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Commit | Line | Data |
---|---|---|
e74335a4 | 1 | * $Id$ |
2 | ||
3 | C********************************************************************* | |
caf658ba | 4 | |
5 | FUNCTION PAWT(A,B,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) | |
8 | ELSE | |
9 | PAWT = 0 | |
10 | ENDIF | |
11 | RETURN | |
12 | END | |
13 | ||
e74335a4 | 14 | SUBROUTINE LUDECY_HIJING(IP) |
15 | ||
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), | |
22 | &WTCOR(10) | |
23 | DATA WTCOR/2.,5.,15.,60.,250.,1500.,1.2E4,1.2E5,150.,16./ | |
24 | ||
25 | C...Functions: momentum in two-particle decays, four-product and | |
26 | C...matrix element times phase space in weak decays. | |
caf658ba | 27 | |
e74335a4 | 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) | |
31 | ||
32 | C...Initial values. | |
33 | NTRY=0 | |
34 | NSAV=N | |
35 | KFA=IABS(K(IP,2)) | |
36 | KFS=ISIGN(1,K(IP,2)) | |
37 | KC=LUCOMP_HIJING(KFA) | |
38 | MSTJ(92)=0 | |
39 | ||
40 | C...Choose lifetime and determine decay vertex. | |
41 | IF(K(IP,1).EQ.5) THEN | |
42 | V(IP,5)=0. | |
43 | ELSEIF(K(IP,1).NE.4) THEN | |
44 | V(IP,5)=-PMAS(KC,4)*LOG(RLU_HIJING(0)) | |
45 | ENDIF | |
46 | DO 100 J=1,4 | |
47 | 100 VDCY(J)=V(IP,J)+V(IP,5)*P(IP,J)/P(IP,5) | |
48 | ||
49 | C...Determine whether decay allowed or not. | |
50 | MOUT=0 | |
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 | |
58 | ENDIF | |
59 | IF(MOUT.EQ.1.AND.K(IP,1).NE.5) THEN | |
60 | K(IP,1)=4 | |
61 | RETURN | |
62 | ENDIF | |
63 | ||
64 | C...Check existence of decay channels. Particle/antiparticle rules. | |
65 | KCA=KC | |
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 | |
69 | ENDIF | |
70 | IF(MDCY(KCA,2).LE.0.OR.MDCY(KCA,3).LE.0) THEN | |
71 | CALL LUERRM_HIJING(9 | |
72 | $ ,'(LUDECY_HIJING:) no decay channel defined') | |
73 | RETURN | |
74 | ENDIF | |
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 | |
77 | KFSP=1 | |
78 | KFSN=0 | |
79 | IF(RLU_HIJING(0).GT.0.5) KFS=-KFS | |
80 | ELSEIF(KFS.GT.0) THEN | |
81 | KFSP=1 | |
82 | KFSN=0 | |
83 | ELSE | |
84 | KFSP=0 | |
85 | KFSN=1 | |
86 | ENDIF | |
87 | ||
88 | C...Sum branching ratios of allowed decay channels. | |
89 | 110 NOPE=0 | |
90 | BRSU=0. | |
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 | |
95 | NOPE=NOPE+1 | |
96 | BRSU=BRSU+BRAT(IDL) | |
97 | 120 CONTINUE | |
98 | IF(NOPE.EQ.0) THEN | |
99 | CALL LUERRM_HIJING(2 | |
100 | $ ,'(LUDECY_HIJING:) all decay channels closed by user') | |
101 | RETURN | |
102 | ENDIF | |
103 | ||
104 | C...Select decay channel among allowed ones. | |
105 | 130 RBR=BRSU*RLU_HIJING(0) | |
106 | IDL=MDCY(KCA,2)-1 | |
107 | 140 IDL=IDL+1 | |
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 | |
113 | ELSE | |
114 | IDC=IDL | |
115 | RBR=RBR-BRAT(IDL) | |
116 | IF(IDL.LT.MDCY(KCA,2)+MDCY(KCA,3)-1.AND.RBR.GT.0.) GOTO 140 | |
117 | ENDIF | |
118 | ||
119 | C...Start readout of decay channel: matrix element, reset counters. | |
120 | MMAT=MDME(IDC,2) | |
121 | 150 NTRY=NTRY+1 | |
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 | |
126 | ENDIF | |
127 | I=N | |
128 | NP=0 | |
129 | NQ=0 | |
130 | MBST=0 | |
131 | IF(MMAT.GE.11.AND.MMAT.NE.46.AND.P(IP,4).GT.20.*P(IP,5)) MBST=1 | |
132 | DO 160 J=1,4 | |
133 | PV(1,J)=0. | |
134 | 160 IF(MBST.EQ.0) PV(1,J)=P(IP,J) | |
