10 |
| 12719 |
C SKIP THE DATA FOR LF EQUAL SEVEN, AND LF EQUAL NINE |
| 12720 |
130 IP=IP+1 |
| 12721 |
NR=IFSE(IP) |
| 12722 |
NE=IFSE(IP+1) |
| 12723 |
IP=IP+2*NR+1 |
| 12724 |
IP=IP+2*NE |
| 12725 |
GO TO 10 |
| 12726 |
C SKIP THE DATA FOR LF EQUAL ELEVEN |
| 12727 |
140 IP=IP+1 |
| 12728 |
NR=IFSE(IP) |
| 12729 |
NE=IFSE(IP+1) |
| 12730 |
IP=IP+2*NR+1 |
| 12731 |
IP=IP+2*NE |
| 12732 |
IP=IP+1 |
| 12733 |
NR=IFSE(IP) |
| 12734 |
NE=IFSE(IP+1) |
| 12735 |
IP=IP+2*NR+1 |
| 12736 |
IP=IP+2*NE |
| 12737 |
GO TO 10 |
| 12738 |
C NOW SELECT THE SECONDARY ENERGY FROM THE CHOSEN DISTRIBUTION |
| 12739 |
150 IP=IP+2*(NP-I) |
| 12740 |
160 CONTINUE |
| 12741 |
IF(LF.EQ.1)CALL SECLF1(FSE(IP+1),IFSE(IP+1),EX,U,E) |
| 12742 |
IF(LF.EQ.5)CALL SECLF5(FSE(IP+1),IFSE(IP+1),EX,U,E) |
| 12743 |
IF(LF.EQ.7)CALL SECLF7(FSE(IP+1),IFSE(IP+1),EX,U,E) |
| 12744 |
IF(LF.EQ.9)CALL SECLF9(FSE(IP+1),IFSE(IP+1),EX,U,E) |
| 12745 |
IF(LF.EQ.11)CALL SECL11(FSE(IP+1),IFSE(IP+1),EX,U,E) |
| 12746 |
RETURN |
| 12747 |
170 CONTINUE |
| 12748 |
C TEMP CARD |
| 12749 |
LF=IFSE(IPP+1) |
| 12750 |
U=FSE(IPP+2) |
| 12751 |
IF(LF.EQ.11)U=FLOAT(IFSE(IPP+2)) |
| 12752 |
NR=IFSE(IPP+3) |
| 12753 |
NP=IFSE(IPP+4) |
| 12754 |
IP=2*NR+2*NP+5 |
| 12755 |
GO TO 160 |
| 12756 |
END |
| 12757 |
*CMZ : 1.04/00 02/02/95 09.23.46 by Christian Zeitnitz |
| 12758 |
*-- Author : |
| 12759 |
SUBROUTINE SECL11(FSE,IFSE,EX,U,E) |
| 12760 |
C THIS ROUTINE SAMPLES AN EXIT ENERGY FROM |
| 12761 |
C AN ENERGY DEPENDENT WATT SPECTRUM |
| 12762 |
#include "minput.inc" |
| 12763 |
*KEND. |
| 12764 |
DIMENSION FSE(*),IFSE(*) |
| 12765 |
SAVE |
| 12766 |
IP=1 |
| 12767 |
NR=IFSE(IP) |
| 12768 |
NE=IFSE(IP+1) |
| 12769 |
IP=2*NR+1 |
| 12770 |
EMAX=E-U |
| 12771 |
C DETERMINE A |
| 12772 |
DO 10 I=1,NE |
| 12773 |
IP=IP+2 |
| 12774 |
IF(E.LE.FSE(IP))GO TO 20 |
| 12775 |
10 CONTINUE |
| 12776 |
GO TO 30 |
| 12777 |
20 IF(I.EQ.1)GO TO 40 |
| 12778 |
C DETERMINE THE INTERPOLATING SCHEME |
| 12779 |
CALL INTSCH(IFSE,I,IS,NR) |
| 12780 |
E1=FSE(IP-2) |
| 12781 |
E2=FSE(IP) |
| 12782 |
T1=FSE(IP-1) |
| 12783 |
T2=FSE(IP+1) |
| 12784 |
CALL INTERP(E,A,E1,T1,E2,T2,IS) |
| 12785 |
GO TO 50 |
| 12786 |
C INCIDENT ENERGY IS ABOVE THE LAST INCIDENT ENERGY GIVEN |
| 12787 |
C USE THE LAST DISTRIBUTION |
| 12788 |
30 IP=2+2*NR+2*NE |
| 12789 |
A=FSE(IP) |
| 12790 |
GO TO 50 |
| 12791 |
C INCIDENT ENERGY IS BELOW THE FIRST INCIDENT ENERGY GIVEN |
| 12792 |
C USE THE FIRST DISTRIBUTION |
| 12793 |
40 A=FSE(4+2*NR) |
| 12794 |
C DETERMINE B |
| 12795 |
50 IP=3+2*NR+2*NE |
| 12796 |
NR1=IFSE(IP) |
| 12797 |
NF=IFSE(IP+1) |
| 12798 |
IP=2*NR+2*NE+2*NR1+3 |
| 12799 |
DO 60 I=1,NF |
| 12800 |
IP=IP+2 |
| 12801 |
IF(E.LE.FSE(IP))GO TO 70 |
| 12802 |
60 CONTINUE |
| 12803 |
GO TO 80 |
| 12804 |
70 IF(I.EQ.1)GO TO 90 |
| 12805 |
CALL INTSCH(IFSE(2*NR+2*NE+3),I,IS,NR1) |
| 12806 |
E1=FSE(IP-2) |
| 12807 |
E2=FSE(IP) |
| 12808 |
T1=FSE(IP-1) |
| 12809 |
T2=FSE(IP+1) |
| 12810 |
CALL INTERP(E,B,E1,T1,E2,T2,IS) |
| 12811 |
GO TO 100 |
| 12812 |
80 IP=2*NR+2*NF+2*NE+2*NR1+4 |
| 12813 |
B=FSE(IP) |
| 12814 |
GO TO 100 |
| 12815 |
90 B=FSE(IP+1) |
| 12816 |
C SELECT THE EXIT ENERGY FROM THE WATT SPECTRUM |
| 12817 |
100 EX=FISRNF(A,B) |
| 12818 |
IF(EX.LE.EMAX)RETURN |
| 12819 |
EX=EMAX |
| 12820 |
RETURN |
| 12821 |
END |
| 12822 |
*CMZ : 1.01/07 24/06/93 21.32.11 by Christian Zeitnitz |
| 12823 |
*-- Author : |
| 12824 |
SUBROUTINE SECLF1(FSE,IFSE,EX,U,E) |
| 12825 |
C THIS ROUTINE SAMPLES AN EXIT ENERGY FROM |
| 12826 |
C A TABULATED DISTRIBUTION |
| 12827 |
#include "minput.inc" |
| 12828 |
*KEND. |
| 12829 |
DIMENSION FSE(*),IFSE(*) |
| 12830 |
SAVE |
| 12831 |
C=0. |
| 12832 |
IP=1 |
| 12833 |
NRE=IFSE(IP) |
| 12834 |
NE=IFSE(IP+1) |
| 12835 |
IP=IP+2*NRE+1 |
| 12836 |
C FIND THE TWO INCIDENT ENERGY DISTRIBUTIONS THAT BOUND E |
| 12837 |
C INCIDENT ENERGY IS BELOW THE FIRST INCIDENT ENERGY GIVEN |
| 12838 |
C USE THE FIRST DISTRIBUTION |
| 12839 |
IP=IP+1 |
| 12840 |
IE=1 |
| 12841 |
E1=FSE(IP) |
| 12842 |
IP1=IP |
| 12843 |
IF(E.GT.E1)GO TO 10 |
| 12844 |
IPR=IP+1 |
| 12845 |
NR=IFSE(IPR) |
| 12846 |
NP=IFSE(IPR+1) |
| 12847 |
GO TO 50 |
| 12848 |
10 IP=IP+1 |
| 12849 |
IPR1=IP |
| 12850 |
NP1=IFSE(IP+1) |
| 12851 |
IP=IP+2*IFSE(IPR1)+1 |
| 12852 |
IP=IP+2*NP1 |
| 12853 |
20 IE=IE+1 |
| 12854 |
IP=IP+1 |
| 12855 |
C INCIDENT ENERGY IS ABOVE THE LAST INCIDENT ENERGY GIVEN |
| 12856 |
C USE THE LAST DISTRIBUTION |
| 12857 |
IF(IE.GT.NE)GO TO 40 |
| 12858 |
E2=FSE(IP) |
| 12859 |
IF(E.LE.E2)GO TO 30 |
| 12860 |
E1=E2 |
| 12861 |
IP1=IP |
| 12862 |
IP=IP+1 |
| 12863 |
IPR1=IP |
| 12864 |
NP1=IFSE(IP+1) |
| 12865 |
IP=IP+2*IFSE(IPR1)+1 |
| 12866 |
IP=IP+2*NP1 |
| 12867 |
GO TO 20 |
| 12868 |
30 IP2=IP |
| 12869 |
IP=IP+1 |
| 12870 |
IPR2=IP |
| 12871 |
NP2=IFSE(IP+1) |
| 12872 |
IP=IP+2*IFSE(IPR2)+1 |
| 12873 |
C DETERMINE THE INTERPOLATING SCHEME |
| 12874 |
CALL INTSCH(IFSE,IE,IS,NRE) |
| 12875 |
C SELECT THE DISTRIBUTION TO SAMPLE FROM |
| 12876 |
R=FLTRNF(0) |
| 12877 |
C INTERPOLATION SCHEMES OF 1 (CONSTANT) OR 2 (LINEAR) ALLOWED |
| 12878 |
IF(IS.GT.2)GO TO 110 |
| 12879 |
PROB=(E2-E)/(E2-E1) |
| 12880 |
IF(IS.EQ.1)PROB=1.0 |
| 12881 |
IF(R.LE.PROB)GO TO 40 |
| 12882 |
C SELECT FROM THE SECOND DISTRIBUTION |
| 12883 |
NP=NP2 |
| 12884 |
IP=IP2 |
| 12885 |
IPR=IPR2 |
| 12886 |
GO TO 50 |
| 12887 |
C SELECT FROM THE FIRST DISTRIBUTION |
| 12888 |
C OR FROM THE LAST INCIDENT ENERGY |
| 12889 |
40 NP=NP1 |
| 12890 |
IP=IP1 |
| 12891 |
IPR=IPR1 |
| 12892 |
C SELECT THE EXIT ENERGY FROM THE TABULATED DISTRIBUTION |
| 12893 |
50 CONTINUE |
| 12894 |
ITRY = 0 |
| 12895 |
60 CONTINUE |
| 12896 |
PROB=0. |
| 12897 |
R=FLTRNF(0) |
| 12898 |
NR=2*IFSE(IPR)+1 |
| 12899 |
DO 90 I=1,NP |
| 12900 |
CALL INTSCH(IFSE(IPR),NP,IS,IFSE(IPR)) |
| 12901 |
N=IP+NR+1+2*I |
| 12902 |
PROB1=PROB |
| 12903 |
IF(I.EQ.1)GO TO 90 |
| 12904 |
IF(IS.EQ.1)GO TO 70 |
| 12905 |
IF(IS.GT.2)GO TO 110 |
| 12906 |
PROB=PROB+(FSE(N)+FSE(N-2))*(FSE(N-1)-FSE(N-3))/2. |
| 12907 |
GO TO 80 |
| 12908 |
70 PROB=PROB+FSE(N-2)*(FSE(N-1)-FSE(N-3)) |
| 12909 |
80 IF(R.LE.PROB)GO TO 100 |
| 12910 |
90 CONTINUE |
| 12911 |
ITRY = ITRY + 1 |
| 12912 |
IF(ITRY.LT.5) GOTO 60 |
| 12913 |
IF(R.LT..998)GO TO 120 |
| 12914 |
100 EX=FSE(N-3)+(R-PROB1)*(FSE(N-1)-FSE(N-3))/(PROB-PROB1) |
| 12915 |
RETURN |
| 12916 |
110 WRITE(IOUT,10000)IS |
| 12917 |
10000 FORMAT(' MICAP: INTERPOLATION SCHEME=',I3,' IN SECLF1') |
| 12918 |
GOTO 130 |
| 12919 |
120 WRITE(IOUT,10100)R,PROB |
| 12920 |
10100 FORMAT(' MICAP: EXIT ENERGY NOT SELECTED IN SECLF1',1P2E13.5) |
| 12921 |
130 WRITE(6,*) ' CALOR: ERROR in SECLF1 =====> STOP ' |
| 12922 |
STOP |
| 12923 |
END |
| 12924 |
*CMZ : 1.04/00 02/02/95 09.24.15 by Christian Zeitnitz |
| 12925 |
*-- Author : |
| 12926 |
SUBROUTINE SECLF5(FSE,IFSE,EX,U,E) |
| 12927 |
C THIS ROUTINE SAMPLES AN EXIT ENERGY FROM |
| 12928 |
C A GENERAL EVAPORATION SPECTRUM |
| 12929 |
#include "minput.inc" |
| 12930 |
*KEND. |
| 12931 |
DIMENSION FSE(*),IFSE(*) |
| 12932 |
SAVE |
| 12933 |
C DETERMINE THETA |
| 12934 |
IP=1 |
| 12935 |
NR=IFSE(IP) |
| 12936 |
NE=IFSE(IP+1) |
| 12937 |
IP=2*NR+IP |
| 12938 |
EMAX=E-U |
| 12939 |
R=FLTRNF(0) |
| 12940 |
DO 10 I=1,NE |
| 12941 |
IP=IP+2 |
| 12942 |
IF(E.LE.FSE(IP))GO TO 20 |
| 12943 |
10 CONTINUE |
| 12944 |
GO TO 80 |
| 12945 |
20 IF(I.EQ.1)GO TO 90 |
| 12946 |
C DETERMINE THE INTERPOLATING SCHEME |
| 12947 |
CALL INTSCH(IFSE,I,IS,NR) |
| 12948 |
E2=FSE(IP) |
| 12949 |
E1=FSE(IP-2) |
| 12950 |
CALL INTERP(E,THETA,E1,FSE(IP-1),E2,FSE(IP+1),IS) |
| 12951 |
IP=IP+2+(NE-I)*2 |
| 12952 |
C DETERMINE X |
| 12953 |
30 NF=IFSE(IP+1) |
| 12954 |
NR=IFSE(IP) |
| 12955 |
IPR=IP |
| 12956 |
IP=IP+1+2*NR |
| 12957 |
PROB=0. |
| 12958 |
DO 60 I=1,NF |
| 12959 |
N=IP+2*I |
| 12960 |
PROB1=PROB |
| 12961 |
CALL INTSCH(IFSE(IPR),I,IS,NR) |
| 12962 |
IF(I.EQ.1)GO TO 60 |
| 12963 |
IF(IS.EQ.1)GO TO 40 |
| 12964 |
IF(IS.GT.2)GO TO 100 |
| 12965 |
PROB=PROB+(FSE(N)+FSE(N-2))*(FSE(N-1)-FSE(N-3))/2. |
| 12966 |
GO TO 50 |
| 12967 |
40 PROB=PROB+FSE(N-2)*(FSE(N-1)-FSE(N-3)) |
| 12968 |
50 CONTINUE |
| 12969 |
IF(R.LE.PROB)GO TO 70 |
| 12970 |
60 CONTINUE |
| 12971 |
70 X=FSE(N-3)+(R-PROB1)*(FSE(N-1)-FSE(N-3))/(PROB-PROB1) |
| 12972 |
C SELECT THE EXIT ENERGY FROM THE GENERAL EVAPORATION SPECTRUM |
| 12973 |
EX=THETA*X |
| 12974 |
IF(EX.LE.EMAX)RETURN |
| 12975 |
EX=EMAX |
| 12976 |
RETURN |
| 12977 |
C INCIDENT ENERGY IS ABOVE THE LAST INCIDENT ENERGY GIVEN |
| 12978 |
C USE THE LAST DISTRIBUTION |
| 12979 |
80 THETA=FSE(IP+1) |
| 12980 |
IP=IP+2 |
| 12981 |
GO TO 30 |
| 12982 |
C INCIDENT ENERGY IS BELOW THE FIRST INCIDENT ENERGY GIVEN |
| 12983 |
C USE THE FIRST DISTRIBUTION |
| 12984 |
90 THETA=FSE(IP+1) |
| 12985 |
IP=IP+2*(NE-I)+2 |
| 12986 |
GO TO 30 |
| 12987 |
100 WRITE(IOUT,10100)IS |
| 12988 |
10100 FORMAT(' MICAP: INTERPOLATION SCHEME=',I3,' IN SECLF5') |
| 12989 |
WRITE(6,*) ' CALOR: ERROR in SECLF5 =====> STOP ' |
| 12990 |
STOP |
| 12991 |
END |
| 12992 |
*CMZ : 1.04/00 02/02/95 09.24.44 by Christian Zeitnitz |
| 12993 |
*-- Author : |
| 12994 |
SUBROUTINE SECLF7(FSE,IFSE,EX,U,E) |
| 12995 |
C THIS ROUTINE SAMPLES AN EXIT ENERGY FROM |
| 12996 |
C A SIMPLE FISSION SPECTRUM |
| 12997 |
#include "minput.inc" |
| 12998 |
*KEND. |
| 12999 |
DIMENSION FSE(*),IFSE(*) |
| 13000 |
SAVE |
| 13001 |
C DETERMINE THETA |
| 13002 |
IP=1 |
| 13003 |
EMAX=E-U |
| 13004 |
NR=IFSE(IP) |
| 13005 |
NE=IFSE(IP+1) |
| 13006 |
IP=2*NR+1 |
| 13007 |
DO 10 I=1,NE |
| 13008 |
IP=IP+2 |
| 13009 |
IF(E.LE.FSE(IP))GO TO 20 |
| 13010 |
10 CONTINUE |
| 13011 |
GO TO 30 |
| 13012 |
20 IF(I.EQ.1)GO TO 40 |
| 13013 |
C DETERMINE THE INTERPOLATING SCHEME |
| 13014 |
CALL INTSCH(IFSE,I,IS,NR) |
| 13015 |
E1=FSE(IP-2) |
| 13016 |
E2=FSE(IP) |
| 13017 |
CALL INTERP(E,THETA,E1,FSE(IP-1),E2,FSE(IP+1),IS) |
| 13018 |
GO TO 50 |
| 13019 |
C INCIDENT ENERGY IS ABOVE THE LAST INCIDENT ENERGY GIVEN |
| 13020 |
C USE THE LAST DISTRIBUTION |
| 13021 |
30 THETA=FSE(IP+1) |
| 13022 |
GO TO 50 |
| 13023 |
C INCIDENT ENERGY IS BELOW THE FIRST INCIDENT ENERGY GIVEN |
| 13024 |
C USE THE FIRST DISTRIBUTION |
| 13025 |
40 THETA=FSE(IP+1) |
| 13026 |
C SELECT THE EXIT ENERGY FROM THE FISSION SPECTRUM |
| 13027 |
50 R1=FLTRNF(0) |
| 13028 |
R2=FLTRNF(0) |
| 13029 |
S=R1**2+R2**2 |
| 13030 |
IF(S.GT.1.)GO TO 50 |
| 13031 |
TAU=(-ALOG(S)/S)*(R1**2) |
| 13032 |
R=FLTRNF(0) |
| 13033 |
W=-ALOG(R)+TAU |
| 13034 |
EX=THETA*W |
| 13035 |
IF(EX.LE.EMAX)RETURN |
| 13036 |
EX=EMAX |
| 13037 |
RETURN |
| 13038 |
END |
| 13039 |
*CMZ : 1.04/00 02/02/95 09.25.31 by Christian Zeitnitz |
| 13040 |
*-- Author : |
| 13041 |
SUBROUTINE SECLF9(FSE,IFSE,EX,U,E) |
| 13042 |
C THIS ROUTINE SAMPLES AN EXIT ENERGY FROM |
| 13043 |
C AN EVAPORATION SPECTRUM |
| 13044 |
#include "minput.inc" |
| 13045 |
*KEND. |
| 13046 |
DIMENSION FSE(*),IFSE(*) |
| 13047 |
SAVE |
| 13048 |
C DETERMINE THETA |
| 13049 |
IP=1 |
| 13050 |
EMAX=E-U |
| 13051 |
NR=IFSE(IP) |
| 13052 |
NE=IFSE(IP+1) |
| 13053 |
IP=2*NR+1 |
| 13054 |
DO 10 I=1,NE |
| 13055 |
IP=IP+2 |
| 13056 |
IF(E.LE.FSE(IP))GO TO 20 |
| 13057 |
10 CONTINUE |
| 13058 |
GO TO 30 |
| 13059 |
20 IF(I.EQ.1)GO TO 40 |
| 13060 |
C DETERMINE THE INTERPOLATING SCHEME |
| 13061 |
CALL INTSCH(IFSE,I,IS,NR) |
| 13062 |
E1=FSE(IP-2) |
| 13063 |
E2=FSE(IP) |
| 13064 |
CALL INTERP(E,THETA,E1,FSE(IP-1),E2,FSE(IP+1),IS) |
| 13065 |
GO TO 50 |
| 13066 |
C INCIDENT ENERGY IS ABOVE THE LAST INCIDENT ENERGY GIVEN |
| 13067 |
C USE THE LAST DISTRIBUTION |
| 13068 |
30 THETA=FSE(IP+1) |
| 13069 |
GO TO 50 |
| 13070 |
C INCIDENT ENERGY IS BELOW THE FIRST INCIDENT ENERGY GIVEN |
| 13071 |
C USE THE FIRST DISTRIBUTION |
| 13072 |
40 THETA=FSE(IP+1) |
| 13073 |
C SELECT THE EXIT ENERGY FROM THE EVAPORATION SPECTRUM |
