3 C*********************************************************************
6 IF(((A**2-(B+C)**2)*(A**2-(B-C)**2)).GT.0) THEN
7 PAWT = SQRT((A**2-(B+C)**2)*(A**2-(B-C)**2))/(2.*A)
14 SUBROUTINE LUDECY_HIJING(IP)
16 C...Purpose: to handle the decay of unstable particles.
17 #include "lujets_hijing.inc"
18 #include "ludat1_hijing.inc"
19 #include "ludat2_hijing.inc"
20 #include "ludat3_hijing.inc"
21 DIMENSION VDCY(4),KFLO(4),KFL1(4),PV(10,5),RORD(10),UE(3),BE(3),
23 DATA WTCOR/2.,5.,15.,60.,250.,1500.,1.2E4,1.2E5,150.,16./
25 C...Functions: momentum in two-particle decays, four-product and
26 C...matrix element times phase space in weak decays.
28 FOUR(I,J)=P(I,4)*P(J,4)-P(I,1)*P(J,1)-P(I,2)*P(J,2)-P(I,3)*P(J,3)
29 HMEPS(HA)=((1.-HRQ-HA)**2+3.*HA*(1.+HRQ-HA))*
30 &SQRT((1.-HRQ-HA)**2-4.*HRQ*HA)
40 C...Choose lifetime and determine decay vertex.
43 ELSEIF(K(IP,1).NE.4) THEN
44 V(IP,5)=-PMAS(KC,4)*LOG(RLU_HIJING(0))
47 100 VDCY(J)=V(IP,J)+V(IP,5)*P(IP,J)/P(IP,5)
49 C...Determine whether decay allowed or not.
51 IF(MSTJ(22).EQ.2) THEN
52 IF(PMAS(KC,4).GT.PARJ(71)) MOUT=1
53 ELSEIF(MSTJ(22).EQ.3) THEN
54 IF(VDCY(1)**2+VDCY(2)**2+VDCY(3)**2.GT.PARJ(72)**2) MOUT=1
55 ELSEIF(MSTJ(22).EQ.4) THEN
56 IF(VDCY(1)**2+VDCY(2)**2.GT.PARJ(73)**2) MOUT=1
57 IF(ABS(VDCY(3)).GT.PARJ(74)) MOUT=1
59 IF(MOUT.EQ.1.AND.K(IP,1).NE.5) THEN
64 C...Check existence of decay channels. Particle/antiparticle rules.
66 IF(MDCY(KC,2).GT.0) THEN
67 MDMDCY=MDME(MDCY(KC,2),2)
68 IF(MDMDCY.GT.80.AND.MDMDCY.LE.90) KCA=MDMDCY
70 IF(MDCY(KCA,2).LE.0.OR.MDCY(KCA,3).LE.0) THEN
72 $ ,'(LUDECY_HIJING:) no decay channel defined')
75 IF(MOD(KFA/1000,10).EQ.0.AND.(KCA.EQ.85.OR.KCA.EQ.87)) KFS=-KFS
76 IF(KCHG(KC,3).EQ.0) THEN
79 IF(RLU_HIJING(0).GT.0.5) KFS=-KFS
88 C...Sum branching ratios of allowed decay channels.
91 DO 120 IDL=MDCY(KCA,2),MDCY(KCA,2)+MDCY(KCA,3)-1
92 IF(MDME(IDL,1).NE.1.AND.KFSP*MDME(IDL,1).NE.2.AND.
93 &KFSN*MDME(IDL,1).NE.3) GOTO 120
94 IF(MDME(IDL,2).GT.100) GOTO 120
100 $ ,'(LUDECY_HIJING:) all decay channels closed by user')
104 C...Select decay channel among allowed ones.
105 130 RBR=BRSU*RLU_HIJING(0)