135 | IF(MBST.EQ.1) PV(1,4)=P(IP,5) | |
136 | PV(1,5)=P(IP,5) | |
137 | PS=0. | |
138 | PSQ=0. | |
139 | MREM=0 | |
140 | ||
141 | C...Read out decay products. Convert to standard flavour code. | |
142 | JTMAX=5 | |
143 | IF(MDME(IDC+1,2).EQ.101) JTMAX=10 | |
144 | DO 170 JT=1,JTMAX | |
145 | IF(JT.LE.5) KP=KFDP(IDC,JT) | |
146 | IF(JT.GE.6) KP=KFDP(IDC+1,JT-5) | |
147 | IF(KP.EQ.0) GOTO 170 | |
148 | KPA=IABS(KP) | |
149 | KCP=LUCOMP_HIJING(KPA) | |
150 | IF(KCHG(KCP,3).EQ.0.AND.KPA.NE.81.AND.KPA.NE.82) THEN | |
151 | KFP=KP | |
152 | ELSEIF(KPA.NE.81.AND.KPA.NE.82) THEN | |
153 | KFP=KFS*KP | |
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 | |
162 | $ ,KFP,KDUMP) | |
163 | IF(KFP.EQ.0) GOTO 150 | |
164 | MSTJ(93)=1 | |
165 | IF(PV(1,5).LT.PARJ(32)+2.*ULMASS_HIJING(KFP)) GOTO 150 | |
166 | ELSEIF(KP.EQ.-82) THEN | |
167 | KFP=-KFP | |
168 | IF(IABS(KFP).GT.10) KFP=KFP+ISIGN(10000,KFP) | |
169 | ENDIF | |
170 | IF(KPA.EQ.81.OR.KPA.EQ.82) KCP=LUCOMP_HIJING(KFP) | |
171 | ||
172 | C...Add decay product to event record or to quark flavour list. | |
173 | KFPA=IABS(KFP) | |
174 | KQP=KCHG(KCP,2) | |
175 | IF(MMAT.GE.11.AND.MMAT.LE.30.AND.KQP.NE.0) THEN | |
176 | NQ=NQ+1 | |
177 | KFLO(NQ)=KFP | |
178 | MSTJ(93)=2 | |
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) | |
181 | &THEN | |
182 | NQ=NQ-1 | |
183 | PS=PS-P(I,5) | |
184 | K(I,1)=1 | |
185 | KFI=K(I,2) | |
186 | CALL LUKFDI_HIJING(KFP,KFI,KFLDMP,K(I,2)) | |
187 | IF(K(I,2).EQ.0) GOTO 150 | |
188 | MSTJ(93)=1 | |
189 | P(I,5)=ULMASS_HIJING(K(I,2)) | |
190 | PS=PS+P(I,5) | |
191 | ELSE | |
192 | I=I+1 | |
193 | NP=NP+1 | |
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 | |
196 | K(I,1)=1+MOD(NQ,2) | |
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 | |
199 | K(I,2)=KFP | |
200 | K(I,3)=IP | |
201 | K(I,4)=0 | |
202 | K(I,5)=0 | |
203 | P(I,5)=ULMASS_HIJING(KFP) | |
204 | IF(MMAT.EQ.45.AND.KFPA.EQ.89) P(I,5)=PARJ(32) | |
205 | PS=PS+P(I,5) | |
206 | ENDIF | |
207 | 170 CONTINUE | |
208 | ||
209 | C...Choose decay multiplicity in phase space model. | |
210 | 180 IF(MMAT.GE.11.AND.MMAT.LE.30) THEN | |
211 | PSP=PS | |
212 | CNDE=PARJ(61)*LOG(MAX((PV(1,5)-PS-PSQ)/PARJ(62),1.1)) | |
213 | IF(MMAT.EQ.12) CNDE=CNDE+PARJ(63) | |
214 | 190 NTRY=NTRY+1 | |
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 | |
219 | ENDIF | |
220 | IF(MMAT.LE.20) THEN | |
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 | |
228 | ELSE | |
229 | ND=MMAT-20 | |
230 | ENDIF | |
231 | ||
232 | C...Form hadrons from flavour content. | |
233 | DO 200 JT=1,4 | |
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 | |
240 | 210 KFL1(JT)=-KFL2 | |
241 | 220 JT=2 | |
242 | JT2=3 | |
243 | JT3=4 | |
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 | |
247 | IF(JT.EQ.3) JT2=2 | |
248 | IF(JT.EQ.4) JT3=2 | |
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 | |
252 | $ ,2)) | |
253 | IF(NQ.EQ.4.AND.K(N+ND,2).EQ.0) GOTO 190 | |
254 | ||
255 | C...Check that sum of decay product masses not too large. | |
256 | PS=PSP | |
257 | DO 230 I=N+NP+1,N+ND | |
258 | K(I,1)=1 | |
259 | K(I,3)=IP | |
260 | K(I,4)=0 | |
261 | K(I,5)=0 | |
262 | P(I,5)=ULMASS_HIJING(K(I,2)) | |
263 | 230 PS=PS+P(I,5) | |
264 | IF(PS+PARJ(64).GT.PV(1,5)) GOTO 190 | |
265 | ||