| 13074 |
50 R1=FLTRNF(0) |
| 13075 |
R2=FLTRNF(0) |
| 13076 |
W=-ALOG(R1*R2) |
| 13077 |
EX=THETA*W |
| 13078 |
IF(EX.LE.EMAX)RETURN |
| 13079 |
EX=EMAX |
| 13080 |
RETURN |
| 13081 |
END |
| 13082 |
*CMZ : 1.01/04 10/06/93 14.43.49 by Christian Zeitnitz |
| 13083 |
*-- Author : Christian Zeitnitz 03/08/92 |
| 13084 |
SUBROUTINE STOPAR(ID,NP) |
| 13085 |
C store particle in MPSTOR common |
| 13086 |
#include "mconst.inc" |
| 13087 |
#include "mpstor.inc" |
| 13088 |
#include "minput.inc" |
| 13089 |
*KEND. |
| 13090 |
C |
| 13091 |
NPSTOR = NPSTOR + 1 |
| 13092 |
IF(NPSTOR.GT.MAXPAR) THEN |
| 13093 |
WRITE(IOUT,'('' MICAP : Cant store particle; bank full'', ' |
| 13094 |
+ //' '' ID='',I3,'' NPSTOR='',I5)') ID,NPSTOR |
| 13095 |
NPSTOR = NPSTOR - 1 |
| 13096 |
ELSE |
| 13097 |
EN(NPSTOR) = EP |
| 13098 |
UN(NPSTOR) = UP |
| 13099 |
VN(NPSTOR) = VP |
| 13100 |
WN(NPSTOR) = WP |
| 13101 |
AMN(NPSTOR) = AMP |
| 13102 |
ZMN(NPSTOR) = ZMP |
| 13103 |
AGEN(NPSTOR) = AGEP |
| 13104 |
MTN(NPSTOR) = MTP |
| 13105 |
IDN(NPSTOR) = ID |
| 13106 |
NP = NP + 1 |
| 13107 |
ENDIF |
| 13108 |
RETURN |
| 13109 |
END |
| 13110 |
*CMZ : 0.92/00 02/12/92 16.02.33 by Christian Zeitnitz |
| 13111 |
*-- Author : |
| 13112 |
SUBROUTINE TBSPLT(A,E,NP,Y) |
| 13113 |
C THIS ROUTINE DETERMINES A CROSS SECTION AT A GIVEN |
| 13114 |
C ENERGY FROM A CROSS SECTION VERSUS ENERGY TABLE USING |
| 13115 |
C A TABLE SPLITTING METHOD |
| 13116 |
DIMENSION A(1) |
| 13117 |
SAVE |
| 13118 |
IPP=1 |
| 13119 |
IF(E.LE.A(1))GO TO 40 |
| 13120 |
IF(E.GE.A(2*NP-1))GO TO 50 |
| 13121 |
INDXH=NP |
| 13122 |
INDXL=0 |
| 13123 |
10 IF(INDXL+1.EQ.INDXH)GO TO 30 |
| 13124 |
J=(INDXH+INDXL)/2 |
| 13125 |
N=2*J-1 |
| 13126 |
IF(E.LE.A(N))GO TO 20 |
| 13127 |
INDXL=J |
| 13128 |
GO TO 10 |
| 13129 |
20 INDXH=J |
| 13130 |
GO TO 10 |
| 13131 |
30 N=2*INDXH-1 |
| 13132 |
Y=A(N-1)+(E-A(N-2))*(A(N+1)-A(N-1))/(A(N)-A(N-2)) |
| 13133 |
RETURN |
| 13134 |
40 Y=A(IPP+1) |
| 13135 |
RETURN |
| 13136 |
50 Y=A(2*NP) |
| 13137 |
RETURN |
| 13138 |
END |
| 13139 |
*CMZ : 1.05/03 27/06/2001 18.34.49 by Christian Zeitnitz |
| 13140 |
*-- Author : |
| 13141 |
SUBROUTINE THRMSC(D,LD,XTHRMS,ITHRMS,LTHRM,E,U,V,W,TEMP,FM,AWR, |
| 13142 |
+ IIN,IFLG,IOUT) |
| 13143 |
C THIS ROUTINE CONTROLS SELECTION OF THE NEUTRON EXIT ENERGY |
| 13144 |
C IN THE THERMAL DATA RANGE |
| 13145 |
#include "mupsca.inc" |
| 13146 |
*KEND. |
| 13147 |
DIMENSION D(*),LD(*),XTHRMS(*),ITHRMS(*),LTHRM(*),AWR(*) |
| 13148 |
REAL HMASSN/0.5044905/,SPI/1.1283792/ |
| 13149 |
C HMASSN EQUALS ONE-HALF THE NEUTRON MASS |
| 13150 |
C SPI EQUALS TWO DIVIDED BY THE SQUARE ROOT OF PI |
| 13151 |
C CONVERT TEMPERATURE FROM DEGREES KELVIN TO EV |
| 13152 |
DATA BK/8.6167E-5/ |
| 13153 |
SAVE |
| 13154 |
C |
| 13155 |
TDK=BK*TEMP |
| 13156 |
AAWR=AWR(IIN) |
| 13157 |
IFLG=0 |
| 13158 |
NE=ITHRMS(IIN) |
| 13159 |
IF(NE.LE.0)GO TO 10 |
| 13160 |
EO=E |
| 13161 |
NP7=ITHRMS(IIN+1) |
| 13162 |
NB7=ITHRMS(IIN+2) |
| 13163 |
CT=ITHRMS(IIN+3) |
| 13164 |
LENMD=ITHRMS(IIN+4) |
| 13165 |
N=NB7*NE |
| 13166 |
CALL THRSEL(NE,NP7,NB7,E,EOUT,FM,CT,XTHRMS(IIN+5), |
| 13167 |
+ XTHRMS(IIN+5+NE),XTHRMS(IIN+5+NE+NP7), |
| 13168 |
+ XTHRMS(IIN+5+NE+NP7+NB7), |
| 13169 |
+ XTHRMS(IIN+5+2*NE+NP7+NB7),XTHRMS(IIN+5+2*NE+NP7+NB7+N), |
| 13170 |
+ XTHRMS(IIN+5+2*NE+NP7+NB7+N+LENMD),AWR,IIN, |
| 13171 |
+ ITHRMS(IIN+5+2*NE+NP7+NB7+N+LENMD+NP7*NB7), |
| 13172 |
+ ITHRMS(IIN+5+2*NE+NP7+NB7+N),IOUT) |
| 13173 |
E=EOUT |
| 13174 |
C IFLG EQUAL TO ONE IMPLIES (FM) IN LABORATORY SYSTEM |
| 13175 |
IFLG=1 |
| 13176 |
RETURN |
| 13177 |
C FREE GAS MODEL |
| 13178 |
10 CONTINUE |
| 13179 |
C SPD IS THE SPEED OF THE INCIDENT NEUTRON |
| 13180 |
SPD=SQRT(E/HMASSN) |
| 13181 |
TAUN=SPI*SQRT(2.0*TDK/AAWR) |
| 13182 |
PTEST=SPD/(SPD+TAUN) |
| 13183 |
C UO, VO, AND WO ARE THE VELOCITY COMPONENTS OF THE INCIDENT |
| 13184 |
C NEUTRON IN TERMS OF THE NEUTRON SPEED |
| 13185 |
UO=SPD*U |
| 13186 |
VO=SPD*V |
| 13187 |
WO=SPD*W |
| 13188 |
20 CONTINUE |
| 13189 |
IF(PTEST.GT.FLTRNF(0))GO TO 30 |
| 13190 |
ETA=-ALOG(FLTRNF(0)*FLTRNF(0))*TDK |
| 13191 |
GO TO 40 |
| 13192 |
30 CONTINUE |
| 13193 |
ETA=RNMAXF(TDK) |
| 13194 |
40 CONTINUE |
| 13195 |
C ERFGM IS THE INITIAL ENERGY OF THE TARGET NUCLEUS |
| 13196 |
ERFGM=ETA |
| 13197 |
C ETA IS THE SPEED OF THE TARGET NUCLEUS |
| 13198 |
ETA=SQRT(2.0*ETA/AAWR) |
| 13199 |
C UN, VN, AND WN ARE THE VELOCITY COMPONENTS OF THE TARGET |
| 13200 |
C NUCLEUS IN TERMS OF THE TARGET NUCLEUS SPEED |
| 13201 |
CALL GTISO(UN,VN,WN) |
| 13202 |
UN=UN*ETA |
| 13203 |
VN=VN*ETA |
| 13204 |
WN=WN*ETA |
| 13205 |
VRELSQ=(UO-UN)**2+(VO-VN)**2+(WO-WN)**2 |
| 13206 |
F2=FLTRNF(0)**2 |
| 13207 |
V2=VRELSQ/(SPD+ETA)**2 |
| 13208 |
IF(F2.GT.V2)GO TO 20 |
| 13209 |
VREL=SQRT(VRELSQ) |
| 13210 |
ALPHA=1.0/(AAWR+1.0) |
| 13211 |
BETA=1.0-ALPHA |
| 13212 |
CALL GTISO(UA,VA,WA) |
| 13213 |
UO=UO*ALPHA+BETA*(UN+VREL*UA) |
| 13214 |
VO=VO*ALPHA+BETA*(VN+VREL*VA) |
| 13215 |
WO=WO*ALPHA+BETA*(WN+VREL*WA) |
| 13216 |
SPDSQ=UO*UO+VO*VO+WO*WO |
| 13217 |
C E IS THE EXIT ENERGY OF THE NEUTRON |
| 13218 |
E=HMASSN*SPDSQ |
| 13219 |
SPD=1.0/SQRT(SPDSQ) |
| 13220 |
FM=(U*UO+V*VO+W*WO)*SPD |
| 13221 |
C U, V, AND W ARE THE EXIT NEUTRON DIRECTION COSINES |
| 13222 |
U=UO*SPD |
| 13223 |
V=VO*SPD |
| 13224 |
W=WO*SPD |
| 13225 |
C IFLG EQUAL TO TWO IMPLIES (U,V,W) IN LABORATORY SYSTEM |
| 13226 |
IFLG=2 |
| 13227 |
RETURN |
| 13228 |
END |
| 13229 |
*CMZ : 1.01/04 10/06/93 14.43.49 by Christian Zeitnitz |
| 13230 |
*-- Author : |
| 13231 |
SUBROUTINE THRSEL(NE,NP7,NB7,E,EOUT,FM,TDK,ETH,ALPHA,BETA,W, |
| 13232 |
+ PMUPS,PMDS,F,AWR,IIN,IPTMD,IPMDS,IOUT) |
| 13233 |
C THIS ROUTINE SELECTS THE EXIT ENERGY AND SCATTERING ANGLE |
| 13234 |
C FROM S(ALPHA,BETA) DATA TABLES |
| 13235 |
DIMENSION ETH(*),ALPHA(*),BETA(*),ABETA2(2),PMDS(*), |
| 13236 |
+ IPTMD(NE),W(NE),IPMDS(*),PMUPS(NB7,NE),F(NP7,NB7),AWR(*) |
| 13237 |
SAVE |
| 13238 |
C |
| 13239 |
AAWR=AWR(IIN) |
| 13240 |
DO 10 IE=1,NE |
| 13241 |
IF(E.LT.ETH(IE))GO TO 20 |
| 13242 |
10 CONTINUE |
| 13243 |
INDX=NE |
| 13244 |
GO TO 30 |
| 13245 |
20 INDX=IE |
| 13246 |
IF(INDX.EQ.1)GO TO 30 |
| 13247 |
R=FLTRNF(0) |
| 13248 |
DELE=(ETH(INDX)-E)/(ETH(INDX)-ETH(INDX-1)) |
| 13249 |
DELEN=DELE |
| 13250 |
GO TO 40 |
| 13251 |
30 DELEN=1.0 |
| 13252 |
INDX=2 |
| 13253 |
40 PROB=DELEN*W(INDX-1)+(1.0-DELEN)*W(INDX) |
| 13254 |
IF(R.LE.PROB)GO TO 120 |
| 13255 |
C NEUTRON DOWNSCATTERS |
| 13256 |
R=FLTRNF(0) |
| 13257 |
DO 90 I=1,2 |
| 13258 |
IP=IPTMD(INDX) |
| 13259 |
NB=IPMDS(IP) |
| 13260 |
DO 50 IB=1,NB |
| 13261 |
IF(R.LE.PMDS(IP+NB+IB))GO TO 60 |
| 13262 |
50 CONTINUE |
| 13263 |
WRITE(IOUT,10000)PMDS(IP+2*NB) |
| 13264 |
10000 FORMAT(' MICAP: CUMULATIVE DOWNSCATTER DIST. DOES NOT END ', |
| 13265 |
+ 'IN 1.0 IN THRSEL',E12.4) |
| 13266 |
PRINT *,' CALOR: ERROR in MICAP ====> STOP ' |
| 13267 |
STOP |
| 13268 |
60 IF(IB.EQ.1)GO TO 70 |
| 13269 |
DELE=(PMDS(IP+NB+IB)-R)/(PMDS(IP+NB+IB)-PMDS(IP+NB+IB-1)) |
| 13270 |
ABETA=DELE*(PMDS(IP+IB-1)-PMDS(IP+IB))+PMDS(IP+IB) |
| 13271 |
GO TO 80 |
| 13272 |
70 ABETA=BETA(IB) |
| 13273 |
80 ABETA2(I)=ABETA |
| 13274 |
INDX=INDX-1 |
| 13275 |
90 CONTINUE |
| 13276 |
ABETA=DELEN*ABETA2(2)+(1.0-DELEN)*ABETA2(1) |
| 13277 |
EOUT=E-TDK*ABETA |
| 13278 |
IF(EOUT.LT.1.0E-05)EOUT=1.0E-05 |
| 13279 |
DO 100 IB=1,NB7 |
| 13280 |
IF(ABETA.LE.BETA(IB))GO TO 110 |
| 13281 |
100 CONTINUE |
| 13282 |
IB=NB7 |
| 13283 |
110 DELE=(ABETA-BETA(IB))/(BETA(IB-1)-BETA(IB)) |
| 13284 |
GO TO 180 |
| 13285 |
C NEUTRON UPSCATTERS |
| 13286 |
120 R=FLTRNF(0) |
| 13287 |
DO 170 I=1,2 |
| 13288 |
DO 130 IB=1,NB7 |
| 13289 |
IF(R.LE.PMUPS(IB,INDX))GO TO 140 |
| 13290 |
130 CONTINUE |
| 13291 |
WRITE(IOUT,10100)PMUPS(NB7,INDX) |
| 13292 |
10100 FORMAT(' MICAP: CUMULATIVE UPSCATTER DIST. DOES NOT END ', |
| 13293 |
+ 'IN 1.0 IN THRSEL',E12.4) |
| 13294 |
PRINT *,' CALOR: ERROR in MICAP ====> STOP ' |
| 13295 |
STOP |
| 13296 |
140 IF(IB.EQ.1)GO TO 150 |
| 13297 |
DELE=(PMUPS(IB,INDX)-R)/(PMUPS(IB,INDX)-PMUPS(IB-1,INDX)) |
| 13298 |
ABETA=DELE*(BETA(IB-1)-BETA(IB))+BETA(IB) |
| 13299 |
GO TO 160 |
| 13300 |
150 WRITE(IOUT,10200)PMUPS(1,INDX) |
| 13301 |
10200 FORMAT(' MICAP: CUMULATIVE UPSCATTER DIST. DOES NOT BEGIN ', |
| 13302 |
+ 'AT 0.0 IN THRSEL',E12.4) |
| 13303 |
PRINT *,' CALOR: ERROR in MICAP ====> STOP ' |
| 13304 |
STOP |
| 13305 |
160 ABETA2(I)=ABETA |
| 13306 |
INDX=INDX-1 |
| 13307 |
170 CONTINUE |
| 13308 |
ABETA=DELEN*ABETA2(2)+(1.0-DELEN)*ABETA2(1) |
| 13309 |
EOUT=E+TDK*ABETA |
| 13310 |
C SELECT ANGLE |
| 13311 |
180 AMAX=(EOUT+E+2.0*SQRT(E*EOUT))/(AAWR*TDK) |
| 13312 |
AMIN=(EOUT+E-2.0*SQRT(E*EOUT))/(AAWR*TDK) |
| 13313 |
DO 190 IA=1,NP7 |
| 13314 |
IF(AMAX.LT.ALPHA(IA))GO TO 200 |
| 13315 |
190 CONTINUE |
| 13316 |
IA=NP7 |
| 13317 |
DELA=0.0 |
| 13318 |
GO TO 210 |
| 13319 |
200 DELA=(ALPHA(IA)-AMAX)/(ALPHA(IA)-ALPHA(IA-1)) |
| 13320 |
210 F4=DELE*(F(IA,IB-1)-F(IA,IB))+F(IA,IB) |
| 13321 |
F3=DELE*(F(IA-1,IB-1)-F(IA-1,IB))+F(IA-1,IB) |
| 13322 |
F2=DELA*(F3-F4)+F4 |
| 13323 |
DO 220 IA=1,NP7 |
| 13324 |
IF(AMIN.LT.ALPHA(IA))GO TO 230 |
| 13325 |
220 CONTINUE |
| 13326 |
IA=NP7 |
| 13327 |
DELA=0.0 |
| 13328 |
GO TO 240 |
| 13329 |
230 DELA=(ALPHA(IA)-AMIN)/(ALPHA(IA)-ALPHA(IA-1)) |
| 13330 |
240 F4=DELE*(F(IA,IB-1)-F(IA,IB))+F(IA,IB) |
| 13331 |
F3=DELE*(F(IA-1,IB-1)-F(IA-1,IB))+F(IA-1,IB) |
| 13332 |
F1=DELA*(F3-F4)+F4 |
| 13333 |
R=FLTRNF(0) |
| 13334 |
F0=R*F2+(1.0-R)*F1 |
| 13335 |
F1=0.0 |
| 13336 |
DO 250 IA=1,NP7 |
| 13337 |
F2=DELE*(F(IA,IB-1)-F(IA,IB))+F(IA,IB) |
| 13338 |
IF(F0.LE.F2)GO TO 260 |
| 13339 |
F1=F2 |
| 13340 |
250 CONTINUE |
| 13341 |
260 IF(F1.EQ.F2)GO TO 270 |
| 13342 |
DELA=(F2-F0)/(F2-F1) |
| 13343 |
GO TO 280 |
| 13344 |
270 ALP=ALPHA(IA) |
| 13345 |
GO TO 290 |
| 13346 |
280 ALP=DELA*ALPHA(IA-1)+(1.0-DELA)*ALPHA(IA) |
| 13347 |
290 FM=(E+EOUT-ALP*AAWR*TDK)/(2.0*SQRT(E*EOUT)) |
| 13348 |
IF(ABS(FM).LE.1.0)RETURN |
| 13349 |
WRITE(IOUT,10300)FM,E,EOUT,R,IA,IB |
| 13350 |
10300 FORMAT(' MICAP: ERROR IN THRSEL, COSINE OF ANGLE >1'/, |
| 13351 |
+' ',1P4E12.4,2I11) |
| 13352 |
FM=2.0*FLTRNF(0)-1.0 |
| 13353 |
RETURN |
| 13354 |
END |
| 13355 |
*CMZ : 1.01/04 10/06/93 14.43.49 by Christian Zeitnitz |
| 13356 |
*-- Author : |
| 13357 |
SUBROUTINE TREBOD(D,LD,KZ1,KZ2,KZ3,A1,A2,A3,Z1,Z2,Z3, |
| 13358 |
+ ATAR,Q,MT) |
| 13359 |
C CZ July 30,1992 Simple aproach to get (N,PA), (N,T2A),(N,D2A) |
| 13360 |
C processes. This is TWOBOD extended to a third particle |
| 13361 |
C THIS ROUTINE CALCULATES THE EXIT ENERGIES AND DIRECTIONAL |
| 13362 |
C COSINES FOR THE CHARGED PARTICLE AND RECOIL NUCLEUS FOR |
| 13363 |
C A THREE-BODY REACTION USING AN EVAPORATION SPECTRUM AND |
| 13364 |
C MOMEMTUM BALANCE. IT ALSO SETS ALL EXIT PARAMETERS FOR |
| 13365 |
C THE COLLISION PRODUCTS AND STORES THEM IN THE RECOIL BANK. |
| 13366 |
#include "minput.inc" |
| 13367 |
#include "mconst.inc" |
| 13368 |
#include "mnutrn.inc" |
| 13369 |
#include "mrecoi.inc" |
| 13370 |
#include "mapoll.inc" |
| 13371 |
#include "mmass.inc" |
| 13372 |
#include "mpstor.inc" |
| 13373 |
*KEND. |
| 13374 |
DIMENSION D(*),LD(*),ER1(3) |
| 13375 |
SAVE |
| 13376 |
C loop over no. of emmitted particles CZ July 30,1992 |
| 13377 |
NPN = 1 |
| 13378 |
IF(MT.EQ.112) NPN = 2 |
| 13379 |
IF(MT.EQ.113) NPN = 3 |
| 13380 |
IF(MT.EQ.114) NPN = 3 |
| 13381 |
PRXO = 0.0 |
| 13382 |
PRYO = 0.0 |
| 13383 |
PRZO = 0.0 |
| 13384 |
DO 10 NP=1,NPN |
| 13385 |
C CALCULATE THE COULOMB BARRIER (CB) |
| 13386 |
CALL BARIER(KZ1,KZ2,A1,A3,CB) |
| 13387 |
C CALCULATE THE CHARGED PARTICLE EXIT ENERGY (EX) |
| 13388 |
CALL CEVAP(EOLD,Q,ATAR,CB,EX) |
| 13389 |
E1=EX+CB |
| 13390 |
ZMSS = Z2 |
| 13391 |
AMSS = A2 |
| 13392 |
KZZ = KZ2 |