108 IF(MDME(IDL,1).NE.1.AND.KFSP*MDME(IDL,1).NE.2.AND.
109 &KFSN*MDME(IDL,1).NE.3) THEN
110 IF(IDL.LT.MDCY(KCA,2)+MDCY(KCA,3)-1) GOTO 140
111 ELSEIF(MDME(IDL,2).GT.100) THEN
112 IF(IDL.LT.MDCY(KCA,2)+MDCY(KCA,3)-1) GOTO 140
116 IF(IDL.LT.MDCY(KCA,2)+MDCY(KCA,3)-1.AND.RBR.GT.0.) GOTO 140
119 C...Start readout of decay channel: matrix element, reset counters.
122 IF(NTRY.GT.1000) THEN
123 CALL LUERRM_HIJING(14
124 $ ,'(LUDECY_HIJING:) caught in infinite loop')
125 IF(MSTU(21).GE.1) RETURN
131 IF(MMAT.GE.11.AND.MMAT.NE.46.AND.P(IP,4).GT.20.*P(IP,5)) MBST=1
134 160 IF(MBST.EQ.0) PV(1,J)=P(IP,J)
135 IF(MBST.EQ.1) PV(1,4)=P(IP,5)
141 C...Read out decay products. Convert to standard flavour code.
143 IF(MDME(IDC+1,2).EQ.101) JTMAX=10
145 IF(JT.LE.5) KP=KFDP(IDC,JT)
146 IF(JT.GE.6) KP=KFDP(IDC+1,JT-5)
149 KCP=LUCOMP_HIJING(KPA)
150 IF(KCHG(KCP,3).EQ.0.AND.KPA.NE.81.AND.KPA.NE.82) THEN
152 ELSEIF(KPA.NE.81.AND.KPA.NE.82) THEN
154 ELSEIF(KPA.EQ.81.AND.MOD(KFA/1000,10).EQ.0) THEN
155 KFP=-KFS*MOD(KFA/10,10)
156 ELSEIF(KPA.EQ.81.AND.MOD(KFA/100,10).GE.MOD(KFA/10,10)) THEN
157 KFP=KFS*(100*MOD(KFA/10,100)+3)
158 ELSEIF(KPA.EQ.81) THEN
159 KFP=KFS*(1000*MOD(KFA/10,10)+100*MOD(KFA/100,10)+1)
160 ELSEIF(KP.EQ.82) THEN
161 CALL LUKFDI_HIJING(-KFS*INT(1.+(2.+PARJ(2))*RLU_HIJING(0)),0
163 IF(KFP.EQ.0) GOTO 150
165 IF(PV(1,5).LT.PARJ(32)+2.*ULMASS_HIJING(KFP)) GOTO 150
166 ELSEIF(KP.EQ.-82) THEN
168 IF(IABS(KFP).GT.10) KFP=KFP+ISIGN(10000,KFP)
170 IF(KPA.EQ.81.OR.KPA.EQ.82) KCP=LUCOMP_HIJING(KFP)
172 C...Add decay product to event record or to quark flavour list.
175 IF(MMAT.GE.11.AND.MMAT.LE.30.AND.KQP.NE.0) THEN
179 PSQ=PSQ+ULMASS_HIJING(KFLO(NQ))
180 ELSEIF(MMAT.GE.42.AND.MMAT.LE.43.AND.NP.EQ.3.AND.MOD(NQ,2).EQ.1)
186 CALL LUKFDI_HIJING(KFP,KFI,KFLDMP,K(I,2))
187 IF(K(I,2).EQ.0) GOTO 150
189 P(I,5)=ULMASS_HIJING(K(I,2))