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). | |
268 | &AND.NP.GE.3) THEN | |
269 | PS=PS-P(N+NP,5) | |
270 | PQT=(P(N+NP,5)+PARJ(65))/PV(1,5) | |
271 | DO 240 J=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 | |
275 | ND=NP-1 | |
276 | MREM=1 | |
277 | ||
278 | C...Phase space factors imposed in W decay. | |
279 | ELSEIF(MMAT.EQ.46) THEN | |
280 | MSTJ(93)=1 | |
281 | PSMC=ULMASS_HIJING(K(N+1,2)) | |
282 | MSTJ(93)=1 | |
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 | |
289 | ND=NP | |
290 | ||
291 | C...Fully specified final state: check mass broadening effects. | |
292 | ELSE | |
293 | IF(NP.GE.2.AND.PS+PARJ(64).GT.PV(1,5)) GOTO 150 | |
294 | ND=NP | |
295 | ENDIF | |
296 | ||
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) | |
305 | ||
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) | |
314 | HM=MIN(1.,HUW-0.001) | |
315 | HMV1=HMEPS(HM/HQW)/((HM-1.)**2+HG**2) | |
316 | 260 HM=HM-HG | |
317 | HMV2=HMEPS(HM/HQW)/((HM-1.)**2+HG**2) | |
318 | HSAV1=HMEPS(HM/HQW) | |
319 | HSAV2=1./((HM-1.)**2+HG**2) | |
320 | IF(HMV2.GT.HMV1.AND.HM-HG.GT.HLW) THEN | |
321 | HMV1=HMV2 | |
322 | GOTO 260 | |
323 | ENDIF | |
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 | |
327 | HM=HM1 | |
328 | ELSEIF(HMV2.LE.HMV1) THEN | |
329 | HM=MAX(HLW,HM-MIN(0.1,1.-HM)) | |
330 | ENDIF | |
331 | HATM=ATAN((HM-1.)/HG) | |
332 | HWT1=(HATM-HATL)/HG | |
333 | HWT2=HMV*(MIN(1.,HUW)-HM) | |
334 | HWT3=0. | |
335 | IF(HUW.GT.1.) THEN | |
336 | HATU=ATAN((HUW-1.)/HG) | |
337 | HMP1=HMEPS(1./HQW) | |
338 | HWT3=HMP1*HATU/HG | |
339 | ENDIF | |
340 | ||
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)) | |
345 | HACC=HMEPS(HW/HQW) | |
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 | |
349 | ELSE | |
350 | HW=1.+HG*TAN(RLU_HIJING(0)*HATU) | |
351 | HACC=HMEPS(HW/HQW)/HMP1 | |
352 | ENDIF | |
353 | IF(HACC.LT.RLU_HIJING(0)) GOTO 270 | |
354 | P(N+1,5)=PMAS(24,1)*SQRT(HW) | |
355 | ENDIF | |
356 | ||
357 | C...Determine position of grandmother, number of sisters, Q -> W sign. | |
358 | NM=0 | |
359 | MSGN=0 | |
360 | IF(MMAT.EQ.3.OR.MMAT.EQ.46) THEN | |
361 | IM=K(IP,3) | |
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) | |
373 | ENDIF | |
374 | ENDIF | |
375 | ||
376 | C...Kinematics of one-particle decays. | |
377 | IF(ND.EQ.1) THEN | |
378 | DO 290 J=1,4 | |
379 | 290 P(N+1,J)=P(IP,J) | |
380 | GOTO 510 | |
381 | ENDIF | |
382 | ||
383 | C...Calculate maximum weight ND-particle decay. | |
384 | PV(ND,5)=P(N+ND,5) | |
385 | IF(ND.GE.3) THEN | |
386 | WTMAX=1./WTCOR(ND-2) | |
387 | PMAX=PV(1,5)-PS+P(N+ND,5) | |
388 | PMIN=0. | |
389 | DO 300 IL=ND-1,1,-1 | |
390 | PMAX=PMAX+P(N+IL,5) | |
391 | PMIN=PMIN+P(N+IL+1,5) | |
392 | 300 WTMAX=WTMAX*PAWT(PMAX,PMIN,P(N+IL,5)) | |
393 | ENDIF | |
394 | ||
395 | C...Find virtual gamma mass in Dalitz decay. | |
396 | 310 IF(ND.EQ.2) THEN | |
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)) | |
407 | ||
408 | C...M-generator gives weight. If rejected, try again. | |
409 | ELSE | |
410 | 330 RORD(1)=1. | |
411 | DO 350 IL1=2,ND-1 | |
412 | RSAV=RLU_HIJING(0) | |
413 | DO 340 IL2=IL1-1,1,-1 | |
414 | IF(RSAV.LE.RORD(IL2)) GOTO 350 | |
415 | 340 RORD(IL2+1)=RORD(IL2) | |
416 | 350 RORD(IL2+1)=RSAV | |
417 | RORD(ND)=0. | |
418 | WT=1. | |
419 | DO 360 IL=ND-1,1,-1 | |
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 | |