| 13393 |
IF(NP.EQ.1) THEN |
| 13394 |
ZMSS = Z1 |
| 13395 |
AMSS = A1 |
| 13396 |
KZZ = KZ1 |
| 13397 |
ENDIF |
| 13398 |
C ASSUME ISOTROPIC CHARGED PARTICLE EMISSION IN THE LABORATORY |
| 13399 |
CALL GTISO(U1,V1,W1) |
| 13400 |
PPN = SQRT(2.0*ZMSS*E1) |
| 13401 |
PRXO = PRXO + U1*PPN |
| 13402 |
PRYO = PRYO + V1*PPN |
| 13403 |
PRZO = PRZO + W1*PPN |
| 13404 |
C CALCULATE AND SET THE CHARGED PARTICLE EXIT PARAMETERS |
| 13405 |
XR=X |
| 13406 |
YR=Y |
| 13407 |
ZR=Z |
| 13408 |
WATER=WTBC |
| 13409 |
NZR=KZZ |
| 13410 |
AGER=AGE |
| 13411 |
NCOLR=NCOL |
| 13412 |
MTNR=MT |
| 13413 |
AR=AMSS |
| 13414 |
ENIR=EOLD |
| 13415 |
UNIR=UOLD |
| 13416 |
VNIR=VOLD |
| 13417 |
WNIR=WOLD |
| 13418 |
ENOR=0.0 |
| 13419 |
UNOR=0.0 |
| 13420 |
VNOR=0.0 |
| 13421 |
WNOR=0.0 |
| 13422 |
WTNR=0.0 |
| 13423 |
QR=Q |
| 13424 |
UR=U1 |
| 13425 |
VR=V1 |
| 13426 |
WR=W1 |
| 13427 |
ER=E1 |
| 13428 |
C STORE THE CHARGED PARTICLE IN THE RECOIL BANK |
| 13429 |
EP = ER |
| 13430 |
UP = UR |
| 13431 |
VP = VR |
| 13432 |
WP = WR |
| 13433 |
AMP = AR |
| 13434 |
ZMP = FLOAT(NZR) |
| 13435 |
AGEP = AGE |
| 13436 |
MTP = MT |
| 13437 |
CALL STOPAR(IDHEVY,NHEVY) |
| 13438 |
A3 = A3 - A2 |
| 13439 |
Z3 = Z3 - Z2 |
| 13440 |
KZ3 = KZ3 - KZ2 |
| 13441 |
10 CONTINUE |
| 13442 |
A3 = A3 + A2 |
| 13443 |
Z3 = Z3 + Z2 |
| 13444 |
KZ3 = KZ3 + KZ2 |
| 13445 |
C CALCULATE THE TOTAL MOMENTUM BEFORE THE COLLISION |
| 13446 |
C NEUTRON MOMENTUM BEFORE COLLISION (PI) EQUALS TOTAL MOMENTUM |
| 13447 |
PI=SQRT(2.0*ZN*EOLD) |
| 13448 |
C CALCULATE THE DIRECTIONAL MOMENTUM OF THE RECOIL NUCLEUS |
| 13449 |
PRX=PI*UOLD - PRXO |
| 13450 |
PRY=PI*VOLD - PRYO |
| 13451 |
PRZ=PI*WOLD - PRZO |
| 13452 |
C CALCULATE THE TOTAL MOMENTUM OF THE RECOIL NUCLEUS |
| 13453 |
PR=SQRT(PRX**2+PRY**2+PRZ**2) |
| 13454 |
C CALCULATE THE RECOIL NUCLEUS DIRECTIONAL COSINES |
| 13455 |
U2=PRX/PR |
| 13456 |
V2=PRY/PR |
| 13457 |
W2=PRZ/PR |
| 13458 |
C CALCULATE THE RECOIL NUCLEUS EXIT ENERGY |
| 13459 |
XM = A2 * 931.075E6 |
| 13460 |
E2 = SQRT(PR**2+XM**2) - XM |
| 13461 |
C CALCULATE AND SET THE CHARGED PARTICLE EXIT PARAMETERS |
| 13462 |
XR=X |
| 13463 |
YR=Y |
| 13464 |
ZR=Z |
| 13465 |
WATER=WTBC |
| 13466 |
NZR=KZ3 |
| 13467 |
AGER=AGE |
| 13468 |
NCOLR=NCOL |
| 13469 |
MTNR=MT |
| 13470 |
AR=A3 |
| 13471 |
ENIR=EOLD |
| 13472 |
UNIR=UOLD |
| 13473 |
VNIR=VOLD |
| 13474 |
WNIR=WOLD |
| 13475 |
ENOR=0.0 |
| 13476 |
UNOR=0.0 |
| 13477 |
VNOR=0.0 |
| 13478 |
WNOR=0.0 |
| 13479 |
WTNR=0.0 |
| 13480 |
QR=Q |
| 13481 |
UR=U2 |
| 13482 |
VR=V2 |
| 13483 |
WR=W2 |
| 13484 |
ER=E2 |
| 13485 |
C STORE THE RECOIL HEAVY ION IN THE RECOIL BANK |
| 13486 |
EP = ER |
| 13487 |
UP = UR |
| 13488 |
VP = VR |
| 13489 |
WP = WR |
| 13490 |
AMP = AR |
| 13491 |
ZMP = FLOAT(NZR) |
| 13492 |
AGEP = AGE |
| 13493 |
MTP = MT |
| 13494 |
CALL STOPAR(IDHEVY,NHEVY) |
| 13495 |
RETURN |
| 13496 |
END |
| 13497 |
*CMZ : 1.04/03 15/02/95 14.00.42 by Christian Zeitnitz |
| 13498 |
*-- Author : |
| 13499 |
SUBROUTINE TWOBOD(D,LD,KZ1,KZ2,A1,A2,Z1,Z2,ATAR,Q,MT) |
| 13500 |
C THIS ROUTINE CALCULATES THE EXIT ENERGIES AND DIRECTIONAL |
| 13501 |
C COSINES FOR THE CHARGED PARTICLE AND RECOIL NUCLEUS FOR |
| 13502 |
C A TWO-BODY REACTION USING AN EVAPORATION SPECTRUM AND |
| 13503 |
C MOMEMTUM BALANCE. IT ALSO SETS ALL EXIT PARAMETERS FOR |
| 13504 |
C THE COLLISION PRODUCTS AND STORES THEM IN THE RECOIL BANK. |
| 13505 |
#include "minput.inc" |
| 13506 |
#include "mconst.inc" |
| 13507 |
#include "mnutrn.inc" |
| 13508 |
#include "mrecoi.inc" |
| 13509 |
#include "mapoll.inc" |
| 13510 |
#include "mmass.inc" |
| 13511 |
#include "mpstor.inc" |
| 13512 |
*KEND. |
| 13513 |
DIMENSION D(*),LD(*) |
| 13514 |
SAVE |
| 13515 |
PRXO = 0.0 |
| 13516 |
PRYO = 0.0 |
| 13517 |
PRZO = 0.0 |
| 13518 |
C loop over no. of emmitted particles CZ July 30,1992 |
| 13519 |
NPN = 1 |
| 13520 |
IF(MT.EQ.108) NPN = 2 |
| 13521 |
IF(MT.EQ.109) NPN = 3 |
| 13522 |
IF(MT.EQ.111) NPN = 2 |
| 13523 |
C CALCULATE THE COULOMB BARRIER (CB) |
| 13524 |
CALL BARIER(KZ1,KZ2,A1,A2,CB) |
| 13525 |
C CALCULATE THE CHARGED PARTICLE EXIT ENERGY (EX) |
| 13526 |
CALL CEVAP(EOLD,Q,ATAR,CB,EX) |
| 13527 |
E1=EX+CB |
| 13528 |
C calculate the massnumber and mass of the residual nucleus |
| 13529 |
A2 = A2 - (NPN-1)*A1 |
| 13530 |
Z2 = Z2 - (NPN-1)*Z1 |
| 13531 |
IF(A2.LT.0.) A2 = 0. |
| 13532 |
IF(Z2.LT.0.) Z2 = 0. |
| 13533 |
IF(NPN.EQ.1) THEN |
| 13534 |
C for 1 final state particle the available kinetic energy is given |
| 13535 |
C by momentum and energy conservation |
| 13536 |
E1 = E1*Z2/(Z1+Z2) |
| 13537 |
ENDIF |
| 13538 |
DO 10 NP=1,NPN |
| 13539 |
C ASSUME ISOTROPIC CHARGED PARTICLE EMISSION IN THE LABORATORY |
| 13540 |
CALL GTISO(U1,V1,W1) |
| 13541 |
IF(NPN.EQ.1) THEN |
| 13542 |
C only one final state particle -> use all the energy available |
| 13543 |
PPN = SQRT(2.0*Z1*E1) |
| 13544 |
EKN = E1 |
| 13545 |
ELSE |
| 13546 |
IF(NP.LT.NPN) THEN |
| 13547 |
EKN = E1*FLTRNF(0) |
| 13548 |
ELSE |
| 13549 |
EKN = E1 |
| 13550 |
ENDIF |
| 13551 |
E1 = E1 - EKN |
| 13552 |
PPN = SQRT(2.0*Z1*EKN) |
| 13553 |
ENDIF |
| 13554 |
PRXO = PRXO + U1*PPN |
| 13555 |
PRYO = PRYO + V1*PPN |
| 13556 |
PRZO = PRZO + W1*PPN |
| 13557 |
C CALCULATE AND SET THE CHARGED PARTICLE EXIT PARAMETERS |
| 13558 |
XR=X |
| 13559 |
YR=Y |
| 13560 |
ZR=Z |
| 13561 |
WATER=WTBC |
| 13562 |
NZR=KZ1 |
| 13563 |
AGER=AGE |
| 13564 |
NCOLR=NCOL |
| 13565 |
MTNR=MT |
| 13566 |
AR=A1 |
| 13567 |
ENIR=EOLD |
| 13568 |
UNIR=UOLD |
| 13569 |
VNIR=VOLD |
| 13570 |
WNIR=WOLD |
| 13571 |
ENOR=0.0 |
| 13572 |
UNOR=0.0 |
| 13573 |
VNOR=0.0 |
| 13574 |
WNOR=0.0 |
| 13575 |
WTNR=0.0 |
| 13576 |
QR=Q |
| 13577 |
UR=U1 |
| 13578 |
VR=V1 |
| 13579 |
WR=W1 |
| 13580 |
ER=EKN |
| 13581 |
C STORE THE CHARGED PARTICLE IN THE RECOIL BANK |
| 13582 |
EP = ER |
| 13583 |
UP = UR |
| 13584 |
VP = VR |
| 13585 |
WP = WR |
| 13586 |
AMP = AR |
| 13587 |
ZMP = FLOAT(NZR) |
| 13588 |
AGEP = AGE |
| 13589 |
MTP = MT |
| 13590 |
CALL STOPAR(IDHEVY,NHEVY) |
| 13591 |
10 CONTINUE |
| 13592 |
C CALCULATE THE TOTAL MOMENTUM BEFORE THE COLLISION |
| 13593 |
C NEUTRON MOMENTUM BEFORE COLLISION (PI) EQUALS TOTAL MOMENTUM |
| 13594 |
PI=SQRT(2.0*ZN*EOLD) |
| 13595 |
C CALCULATE THE DIRECTIONAL MOMENTUM OF THE RECOIL NUCLEUS |
| 13596 |
PRX=PI*UOLD - PRXO |
| 13597 |
PRY=PI*VOLD - PRYO |
| 13598 |
PRZ=PI*WOLD - PRZO |
| 13599 |
C CALCULATE THE TOTAL MOMENTUM OF THE RECOIL NUCLEUS |
| 13600 |
PR=SQRT(PRX**2+PRY**2+PRZ**2) |
| 13601 |
C CALCULATE THE RECOIL NUCLEUS DIRECTIONAL COSINES |
| 13602 |
U2=PRX/PR |
| 13603 |
V2=PRY/PR |
| 13604 |
W2=PRZ/PR |
| 13605 |
C CALCULATE THE RECOIL NUCLEUS EXIT ENERGY |
| 13606 |
XM = A2*931.075E6 |
| 13607 |
E2 = SQRT(PR**2+XM**2) - XM |
| 13608 |
C CALCULATE AND SET THE CHARGED PARTICLE EXIT PARAMETERS |
| 13609 |
XR=X |
| 13610 |
YR=Y |
| 13611 |
ZR=Z |
| 13612 |
WATER=WTBC |
| 13613 |
NZR=KZ2 |
| 13614 |
AGER=AGE |
| 13615 |
NCOLR=NCOL |
| 13616 |
MTNR=MT |
| 13617 |
AR=A2 |
| 13618 |
ENIR=EOLD |
| 13619 |
UNIR=UOLD |
| 13620 |
VNIR=VOLD |
| 13621 |
WNIR=WOLD |
| 13622 |
ENOR=0.0 |
| 13623 |
UNOR=0.0 |
| 13624 |
VNOR=0.0 |
| 13625 |
WNOR=0.0 |
| 13626 |
WTNR=0.0 |
| 13627 |
QR=Q |
| 13628 |
UR=U2 |
| 13629 |
VR=V2 |
| 13630 |
WR=W2 |
| 13631 |
ER=E2 |
| 13632 |
C STORE THE RECOIL HEAVY ION IN THE RECOIL BANK |
| 13633 |
EP = ER |
| 13634 |
UP = UR |
| 13635 |
VP = VR |
| 13636 |
WP = WR |
| 13637 |
AMP = AR |
| 13638 |
ZMP = FLOAT(NZR) |
| 13639 |
AGEP = AGE |
| 13640 |
MTP = MT |
| 13641 |
CALL STOPAR(IDHEVY,NHEVY) |
| 13642 |
RETURN |
| 13643 |
END |
| 13644 |
*CMZ : 1.05/04 30/11/2005 11.04.02 by Christian Zeitnitz |
| 13645 |
*-- Author : |
| 13646 |
SUBROUTINE XSECN1(NII,KE,IN,ICOM,IREC,IUNIT,LNUMB,IND, |
| 13647 |
+ BUF,IBUF,INEL) |
| 13648 |
C THIS ROUTINE READS THE SECOND RECORD ON INPUT |
| 13649 |
C I/O UNIT (MICROS) (I.E. THE B CONTROL BLOCK) |
| 13650 |
#include "minput.inc" |
| 13651 |
#include "mmicap.inc" |
| 13652 |
#include "mconst.inc" |
| 13653 |
*KEND. |
| 13654 |
DIMENSION BUF(*),IBUF(*),ICOM(*),KE(*),IREC(*),IND(*),IN(*) |
| 13655 |
DIMENSION INEL(*),LNUMB(*),IUNIT(*) |
| 13656 |
INTEGER NII |
| 13657 |
C READ THE B CONTROL BLOCK OFF INPUT I/O UNIT |
| 13658 |
LT = LTEMP |
| 13659 |
LZ = 1 |
| 13660 |
IU = 1 |
| 13661 |
10 CONTINUE |
| 13662 |
NU = IQ(LT+NTUNIT) |
| 13663 |
NIJ = IQ(LT+NTMPNI) |
| 13664 |
LZZ=3*NIJ |
| 13665 |
READ(NU,'((8I10))')(IBUF(I),I=LZ,LZZ+LZ-1) |
| 13666 |
C INITIALIZE IND ARRAY AND IREC ARRAY TO ZERO |
| 13667 |
DO 20 I=IU,IU+NIJ-1 |
| 13668 |
IUNIT(I) = NU |
| 13669 |
20 CONTINUE |
| 13670 |
IU = IU+NIJ |
| 13671 |
LZ = LZ + LZZ |
| 13672 |
LT = LQ(LT) |
| 13673 |
IF(LT.GT.0) GOTO 10 |
| 13674 |
DO 30 I=1,NII |
| 13675 |
INEL(I)=0 |
| 13676 |
IREC(I)=0 |
| 13677 |
30 CONTINUE |
| 13678 |
DO 40 I=1,NMIX |
| 13679 |
40 IND(I)=0 |
| 13680 |
II=0 |
| 13681 |
JI=0 |
| 13682 |
50 II=II+1 |
| 13683 |
CZ IF(II.GT.NII)GO TO 90 |
| 13684 |
IF(3*II.GT.LZ)GO TO 90 |
| 13685 |
NEL=IBUF(3*II-2) |
| 13686 |
INEL(II)=NEL |
| 13687 |
DO 60 IJ=1,NMIX |
| 13688 |
C correct element AND the correct unit ? |
| 13689 |
IF(NEL.EQ.KE(IJ)) GO TO 70 |
| 13690 |
60 CONTINUE |
| 13691 |
IREC(II)=0 |
| 13692 |
GO TO 50 |
| 13693 |
70 I=IN(IJ) |
| 13694 |
C ICOM RELATES THE ISOTOPE NUMBER TO THE DICTIONARY NUMBER |
| 13695 |
IF(ICOM(I).GT.0) IREC(ICOM(I)) = 0 |
| 13696 |
ICOM(I)=II |
| 13697 |
C total length of x-section data in words |
| 13698 |
LNUMB(I) = IBUF(3*II) |
| 13699 |
IREC(II) = IBUF(3*II-1) |
| 13700 |
C SET INDICATORS |
| 13701 |
DO 80 I=IJ,NMIX |
| 13702 |
IF(NEL.NE.KE(I))GO TO 80 |
| 13703 |
IND(I)=1 |
| 13704 |
JI=JI+1 |
| 13705 |
80 CONTINUE |
| 13706 |
GO TO 50 |
| 13707 |
90 RETURN |
| 13708 |
END |
| 13709 |
*CMZ : 1.05/03 27/06/2001 18.41.30 by Christian Zeitnitz |
| 13710 |
*-- Author : |
| 13711 |
SUBROUTINE XSECN2(ICOM,IREC,IUNIT,IGAMS,LGAM,ELTOL,INABS,LNAB, |
| 13712 |
+ ITHRMS,LTHRM,IDICTS,LDICT,NTX,NTS,IGCBS,LGCB,AWR,Q,LR,QLR, |
| 13713 |
+ BUF,IBUF,LIM,LAST,INEL) |
| 13714 |
C THIS ROUTINE READS THE REMAINDER OF INPUT I/O UNIT(s), |
| 13715 |
C SELECTS THE ELEMENTS NEEDED FOR THE CALCULATIONS, |
| 13716 |
C AND STORES THE CROSS SECTION DATA IN CORE |
| 13717 |
#include "minput.inc" |
| 13718 |
#include "mconst.inc" |
| 13719 |
#include "mmicab.inc" |
| 13720 |
*KEND. |
| 13721 |
CHARACTER*4 MARK |
| 13722 |
DIMENSION BUF(*),IBUF(*),ICOM(*),IGAMS(*),LGAM(*),INABS(*), |
| 13723 |
+LNAB(*),ITHRMS(*),LTHRM(*),AWR(*),IDICTS(NNR,NNUC),ELTOL(*), |
| 13724 |
+LDICT(NNR,NNUC),Q(NQ,NNUC),NTX(*),NTS(*),IGCBS(NGR,NNUC), |
| 13725 |
+LGCB(NGR,NNUC),IREC(*),LR(NQ,NNUC),QLR(NQ,NNUC) |
| 13726 |
DIMENSION INEL(*),IUNIT(*) |
| 13727 |
C ASSIGN THE DEFAULT VALUES |
| 13728 |
LEN=0 |
| 13729 |
C INITIALIZE THE COUNTERS FOR THE LOOP |
| 13730 |
C NISR EQUALS THE NUMBER OF ISOTOPES READ |
| 13731 |
C IRECNO EQUALS THE NEXT RECORD NUMBER TO BE READ ON INPUT |
| 13732 |
C I/O UNIT (NUNIT) |
| 13733 |
C LAST EQUALS THE LAST CORE POSITION USED IN THE CALLING |
| 13734 |
CROUTINE (INPUT1) |
| 13735 |
C LST EQUALS THE LAST POSITION USED IN THE BUF ARRAY |
| 13736 |
C (I.E. (BUF(LST) = D(LAST))) |
| 13737 |
NISR=0 |
| 13738 |
IRECNO=1 |
| 13739 |
LST=0 |
| 13740 |
C PRINT OUT THE CROSS SECTION DIRECTORY IF CALLED FOR |
| 13741 |
10 CONTINUE |
| 13742 |
C START LOOP TO READ IN THE DATA ON INPUT I/O UNIT |
| 13743 |
DO 370 II=1,NI |
| 13744 |
IR = IREC(II) |
| 13745 |
IF(NUNIT.NE.IUNIT(II)) IRECNO = 1 |
| 13746 |
NUNIT= IUNIT(II) |
| 13747 |
IF(NUNIT.LE.0) THEN |
| 13748 |
WRITE(IOUT,'(/,'' XSECN2 : Wrong unit number '',I10)') NUNIT |
| 13749 |
GOTO 370 |
| 13750 |
ENDIF |
| 13751 |
IF(NISR.GE.NNUC)GO TO 370 |
| 13752 |
IF(IR.EQ.0)GO TO 370 |
| 13753 |