194 IF(MMAT.NE.33.AND.KQP.NE.0) NQ=NQ+1
195 IF(MMAT.EQ.33.AND.KQP.NE.0.AND.KQP.NE.2) NQ=NQ+1
197 IF(MMAT.EQ.4.AND.JT.LE.2.AND.KFP.EQ.21) K(I,1)=2
198 IF(MMAT.EQ.4.AND.JT.EQ.3) K(I,1)=1
203 P(I,5)=ULMASS_HIJING(KFP)
204 IF(MMAT.EQ.45.AND.KFPA.EQ.89) P(I,5)=PARJ(32)
209 C...Choose decay multiplicity in phase space model.
210 180 IF(MMAT.GE.11.AND.MMAT.LE.30) THEN
212 CNDE=PARJ(61)*LOG(MAX((PV(1,5)-PS-PSQ)/PARJ(62),1.1))
213 IF(MMAT.EQ.12) CNDE=CNDE+PARJ(63)
215 IF(NTRY.GT.1000) THEN
216 CALL LUERRM_HIJING(14
217 $ ,'(LUDECY_HIJING:) caught in infinite loop')
218 IF(MSTU(21).GE.1) RETURN
221 GAUSS=SQRT(-2.*CNDE*LOG(MAX(1E-10,RLU_HIJING(0))))*
222 & SIN(PARU(2)*RLU_HIJING(0))
223 ND=0.5+0.5*NP+0.25*NQ+CNDE+GAUSS
224 IF(ND.LT.NP+NQ/2.OR.ND.LT.2.OR.ND.GT.10) GOTO 190
225 IF(MMAT.EQ.13.AND.ND.EQ.2) GOTO 190
226 IF(MMAT.EQ.14.AND.ND.LE.3) GOTO 190
227 IF(MMAT.EQ.15.AND.ND.LE.4) GOTO 190
232 C...Form hadrons from flavour content.
234 200 KFL1(JT)=KFLO(JT)
235 IF(ND.EQ.NP+NQ/2) GOTO 220
236 DO 210 I=N+NP+1,N+ND-NQ/2
237 JT=1+INT((NQ-1)*RLU_HIJING(0))
238 CALL LUKFDI_HIJING(KFL1(JT),0,KFL2,K(I,2))
239 IF(K(I,2).EQ.0) GOTO 190
244 IF(NQ.EQ.4.AND.RLU_HIJING(0).LT.PARJ(66)) JT=4
245 IF(JT.EQ.4.AND.ISIGN(1,KFL1(1)*(10-IABS(KFL1(1))))*
246 & ISIGN(1,KFL1(JT)*(10-IABS(KFL1(JT)))).GT.0) JT=3
249 CALL LUKFDI_HIJING(KFL1(1),KFL1(JT),KFLDMP,K(N+ND-NQ/2+1,2))
250 IF(K(N+ND-NQ/2+1,2).EQ.0) GOTO 190
251 IF(NQ.EQ.4) CALL LUKFDI_HIJING(KFL1(JT2),KFL1(JT3),KFLDMP,K(N+ND
253 IF(NQ.EQ.4.AND.K(N+ND,2).EQ.0) GOTO 190
255 C...Check that sum of decay product masses not too large.
262 P(I,5)=ULMASS_HIJING(K(I,2))
264 IF(PS+PARJ(64).GT.PV(1,5)) GOTO 190
266 C...Rescale energy to subtract off spectator quark mass.
267 ELSEIF((MMAT.EQ.31.OR.MMAT.EQ.33.OR.MMAT.EQ.44.OR.MMAT.EQ.45).
270 PQT=(P(N+NP,5)+PARJ(65))/PV(1,5)
272 P(N+NP,J)=PQT*PV(1,J)
273 240 PV(1,J)=(1.-PQT)*PV(1,J)