C LOOP TO LOCATE THE I CONTROL BLOCK RECORD (IR=IREC(II)) |
| 13754 |
CZ x-section endmark = 'ENDE' |
| 13755 |
CZ file endmark ='ENDF' |
| 13756 |
MARK = ' ' |
| 13757 |
20 IF(MARK.EQ.'ENDE') IRECNO = IRECNO + 1 |
| 13758 |
IF(MARK.EQ.'ENDF') GOTO 50 |
| 13759 |
IF(IR.EQ.IRECNO) GOTO 30 |
| 13760 |
READ(NUNIT,'(A)') MARK |
| 13761 |
GO TO 20 |
| 13762 |
C CHECK TO DETERMINE THE ISOTOPE NUMBER FOR THE RANDOM WALK |
| 13763 |
30 DO 40 I=1,NNUC |
| 13764 |
IF(ICOM(I).EQ.II)GO TO 60 |
| 13765 |
40 CONTINUE |
| 13766 |
50 WRITE(IOUT,10000)II |
| 13767 |
10000 FORMAT('0',10X,'ERROR IN ROUTINE XSECN2, II=',I6,/) |
| 13768 |
GO TO 390 |
| 13769 |
C READ I CONTROL BLOCK RECORD OFF INPUT I/O UNIT (NUNIT) FOR |
| 13770 |
C THE ELEMENT CORRESPONDING TO IREC(II) AND ICOM(I) |
| 13771 |
60 IJK=I |
| 13772 |
READ(NUNIT,'(I10,4G13.7,1I10,/,6I10)') IBUF(LST+1),(BUF(LST+ |
| 13773 |
+ IK),IK=2,5),(IBUF(LST+IJ),IJ=6,12) |
| 13774 |
NISR=NISR+1 |
| 13775 |
C ASSIGN VALUES TO ARRAYS NEEDED FOR THE RANDOM WALK |
| 13776 |
ISO=IJK |
| 13777 |
NEL=INEL(II) |
| 13778 |
AWR(ISO)=BUF(LST+2) |
| 13779 |
CZ store accuracy of xs |
| 13780 |
ELTOL(ISO) = BUF(LST+4) |
| 13781 |
IFLAGU=IBUF(LST+6) |
| 13782 |
LGAM(ISO)=IBUF(LST+7) |
| 13783 |
NTX(ISO)=IBUF(LST+8) |
| 13784 |
NTS(ISO)=IBUF(LST+9) |
| 13785 |
LTHRM(ISO)=IBUF(LST+11) |
| 13786 |
LNAB(ISO)=IBUF(LST+12) |
| 13787 |
C READ IN THE ISOTOPE DICTIONARY (IDICT ARRAY) |
| 13788 |
C FROM INPUT I/O UNIT (NUNIT) |
| 13789 |
READ(NUNIT,'((8I10))')(LDICT(J,ISO),J=1,NNR) |
| 13790 |
70 CONTINUE |
| 13791 |
C READ IN ENDF/B FILE3 CROSS SECTION DATA |
| 13792 |
C READ IN ENDF/B FILE4 ANGULAR DISTRIBUTION DATA |
| 13793 |
C READ IN ENDF/B FILE5 SECONDARY ENERGY DISTRIBUTION DATA |
| 13794 |
DO 190 I2=1,NNR |
| 13795 |
LZ=LDICT(I2,ISO) |
| 13796 |
IF(LZ.EQ.0)GO TO 190 |
| 13797 |
LEN=LIM-LAST |
| 13798 |
IF(LEN.LT.LZ)GO TO 380 |
| 13799 |
IDICTS(I2,ISO)=LAST+1-LMOX2 |
| 13800 |
CZ changed in order to read ASCII input file |
| 13801 |
C I2 < 67 -> x-section data |
| 13802 |
C I2 < 123 -> angular distribution |
| 13803 |
C I2 < 134 -> secondary energy distribution |
| 13804 |
C I2 = 134 -> |
| 13805 |
IF(I2.LT.67) THEN |
| 13806 |
READ(NUNIT,'((6G13.7))')(BUF(LST+I),I=1,LZ) |
| 13807 |
ELSE IF(I2.LT.123) THEN |
| 13808 |
C ------------------- I2 = 67 ----------------------------- |
| 13809 |
READ(NUNIT,'((8I10))') (IBUF(LST+I),I=1,2), (IBUF(LST+ |
| 13810 |
+ J+2),J=1,2*IBUF(LST+1)) |
| 13811 |
K = 2*IBUF(LST+1) + 2 + 1 |
| 13812 |
DO 80 J=1,IBUF(LST+2) |
| 13813 |
READ(NUNIT,'(G13.7,I10,/,(6G13.7))') BUF(LST+K), IBUF(LST |
| 13814 |
+ +K+1), (BUF(LST+IK+K+1),IK=1,IBUF(LST+K+1)*2) |
| 13815 |
K = K + 2 + IBUF(LST+K+1)*2 |
| 13816 |
80 CONTINUE |
| 13817 |
ELSE IF(I2.LT.134) THEN |
| 13818 |
C-------------------- I2 = 123 ---------------------------- |
| 13819 |
C first header is different, because of nk in first position |
| 13820 |
read(nunit,'(2I10,G13.7,2I10,/,(8I10))') (IBUF(LST+I), |
| 13821 |
+ I=1,2),BUF(LST+3),(IBUF(LST+J),J=4,5), (IBUF(LST+K+5), |
| 13822 |
+ K=1,2*IBUF(LST+4)) |
| 13823 |
C define buffer position to start at LF type |
| 13824 |
IP = 2 |
| 13825 |
do nk=1,IBUF(LST+1) |
| 13826 |
if(nk.gt.1) then |
| 13827 |
read(nunit,'(I10,G13.7,2I10,/,(8I10))') IBUF(LST+IP), |
| 13828 |
+ BUF(LST+IP+1),(IBUF(LST+IP+J),J=2,3), (IBUF(LST+IP+K+3) |
| 13829 |
+ ,K=1,2*IBUF(LST+IP+2)) |
| 13830 |
endif |
| 13831 |
ID = IP - 2 + 2*IBUF(LST+IP+2) + 5 |
| 13832 |
LF = IBUF(LST+IP) |
| 13833 |
NP2 = 2*IBUF(LST+IP+3) |
| 13834 |
READ(NUNIT,'((6G13.7))') (BUF(LST+ID+I),I=1,NP2) |
| 13835 |
ID = ID + NP2 |
| 13836 |
KEND = 1 |
| 13837 |
IF(LF.EQ.5.OR.LF.EQ.11) KEND = 2 |
| 13838 |
DO 100 K=1,KEND |
| 13839 |
READ(NUNIT,'((8I10))') (IBUF(LST+ID+I),I=1,2) |
| 13840 |
NR2 = 2*IBUF(LST+ID+1) |
| 13841 |
NE = IBUF(LST+ID+2) |
| 13842 |
ID = ID + 2 |
| 13843 |
READ(NUNIT,'((8I10))') (IBUF(LST+ID+I),I=1,NR2) |
| 13844 |
ID = ID + NR2 |
| 13845 |
IEND = NE |
| 13846 |
IF(LF.EQ.5.OR.LF.EQ.11) IEND = 1 |
| 13847 |
IF(LF.EQ.7.OR.LF.EQ.9) IEND = 1 |
| 13848 |
DO 90 I=1,IEND |
| 13849 |
IF(LF.EQ.1) THEN |
| 13850 |
READ(NUNIT,'(G13.7,2I10)') BUF(LST+ID+1), (IBUF(LST |
| 13851 |
+ +ID+J),J=2,3) |
| 13852 |
NR2 = 2*IBUF(LST+ID+2) |
| 13853 |
NP2 = 2*IBUF(LST+ID+3) |
| 13854 |
ID = ID + 3 |
| 13855 |
READ(NUNIT,'((8I10))') (IBUF(LST+ID+J),J=1, NR2) |
| 13856 |
ID = ID + NR2 |
| 13857 |
ELSE |
| 13858 |
NP2 = 2*NE |
| 13859 |
ENDIF |
| 13860 |
READ(NUNIT,'((6G13.7))') (BUF(LST+ID+J),J=1,NP2) |
| 13861 |
ID = ID + NP2 |
| 13862 |
90 Continue |
| 13863 |
100 CONTINUE |
| 13864 |
IP = ID + 1 |
| 13865 |
enddo |
| 13866 |
ELSE |
| 13867 |
C ------------------ I2 = 134 -------------------------------------- |
| 13868 |
READ(NUNIT,'(I10)') IBUF(LST+1) |
| 13869 |
LNU = IBUF(LST+1) |
| 13870 |
IF(LNU.NE.2) THEN |
| 13871 |
READ(NUNIT,'(I10,/,(6G13.7))') IBUF(LST+2), (BUF(LST |
| 13872 |
+ +I+2),I=1,IBUF(LST+2)) |
| 13873 |
ELSE |
| 13874 |
READ(NUNIT,'((8I10))') (IBUF(LST+I),I=2,3) |
| 13875 |
NR2 = IBUF(LST+2)*2 |
| 13876 |
READ(NUNIT,'((8I10))') (IBUF(LST+3+J),J=1,NR2) |
| 13877 |
NP2 = IBUF(LST+3)*2 |
| 13878 |
READ(NUNIT,'((6G13.7))') (BUF(LST+3+NR2+J),J=1,NP2) |
| 13879 |
ENDIF |
| 13880 |
ENDIF |
| 13881 |
CZ end of change |
| 13882 |
IF(I2.GT.66)GO TO 120 |
| 13883 |
110 CONTINUE |
| 13884 |
GO TO 180 |
| 13885 |
120 IF(I2.GT.122)GO TO 150 |
| 13886 |
130 CONTINUE |
| 13887 |
CALL ANGCDF(BUF(LST+1),IBUF(LST+1),LZ) |
| 13888 |
140 CONTINUE |
| 13889 |
GO TO 180 |
| 13890 |
150 IF(I2.GT.133)GO TO 170 |
| 13891 |
160 CONTINUE |
| 13892 |
GO TO 180 |
| 13893 |
170 CONTINUE |
| 13894 |
180 CONTINUE |
| 13895 |
LAST=LAST+LZ |
| 13896 |
LST=LST+LZ |
| 13897 |
190 CONTINUE |
| 13898 |
C READ IN THE AVERAGE PHOTON PRODUCTION ARRAY |
| 13899 |
LZ=LGAM(ISO) |
| 13900 |
IF(LZ.EQ.0)GO TO 210 |
| 13901 |
LEN=LIM-LAST |
| 13902 |
IF(LEN.LT.LZ)GO TO 380 |
| 13903 |
IGAMS(ISO)=LAST+1-LMOX2 |
| 13904 |
READ(NUNIT,'((6G13.7))')(BUF(LST+I),I=1,LZ) |
| 13905 |
200 CONTINUE |
| 13906 |
LAST=LAST+LZ |
| 13907 |
LST=LST+LZ |
| 13908 |
210 CONTINUE |
| 13909 |
C READ IN THE TOTAL NEUTRON DISAPPERANCE ARRAY |
| 13910 |
LZ=LNAB(ISO) |
| 13911 |
IF(LZ.EQ.0)GO TO 230 |
| 13912 |
LEN=LIM-LAST |
| 13913 |
IF(LEN.LT.LZ)GO TO 380 |
| 13914 |
INABS(ISO)=LAST+1-LMOX2 |
| 13915 |
READ(NUNIT,'((6G13.7))')(BUF(LST+I),I=1,LZ) |
| 13916 |
220 CONTINUE |
| 13917 |
LAST=LAST+LZ |
| 13918 |
LST=LST+LZ |
| 13919 |
230 CONTINUE |
| 13920 |
C READ IN THE Q VALUE ARRAY |
| 13921 |
READ(NUNIT,'((6G13.7))')(Q(I,ISO),I=1,NQ) |
| 13922 |
240 CONTINUE |
| 13923 |
C READ IN THE LR VALUE ARRAY |
| 13924 |
READ(NUNIT,'((8I10))')(LR(I,ISO),I=1,NQ) |
| 13925 |
250 CONTINUE |
| 13926 |
C READ IN THE QLR VALUE ARRAY |
| 13927 |
READ(NUNIT,'((6G13.7))')(QLR(I,ISO),I=1,NQ) |
| 13928 |
260 CONTINUE |
| 13929 |
C READ IN THE PHOTON DATA DICTIONARY (GCB ARRAY) |
| 13930 |
C FROM INPUT I/O UNIT (NUNIT) |
| 13931 |
C CURRENT STORAGE IS SET TO ACCOMODATE UP TO 30 INTERACTIONS |
| 13932 |
C (I.E. (2*NTX(ISO)+2*NTS(ISO)).LE.NGR) |
| 13933 |
L=2*NTX(ISO)+2*NTS(ISO) |
| 13934 |
IF(L.EQ.0)GO TO 350 |
| 13935 |
L1=2*NTX(ISO) |
| 13936 |
L2=L1+1 |
| 13937 |
READ(NUNIT,'((8I10))')(LGCB(J,ISO),J=1,L) |
| 13938 |
270 CONTINUE |
| 13939 |
C READ IN ENDF/B FILE12 PHOTON MULTIPLICATION DATA |
| 13940 |
C READ IN ENDF/B FILE13 PHOTON CROSS SECTION DATA |
| 13941 |
NNTX=NTX(ISO) |
| 13942 |
DO 300 I2=1,NNTX |
| 13943 |
LZ=LGCB(2*I2,ISO) |
| 13944 |
IF(LZ.EQ.0)GO TO 300 |
| 13945 |
LEN=LIM-LAST |
| 13946 |
IF(LEN.LT.LZ)GO TO 380 |
| 13947 |
IGCBS(2*I2-1,ISO)=LGCB(2*I2-1,ISO) |
| 13948 |
IGCBS(2*I2,ISO)=LAST+1-LMOX2 |
| 13949 |
CZ changed in order to read ASCII xsection file |
| 13950 |
READ(NUNIT,'((8I10))') (IBUF(LST+I),I=1,2) |
| 13951 |
READ(NUNIT,'((6G13.7))') (BUF(LST+J+2),J=1,IBUF(LST+2)) |
| 13952 |
ID = IBUF(LST+2) + 2 + LST |
| 13953 |
DO 280 K = 1, IBUF(LST+1) |
| 13954 |
READ(NUNIT,'(2(G13.7,I10))') BUF(ID+1),IBUF(ID+2), BUF(ID+3 |
| 13955 |
+ ),IBUF(ID+4) |
| 13956 |
ID = ID + 4 |
| 13957 |
READ(NUNIT,'((6G13.7))') (BUF(ID + J),J=1,IBUF(LST+2)) |
| 13958 |
ID = ID + IBUF(LST+2) |
| 13959 |
280 CONTINUE |
| 13960 |
CZ end of change |
| 13961 |
290 CONTINUE |
| 13962 |
LAST=LAST+LZ |
| 13963 |
LST=LST+LZ |
| 13964 |
300 CONTINUE |
| 13965 |
C READ IN ENDF/B FILE15 PHOTON SECONDARY ENERGY DISTRIBUTIONS |
| 13966 |
NNTS=NTS(ISO) |
| 13967 |
IF(NNTS.EQ.0)GO TO 350 |
| 13968 |
DO 340 I2=1,NNTS |
| 13969 |
LZ=LGCB(L1+2*I2,ISO) |
| 13970 |
IF(LZ.EQ.0)GO TO 340 |
| 13971 |
LEN=LIM-LAST |
| 13972 |
IF(LEN.LT.LZ)GO TO 380 |
| 13973 |
IGCBS(L1+2*I2-1,ISO)=LGCB(L1+2*I2-1,ISO) |
| 13974 |
IGCBS(L1+2*I2,ISO)=LAST+1-LMOX2 |
| 13975 |
CZ changed in order to read ASCII xsection file |
| 13976 |
READ(NUNIT,'(2I10,G13.7,2I10,/,(8I10))') (IBUF(LST+I),I=1, |
| 13977 |
+ 2),BUF(LST+3), (IBUF(LST+J),J=4,5), (IBUF(LST+K+5),K=1,2* |
| 13978 |
+ IBUF(LST+4)) |
| 13979 |
ID = 2*IBUF(LST+4) + 5 |
| 13980 |
LF = IBUF(LST+2) |
| 13981 |
NP2 = 2*IBUF(LST+5) |
| 13982 |
READ(NUNIT,'((6G13.7))') (BUF(LST+ID+I),I=1,NP2) |
| 13983 |
ID = ID + NP2 |
| 13984 |
KEND = 1 |
| 13985 |
IF(LF.EQ.5.OR.LF.EQ.11) KEND = 2 |
| 13986 |
DO 320 K=1,KEND |
| 13987 |
READ(NUNIT,'((8I10))') (IBUF(LST+ID+I),I=1,2) |
| 13988 |
NR2 = 2*IBUF(LST+ID+1) |
| 13989 |
NE = IBUF(LST+ID+2) |
| 13990 |
ID = ID + 2 |
| 13991 |
READ(NUNIT,'((8I10))') (IBUF(LST+ID+I),I=1,NR2) |
| 13992 |
ID = ID + NR2 |
| 13993 |
IEND = NE |
| 13994 |
IF(LF.EQ.5.OR.LF.EQ.11) IEND = 1 |
| 13995 |
IF(LF.EQ.7.OR.LF.EQ.9) IEND = 1 |
| 13996 |
DO 310 I=1,IEND |
| 13997 |
IF(LF.EQ.1) THEN |
| 13998 |
READ(NUNIT,'(G13.7,2I10)') BUF(LST+ID+1), (IBUF(L |
| 13999 |
+ ST+ID+J),J=2,3) |
| 14000 |
NR2 = 2*IBUF(LST+ID+2) |
| 14001 |
NP2 = 2*IBUF(LST+ID+3) |
| 14002 |
ID = ID + 3 |
| 14003 |
READ(NUNIT,'((8I10))') (IBUF(LST+ID+J),J=1,NR2) |
| 14004 |
ID = ID + NR2 |
| 14005 |
ELSE |
| 14006 |
NP2 = 2*NE |
| 14007 |
ENDIF |
| 14008 |
READ(NUNIT,'((6G13.7))') (BUF(LST+ID+J),J=1,NP2) |
| 14009 |
ID = ID + NP2 |
| 14010 |
310 CONTINUE |
| 14011 |
320 CONTINUE |
| 14012 |
CZ end of change |
| 14013 |
330 CONTINUE |
| 14014 |
LAST=LAST+LZ |
| 14015 |
LST=LST+LZ |
| 14016 |
340 CONTINUE |
| 14017 |
350 CONTINUE |
| 14018 |
C READ IN THE THERMAL CROSS SECTION DATA ARRAY |
| 14019 |
LZ=LTHRM(ISO) |
| 14020 |
IF(LZ.EQ.0)GO TO 360 |
| 14021 |
LEN=LIM-LAST |
| 14022 |
IF(LEN.LT.LZ)GO TO 380 |
| 14023 |
ITHRMS(ISO)=LAST+1 |
| 14024 |
READ(NUNIT,'((6G13.7))')(BUF(LST+I),I=1,LZ) |
| 14025 |
LAST=LAST+LZ |
| 14026 |
LST=LST+LZ |
| 14027 |
360 CONTINUE |
| 14028 |
370 CONTINUE |
| 14029 |
GO TO 400 |
| 14030 |
380 WRITE(IOUT,10100)LZ,LEN |
| 14031 |
10100 FORMAT('0','NOT ENOUGH SPACE TO READ IN RECORD',/,5X, |
| 14032 |
+'LENGTH OF RECORD=',I10,/,5X,'SPACE AVAILABLE=',I10) |
| 14033 |
390 PRINT '('' CALOR: ERROR in XSECN2 ====> STOP '')' |
| 14034 |
STOP |
| 14035 |
400 RETURN |
| 14036 |
END |
| 14037 |
*CMZ : 0.94/04 18/03/93 22.51.31 by Christian Zeitnitz |
| 14038 |
*-- Author : |
| 14039 |
SUBROUTINE XSECN3(KM,KE,RHO,IN,IDICTS,LDICT,ISIGTS,LSIGT,BUF, |
| 14040 |
+IBUF,TCS,LIM,LAST) |
| 14041 |
C THIS ROUTINE CREATES MACROSCOPIC TOTAL CROSS SECTIONS |
| 14042 |
C AND THEN MIXES AND THINS THESE CROSS SECTIONS ACCORDING |
| 14043 |
C TO THE MIXING TABLE |
| 14044 |
#include "minput.inc" |
| 14045 |
#include "mconst.inc" |
| 14046 |
#include "mpoint.inc" |
| 14047 |
#include "mmicab.inc" |
| 14048 |
*KEND. |
| 14049 |
DIMENSION BUF(*),IBUF(*),KM(*),KE(*),RHO(*),IN(*), |
| 14050 |
+IDICTS(NNR,NNUC),LDICT(NNR,NNUC),ISIGTS(*),LSIGT(*),TCS(*) |
| 14051 |
C ASSIGN THE INITIAL VALUES |
| 14052 |
C LST EQUALS THE LAST POSITION USED IN THE BUF ARRAY |
| 14053 |
C (I.E. (BUF(LST) = D(LAST))) |
| 14054 |
C LEN EQUALS THE CORE SPACE AVAILABLE |
| 14055 |
LST=0 |
| 14056 |
LEN=LIM-LAST |
| 14057 |
TOL = 1.0 |
| 14058 |
C READ IN TWO CROSS SECTION ARRAYS AND CREATE |
| 14059 |
C MACROSCOPIC CROSS SECTIONS |
| 14060 |
DO 160 J=1,MEDIA |
| 14061 |
JI=0 |
| 14062 |
K=0 |
| 14063 |
C READ IN THE FIRST ARRAY |
| 14064 |
DO 140 IJ=1,NMIX |
| 14065 |
IF(KM(IJ).NE.J)GO TO 140 |
| 14066 |
JI=JI+1 |
| 14067 |
K=K+1 |
| 14068 |
II=IN(IJ) |
| 14069 |
TOL = AMIN1(TCS(LFP210+II-1)/5.,TOL) |
| 14070 |
IF(JI.EQ.2)GO TO 20 |
| 14071 |
LZ=LDICT(1,II) |
| 14072 |
ISLZ=IDICTS(1,II)+LMOX2 |
| 14073 |
N=LZ |
| 14074 |
IF(LEN.LT.N)GO TO 180 |
| 14075 |
NP=LZ/2 |
| 14076 |
DO 10 M=1,NP |
| 14077 |
BUF(LST+2*M-1)=TCS(ISLZ+2*(M-1)) |
| 14078 |
BUF(LST+2*M)=TCS(ISLZ+2*M-1)*RHO(IJ) |
| 14079 |
10 CONTINUE |
| 14080 |
GO TO 140 |
| 14081 |
20 CONTINUE |
| 14082 |
C READ IN THE SECOND ARRAY |
| 14083 |
LZ2=LZ+1 |
| 14084 |
LZ1=LZ |
| 14085 |
LZ=LDICT(1,II) |
| 14086 |
ISLZ=IDICTS(1,II)+LMOX2 |
| 14087 |
N=2*(LZ+LZ1) |
| 14088 |
IF(N.GE.LEN)GO TO 180 |
| 14089 |
NP=LZ/2 |
| 14090 |
DO 30 M=1,NP |
| 14091 |
BUF(LST+LZ1+2*M-1)=TCS(ISLZ+2*(M-1)) |
| 14092 |
BUF(LST+LZ1+2*M)=TCS(ISLZ+2*M-1)*RHO(IJ) |
| 14093 |
30 CONTINUE |
| 14094 |
GO TO 40 |
| 14095 |
C MIX THE TWO ARRAYS |
| 14096 |
40 K=2 |
| 14097 |
L=2 |
| 14098 |
IF(BUF(LST+1).NE.1.E-5)GO TO 170 |
| 14099 |
IF(BUF(LST+LZ2).NE.1.E-5)GO TO 170 |
| 14100 |
NXSEC=1 |
| 14101 |
BUF(LST+LZ1+LZ+1)=1.E-5 |
| 14102 |
BUF(LST+LZ1+LZ+2)=BUF(LST+2)+BUF(LST+LZ2+1) |
| 14103 |
C DETERMINE THE NEXT ENERGY POINT |
| 14104 |
50 IF(BUF(LST+1+K).EQ.BUF(LST+LZ2+L))GO TO 90 |
| 14105 |
IF(BUF(LST+1+K).LT.BUF(LST+LZ2+L))GO TO 70 |
| 14106 |
C DETERMINE THE CROSS SECTION AT ENERGY POINT BUF(LST+LZ2+L) |
| 14107 |
CALL CTERP(BUF(LST+K-1),BUF(LST+K+1),BUF(LST+LZ2+L), |
| 14108 |
+ BUF(LST+K), BUF(LST+K+2),SIGMA) |
| 14109 |
NXSEC=NXSEC+1 |
| 14110 |
LP=LZ1+LZ+1+2*(NXSEC-1) |
| 14111 |
BUF(LST+LP)=BUF(LST+LZ2+L) |
| 14112 |
BUF(LST+LP+1)=BUF(LST+LZ2+L+1)+SIGMA |
| 14113 |
L=L+2 |
| 14114 |
IF(L.LT.LZ)GO TO 50 |
| 14115 |
C ALL THE POINTS IN THE SECOND ARRAY HAVE NOW BEEN USED |
| 14116 |
60 NXSEC=NXSEC+1 |
| 14117 |
LP=LZ1+LZ+1+2*(NXSEC-1) |
| 14118 |
BUF(LST+LP)=BUF(LST+1+K) |
| 14119 |
BUF(LST+LP+1)=BUF(LST+2+K) |
| 14120 |
K=K+2 |
| 14121 |
IF(K.LT.LZ1)GO TO 60 |
| 14122 |
GO TO 100 |
| 14123 |
C DETERMINE THE CROSS SECTION AT ENERGY POINT BUF(LST+1+K) |
| 14124 |
70 CALL CTERP(BUF(LST+LZ2+L-2),BUF(LST+LZ2+L),BUF(LST+1+K), |
| 14125 |
+ BUF(LST+LZ2+L-1),BUF(LST+LZ2+L+1),SIGMA) |
| 14126 |
NXSEC=NXSEC+1 |
| 14127 |
LP=LZ1+LZ+1+2*(NXSEC-1) |
| 14128 |
BUF(LST+LP)=BUF(LST+1+K) |
| 14129 |
BUF(LST+LP+1)=BUF(LST+K+2)+SIGMA |
| 14130 |
K=K+2 |
| 14131 |
IF(K.LT.LZ1)GO TO 50 |
| 14132 |
C ALL THE POINTS IN THE FIRST ARRAY HAVE NOW BEEN USED |
| 14133 |
80 NXSEC=NXSEC+1 |
| 14134 |
LP=LZ1+LZ+2*NXSEC-1 |
| 14135 |
BUF(LST+LP)=BUF(LST+LZ2+L) |
| 14136 |
BUF(LST+LP+1)=BUF(LST+LZ2+L+1) |
| 14137 |
L=L+2 |
| 14138 |
IF(L.LT.LZ)GO TO 80 |
| 14139 |
GO TO 100 |
| 14140 |
C THE ENERGY POINTS COINCIDE |
| 14141 |
90 NXSEC=NXSEC+1 |
| 14142 |
LP=LZ1+LZ+1+2*(NXSEC-1) |
| 14143 |
BUF(LST+LP)=BUF(LST+LZ2+L) |
| 14144 |
BUF(LST+LP+1)=BUF(LST+2+K)+BUF(LST+LZ2+L+1) |
| 14145 |
L=L+2 |
| 14146 |
K=K+2 |
| 14147 |
IF((L.LT.LZ).AND.(K.LT.LZ1))GO TO 50 |
| 14148 |
IF((L.GT.LZ).AND.(K.LT.LZ1))GO TO 60 |
| 14149 |
IF((L.LT.LZ).AND.(K.GT.LZ1))GO TO 80 |
| 14150 |
C FINISHED MIXING NOW THIN |
| 14151 |
100 L=1 |
| 14152 |
NXSEC2=1 |
| 14153 |
LP=LZ1+LZ |
| 14154 |
BUF(LST+NXSEC2)=BUF(LST+LP+L) |
| 14155 |
BUF(LST+NXSEC2+1)=BUF(LST+LP+L+1) |
| 14156 |
KI=0 |
| 14157 |
110 L=L+2 |
| 14158 |
KI=KI+1 |
| 14159 |
C CHECK TO SEE IF AT END OF CROSS SECTION ARRAY |
| 14160 |
L2=L+2 |
| 14161 |
N=2*NXSEC |
| 14162 |
IF(L2.LT.N)GO TO 120 |
| 14163 |
C FINISHED THINING |
| 14164 |
NXSEC2=NXSEC2+1 |
| 14165 |
N=2*(NXSEC2-1) |
| 14166 |
BUF(LST+1+N)=BUF(LST+LP+L) |
| 14167 |
BUF(LST+2+N)=BUF(LST+LP+L+1) |
| 14168 |
LZ=2*NXSEC2 |
| 14169 |
JI=1 |
| 14170 |
GO TO 140 |
| 14171 |
120 DO 130 I=1,KI |
| 14172 |
C ESTIMATE THE CROSS SECTION AT KI NODES |
| 14173 |
CALL CTERP(BUF(LST+LP+L-2*KI),BUF(LST+LP+L2), |
| 14174 |
+ BUF(LST+LP+L-2*I+2),BUF(LST+LP+L-2*KI+1), |
| 14175 |
+ BUF(LST+LP+L2+1),SIGMA) |
| 14176 |
ER=ABS(SIGMA-BUF(LST+LP+L-2*I+3)) |
| 14177 |
C IF ERROR IS WITHIN ALLOWABLE TOLERANCE, CHECK NEXT POINT |
| 14178 |
ERMAX=BUF(LST+LP+L-2*I+3)*TOL |
| 14179 |
IF(ER.LE.ERMAX)GO TO 130 |
| 14180 |
C NOT WITHIN ALLOWABLE TOLERANCE, MUST ADD NODE L-2 TO MESH |
| 14181 |
IF(L.GT.3.AND.KI.GT.1) L = L - 2 |
| 14182 |
NXSEC2=NXSEC2+1 |
| 14183 |
N=2*(NXSEC2-1) |
| 14184 |
BUF(LST+1+N)=BUF(LST+LP+L) |
| 14185 |
BUF(LST+2+N)=BUF(LST+LP+L+1) |
| 14186 |
KI = 0 |
| 14187 |
GO TO 110 |
| 14188 |
130 CONTINUE |
| 14189 |
C ALL KI POINTS ARE WITHIN ALLOWABLE TOLERANCE |
| 14190 |
C CHECK THE NEXT POINT |
| 14191 |
GO TO 110 |
| 14192 |
140 CONTINUE |
| 14193 |
C FINISHED WITH MEDIUM J, NOW STORE IN CORE |
| 14194 |
N=2*NXSEC2 |
| 14195 |
IF(K.EQ.1)N=LZ |
| 14196 |
LSIGT(J)=N |
| 14197 |
ISIGTS(J)=LAST+1-LMOX3 |
| 14198 |
150 CONTINUE |
| 14199 |
LAST=LAST+N |
| 14200 |
LST=LST+N |
| 14201 |
C FINISHED MIXING AND THINING |
| 14202 |
160 CONTINUE |
| 14203 |
GO TO 200 |
| 14204 |
170 WRITE(IOUT,10000)BUF(LST+1),BUF(LST+LZ2) |
| 14205 |
10000 FORMAT(' MICAP: ERROR-BEGINNING ENERGY DOES NOT START AT 1.-5', |
| 14206 |
+1P2E12.4) |
| 14207 |
GOTO 190 |
| 14208 |
180 CONTINUE |
| 14209 |
L=LEN |
| 14210 |
WRITE(IOUT,10100)L,N |
| 14211 |
10100 FORMAT(' MICAP: NOT ENOUGH ROOM TO MIX CROSS SECTIONS',/,5X, |
| 14212 |
+'SPACE AVAILABLE=',I10,/,5X,'SPACE NEEDED=',I10) |
| 14213 |
190 PRINT '('' CALOR: ERROR in XSECN3 ====> STOP'')' |
| 14214 |
STOP |
| 14215 |
200 RETURN |
| 14216 |
END |
| 14217 |
*CMZ : 1.01/04 10/06/93 14.43.49 by Christian Zeitnitz |
| 14218 |
*-- Author : |
| 14219 |
SUBROUTINE XSECN5(NTX,IGCBS,LGCB,IGCBS2,LGCB2,BUF,IBUF,D,LD, |
| 14220 |
+LIM,LAST) |
| 14221 |
C THIS ROUTINE READS THE PHOTON PARTIAL DISTRIBUTIONS FOR EACH |
| 14222 |
C REACTION LISTED IN THE GCB ARRAYS AND SUMS THEM UP TO |
| 14223 |
C CREATE A TOTAL MULTIPLICITY * CROSS SECTION ARRAY FOR |
| 14224 |
C EACH REACTION AND STORES THIS CROSS SECTION DATA IN CORE |
| 14225 |
#include "minput.inc" |
| 14226 |
#include "mconst.inc" |
| 14227 |
#include "mmicab.inc" |
| 14228 |
*KEND. |
| 14229 |
DIMENSION NTX(NNUC),IGCBS(NGR,NNUC),LGCB(NGR,NNUC), |
| 14230 |
+IGCBS2(NGR,NNUC),LGCB2(NGR,NNUC),BUF(*),IBUF(*),D(*),LD(*) |
| 14231 |
C ASSIGN THE DEFAULT VALUES |
| 14232 |
LEN=0 |
| 14233 |
C INITIALIZE THE COUNTERS FOR THE LOOP |
| 14234 |
C LAST EQUALS THE LAST CORE POSITION USED IN THE CALLING |
| 14235 |
CROUTINE (INPUT1) |
| 14236 |
C LST EQUALS THE LAST POSITION USED IN THE BUF ARRAY |
| 14237 |
C (I.E. (BUF(LST) = D(LAST))) |
| 14238 |
LST=0 |
| 14239 |
DO 70 I=1,NNUC |
| 14240 |
NNTX=NTX(I) |
| 14241 |
L=2*NNTX |
| 14242 |
IF(L.EQ.0)GO TO 70 |
| 14243 |
DO 60 I2=1,NNTX |
| 14244 |
LZ=LGCB(2*I2,I) |
| 14245 |
IF(LZ.EQ.0)GO TO 60 |
| 14246 |
LEN=LIM-LAST |
| 14247 |
IF(LEN.LT.LZ)GO TO 80 |
| 14248 |
C EQUATE THE MT NUMBERS IN THE GCB AND GCB2 DICTIONARIES |
| 14249 |
IGCBS2(2*I2-1,I)=IGCBS(2*I2-1,I) |
| 14250 |
LGCB2(2*I2-1,I)=LGCB(2*I2-1,I) |
| 14251 |
C SET THE STARTING LOCATION FOR THE PHOTON TOTAL CROSS SECTION |
| 14252 |
IGCBS2(2*I2,I)=LAST+1-LMOX4 |
| 14253 |
C OBTAIN THE STARTING LOCATION OF THE PARTIAL DISTRIBUTIONS |
| 14254 |
IST=IGCBS(2*I2,I)+LMOX2 |
| 14255 |
NK=LD(IST) |
| 14256 |
NP=LD(IST+1) |
| 14257 |
NP2=2*NP |
| 14258 |
LGCB2(2*I2,I)=NP2 |
| 14259 |
C ZERO OUT THE CORE AREA TO STORE THE TOTAL PHOTON |
| 14260 |
C MULTIPLICITY * CROSS SECTION ARRAYS |
| 14261 |
DO 10 IP=1,NP2 |
| 14262 |
BUF(LST+IP)=0.0 |
| 14263 |
10 CONTINUE |
| 14264 |
C SET UP THE ENERGY BOUNDARIES FOR THE (E,XS) TABLE |
| 14265 |
DO 20 J=1,NP |
| 14266 |
BUF(LST+2*J-1)=D(IST+J+2-1) |
| 14267 |
20 CONTINUE |
| 14268 |
II=NP+2 |
| 14269 |
AWRI=D(IST+II+3-1) |
| 14270 |
C SUM THE PARTIAL DISTRIBUTIONS TO OBTAIN THE TOTAL |
| 14271 |
C MULTIPLICITY * CROSS SECTION ARRAY AND STORE IN THE |
| 14272 |
C ENERGY,CROSS SECTION TABLE |
| 14273 |
DO 40 J=1,NK |
| 14274 |
II=II+4 |
| 14275 |
DO 30 K=1,NP |
| 14276 |
BUF(LST+2*K)=BUF(LST+2*K)+D(IST+II+K-1) |
| 14277 |
30 CONTINUE |
| 14278 |
II=II+NP |
| 14279 |
40 CONTINUE |
| 14280 |
50 CONTINUE |
| 14281 |
C UPDATE CORE LOCATION POINTERS |
| 14282 |
LAST=LAST+NP2 |
| 14283 |
LST=LST+NP2 |
| 14284 |
60 CONTINUE |
| 14285 |
70 CONTINUE |
| 14286 |
RETURN |
| 14287 |
80 WRITE(IOUT,10000)LZ,LEN |
| 14288 |
10000 FORMAT(' MICAP: NOT ENOUGH SPACE TO READ IN RECORD',/,5X, |
| 14289 |
+'LENGTH OF RECORD=',I10,/,5X,'SPACE AVAILABLE=',I10) |
| 14290 |
PRINT '('' CALOR: ERROR in XSECN5 ====> STOP '')' |
| 14291 |
STOP |
| 14292 |
END |
| 14293 |
*CMZ : 1.01/04 10/06/93 14.43.49 by Christian Zeitnitz |
| 14294 |
*-- Author : |
| 14295 |
SUBROUTINE XSECNU(BUF,LEN,E,XSC,L1,L2) |
| 14296 |
C THIS ROUTINE DETERMINES A CROSS SECTION AT A GIVEN ENERGY |
| 14297 |
C FROM A CROSS SECTION VERSUS ENERGY TABLE |
| 14298 |
DIMENSION BUF(*) |
| 14299 |
SAVE |
| 14300 |
IF(E.LT.BUF(L1))GO TO 40 |
| 14301 |
DO 10 J=1,LEN |
| 14302 |
N=L1+2*(J-1) |
| 14303 |
IF(E.LE.BUF(N))GO TO 20 |
| 14304 |
10 CONTINUE |
| 14305 |
XSC=BUF(L2) |
| 14306 |
RETURN |
| 14307 |
20 IF(J.EQ.1)GO TO 30 |
| 14308 |
XSC=BUF(N-1)+(E-BUF(N-2))*(BUF(N+1)-BUF(N-1))/ |
| 14309 |
+(BUF(N)-BUF(N-2)) |
| 14310 |
RETURN |
| 14311 |
30 XSC=BUF(N+1) |
| 14312 |
RETURN |
| 14313 |
40 XSC=0.0 |
| 14314 |
RETURN |
| 14315 |
END |
| 14316 |
*CMZ : 1.03/00 27/05/94 16.22.23 by Christian Zeitnitz |
| 14317 |
*-- Author : Christian Zeitnitz 27/05/94 |
| 14318 |
SUBROUTINE MICSET(MATNO,NKEY) |
| 14319 |
C*********************************************************************** |
| 14320 |
C set a option in MICAP |
| 14321 |
C |
| 14322 |
C INPUT: MATNO - GEANT material number |
| 14323 |
C NKEY - 0 -> use single isotopes instead of the |
| 14324 |
C natural composition in material MATNO |
| 14325 |
C 1 -> use natural composition |
| 14326 |
C |
| 14327 |
C************************************************************************ |
| 14328 |
C |
| 14329 |
#include "mmicap.inc" |
| 14330 |
*KEND. |
| 14331 |
C |
| 14332 |
LOGICAL FIRST |
| 14333 |
DATA FIRST/.TRUE./ |
| 14334 |
C |
| 14335 |
IF(FIRST) THEN |
| 14336 |
FIRST = .FALSE. |
| 14337 |
NWW = 100 |
| 14338 |
CALL CHKZEB(NWW,IXCONS) |
| 14339 |
CALL MZLINK(IXCONS,'MICPAR',LMIST,LMIST,LMIST) |
| 14340 |
CALL MZBOOK(IXCONS,LMIST,0,2,'MIST',0,0,NWW,0,0) |
| 14341 |
ENDIF |
| 14342 |
10 CONTINUE |
| 14343 |
DO 20 I=1,IQ(LMIST-1),2 |
| 14344 |
IF(IQ(LMIST+I).EQ.MATNO) THEN |
| 14345 |
IQ(LMIST+I+1) = NKEY |
| 14346 |
GOTO 999 |
| 14347 |
ENDIF |
| 14348 |
IF(IQ(LMIST+I).EQ.0) THEN |
| 14349 |
IQ(LMIST+I) = MATNO |
| 14350 |
IQ(LMIST+I+1) = NKEY |
| 14351 |
GOTO 999 |
| 14352 |
ENDIF |
| 14353 |
20 CONTINUE |
| 14354 |
C |
| 14355 |
C Bank got to small, increase the size |
| 14356 |
NWW = 100 + IQ(LMIST-1) |
| 14357 |
CALL CHKZEB(NWW,IXCONS) |
| 14358 |
CALL MZPUSH(IXCONS,LMIST,0,100,'I') |
| 14359 |
GOTO 10 |
| 14360 |
999 RETURN |
| 14361 |
END |
| 14362 |
*CMZ : 1.04/01 09/02/95 17.09.56 by Christian Zeitnitz |
| 14363 |
*-- Author : Christian Zeitnitz 9/02/95 |
| 14364 |
SUBROUTINE MICFIL(CNAME) |
| 14365 |
C*********************************************************************** |
| 14366 |
C set a option in MICAP |
| 14367 |
C |
| 14368 |
C INPUT: |
| 14369 |
C CNAME - in case NKEY=10 the file name |
| 14370 |
C |
| 14371 |
C************************************************************************ |
| 14372 |
C |
| 14373 |
#include "mmicap.inc" |
| 14374 |
*KEND. |
| 14375 |
C |
| 14376 |
CHARACTER*(*) CNAME |
| 14377 |
C |
| 14378 |
LOGICAL FIRST |
| 14379 |