274 IF(PS+PARJ(64).GT.PV(1,5)) GOTO 150
278 C...Phase space factors imposed in W decay.
279 ELSEIF(MMAT.EQ.46) THEN
281 PSMC=ULMASS_HIJING(K(N+1,2))
283 PSMC=PSMC+ULMASS_HIJING(K(N+2,2))
284 IF(MAX(PS,PSMC)+PARJ(32).GT.PV(1,5)) GOTO 130
285 HR1=(P(N+1,5)/PV(1,5))**2
286 HR2=(P(N+2,5)/PV(1,5))**2
287 IF((1.-HR1-HR2)*(2.+HR1+HR2)*SQRT((1.-HR1-HR2)**2-4.*HR1*HR2).
288 & LT.2.*RLU_HIJING(0)) GOTO 130
291 C...Fully specified final state: check mass broadening effects.
293 IF(NP.GE.2.AND.PS+PARJ(64).GT.PV(1,5)) GOTO 150
297 C...Select W mass in decay Q -> W + q, without W propagator.
298 IF(MMAT.EQ.45.AND.MSTJ(25).LE.0) THEN
299 HLQ=(PARJ(32)/PV(1,5))**2
300 HUQ=(1.-(P(N+2,5)+PARJ(64))/PV(1,5))**2
301 HRQ=(P(N+2,5)/PV(1,5))**2
302 250 HW=HLQ+RLU_HIJING(0)*(HUQ-HLQ)
303 IF(HMEPS(HW).LT.RLU_HIJING(0)) GOTO 250
304 P(N+1,5)=PV(1,5)*SQRT(HW)
306 C...Ditto, including W propagator. Divide mass range into three regions.
307 ELSEIF(MMAT.EQ.45) THEN
308 HQW=(PV(1,5)/PMAS(24,1))**2
309 HLW=(PARJ(32)/PMAS(24,1))**2
310 HUW=((PV(1,5)-P(N+2,5)-PARJ(64))/PMAS(24,1))**2
311 HRQ=(P(N+2,5)/PV(1,5))**2
312 HG=PMAS(24,2)/PMAS(24,1)
313 HATL=ATAN((HLW-1.)/HG)
315 HMV1=HMEPS(HM/HQW)/((HM-1.)**2+HG**2)
317 HMV2=HMEPS(HM/HQW)/((HM-1.)**2+HG**2)
319 HSAV2=1./((HM-1.)**2+HG**2)
320 IF(HMV2.GT.HMV1.AND.HM-HG.GT.HLW) THEN
324 HMV=MIN(2.*HMV1,HMEPS(HM/HQW)/HG**2)
325 HM1=1.-SQRT(1./HMV-HG**2)
326 IF(HM1.GT.HLW.AND.HM1.LT.HM) THEN
328 ELSEIF(HMV2.LE.HMV1) THEN
329 HM=MAX(HLW,HM-MIN(0.1,1.-HM))
331 HATM=ATAN((HM-1.)/HG)
333 HWT2=HMV*(MIN(1.,HUW)-HM)
336 HATU=ATAN((HUW-1.)/HG)
341 C...Select mass region and W mass there. Accept according to weight.
342 270 HREG=RLU_HIJING(0)*(HWT1+HWT2+HWT3)
343 IF(HREG.LE.HWT1) THEN
344 HW=1.+HG*TAN(HATL+RLU_HIJING(0)*(HATM-HATL))
346 ELSEIF(HREG.LE.HWT1+HWT2) THEN
347 HW=HM+RLU_HIJING(0)*(MIN(1.,HUW)-HM)
348 HACC=HMEPS(HW/HQW)/((HW-1.)**2+HG**2)/HMV
350 HW=1.+HG*TAN(RLU_HIJING(0)*HATU)
351 HACC=HMEPS(HW/HQW)/HMP1
353 IF(HACC.LT.RLU_HIJING(0)) GOTO 270
354 P(N+1,5)=PMAS(24,1)*SQRT(HW)
357 C...Determine position of grandmother, number of sisters, Q -> W sign.
360 IF(MMAT.EQ.3.OR.MMAT.EQ.46) THEN
362 IF(IM.LT.0.OR.IM.GE.IP) IM=0
363 IF(IM.NE.0) KFAM=IABS(K(IM,2))
364 IF(IM.NE.0.AND.MMAT.EQ.3) THEN
365 DO 280 IL=MAX(IP-2,IM+1),MIN(IP+2,N)
366 280 IF(K(IL,3).EQ.IM) NM=NM+1
367 IF(NM.NE.2.OR.KFAM.LE.100.OR.MOD(KFAM,10).NE.1.OR.
368 & MOD(KFAM/1000,10).NE.0) NM=0
369 ELSEIF(IM.NE.0.AND.MMAT.EQ.46) THEN
370 MSGN=ISIGN(1,K(IM,2)*K(IP,2))
371 IF(KFAM.GT.100.AND.MOD(KFAM/1000,10).EQ.0) MSGN=
372 & MSGN*(-1)**MOD(KFAM/100,10)