DATA FIRST/.TRUE./ |
| 14380 |
C |
| 14381 |
IF(FIRST) THEN |
| 14382 |
FIRST = .FALSE. |
| 14383 |
NFIL = 101 |
| 14384 |
CALL CHKZEB(NFIL,IXCONS) |
| 14385 |
CALL MZLINK(IXCONS,'MICFIL',LMIFIL,LMIFIL,LMIFIL) |
| 14386 |
CALL MZBOOK(IXCONS,LMIFIL,0,2,'MIFL',0,0,NFIL,0,0) |
| 14387 |
ELSE |
| 14388 |
C increase the bank for the x-section file name |
| 14389 |
NFIL = 101 + IQ(LMIFIL-1) |
| 14390 |
CALL CHKZEB(NFIL,IXCONS) |
| 14391 |
CALL MZPUSH(IXCONS,LMIFIL,0,101,'I') |
| 14392 |
ENDIF |
| 14393 |
C store x-section file name in bank 'MIFL' |
| 14394 |
C find the last free index in the bank |
| 14395 |
IF(LNBLNK(CNAME).GT.0) THEN |
| 14396 |
I = LMIFIL+IQ(LMIFIL-1)-100+1 |
| 14397 |
CALL UCTOH(CNAME,IQ(I),4,LNBLNK(CNAME)) |
| 14398 |
IQ(I-1) = LNBLNK(CNAME) |
| 14399 |
ELSE |
| 14400 |
PRINT*,' MICSET : invalid file name ' |
| 14401 |
ENDIF |
| 14402 |
30 RETURN |
| 14403 |
END |
| 14404 |
*CMZ : 1.01/10 30/06/93 13.51.55 by Christian Zeitnitz |
| 14405 |
*-- Author : |
| 14406 |
SUBROUTINE CSKALE(IBERT,F,NOFAS,ITSLO,EFAS,ALPFAS,BETFAS,GAMFAS, |
| 14407 |
+ EHICUT,RMFAS,EXFAS,REFAS) |
| 14408 |
C |
| 14409 |
CZ modified SKALE -- generate WT particles |
| 14410 |
C |
| 14411 |
DIMENSION F(*) , ITSLO(*) , EFAS(*) , ALPFAS(*) , BETFAS(*) , |
| 14412 |
+ GAMFAS(*), WTFAS(200), ESLO(200), ALPSLO(200), |
| 14413 |
+ BETSLO(200), GAMSLO(200), NPI(200) |
| 14414 |
C |
| 14415 |
LOGICAL FTROBL |
| 14416 |
C |
| 14417 |
DATA IELAS/1/ |
| 14418 |
SAVE |
| 14419 |
C |
| 14420 |
NKEY=2 |
| 14421 |
NCT=1 |
| 14422 |
10 ESTOR=F(3) |
| 14423 |
F(3)=EHICUT |
| 14424 |
C |
| 14425 |
CALL CABERT(IBERT,F,NOSLO,ITSLO,ESLO,ALPSLO,BETSLO,GAMSLO) |
| 14426 |
IBERT=1 |
| 14427 |
F(3)=ESTOR |
| 14428 |
C |
| 14429 |
IF(NOSLO.GT.0) GO TO 70 |
| 14430 |
NOFAS=NOSLO |
| 14431 |
20 CONTINUE |
| 14432 |
C |
| 14433 |
C scaling within geant |
| 14434 |
C generate N particles with RND*WT*Ei energy |
| 14435 |
C check for depletion of nucleus |
| 14436 |
C |
| 14437 |
IF(NOFAS.LE.0) RETURN |
| 14438 |
C first determine recoil nucleus parameters |
| 14439 |
FTROBL = .FALSE. |
| 14440 |
30 CONTINUE |
| 14441 |
AR=F(1) |
| 14442 |
ZR=F(2) |
| 14443 |
PI0NO = 0.0 |
| 14444 |
PIPNO = 0.0 |
| 14445 |
PIMNO = 0.0 |
| 14446 |
PRONO = 0.0 |
| 14447 |
XNEUT = 0.0 |
| 14448 |
DO 40 I=1,NOFAS |
| 14449 |
IF(ITSLO(I).LE.0) PRONO = PRONO + 1.0 |
| 14450 |
IF(ITSLO(I).LE.1) XNEUT = XNEUT + 1.0 |
| 14451 |
IF(ITSLO(I).EQ.2) THEN |
| 14452 |
CALL GRNDM(R,1) |
| 14453 |
NPI(I) = INT(WTFAS(I)) |
| 14454 |
XN = WTFAS(I) - FLOAT(NPI(I)) - R |
| 14455 |
IF(XN.GT.0.0) NPI(I) = NPI(I) + 1 |
| 14456 |
IF(NPI(I).LE.0.OR.FTROBL) NPI(I) = 1 |
| 14457 |
PIPNO = PIPNO + FLOAT(NPI(I)) |
| 14458 |
ELSE IF(ITSLO(I).EQ.4) THEN |
| 14459 |
CALL GRNDM(R,1) |
| 14460 |
NPI(I) = INT(WTFAS(I)) |
| 14461 |
XN = WTFAS(I) - FLOAT(NPI(I)) - R |
| 14462 |
IF(XN.GT.0.0) NPI(I) = NPI(I) + 1 |
| 14463 |
IF(NPI(I).LE.0.OR.FTROBL) NPI(I) = 1 |
| 14464 |
PIMNO = PIMNO + FLOAT(NPI(I)) |
| 14465 |
ELSE IF(ITSLO(I).EQ.3) THEN |
| 14466 |
CALL GRNDM(R,1) |
| 14467 |
NPI(I) = INT(WTFAS(I)) |
| 14468 |
XN = WTFAS(I) - FLOAT(NPI(I)) - R |
| 14469 |
IF(XN.GT.0.0) NPI(I) = NPI(I) + 1 |
| 14470 |
IF(NPI(I).LE.0.OR.FTROBL) NPI(I) = 1 |
| 14471 |
ENDIF |
| 14472 |
40 CONTINUE |
| 14473 |
AADD = 1. |
| 14474 |
IF(F(7).GT.1) AADD = 0.0 |
| 14475 |
ZADD = 1. - F(7) |
| 14476 |
IF(F(7).GT.1) ZADD = 3.-F(7) |
| 14477 |
AR = AR + AADD - PRONO - XNEUT |
| 14478 |
ZR = ZR + ZADD - PRONO - PIPNO + PIMNO |
| 14479 |
IF((ZR.LT.0.OR.AR.LT.ZR).AND..NOT.FTROBL) THEN |
| 14480 |
FTROBL = .TRUE. |
| 14481 |
GOTO 30 |
| 14482 |
ENDIF |
| 14483 |
C start generating more particles |
| 14484 |
K = NOFAS + 1 |
| 14485 |
C loop over particles |
| 14486 |
DO 60 I=1,NOFAS |
| 14487 |
C don't scale nucleons |
| 14488 |
IF(ITSLO(I).LE.1) THEN |
| 14489 |
EFAS(I) = EFAS(I)*WTFAS(I) |
| 14490 |
ELSE |
| 14491 |
DO 50 J=1,NPI(I) |
| 14492 |
IF(J.EQ.NPI(I)) THEN |
| 14493 |
IF(WTFAS(I).GT.0.0) EFAS(I) = EFAS(I)*WTFAS(I) |
| 14494 |
ELSE |
| 14495 |
WTFAS(I) = WTFAS(I) - 1. |
| 14496 |
EFAS(K) = EFAS(I) |
| 14497 |
ITSLO(K) = ITSLO(I) |
| 14498 |
ALPFAS(K) = ALPFAS(I) |
| 14499 |
BETFAS(K) = BETFAS(I) |
| 14500 |
GAMFAS(K) = GAMFAS(I) |
| 14501 |
K = K + 1 |
| 14502 |
ENDIF |
| 14503 |
50 CONTINUE |
| 14504 |
ENDIF |
| 14505 |
60 CONTINUE |
| 14506 |
NOFAS=K-1 |
| 14507 |
RETURN |
| 14508 |
70 IF(IELAS.EQ.0) GO TO 80 |
| 14509 |
CALL ESKALE(IE,EHICUT,F,NOFAS,ITSLO,EFAS,ALPFAS,BETFAS,GAMFAS, |
| 14510 |
+ WTFAS,RMFAS,EXFAS,REFAS,NOSLO,ESLO,ALPSLO,BETSLO,GAMSLO) |
| 14511 |
GO TO (80,10,20),IE |
| 14512 |
80 ATAR=F(1) |
| 14513 |
EINC=F(3) |
| 14514 |
ITINC=F(7) |
| 14515 |
CALL MCMOSC(NKEY,ATAR,ITINC,EINC,EHICUT,NOSLO,ITSLO,ESLO,ALPSLO, |
| 14516 |
+ BETSLO,GAMSLO,EFAS,WTFAS,ALPFAS,BETFAS,GAMFAS,RMFAS,NOFAS,EXFAS, |
| 14517 |
+ REFAS,WHY) |
| 14518 |
IF(NOFAS.EQ.0) GO TO 10 |
| 14519 |
GOTO 20 |
| 14520 |
END |
| 14521 |
*CMZ : 1.01/09 29/06/93 12.26.35 by Christian Zeitnitz |
| 14522 |
*-- Author : |
| 14523 |
SUBROUTINE ESKALE(IE,EHICUT,FIN,NOFAS,ITSLO,EFAS,ALPFAS,BETFAS, |
| 14524 |
+ GAMFAS,WTFAS,RMFAS,EXFAS,REFAS,NOSLO,ESLO,ALPSLO,BETSLO,GAMSLO) |
| 14525 |
C |
| 14526 |
C changed 10 Nov. 1992 C.Zeitnitz |
| 14527 |
C |
| 14528 |
DIMENSION FIN(*) , ITSLO(*) , EFAS(*) , ALPFAS(*) , |
| 14529 |
+ BETFAS(*) , GAMFAS(*) , WTFAS(*) , ESLO(*) , |
| 14530 |
+ ALPSLO(*) , BETSLO(*) , GAMSLO(*) , ITSLO2(200), |
| 14531 |
+ EFAS2(200), WTFAS2(200), ALPFA2(200), BETFA2(200), |
| 14532 |
+ GAMFA2(200) |
| 14533 |
C |
| 14534 |
#include "cinout.inc" |
| 14535 |
#include "cbert.inc" |
| 14536 |
*KEND. |
| 14537 |
C |
| 14538 |
REAL*8 F,PRTIN2,FEINC |
| 14539 |
REAL*4 W |
| 14540 |
C |
| 14541 |
DATA F /0.95D0/ |
| 14542 |
DATA W /0.2/ |
| 14543 |
SAVE |
| 14544 |
C |
| 14545 |
IND = 1 |
| 14546 |
EINC = DBLE(FIN(3)) |
| 14547 |
EPART= FIN(3) |
| 14548 |
FIN(3) = EHICUT |
| 14549 |
FEINC = DBLE(EHICUT) * F |
| 14550 |
PRTIN2 = DBLE(FIN(7)) + 1.D0 |
| 14551 |
C** |
| 14552 |
C** NEP = NO. OF ESCAPING PARTICLES |
| 14553 |
C** |
| 14554 |
10 NEP = IDINT(ESPS(1) + 1.0D-2) |
| 14555 |
C |
| 14556 |
C** CHECK FOR PIONS |
| 14557 |
C |
| 14558 |
J = 2 |
| 14559 |
DO 20 I = 1,NEP |
| 14560 |
IF(ESPS(J).GE.3.D0) GO TO 50 |
| 14561 |
J = J + 8 |
| 14562 |
20 CONTINUE |
| 14563 |
ITEST1 = ITEST1 + 1 |
| 14564 |
J = 2 |
| 14565 |
DO 40 I=1,NEP |
| 14566 |
C |
| 14567 |
C** CHECK FOR ESCAPING PARTICLE SAME AS INCIDENT PARTICLE |
| 14568 |
C |
| 14569 |
IF(ESPS(J).NE.PRTIN2) GO TO 30 |
| 14570 |
C |
| 14571 |
C** CHECK FOR ENERGY OF ESCAPING PARTICLE GREATER THAN F * ENERGY |
| 14572 |
C** OF INCIDENT PARTICLE |
| 14573 |
C |
| 14574 |
IF(ESPS(J+1).GT.FEINC) GO TO 60 |
| 14575 |
30 J = J + 8 |
| 14576 |
40 CONTINUE |
| 14577 |
C |
| 14578 |
C** A 'NON-ELASTIC' COLLISION HAS OCCURRED |
| 14579 |
C |
| 14580 |
50 GO TO (160 ,120),IND |
| 14581 |
C |
| 14582 |
C** AN 'ELASTIC' COLLISION HAS OCCURRED |
| 14583 |
C |
| 14584 |
60 CONTINUE |
| 14585 |
70 GO TO (80,110),IND |
| 14586 |
80 ATAR = FIN(1) |
| 14587 |
NKEY = 2 |
| 14588 |
NELAST = NELAST + 1 |
| 14589 |
ITINC = FIN(7) |
| 14590 |
CALL MCMOSC(NKEY,ATAR,ITINC,EPART,EHICUT,NOSLO,ITSLO,ESLO, |
| 14591 |
+ ALPSLO,BETSLO,GAMSLO,EFAS,WTFAS,ALPFAS,BETFAS,GAMFAS,RMFAS, |
| 14592 |
+ NOFAS,EXFAS,REFAS,WHY) |
| 14593 |
NOFAS1 = NOFAS |
| 14594 |
IF(NOFAS1.GT.0) GO TO 90 |
| 14595 |
IE = 2 |
| 14596 |
GO TO 170 |
| 14597 |
C |
| 14598 |
C** MULTIPLY ALL PARTICLE WEIGHTS FOR THIS COLLISION BY W |
| 14599 |
C |
| 14600 |
90 DO 100 I=1,NOFAS1 |
| 14601 |
WTFAS(I) = WTFAS(I) * W |
| 14602 |
100 CONTINUE |
| 14603 |
110 IBERT = 1 |
| 14604 |
CALL CABERT(IBERT,FIN,NOSLO,ITSLO2,ESLO,ALPSLO,BETSLO,GAMSLO) |
| 14605 |
IF(NOSLO.LE.0) GO TO 110 |
| 14606 |
IND = 2 |
| 14607 |
GO TO 10 |
| 14608 |
120 CALL MCMOSC(NKEY,ATAR,ITINC,EPART,EHICUT,NOSLO,ITSLO2,ESLO, |
| 14609 |
+ ALPSLO,BETSLO,GAMSLO,EFAS2,WTFAS2,ALPFA2,BETFA2,GAMFA2,RMFAS2, |
| 14610 |
+ NOFAS2,EXFAS2,REFAS2,WHY) |
| 14611 |
IF(NOFAS2.LE.0) GO TO 110 |
| 14612 |
C |
| 14613 |
C** MULTIPLY ALL PARTICLE WEIGHTS BY 1.-W |
| 14614 |
W2 = 1.0 - W |
| 14615 |
DO 130 I=1,NOFAS2 |
| 14616 |
WTFAS2(I) = WTFAS2(I) * W2 |
| 14617 |
130 CONTINUE |
| 14618 |
C |
| 14619 |
C** COMBINE TWO COLLISIONS |
| 14620 |
C |
| 14621 |
IF(NOFAS1 + NOFAS2.LE.60) GO TO 140 |
| 14622 |
WRITE(IO,10000) NOFAS1,NOFAS2 |
| 14623 |
10000 FORMAT(' HETC: Too many particles in ESKALE -- NOFAS1 = ',I2, |
| 14624 |
+ ' NOFAS2 = ',I2) |
| 14625 |
IF(NOFAS1.EQ.60) NOFAS1 = 59 |
| 14626 |
NOFAS2 = 60 - NOFAS1 |
| 14627 |
140 NOFAS = NOFAS1 + NOFAS2 |
| 14628 |
DO 150 I = 1,NOFAS2 |
| 14629 |
J = NOFAS1 + I |
| 14630 |
ITSLO(J) = ITSLO2(I) |
| 14631 |
EFAS(J) = EFAS2(I) |
| 14632 |
WTFAS(J) = WTFAS2(I) |
| 14633 |
ALPFAS(J) = ALPFA2(I) |
| 14634 |
BETFAS(J) = BETFA2(I) |
| 14635 |
GAMFAS(J) = GAMFA2(I) |
| 14636 |
150 CONTINUE |
| 14637 |
EXFAS = EXFAS * W + EXFAS2 * (1.-W) |
| 14638 |
RMFAS = RMFAS * W + RMFAS2 * (1.-W) |
| 14639 |
REFAS = REFAS * W + REFAS2 * (1.-W) |
| 14640 |
IE = 3 |
| 14641 |
GO TO 170 |
| 14642 |
160 IE = 1 |
| 14643 |
170 FIN(3) = SNGL(EINC) |
| 14644 |
RETURN |
| 14645 |
END |
| 14646 |
*CMZ : 1.01/09 29/06/93 12.23.58 by Christian Zeitnitz |
| 14647 |
*-- Author : |
| 14648 |
SUBROUTINE MCMOSC(NKEY,ATAR,ITINC,EOPRS,EINCS,NOSLO,ITSLO,ESLO, |
| 14649 |
+ ALPSLO,BETSLO,GAMSLO,EFAS,WTFAS,ALPFAS,BETFAS,GAMFAS,RMFAS,NOFAS, |
| 14650 |
+ EXFAS,REFAS,WHY) |
| 14651 |
C |
| 14652 |
C CALCULATION OF MOMENTUM SPECTRA |
| 14653 |
C FOR SCALED-UP INCIDENT PARTICLE ENERGIES |
| 14654 |
C |
| 14655 |
REAL*8 AMASNO, EINC, ARRAY, BRRAY, BARB, EINCT, NUMBEA, TARMAT |
| 14656 |
REAL*8 EOPR,TARMAS,FUG,AMORNT,AMRNST,ESTART, ERNPRT,ERNT,AMASIN, |
| 14657 |
+EMASS,PMAX,AMOINC,CHEINC,RESMAS,ETOT,ETOTPR, AMOIPR,BETA,BETAPR, |
| 14658 |
+GAMMA,GAMPR,ECM,RECAL1,RECAL2,RECAL3,ECMPR, CUTL,CUTCM,ECMOKE, |
| 14659 |
+PCMO,YIELD,AVERE,BTOT,BTOTPR,ZKZ,BPRLAB,ECMKE, PLICIT,EXCIT,PX, |
| 14660 |
+PY,PZ,PXS,PYS,PZS,P,CHECK,WEIGHT,PCM,EPRCM, PTEMP,WCM,W,PPR, |
| 14661 |
+PSTOR1,PSTOR2,B,ESUM,BLANK,BLANK1,AMORN, ERN,ERNPR,AESUM,ESTAR, |
| 14662 |
+ESTARP,TOTAL,ANSWER,A1,A2,A3,A4,A5,A11,B11 ,C11,ANSPLU,ANSMIN,A6, |
| 14663 |
+A7,D1,STO,STOO,A8,ESUMPR,BTOLAB,ARRMON |
| 14664 |
C |
| 14665 |
#include "camass.inc" |
| 14666 |
*KEND. |
| 14667 |
DIMENSION PART(5),EMASS(5),CTOFM(5),ARRAY(500) |
| 14668 |
DIMENSION BRRAY(500),WEIGHT(65),CUTL(5),CUTCM(5),RESMAS(5), |
| 14669 |
+ AVERE(10),YIELD(10),ECMKE(5),PLICIT(5),EPRCM(65),FUG(5) |
| 14670 |
C |
| 14671 |
DIMENSION ITSLO(*),ESLO(*),ALPSLO(*),BETSLO(*),GAMSLO(*), |
| 14672 |
+ EFAS(*),WTFAS(*),ALPFAS(*),BETFAS(*),GAMFAS(*) |
| 14673 |
C |
| 14674 |
DIMENSION EINCT(10), NUMBEA(10) |
| 14675 |
LOGICAL INIT |
| 14676 |
C |
| 14677 |
EQUIVALENCE(CUTCM(1),RESMAS(1),CUTL(1),EMASS(1)) |
| 14678 |
C |
| 14679 |
DATA INIT/.TRUE./ |
| 14680 |
SAVE |
| 14681 |
C |
| 14682 |
10 IF(INIT) THEN |
| 14683 |
20 COUNT = 0. |
| 14684 |
TARMAT=0. |
| 14685 |
COUNT1 = 0. |
| 14686 |
COUNT2=0. |
| 14687 |
COUNT3=0. |
| 14688 |
COUNT4 = 0. |
| 14689 |
COUNT5 = 0. |
| 14690 |
NTTME=0 |
| 14691 |
AMORNT = 0.0 |
| 14692 |
AMRNST = 0.0 |
| 14693 |
ESTART=0. |
| 14694 |
ZKZ=0. |
| 14695 |
NMLTEO = 0 |
| 14696 |
ERNPRT = 0.0 |
| 14697 |
ERNT = 0.0 |
| 14698 |
CHECK7=0. |
| 14699 |
CHECK8=0. |
| 14700 |
DO 30 III=1,500 |
| 14701 |
BRRAY(III)=0. |
| 14702 |
ARRAY(III)=0. |
| 14703 |
30 CONTINUE |
| 14704 |
DO 40 IHK = 1,10 |
| 14705 |
EINCT(IHK)=0. |
| 14706 |
NUMBEA(IHK)=0. |
| 14707 |
YIELD(IHK) = 0.0 |
| 14708 |
C WILL CONTAIN AVERAGE MULTIPLICITIES WHEN DIVIDED BY # OF COLLISION |
| 14709 |
AVERE(IHK) = 0.0 |
| 14710 |
40 CONTINUE |
| 14711 |
C WILL CONTAIN AVERAGE ENERGY WHEN DIVIDED BY # OF COLLISIONS |
| 14712 |
BTOT = 0.0 |
| 14713 |
BTOTPR=0.0 |
| 14714 |
C SETTING MASSES FOR THE 5 POSSIBLE EMERGENT PARTICLES |
| 14715 |
RESMAS(1) = XMASS(0)*1000. |
| 14716 |
RESMAS(2) = XMASS(1)*1000. |
| 14717 |
RESMAS(3)= XMASS(2)*1000. |
| 14718 |
RESMAS(4)= XMASS(2)*1000. |
| 14719 |
RESMAS(5) = XMASS(3)*1000. |
| 14720 |
FUG(3)=1.0D0 |
| 14721 |
FUG(4)=1.0D0 |
| 14722 |
FUG(5)=1.0D0 |
| 14723 |
INIT = .FALSE. |
| 14724 |
ENDIF |
| 14725 |
GO TO (50 ,70 ,50 ,440),NKEY |
| 14726 |
50 RETURN |
| 14727 |
C DEFINES INCIDENT PARTICLE |
| 14728 |
60 EINCT(IPIN)=EINCT(IPIN)-EINC |
| 14729 |
EINCT(IPIN+5)=EINCT(IPIN+5)-EOPR |
| 14730 |
NUMBEA(IPIN)=NUMBEA(IPIN)-1.D0 |
| 14731 |
NUMBEA(IPIN+5)=NUMBEA(IPIN+5)-1.D0 |
| 14732 |
TARMAT = TARMAT-TARMAS |
| 14733 |
RETURN |
| 14734 |
70 PIN = ITINC +1 |
| 14735 |
ZKZ=ZKZ+1.D0 |
| 14736 |
IPIN= PIN |
| 14737 |
NOFAS=0 |
| 14738 |
WHY=0. |
| 14739 |
INTYPE=ITINC+1 |
| 14740 |
GOTO(80 ,90 ,100 ,100 ,100 ),INTYPE |
| 14741 |
80 FUG(1)=1.00D0 |
| 14742 |
FUG(2)=1.00D0 |
| 14743 |
GOTO 110 |
| 14744 |
90 FUG(1)=1.00D0 |
| 14745 |
FUG(2)=1.00D0 |
| 14746 |
GOTO 110 |
| 14747 |
100 FUG(1)=1.0 |
| 14748 |
FUG(2)=1.0 |
| 14749 |
110 CONTINUE |
| 14750 |
AMASNO= ATAR |
| 14751 |
TARMAS= 931.49432D0*AMASNO |
| 14752 |
TARMAT=TARMAT+TARMAS |
| 14753 |
AMASIN=RESMAS(IPIN) |
| 14754 |
EOPR=EOPRS |
| 14755 |
EINC=EINCS |
| 14756 |
CHEINC = 1.D0 |
| 14757 |
IF(IPIN.GT.2) CHEINC = 0.0 |
| 14758 |
EINCT(IPIN)=EINCT(IPIN)+EINC |
| 14759 |
NUMBEA(IPIN)=NUMBEA(IPIN)+1.D0 |
| 14760 |
EINCT(IPIN+5)=EINCT(IPIN+5)+EOPR |
| 14761 |
NUMBEA(IPIN+5)=NUMBEA(IPIN+5)+1.D0 |
| 14762 |
DO 120 I = 1,5 |
| 14763 |
ECMKE(I) = 0.0 |
| 14764 |
C TEMPORARY STORAGE FOR UNSCALED K.E. IN C.M. USED IN WEIGHT CALCULA |
| 14765 |
PLICIT(I) = 0.0 |
| 14766 |
120 CONTINUE |
| 14767 |
C TEMPORARY STORAGE FOR UNSCALED MULTIPLICITIES USED IN WEIGHT CALCU |
| 14768 |
NWDS = NOSLO*8+1 |
| 14769 |
DO 130 III=2,NWDS,8 |
| 14770 |
M8=(III+6)/8 |
| 14771 |
ARRAY(III)=ITSLO(M8)+1 |
| 14772 |
ARRAY(III+1)=ESLO(M8) |
| 14773 |
ARRAY(III+2)=ALPSLO(M8) |
| 14774 |
ARRAY(III+3)=BETSLO(M8) |
| 14775 |
ARRAY(III+4)=GAMSLO(M8) |
| 14776 |
130 CONTINUE |
| 14777 |
C TOTAL ENERGY OF INCIDENT PARTICLE LAB |
| 14778 |
ETOT=EINC+AMASIN |
| 14779 |
C TOTAL ENERGY OF SCALED INCIDENT PARTICLE LAB |
| 14780 |
ETOTPR=EOPR+AMASIN |
| 14781 |
C MOMENTUM OF INCIDENT PARTICLE LAB |
| 14782 |
AMOINC =DSQRT (EINC*(EINC + 2.0D0*AMASIN)) |
| 14783 |
C MOMENTUM OF SCALED INCIDENT PARTICLE LAB |
| 14784 |
AMOIPR=DSQRT(ETOTPR*ETOTPR-AMASIN*AMASIN) |
| 14785 |
C BETA FOR INCIDENT PARTICLE AND TARGET |
| 14786 |
BETA=AMOINC/(ETOT+TARMAS) |
| 14787 |
C BETA FOR SCALED INCIDENT PARTICLE AND TARGET |
| 14788 |
BETAPR=AMOIPR/(ETOTPR+TARMAS) |
| 14789 |
C GAMMA FOR INCIDENT PARTICLE |
| 14790 |
GAMMA=1.D0/DSQRT(1.D0-BETA*BETA) |
| 14791 |
C GAMMA FOR SCALED INCIDENT PARTICLE |
| 14792 |
GAMPR=1.D0/DSQRT(1.D0-BETAPR*BETAPR) |
| 14793 |
C TOTAL ENERGY OF INCIDENT PARTICLE IN C.M. |
| 14794 |
ECM=GAMMA*(ETOT-BETA*AMOINC) |
| 14795 |
RECAL1=ECM |
| 14796 |
C TOTAL ENERGY OF SCALED INCIDENT PARTICLE IN C.M. |
| 14797 |
ECMPR=GAMPR*(ETOTPR-BETAPR*AMOIPR) |
| 14798 |
C TOTAL CUTOFF ENERGY IN LAB SYSTEM FOR THE FIVE PARTICLES |
| 14799 |
C KINETIC ENERGY OF INCIDENT PARTICLE IN C.M. SYSTEM |
| 14800 |
ECMOKE=ECM-RESMAS(IPIN) |
| 14801 |
RECAL2=ECMOKE |
| 14802 |
C MOMENTUM OF INCIDENT PARTICLE IN C.M. SYSTEM |
| 14803 |
PCMO=DSQRT(ECM*ECM-RESMAS(IPIN)*RESMAS(IPIN)) |
| 14804 |
RECAL3=PCMO |
| 14805 |
C COUNTER FOR NUMBER OF COLLISIONS |
| 14806 |
140 ECM=RECAL1 |
| 14807 |
ECMOKE=RECAL2 |
| 14808 |
PCMO=RECAL3 |
| 14809 |
DO 150 III = 2,NWDS |
| 14810 |
150 BRRAY(III) = ARRAY(III) |
| 14811 |
160 EXCIT = EINC + RESMAS(IPIN)*(1.D0-CHEINC) |
| 14812 |
PX = 0. |
| 14813 |
PY = 0. |
| 14814 |
PZ = AMOINC |
| 14815 |
PXS = 0. |
| 14816 |
PYS = 0. |
| 14817 |
PZS = AMOIPR |
| 14818 |
C SETUP OF INITIAL LAB MOMENTUM |
| 14819 |
DO 190 III = 2,NWDS,8 |
| 14820 |
KTYPE=ARRAY(III) |
| 14821 |
C DEFINES TYPE OF ESCAPING PARTICLE |
| 14822 |
M8 = (III+6)/8 |
| 14823 |
ARRAY(III+1) = ARRAY(III+1)+RESMAS(KTYPE) |
| 14824 |
C TOTAL ENERGY OF ESCAPING PARTICLE |
| 14825 |
AVERE(KTYPE) = ARRAY(III+1)+AVERE(KTYPE)-CUTL(KTYPE) |
| 14826 |
C ENERGY CONSERVATION CHECK OF UNSCALED SYSTEM IN LAB |
| 14827 |
YIELD(KTYPE)=YIELD(KTYPE)+1.D0 |
| 14828 |
C SUMMING UP PARTICLES FOR MULTIPLICITY |
| 14829 |
PLICIT(KTYPE) = PLICIT(KTYPE) + 1.0D0 |
| 14830 |
C MULTIPLICITY OF ESCAPING PARTICLES FOR THIS COLLISION |
| 14831 |
P=(ARRAY(III+1)*ARRAY(III+1)-RESMAS(KTYPE)*RESMAS(KTYPE))**.5 |
| 14832 |
C MOMENTUM IN LAB OF ESCAPING UNSCALED PARTICLE |
| 14833 |
PX=PX+P*ARRAY(III+2) |
| 14834 |
PY=PY+P*ARRAY(III+3) |
| 14835 |
PZ=PZ-P*ARRAY(III+4) |
| 14836 |
C THREE MOMENTUM COMPONENTS IN LAB OF ESCAPING UNSCALED PARTICLE |
| 14837 |
CHECK = 0. |
| 14838 |
IF(KTYPE.LT.3) CHECK=1.D0 |
| 14839 |
EXCIT=EXCIT-ARRAY(III+1)+RESMAS(KTYPE)*CHECK |
| 14840 |
C PRELIMINARY CALCULATION TO OBTAIN EXCITATION ENERGY |
| 14841 |
170 WEIGHT(M8)=GAMMA*(ARRAY(III+1)-ARRAY(III+4)*P*BETA) |
| 14842 |
IF(WEIGHT(M8).GT.ECM) COUNT = COUNT + 1. |
| 14843 |
C WILL BE USED IN WEIGHT CALCULATION. |
| 14844 |
C NOW CONTAINS T.E. IN CM OF UNSCALED ESCAPING PARTICLE |
| 14845 |
IF(WEIGHT(M8).GT.ECM) ECMOKE=WEIGHT(M8)-RESMAS(IPIN) |
| 14846 |
IF(WEIGHT(M8).GT.ECM) PCMO=DSQRT(WEIGHT(M8)**2-RESMAS(IPIN)** |
| 14847 |
+ 2) |
| 14848 |
IF(WEIGHT(M8).GT.ECM) ECM=WEIGHT(M8) |
| 14849 |
ECMKE(KTYPE)=ECMKE(KTYPE)+WEIGHT(M8)-RESMAS(KTYPE) |
| 14850 |
C CM KE OF UNSCALED PARTICLES....USED IN CALCULATING B |
| 14851 |
PCM=(WEIGHT(M8)*WEIGHT(M8)-RESMAS(KTYPE)*RESMAS(KTYPE))**.5 |
| 14852 |
C MOMENTUM IN CM OF UNSCALED ESCAPING PARTICLE |
| 14853 |
EPRCM(M8)=((WEIGHT(M8)-CUTCM(KTYPE))/(ECM-CUTCM(IPIN )))** |
| 14854 |
+ (1.D0/FUG(KTYPE))*(ECMPR-CUTCM(IPIN ))+CUTCM(KTYPE) |
| 14855 |
C SCALED UP TOTAL ENERGY OF ESCAPING PARTICLE IN CM |
| 14856 |
PTEMP=DSQRT(EPRCM(M8)*EPRCM(M8)-RESMAS(KTYPE)*RESMAS(KTYPE)) |
| 14857 |
C MOMENTUM OF SCALED UP PARTICLE IN CM |
| 14858 |
W=1.D0-(P/PTEMP)**2+((P/PTEMP)**2)*ARRAY(III+4)*ARRAY(III+4) |
| 14859 |
IF(W.LE.0.) CHECK8=CHECK8+1. |
| 14860 |
IF(W.LE.0.) W=0. |
| 14861 |
IF(W.LE.0.) GO TO 180 |
| 14862 |
W=DSQRT(W) |
| 14863 |
C POLAR ANGLE IN CM...COMES FROM CONSERVATION OF TRANSVERSE MOMENTUM |
| 14864 |
WCM=GAMMA*(P*ARRAY(III+4)-BETA*ARRAY(III+1))/PCM |
| 14865 |
C THE SIGN OF W IS CHECKED NEXT |
| 14866 |
C UNSCALED CM POLAR ANGLE |
| 14867 |
IF(WCM.LT.0.) W=-W |
| 14868 |
180 CONTINUE |
| 14869 |
ARRAY(III+1)=GAMPR*(EPRCM(M8)+BETAPR*PTEMP*W) |
| 14870 |
C CONTAINS TOTAL SCALED ENERGY IN LAB |
| 14871 |
PPR=(ARRAY(III+1)*ARRAY(III+1)-RESMAS(KTYPE)*RESMAS(KTYPE))** |
| 14872 |
+ .5 |
| 14873 |
C MOMENTUM OF SCALED PARTICLE IN LAB |
| 14874 |
ARRAY(III+4)=GAMPR*(PTEMP*W+BETAPR*EPRCM(M8))/PPR |
| 14875 |
C CORRECTED POLAR ANGLE IN LAB TO CONSERVE TRANSVERSE MOMENTUM |
| 14876 |
ARRAY(III+1)=ARRAY(III+1)-RESMAS(KTYPE) |
| 14877 |
C K.E. IN LAB OF SCALED PARTICLE |
| 14878 |
PSTOR1=DSQRT(1.D0-ARRAY(III+4)*ARRAY(III+4))* DCOS(DATAN(ARRAY |
| 14879 |
+ (III+3)/ARRAY(III+2))) |
| 14880 |
PSTOR1=DABS(PSTOR1) |
| 14881 |
PSTOR2=DSQRT(1.D0-ARRAY(III+4)*ARRAY(III+4))* DSIN(DATAN(ARRAY |
| 14882 |
+ (III+3)/ARRAY(III+2))) |
| 14883 |
PSTOR2=DABS(PSTOR2) |
| 14884 |
IF(ARRAY(III+2).LT.0.) PSTOR1=-PSTOR1 |
| 14885 |
IF(ARRAY(III+3).LT.0.) PSTOR2=-PSTOR2 |
| 14886 |
C SETTING UP MODIFIED PX,PY TO PRESERVE THE AZIMUTHAL ANGLE |
| 14887 |
ARRAY(III+2)=PSTOR1 |
| 14888 |
ARRAY(III+3)=PSTOR2 |
| 14889 |
C RESTORING CORRECTED X AND Y COSINES |
| 14890 |
190 CONTINUE |
| 14891 |
B = ECMOKE + AMASIN*(1.D0-CHEINC) |
| 14892 |
DO 200 IIV = 1,5 |
| 14893 |
200 B=B-ECMKE(IIV)+PLICIT(IIV)*(CUTCM(IIV)-RESMAS(IIV)) |
| 14894 |
BTOT = BTOT + B |
| 14895 |
BLANK = 1.D0 |
| 14896 |
BLANK1 = 1.D0/(ECM-CHEINC*AMASIN-B) |
| 14897 |
DO 210 J = 2,NWDS,8 |
| 14898 |
KTYPE = ARRAY(J) |
| 14899 |
M9 = (J+6)/8 |
| 14900 |
IF(KTYPE.LE.2)WEIGHT(M9)=(WEIGHT(M9)-CUTCM(KTYPE))/ (EPRCM(M9) |
| 14901 |
+ -CUTCM(KTYPE)) |
| 14902 |
IF(KTYPE.GT.2)WEIGHT(M9)=WEIGHT(M9)/EPRCM(M9) |
| 14903 |
210 CONTINUE |
| 14904 |
AMORN=TARMAS+CHEINC*AMASIN - PLICIT(1)*RESMAS(1)-PLICIT(2)* |
| 14905 |
+ RESMAS(2) +(PLICIT(1)+PLICIT(2))*7.0D0-CHEINC*7.D0 |
| 14906 |
C MASS OF RESIDUAL NUCLEUS |
| 14907 |
IF(AMORN.LE.0.)WHY=1. |
| 14908 |
C WHY=1 UNSCALED RESIDUAL MASS.LE.0 |
| 14909 |
IF(AMORN.LE.0.) GO TO 220 |
| 14910 |
AMORNT = AMORNT + AMORN |
| 14911 |
ERN=DSQRT(PX*PX+PY*PY+PZ*PZ+AMORN*AMORN)-AMORN |
| 14912 |
C ENERGY OF RECOILING NUCLEUS (UNSCALED) |
| 14913 |
ERNT=ERNT+ERN |
| 14914 |
C SUMMING TOTAL RECOIL ENERGIES FOR ALL COLLISIONS UNSCALED |
| 14915 |
ESTAR=EXCIT-ERN-(PLICIT(1)+PLICIT(2)-1.D0*CHEINC)*7.D0 |
| 14916 |
ESTART=ESTART+ESTAR |
| 14917 |
IF(ESTAR.LT.0.) CHECK7=CHECK7+1. |
| 14918 |
IF(ESTAR.LT.0.) GO TO 270 |
| 14919 |
GO TO 290 |
| 14920 |
220 NMLTEO=NMLTEO+1 |
| 14921 |
ZKZ = ZKZ - 1.D0 |
| 14922 |
230 BTOT = BTOT - B |
| 14923 |
DO 240 III = 2,NWDS,8 |
| 14924 |
KTYPE = ARRAY(III) |
| 14925 |
YIELD(KTYPE)=YIELD(KTYPE)-1.D0 |
| 14926 |
AVERE(KTYPE)=AVERE(KTYPE)-BRRAY(III+1)+(CUTL(KTYPE)- RESMAS(KT |
| 14927 |
+ YPE)) |
| 14928 |
240 CONTINUE |
| 14929 |
GO TO 60 |
| 14930 |
250 DO 260 III = 2,NWDS,8 |
| 14931 |
KTYPE = ARRAY(III) |
| 14932 |
M8 = (III+6)/8 |
| 14933 |
YIELD(KTYPE)=YIELD(KTYPE)-1.D0 |
| 14934 |
AVERE(KTYPE)=AVERE(KTYPE)-BRRAY(III+1)+(CUTL(KTYPE)- RESMAS(KT |
| 14935 |
+ YPE)) |
| 14936 |
YIELD(KTYPE+5) = YIELD(KTYPE+5) - WEIGHT(M8) |
| 14937 |
AVERE(KTYPE+5)=AVERE(KTYPE+5)-ARRAY(III+1)*WEIGHT(M8)+ (CUTL(K |
| 14938 |
+ TYPE)-RESMAS(KTYPE))*WEIGHT(M8) |
| 14939 |
260 CONTINUE |
| 14940 |
BTOT = BTOT-B |
| 14941 |
ZKZ = ZKZ - 1.D0 |
| 14942 |
ERNT=ERNT-ERN |
| 14943 |
ESTART=ESTART-ESTAR |
| 14944 |
AMORNT=AMORNT-AMORN |
| 14945 |
GO TO 60 |
| 14946 |
270 ERNT = ERNT - ERN |
| 14947 |
ERN = ERN+ESTAR |
| 14948 |
ESTART = ESTART-ESTAR |
| 14949 |
ERNT=ERNT+ERN |
| 14950 |
ESTAR=0. |
| 14951 |
IF(ERN.LT.0.) COUNT5 = COUNT5 + 1. |
| 14952 |
IF(ERN.LT.0.)WHY=2 |
| 14953 |
C WHY=2 ENERGY OF UNSCALED RECOILING NUCLEUS.LT.0 WHEN ESTAR.LT.0. |
| 14954 |
C ERN=ERN+ESTAR.......ERN.LT.0 |
| 14955 |
IF(ERN.GE.0.) GO TO 290 |
| 14956 |
ZKZ=ZKZ-1.D0 |
| 14957 |
AMORNT=AMORNT-AMORN |
| 14958 |
BTOT=BTOT-B |
| 14959 |
ERNT=ERNT-ERN |
| 14960 |
DO 280 III=2,NWDS,8 |
| 14961 |
KTYPE=ARRAY(III) |
| 14962 |
YIELD(KTYPE)=YIELD(KTYPE)-1.D0 |
| 14963 |
AVERE(KTYPE)=AVERE(KTYPE)-BRRAY(III+1)+(CUTL(KTYPE)- RESMAS(KT |
| 14964 |
+ YPE)) |
| 14965 |
280 CONTINUE |
| 14966 |
GO TO 60 |
| 14967 |
290 CONTINUE |
| 14968 |
C*****CALCULATIONS DEALING WITH SCALED UP NUCLEAR RECOIL AND BPR******** |
| 14969 |
A1=0. |
| 14970 |
A2=0. |
| 14971 |
A3=0. |
| 14972 |
A4=0. |
| 14973 |
A5=0. |
| 14974 |
DO 300 III=2,NWDS,8 |
| 14975 |
M8=(III+6)/8 |
| 14976 |
KTYPE=ARRAY(III) |
| 14977 |
P=((ARRAY(III+1)+RESMAS(KTYPE))**2-RESMAS(KTYPE)**2)**.5 |
| 14978 |
A1=P*ARRAY(III+2)*WEIGHT(M8)+A1 |
| 14979 |
A2=P*ARRAY(III+3)*WEIGHT(M8)+A2 |
| 14980 |
A3=P*ARRAY(III+4)*WEIGHT(M8)+A3 |
| 14981 |
A4=(ARRAY(III+1)+RESMAS(KTYPE))*WEIGHT(M8)+A4 |
| 14982 |
IF(KTYPE.GT.2.) GO TO 300 |
| 14983 |
A5=(7.D0-RESMAS(KTYPE))*WEIGHT(M8)+A5 |
| 14984 |
300 CONTINUE |
| 14985 |
A11=A1*A1+A2*A2+A3*A3+A5*A5-A4*A4 |
| 14986 |
B11=2.D0*((TARMAS+(AMASIN-7.D0)*CHEINC)*A5-AMOIPR*A3+A4*(ETOTPR |
| 14987 |
+ +TARMAS-ESTAR)) |
| 14988 |
C11=AMOIPR*AMOIPR+(TARMAS+(AMASIN-7.D0)*CHEINC)**2 |
| 14989 |
+ -(ETOTPR+TARMAS-ESTAR)**2 |
| 14990 |
IF(A11.EQ.0.) COUNT1=COUNT1 + 1. |
| 14991 |
IF(A11.EQ.0.) GO TO 310 |
| 14992 |
ANSPLU=(-B11+DSQRT(B11**2-4.D0*A11*C11))/(2.D0*A11) |
| 14993 |
ANSMIN=(-B11-DSQRT(B11**2-4.D0*A11*C11))/(2.D0*A11) |
| 14994 |
GO TO 320 |
| 14995 |