376 C...Kinematics of one-particle decays.
383 C...Calculate maximum weight ND-particle decay.
387 PMAX=PV(1,5)-PS+P(N+ND,5)
391 PMIN=PMIN+P(N+IL+1,5)
392 300 WTMAX=WTMAX*PAWT(PMAX,PMIN,P(N+IL,5))
395 C...Find virtual gamma mass in Dalitz decay.
397 ELSEIF(MMAT.EQ.2) THEN
398 PMES=4.*PMAS(11,1)**2
399 PMRHO2=PMAS(131,1)**2
400 PGRHO2=PMAS(131,2)**2
401 320 PMST=PMES*(P(IP,5)**2/PMES)**RLU_HIJING(0)
402 WT=(1+0.5*PMES/PMST)*SQRT(MAX(0.,1.-PMES/PMST))*
403 & (1.-PMST/P(IP,5)**2)**3*(1.+PGRHO2/PMRHO2)/
404 & ((1.-PMST/PMRHO2)**2+PGRHO2/PMRHO2)
405 IF(WT.LT.RLU_HIJING(0)) GOTO 320
406 PV(2,5)=MAX(2.00001*PMAS(11,1),SQRT(PMST))
408 C...M-generator gives weight. If rejected, try again.
413 DO 340 IL2=IL1-1,1,-1
414 IF(RSAV.LE.RORD(IL2)) GOTO 350
415 340 RORD(IL2+1)=RORD(IL2)
420 PV(IL,5)=PV(IL+1,5)+P(N+IL,5)+(RORD(IL)-RORD(IL+1))*(PV(1,5)-PS)
421 360 WT=WT*PAWT(PV(IL,5),PV(IL+1,5),P(N+IL,5))
422 IF(WT.LT.RLU_HIJING(0)*WTMAX) GOTO 330
425 C...Perform two-particle decays in respective CM frame.
427 PA=PAWT(PV(IL,5),PV(IL+1,5),P(N+IL,5))
428 UE(3)=2.*RLU_HIJING(0)-1.
429 PHI=PARU(2)*RLU_HIJING(0)
430 UE(1)=SQRT(1.-UE(3)**2)*COS(PHI)
431 UE(2)=SQRT(1.-UE(3)**2)*SIN(PHI)
434 380 PV(IL+1,J)=-PA*UE(J)
435 P(N+IL,4)=SQRT(PA**2+P(N+IL,5)**2)
436 390 PV(IL+1,4)=SQRT(PA**2+PV(IL+1,5)**2)
438 C...Lorentz transform decay products to lab frame.
440 400 P(N+ND,J)=PV(ND,J)
443 410 BE(J)=PV(IL,J)/PV(IL,4)
446 BEP=BE(1)*P(I,1)+BE(2)*P(I,2)+BE(3)*P(I,3)
448 420 P(I,J)=P(I,J)+GA*(GA*BEP/(1.+GA)+P(I,4))*BE(J)
449 430 P(I,4)=GA*(P(I,4)+BEP)
451 C...Matrix elements for omega and phi decays.
453 WT=(P(N+1,5)*P(N+2,5)*P(N+3,5))**2-(P(N+1,5)*FOUR(N+2,N+3))**2
454 & -(P(N+2,5)*FOUR(N+1,N+3))**2-(P(N+3,5)*FOUR(N+1,N+2))**2
455 & +2.*FOUR(N+1,N+2)*FOUR(N+1,N+3)*FOUR(N+2,N+3)