310 ANSWER=-C11/B11 |
| 14996 |
IF(ANSWER.LE.0.) COUNT2=COUNT2+1. |
| 14997 |
IF(ANSWER.LE.0.) WHY=3 |
| 14998 |
C SOLUTION TO ENERGY BALANCE EQUATION IS .LE. 0. |
| 14999 |
IF(ANSWER.LE.0.) GO TO 350 |
| 15000 |
ANSMIN=ANSWER |
| 15001 |
ANSPLU=ANSWER |
| 15002 |
C$$$$$PUT IN CHECK |
| 15003 |
320 SCORE=0. |
| 15004 |
CHECK=0. |
| 15005 |
DO 340 I=1,2 |
| 15006 |
A1=0. |
| 15007 |
A2=0. |
| 15008 |
A3=0. |
| 15009 |
A4=0. |
| 15010 |
A5=0. |
| 15011 |
ANSWER=ANSPLU |
| 15012 |
IF(I.EQ.2) ANSWER=ANSMIN |
| 15013 |
DO 330 III=2,NWDS,8 |
| 15014 |
M8=(III+6)/8 |
| 15015 |
KTYPE=ARRAY(III) |
| 15016 |
P=((ARRAY(III+1)+RESMAS(KTYPE))**2-RESMAS(KTYPE)**2)**.5 |
| 15017 |
A6=ANSWER*WEIGHT(M8) |
| 15018 |
A1=A1+P*ARRAY(III+2)*A6 |
| 15019 |
A2=A2+P*ARRAY(III+3)*A6 |
| 15020 |
A3=A3+P*ARRAY(III+4)*A6 |
| 15021 |
IF(KTYPE.LT.3) A4=A4+(7.D0-RESMAS(KTYPE))*A6 |
| 15022 |
A5 = A5 + (ARRAY(III+1)+RESMAS(KTYPE))*WEIGHT(M8) |
| 15023 |
330 CONTINUE |
| 15024 |
A7=A1*A1+A2*A2+(AMOIPR-A3)**2+(TARMAS+(AMASIN-7.D0)*CHEINC |
| 15025 |
+ +A4)**2 |
| 15026 |
A7=DSQRT(A7) |
| 15027 |
D1 = (ETOTPR + TARMAS - ESTAR - A7)/A5 |
| 15028 |
STO =DABS((ANSWER-D1)/ANSWER) |
| 15029 |
IF(I.EQ.1) A8=A7 |
| 15030 |
IF(I.EQ.1) STOO = STO |
| 15031 |
IF(STO.LE..00001) COUNT3 = COUNT3 + 1. |
| 15032 |
IF(STO.LE..00001) CHECK=I |
| 15033 |
IF(STO.LE..00001) SCORE=SCORE+1. |
| 15034 |
340 CONTINUE |
| 15035 |
IF(SCORE.EQ.0.) WHY=5 |
| 15036 |
C WHY=5 ENERGY EQUATION NOT SATISFIED |
| 15037 |
IF(SCORE.NE.0.) GO TO 360 |
| 15038 |
350 ZKZ = ZKZ-1.D0 |
| 15039 |
NTTME=NTTME+1 |
| 15040 |
ERNT=ERNT-ERN |
| 15041 |
ESTART=ESTART-ESTAR |
| 15042 |
AMORNT=AMORNT-AMORN |
| 15043 |
GO TO 230 |
| 15044 |
360 CONTINUE |
| 15045 |
IF(SCORE.EQ.2.) GO TO 370 |
| 15046 |
IF(CHECK.EQ.1.D0) ANSWER = ANSPLU |
| 15047 |
IF(ANSWER.LE.0.) COUNT2=COUNT2+1. |
| 15048 |
IF(ANSWER.LE.0.) WHY=3 |
| 15049 |
IF(ANSWER.LT.0.) GO TO 350 |
| 15050 |
GO TO 390 |
| 15051 |
370 IF(ANSPLU.GT.0.AND.ANSMIN.GT.0.) GO TO 380 |
| 15052 |
IF(ANSPLU.GT.0.) ANSWER=ANSPLU |
| 15053 |
IF(ANSMIN.GT.0.) ANSWER=ANSMIN |
| 15054 |
GO TO 390 |
| 15055 |
380 IF(A8.LT.A7) ANSWER=ANSPLU |
| 15056 |
IF(ANSWER.LE.0.) COUNT2=COUNT2+1. |
| 15057 |
IF(ANSWER.LE.0.) WHY=3 |
| 15058 |
IF(ANSWER.LE.0.) GO TO 350 |
| 15059 |
390 D1=0. |
| 15060 |
DO 410 III=2,NWDS,8 |
| 15061 |
KTYPE=ARRAY(III) |
| 15062 |
M8=(III+6)/8 |
| 15063 |
WEIGHT(M8)=ANSWER*WEIGHT(M8) |
| 15064 |
IF(KTYPE.GT.2) GO TO 400 |
| 15065 |
D1=D1+WEIGHT(M8)*RESMAS(KTYPE)-7.D0*WEIGHT(M8) |
| 15066 |
P=((ARRAY(III+1)+RESMAS(KTYPE))**2-RESMAS(KTYPE)**2)**.5 |
| 15067 |
400 CONTINUE |
| 15068 |
AVERE(KTYPE+5)=AVERE(KTYPE+5)+ARRAY(III+1)*WEIGHT(M8)- (CUTL(K |
| 15069 |
+ TYPE)-RESMAS(KTYPE))*WEIGHT(M8) |
| 15070 |
C CALCULATION FOR SCALED-UP ENERGY |
| 15071 |
YIELD(KTYPE+5)=YIELD(KTYPE+5)+WEIGHT(M8) |
| 15072 |
C CALCULATION FOR MULTIPLICITY OF SCALED-UP PARTICLES |
| 15073 |
PXS=PXS+WEIGHT(M8)*P*ARRAY(III+2) |
| 15074 |
PYS=PYS+WEIGHT(M8)*P*ARRAY(III+3) |
| 15075 |
PZS=PZS-WEIGHT(M8)*P*ARRAY(III+4) |
| 15076 |
410 CONTINUE |
| 15077 |
BARB=TARMAS+(AMASIN-7.D0)*CHEINC-D1 |
| 15078 |
IF(BARB.LE.0.) COUNT4=COUNT4+1. |
| 15079 |
IF(BARB.LE.0.)WHY=4. |
| 15080 |
C WHY=4 SCALED UP RESIDUAL MASS LE.0 |
| 15081 |
IF(BARB.LE.0.) GO TO 250 |
| 15082 |
ERNPR=(PXS*PXS+PYS*PYS+PZS*PZS+(TARMAS+(AMASIN-7.D0)*CHEINC-D1)**2 |
| 15083 |
+)**.5-TARMAS-(AMASIN-7.D0)*CHEINC+D1 |
| 15084 |
ERNPRT=ERNPR+ERNPRT |
| 15085 |
BTOTPR=BTOTPR+ECMPR-ANSWER/BLANK1-RESMAS(IPIN)*CHEINC |
| 15086 |
AMRNST = AMRNST + (TARMAS+(AMASIN-7.D0)*CHEINC-D1) |
| 15087 |
RMFAS=BARB |
| 15088 |
REFAS=ERNPR |
| 15089 |
EXFAS=ESTAR |
| 15090 |
NOFAS=NOSLO |
| 15091 |
C*****END CALCULATIONS DEALING WITH SCALED UP NUCLEAR RECOIL AND BPR**** |
| 15092 |
420 CONTINUE |
| 15093 |
DO 430 III=2,NWDS,8 |
| 15094 |
M8=(III+6)/8 |
| 15095 |
EFAS(M8)=ARRAY(III+1) |
| 15096 |
ALPFAS(M8)=ARRAY(III+2) |
| 15097 |
BETFAS(M8)=ARRAY(III+3) |
| 15098 |
GAMFAS(M8)=ARRAY(III+4) |
| 15099 |
WTFAS(M8)=WEIGHT(M8) |
| 15100 |
430 CONTINUE |
| 15101 |
RETURN |
| 15102 |
440 DO 450 IHK=1,10 |
| 15103 |
NUMBEA(IHK)=NUMBEA(IHK)/ZKZ |
| 15104 |
EINCT(IHK)=EINCT(IHK)/ZKZ |
| 15105 |
YIELD(IHK)=YIELD(IHK)/ZKZ |
| 15106 |
AVERE(IHK)=AVERE(IHK)/ZKZ |
| 15107 |
450 CONTINUE |
| 15108 |
ESTART = ESTART/ZKZ |
| 15109 |
TARMAT=TARMAT/ZKZ |
| 15110 |
BTOTPR=BTOTPR/ZKZ |
| 15111 |
AMORNT = AMORNT/ZKZ |
| 15112 |
AMRNST = AMRNST/ZKZ |
| 15113 |
ERNT=ERNT/ZKZ |
| 15114 |
ERNPRT=ERNPRT/ZKZ |
| 15115 |
BTOT = BTOT/ZKZ |
| 15116 |
ETOT=0. |
| 15117 |
ETOTPR=0. |
| 15118 |
DO 460 I=1,5 |
| 15119 |
ETOT=ETOT+EINCT(I)+RESMAS(I)*NUMBEA(I) |
| 15120 |
ETOTPR=ETOTPR+EINCT(I+5)+RESMAS(I)*NUMBEA(I+5) |
| 15121 |
460 CONTINUE |
| 15122 |
ESUM = 0.0 |
| 15123 |
ESUMPR = 0.0 |
| 15124 |
DO 470 I = 1,5 |
| 15125 |
ESUM = ESUM + AVERE(I) |
| 15126 |
ESUMPR = ESUMPR + AVERE(I+5) |
| 15127 |
470 CONTINUE |
| 15128 |
RETURN |
| 15129 |
END |
| 15130 |
*CMZ : 0.93/08 02/03/93 09.35.17 by Christian Zeitnitz |
| 15131 |
*-- Author : |
| 15132 |
SUBROUTINE SHXSEC(E,INC,SIGT,SIGEL,SIGNEL) |
| 15133 |
C |
| 15134 |
#include "cinout.inc" |
| 15135 |
*KEND. |
| 15136 |
C |
| 15137 |
C CALCULATES PROTON AND NEUTRON CROSS SECTIONS FOR E > 3.5 GeV |
| 15138 |
C CALCULATES PI+ AND PI- CROSS SECTIONS FOR E > 2.5 GeV |
| 15139 |
C THE TARGET PARTICLE IS A PROTON |
| 15140 |
C E ------- KINETIC ENERGY OF INCIDENT PARTICLE(MEV) |
| 15141 |
C INC ----- TYPE OF INCIDENT PARTICLE |
| 15142 |
C 0 -- PROTON |
| 15143 |
C 1 NEUTRON |
| 15144 |
C 2 PI+ |
| 15145 |
C 3 NOT USED |
| 15146 |
C 4 PI- |
| 15147 |
C SIGT ---- TOTAL CROSS SECTION(CM**2) |
| 15148 |
C SIGEL --- ELASTIC CROSS SECTION(CM**2) |
| 15149 |
C SIGNEL -- NONELASTIC CROSS SECTION(CM**2) |
| 15150 |
C |
| 15151 |
REAL*8 E1 |
| 15152 |
IN = INC + 1 |
| 15153 |
E1 = E*1.D-3 |
| 15154 |
GO TO (20,30,50,10,80),IN |
| 15155 |
10 CALL CERROR('CRSEC1') |
| 15156 |
C |
| 15157 |
20 SIGT = 37.5D0 + 7.D0/(DSQRT(E1)) |
| 15158 |
SIGEL = 7.D0 + 21.03D0/(E1**0.873D0) |
| 15159 |
GO TO 110 |
| 15160 |
C |
| 15161 |
C |
| 15162 |
30 IF(E1.GT.8.D0) GO TO 40 |
| 15163 |
SIGT = 42.D0 |
| 15164 |
SIGEL = -0.222D0*E1+12.48D0 |
| 15165 |
GO TO 110 |
| 15166 |
40 SIGT = 37.5D0 + 26.45D0/(E1**0.852D0) |
| 15167 |
SIGEL = 6.0D0 + 73.144D0/(E1**1.32D0) |
| 15168 |
GO TO 110 |
| 15169 |
C |
| 15170 |
C |
| 15171 |
50 IF(E1.GT.3.D0) GO TO 60 |
| 15172 |
SIGT = -4.66D0*E1 + 42.95D0 |
| 15173 |
SIGEL = -1.40D0*E1 + 10.0D0 |
| 15174 |
GO TO 110 |
| 15175 |
60 IF(E1.GT.6.D0) GO TO 70 |
| 15176 |
SIGT = -0.7567D0*E1 + 31.24D0 |
| 15177 |
SIGEL = -0.166D0*E1 + 6.298D0 |
| 15178 |
GO TO 110 |
| 15179 |
70 SIGT = 21.50D0 + 18.914D0/(E1**.7155D0) |
| 15180 |
SIGEL = 3.5D0 + 9.93D0/(E1**.953D0) |
| 15181 |
GO TO 110 |
| 15182 |
C |
| 15183 |
C |
| 15184 |
80 IF(E1.GT.5.D0) GO TO 90 |
| 15185 |
SIGT = -1.66D0*E1 + 37.34D0 |
| 15186 |
GO TO 100 |
| 15187 |
90 SIGT = 23.60D0 + 25.51D0/(E1**0.959D0) |
| 15188 |
100 SIGEL = 3.8D0 + 7.273D0/(E1**0.896D0) |
| 15189 |
C |
| 15190 |
C |
| 15191 |
110 SIGT = SIGT*1.E-27 |
| 15192 |
SIGEL = SIGEL*1.E-27 |
| 15193 |
SIGNEL = SIGT - SIGEL |
| 15194 |
C |
| 15195 |
IF((IN.LE.2).AND.(E1.LT.3.4949D0)) WRITE(IO,10000) E1 |
| 15196 |
IF((IN.GT.2).AND.(E1.LT.2.4949D0)) WRITE(IO,10100) E1 |
| 15197 |
10000 FORMAT(' HETC: PROTON OR NEUTRON CROSS-SECTIONS ARE BEING |
| 15198 |
+ REQUESTED FOR AN ENERGY LESS THAN 3.5-GEV in SHXSEC E=',G18.7) |
| 15199 |
10100 FORMAT(' HETC: PI+ OR PI- CROSS-SECTIONS ARE BEING REQUESTED |
| 15200 |
+ FOR AN ENERGY LESS THAN 2.5-GEV in SHXSEC E=',G18.7) |
| 15201 |
RETURN |
| 15202 |
END |
| 15203 |
*CMZ : 1.01/04 10/06/93 14.43.50 by Christian Zeitnitz |
| 15204 |
*-- Author : Christian Zeitnitz 19/11/92 |
| 15205 |
SUBROUTINE SKALEH(IBERT,ITINC,HSIG,EINC,NOFAS,ITFAS,EFAS,ALPHAS, |
| 15206 |
+ BETFAS,GAMFAS,EHICUT) |
| 15207 |
C |
| 15208 |
#include "cmass.inc" |
| 15209 |
*KEND. |
| 15210 |
DIMENSION ITFAS(*), EFAS(*) , ALPHAS(*) , BETFAS(*) , GAMFAS(*) |
| 15211 |
DIMENSION R(60) |
| 15212 |
SAVE |
| 15213 |
C |
| 15214 |
ITYPE = ITINC + 1 |
| 15215 |
CALL CPCOL(IBERT,ITYPE,HSIG,EHICUT,NOFAS,ITFAS,EFAS,ALPFAS,BETFAS, |
| 15216 |
+ GAMFAS) |
| 15217 |
IF(NOFAS.LE.0) RETURN |
| 15218 |
CZ simple scaling for H-collision, conserve energy 19 Nov. 1992 |
| 15219 |
EI=EINC+PMASS(ITINC+1) |
| 15220 |
ESUMF = 0.0 |
| 15221 |
DO 10 I=1,NOFAS |
| 15222 |
ESUMF=ESUMF+PMASS(ITFAS(I)+1)+EFAS(I) |
| 15223 |
10 CONTINUE |
| 15224 |
EDIV = EI-ESUMF |
| 15225 |
IF(EDIV.LE.0.0) RETURN |
| 15226 |
CALL GRNDM(R,NOFAS) |
| 15227 |
RS=0.0 |
| 15228 |
DO 20 I=1,NOFAS |
| 15229 |
RS=RS+R(I) |
| 15230 |
20 CONTINUE |
| 15231 |
DO 30 I=1,NOFAS |
| 15232 |
EFAS(I) = EFAS(I)+R(I)/RS*EDIV |
| 15233 |
30 CONTINUE |
| 15234 |
RETURN |
| 15235 |
END |
| 15236 |
*CMZ : 0.93/01 08/02/93 14.21.45 by Christian Zeitnitz |
| 15237 |
*-- Author : |
| 15238 |
SUBROUTINE CSCATT(INC,EKE1,ITFAS,EFAS,ALPFAS,BETFAS,GAMFAS) |
| 15239 |
C |
| 15240 |
C |
| 15241 |
C INC = TYPE OF INCIDENT PARTICLE |
| 15242 |
C = 0 PROTON |
| 15243 |
C = 1 NEUTRON |
| 15244 |
C = 2 PI + |
| 15245 |
C = 3 NOT USED |
| 15246 |
C = 4 PI - |
| 15247 |
C EKE1 = KINETIC ENERGY OF INCIDENT PARTICLE(MEV) |
| 15248 |
C ITFAS = TYPE OF PARTICLE (SAME AS ABOVE) |
| 15249 |
C EFAS = KINETIC ENERGY OF PARTICLES (MEV) |
| 15250 |
C ALPFAS = X-DIRECTION COSINE |
| 15251 |
C BETFAS = Y-DIRECTION COSINE |
| 15252 |
C GAMFAS = Z-DIRECTION COSINE |
| 15253 |
C RANDS = LOCATION OF RANDOM NUMBER SEQUENCE |
| 15254 |
C |
| 15255 |
C SUBROUTINES CALLED CAAZIO. |
| 15256 |
C |
| 15257 |
DIMENSION ITFAS(2),EFAS(2),ALPFAS(2),BETFAS(2),GAMFAS(2),RANDS(4) |
| 15258 |
REAL*8 B,M1,M2,E1,P1,ECM1,PCM1,ETLAB,ETCM,BETA,GAMMA,T1,T2,T3,T4, |
| 15259 |
1 T5,T6,T7,T8,T9,T10,T11,T12,PLAB1,PLAB2,CST,SNT,TB |
| 15260 |
#include "crandm.inc" |
| 15261 |
*KEND. |
| 15262 |
C |
| 15263 |
DATA M2/940.075D0/ |
| 15264 |
SAVE |
| 15265 |
C |
| 15266 |
T2 = M2*M2 |
| 15267 |
IN=INC+1 |
| 15268 |
GO TO (10,10,20,30,40),IN |
| 15269 |
10 M1=940.075D0 |
| 15270 |
GO TO 60 |
| 15271 |
20 B=7.040D-6 |
| 15272 |
GO TO 50 |
| 15273 |
30 CALL CERROR('SCATT1') |
| 15274 |
40 B=7.575D-6 |
| 15275 |
50 M1=139.89D0 |
| 15276 |
60 E1=EKE1+M1 |
| 15277 |
T1=M1*M1 |
| 15278 |
P1=DSQRT(E1*E1-T1) |
| 15279 |
IF(IN.GT.2) GO TO 70 |
| 15280 |
B=7.26D-6+ (3.13D-11)*P1 |
| 15281 |
70 ETLAB=E1+M2 |
| 15282 |
BETA=P1/ETLAB |
| 15283 |
GAMMA=1.D0/DSQRT(1.D0-BETA*BETA) |
| 15284 |
ETCM=ETLAB/GAMMA |
| 15285 |
T3=T1+T2 |
| 15286 |
T4=T1-T2 |
| 15287 |
T4=T4*T4 |
| 15288 |
T5=ETCM*ETCM |
| 15289 |
T6=T5*T5 |
| 15290 |
T7=B*(T6-2.D0*T5*T3+T4)/(2.D0*T5) |
| 15291 |
T8 = RANDC(ISEED) |
| 15292 |
TB=T7 |
| 15293 |
IF(T7.GT.50.D0) TB=50.D0 |
| 15294 |
CST=1.D0+(DLOG(1.D0-T8*(1.D0-DEXP(-TB))))/T7 |
| 15295 |
SNT=DSQRT(1.D0-CST*CST) |
| 15296 |
CALL CAAZIO(T9,T10) |
| 15297 |
ECM1=(T5+T1-T2)/(2.D0*ETCM ) |
| 15298 |
PCM1=DSQRT(ECM1*ECM1-T1) |
| 15299 |
ITFAS(1)=INC |
| 15300 |
ITFAS(2)=0. |
| 15301 |
T11 = GAMMA*(ECM1+PCM1*CST*BETA) - M1 |
| 15302 |
T12 = ETLAB - T11 -M1 - M2 |
| 15303 |
PLAB1 = DSQRT(2.D0*M1*T11 + T11*T11) |
| 15304 |
PLAB2 = DSQRT(2.D0*M2*T12 + T12*T12) |
| 15305 |
EFAS(1) = T11 |
| 15306 |
EFAS(2) = T12 |
| 15307 |
ALPFAS(1)=PCM1*SNT*T9 |
| 15308 |
ALPFAS(2)= -ALPFAS(1) |
| 15309 |
ALPFAS(1)=ALPFAS(1)/PLAB1 |
| 15310 |
ALPFAS(2)=ALPFAS(2)/PLAB2 |
| 15311 |
BETFAS(1)=PCM1*SNT*T10 |
| 15312 |
BETFAS(2)=-BETFAS(1) |
| 15313 |
BETFAS(1)=BETFAS(1)/PLAB1 |
| 15314 |
BETFAS(2)=BETFAS(2)/PLAB2 |
| 15315 |
GAMFAS(1)= GAMMA*(PCM1*CST+BETA*ECM1) |
| 15316 |
GAMFAS(2)= -GAMFAS(1)+P1 |
| 15317 |
GAMFAS(1)= GAMFAS(1)/PLAB1 |
| 15318 |
GAMFAS(2)= GAMFAS(2)/PLAB2 |
| 15319 |
RETURN |
| 15320 |
END |
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