456 IF(MAX(WT*WTCOR(9)/P(IP,5)**6,0.001).LT.RLU_HIJING(0)) GOTO 310
458 C...Matrix elements for pi0 or eta Dalitz decay to gamma e+ e-.
459 ELSEIF(MMAT.EQ.2) THEN
462 FOUR23=0.5*PMST-0.25*PMES
463 WT=(PMST-0.5*PMES)*(FOUR12**2+FOUR13**2)+
464 & PMES*(FOUR12*FOUR13+FOUR12**2+FOUR13**2)
465 IF(WT.LT.RLU_HIJING(0)*0.25*PMST*(P(IP,5)**2-PMST)**2) GOTO 370
467 C...Matrix element for S0 -> S1 + V1 -> S1 + S2 + S3 (S scalar,
468 C...V vector), of form cos**2(theta02) in V1 rest frame.
469 ELSEIF(MMAT.EQ.3.AND.NM.EQ.2) THEN
470 IF((P(IP,5)**2*FOUR(IM,N+1)-FOUR(IP,IM)*FOUR(IP,N+1))**2.LE.
471 & RLU_HIJING(0)*(FOUR(IP,IM)**2-(P(IP,5)*P(IM,5))**2)
472 $ *(FOUR(IP,N+1)**2-(P(IP,5)*P(N+1,5))**2)) GOTO 370
474 C...Matrix element for "onium" -> g + g + g or gamma + g + g.
475 ELSEIF(MMAT.EQ.4) THEN
476 HX1=2.*FOUR(IP,N+1)/P(IP,5)**2
477 HX2=2.*FOUR(IP,N+2)/P(IP,5)**2
478 HX3=2.*FOUR(IP,N+3)/P(IP,5)**2
479 WT=((1.-HX1)/(HX2*HX3))**2+((1.-HX2)/(HX1*HX3))**2+
480 & ((1.-HX3)/(HX1*HX2))**2
481 IF(WT.LT.2.*RLU_HIJING(0)) GOTO 310
482 IF(K(IP+1,2).EQ.22.AND.(1.-HX1)*P(IP,5)**2.LT.4.*PARJ(32)**2)
485 C...Effective matrix element for nu spectrum in tau -> nu + hadrons.
486 ELSEIF(MMAT.EQ.41) THEN
487 HX1=2.*FOUR(IP,N+1)/P(IP,5)**2
488 IF(8.*HX1*(3.-2.*HX1)/9..LT.RLU_HIJING(0)) GOTO 310
490 C...Matrix elements for weak decays (only semileptonic for c and b)
491 ELSEIF(MMAT.GE.42.AND.MMAT.LE.44.AND.ND.EQ.3) THEN
492 IF(MBST.EQ.0) WT=FOUR(IP,N+1)*FOUR(N+2,N+3)
493 IF(MBST.EQ.1) WT=P(IP,5)*P(N+1,4)*FOUR(N+2,N+3)
494 IF(WT.LT.RLU_HIJING(0)*P(IP,5)*PV(1,5)**3/WTCOR(10)) GOTO 310
495 ELSEIF(MMAT.GE.42.AND.MMAT.LE.44) THEN
499 440 P(N+NP+1,J)=P(N+NP+1,J)+P(IS,J)
500 IF(MBST.EQ.0) WT=FOUR(IP,N+1)*FOUR(N+2,N+NP+1)
501 IF(MBST.EQ.1) WT=P(IP,5)*P(N+1,4)*FOUR(N+2,N+NP+1)
502 IF(WT.LT.RLU_HIJING(0)*P(IP,5)*PV(1,5)**3/WTCOR(10)) GOTO 310
504 C...Angular distribution in W decay.
505 ELSEIF(MMAT.EQ.46.AND.MSGN.NE.0) THEN
506 IF(MSGN.GT.0) WT=FOUR(IM,N+1)*FOUR(N+2,IP+1)
507 IF(MSGN.LT.0) WT=FOUR(IM,N+2)*FOUR(N+1,IP+1)
508 IF(WT.LT.RLU_HIJING(0)*P(IM,5)**4/WTCOR(10)) GOTO 370
511 C...Scale back energy and reattach spectator.
514 450 PV(1,J)=PV(1,J)/(1.-PQT)
519 C...Low invariant mass for system with spectator quark gives particle,
520 C...not two jets. Readjust momenta accordingly.
521 IF((MMAT.EQ.31.OR.MMAT.EQ.45).AND.ND.EQ.3) THEN
523 PM2=ULMASS_HIJING(K(N+2,2))
525 PM3=ULMASS_HIJING(K(N+3,2))
526 IF(P(N+2,5)**2+P(N+3,5)**2+2.*FOUR(N+2,N+3).GE.
527 & (PARJ(32)+PM2+PM3)**2) GOTO 510
530 CALL LUKFDI_HIJING(KFTEMP,K(N+3,2),KFLDMP,K(N+2,2))
531 IF(K(N+2,2).EQ.0) GOTO 150
532 P(N+2,5)=ULMASS_HIJING(K(N+2,2))
538 ELSEIF(MMAT.EQ.44) THEN
540 PM3=ULMASS_HIJING(K(N+3,2))
542 PM4=ULMASS_HIJING(K(N+4,2))
543 IF(P(N+3,5)**2+P(N+4,5)**2+2.*FOUR(N+3,N+4).GE.
544 & (PARJ(32)+PM3+PM4)**2) GOTO 480
547 CALL LUKFDI_HIJING(KFTEMP,K(N+4,2),KFLDMP,K(N+3,2))
548 IF(K(N+3,2).EQ.0) GOTO 150
549 P(N+3,5)=ULMASS_HIJING(K(N+3,2))
551 460 P(N+3,J)=P(N+3,J)+P(N+4,J)
552 P(N+3,4)=SQRT(P(N+3,1)**2+P(N+3,2)**2+P(N+3,3)**2+P(N+3,5)**2)
553 HA=P(N+1,4)**2-P(N+2,4)**2
554 HB=HA-(P(N+1,5)**2-P(N+2,5)**2)
555 HC=(P(N+1,1)-P(N+2,1))**2+(P(N+1,2)-P(N+2,2))**2+
556 & (P(N+1,3)-P(N+2,3))**2
557 HD=(PV(1,4)-P(N+3,4))**2
558 HE=HA**2-2.*HD*(P(N+1,4)**2+P(N+2,4)**2)+HD**2
561 HH=(SQRT(HG**2+HE*HF)-HG)/(2.*HF)
563 PCOR=HH*(P(N+1,J)-P(N+2,J))
564 P(N+1,J)=P(N+1,J)+PCOR
565 470 P(N+2,J)=P(N+2,J)-PCOR
566 P(N+1,4)=SQRT(P(N+1,1)**2+P(N+1,2)**2+P(N+1,3)**2+P(N+1,5)**2)
567 P(N+2,4)=SQRT(P(N+2,1)**2+P(N+2,2)**2+P(N+2,3)**2+P(N+2,5)**2)
571 C...Check invariant mass of W jets. May give one particle or start over.
572 480 IF(MMAT.GE.42.AND.MMAT.LE.44.AND.IABS(K(N+1,2)).LT.10) THEN
573 PMR=SQRT(MAX(0.,P(N+1,5)**2+P(N+2,5)**2+2.*FOUR(N+1,N+2)))
575 PM1=ULMASS_HIJING(K(N+1,2))
577 PM2=ULMASS_HIJING(K(N+2,2))
578 IF(PMR.GT.PARJ(32)+PM1+PM2) GOTO 490
579 KFLDUM=INT(1.5+RLU_HIJING(0))
580 CALL LUKFDI_HIJING(K(N+1,2),-ISIGN(KFLDUM,K(N+1,2)),KFLDMP,KF1)
581 CALL LUKFDI_HIJING(K(N+2,2),-ISIGN(KFLDUM,K(N+2,2)),KFLDMP,KF2)
582 IF(KF1.EQ.0.OR.KF2.EQ.0) GOTO 150
583 PSM=ULMASS_HIJING(KF1)+ULMASS_HIJING(KF2)
584 IF(MMAT.EQ.42.AND.PMR.GT.PARJ(64)+PSM) GOTO 490
585 IF(MMAT.GE.43.AND.PMR.GT.0.2*PARJ(32)+PSM) GOTO 490
586 IF(ND.EQ.4.OR.KFA.EQ.15) GOTO 150
589 CALL LUKFDI_HIJING(KFTEMP,K(N+2,2),KFLDMP,K(N+1,2))
590 IF(K(N+1,2).EQ.0) GOTO 150
591 P(N+1,5)=ULMASS_HIJING(K(N+1,2))
601 C...Phase space decay of partons from W decay.
602 490 IF(MMAT.EQ.42.AND.IABS(K(N+1,2)).LT.10) THEN
608 PV(1,J)=P(N+1,J)+P(N+2,J)
609 500 P(N+1,J)=P(N+3,J)
616 PSQ=ULMASS_HIJING(KFLO(1))
618 PSQ=PSQ+ULMASS_HIJING(KFLO(2))
623 C...Boost back for rapidly moving particle.
627 520 BE(J)=P(IP,J)/P(IP,4)
630 BEP=BE(1)*P(I,1)+BE(2)*P(I,2)+BE(3)*P(I,3)
632 530 P(I,J)=P(I,J)+GA*(GA*BEP/(1.+GA)+P(I,4))*BE(J)
633 540 P(I,4)=GA*(P(I,4)+BEP)
636 C...Fill in position of decay vertex.
642 C...Set up for parton shower evolution from jets.
643 IF(MSTJ(23).GE.1.AND.MMAT.EQ.4.AND.K(NSAV+1,2).EQ.21) THEN
647 K(NSAV+1,4)=MSTU(5)*(NSAV+2)
648 K(NSAV+1,5)=MSTU(5)*(NSAV+3)
649 K(NSAV+2,4)=MSTU(5)*(NSAV+3)
650 K(NSAV+2,5)=MSTU(5)*(NSAV+1)
651 K(NSAV+3,4)=MSTU(5)*(NSAV+1)
652 K(NSAV+3,5)=MSTU(5)*(NSAV+2)
654 ELSEIF(MSTJ(23).GE.1.AND.MMAT.EQ.4) THEN
657 K(NSAV+2,4)=MSTU(5)*(NSAV+3)
658 K(NSAV+2,5)=MSTU(5)*(NSAV+3)
659 K(NSAV+3,4)=MSTU(5)*(NSAV+2)
660 K(NSAV+3,5)=MSTU(5)*(NSAV+2)
662 ELSEIF(MSTJ(23).GE.1.AND.(MMAT.EQ.32.OR.MMAT.EQ.44.OR.MMAT.EQ.46).
663 &AND.IABS(K(NSAV+1,2)).LE.10.AND.IABS(K(NSAV+2,2)).LE.10) THEN
666 K(NSAV+1,4)=MSTU(5)*(NSAV+2)
667 K(NSAV+1,5)=MSTU(5)*(NSAV+2)
668 K(NSAV+2,4)=MSTU(5)*(NSAV+1)
669 K(NSAV+2,5)=MSTU(5)*(NSAV+1)
671 ELSEIF(MSTJ(23).GE.1.AND.MMAT.EQ.33.AND.IABS(K(NSAV+2,2)).EQ.21)
676 KCP=LUCOMP_HIJING(K(NSAV+1,2))
677 KQP=KCHG(KCP,2)*ISIGN(1,K(NSAV+1,2))
680 K(NSAV+1,JCON)=MSTU(5)*(NSAV+2)
681 K(NSAV+2,9-JCON)=MSTU(5)*(NSAV+1)
682 K(NSAV+2,JCON)=MSTU(5)*(NSAV+3)
683 K(NSAV+3,9-JCON)=MSTU(5)*(NSAV+2)
685 ELSEIF(MSTJ(23).GE.1.AND.MMAT.EQ.33) THEN
688 K(NSAV+1,4)=MSTU(5)*(NSAV+3)
689 K(NSAV+1,5)=MSTU(5)*(NSAV+3)
690 K(NSAV+3,4)=MSTU(5)*(NSAV+1)
691 K(NSAV+3,5)=MSTU(5)*(NSAV+1)
695 C...Mark decayed particle.
696 IF(K(IP,1).EQ.5) K(IP,1)=15
697 IF(K(IP,1).LE.10) K(IP,1)=11