423 | ENDIF | |
424 | ||
425 | C...Perform two-particle decays in respective CM frame. | |
426 | 370 DO 390 IL=1,ND-1 | |
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) | |
432 | DO 380 J=1,3 | |
433 | P(N+IL,J)=PA*UE(J) | |
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) | |
437 | ||
438 | C...Lorentz transform decay products to lab frame. | |
439 | DO 400 J=1,4 | |
440 | 400 P(N+ND,J)=PV(ND,J) | |
441 | DO 430 IL=ND-1,1,-1 | |
442 | DO 410 J=1,3 | |
443 | 410 BE(J)=PV(IL,J)/PV(IL,4) | |
444 | GA=PV(IL,4)/PV(IL,5) | |
445 | DO 430 I=N+IL,N+ND | |
446 | BEP=BE(1)*P(I,1)+BE(2)*P(I,2)+BE(3)*P(I,3) | |
447 | DO 420 J=1,3 | |
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) | |
450 | ||
451 | C...Matrix elements for omega and phi decays. | |
452 | IF(MMAT.EQ.1) THEN | |
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 | |
457 | ||
458 | C...Matrix elements for pi0 or eta Dalitz decay to gamma e+ e-. | |
459 | ELSEIF(MMAT.EQ.2) THEN | |
460 | FOUR12=FOUR(N+1,N+2) | |
461 | FOUR13=FOUR(N+1,N+3) | |
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 | |
466 | ||
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 | |
473 | ||
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) | |
483 | & GOTO 310 | |
484 | ||
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 | |
489 | ||
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 | |
496 | DO 440 J=1,4 | |
497 | P(N+NP+1,J)=0. | |
498 | DO 440 IS=N+3,N+NP | |
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 | |
503 | ||
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 | |
509 | ENDIF | |
510 | ||
511 | C...Scale back energy and reattach spectator. | |
512 | IF(MREM.EQ.1) THEN | |
513 | DO 450 J=1,5 | |
514 | 450 PV(1,J)=PV(1,J)/(1.-PQT) | |
515 | ND=ND+1 | |
516 | MREM=0 | |
517 | ENDIF | |
518 | ||
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 | |
522 | MSTJ(93)=1 | |
523 | PM2=ULMASS_HIJING(K(N+2,2)) | |
524 | MSTJ(93)=1 | |
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 | |
528 | K(N+2,1)=1 | |
529 | KFTEMP=K(N+2,2) | |
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)) | |
533 | PS=P(N+1,5)+P(N+2,5) | |
534 | PV(2,5)=P(N+2,5) | |
535 | MMAT=0 | |
536 | ND=2 | |
537 | GOTO 370 | |
538 | ELSEIF(MMAT.EQ.44) THEN | |
539 | MSTJ(93)=1 | |
540 | PM3=ULMASS_HIJING(K(N+3,2)) | |
541 | MSTJ(93)=1 | |
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 | |
545 | K(N+3,1)=1 | |
546 | KFTEMP=K(N+3,2) | |
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)) | |
550 | DO 460 J=1,3 | |
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 | |
559 | HF=HD*HC-HB**2 | |
560 | HG=HD*HC-HA*HB | |
561 | HH=(SQRT(HG**2+HE*HF)-HG)/(2.*HF) | |
562 | DO 470 J=1,3 | |
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) | |
568 | ND=ND-1 | |
569 | ENDIF | |
570 | ||
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))) | |
574 | MSTJ(93)=1 | |
575 | PM1=ULMASS_HIJING(K(N+1,2)) | |
576 | MSTJ(93)=1 | |
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 | |
587 | K(N+1,1)=1 | |
588 | KFTEMP=K(N+1,2) | |
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)) | |
592 | K(N+2,2)=K(N+3,2) | |
593 | P(N+2,5)=P(N+3,5) | |
594 | PS=P(N+1,5)+P(N+2,5) | |
595 | PV(2,5)=P(N+3,5) | |
596 | MMAT=0 | |
597 | ND=2 | |
598 | GOTO 370 | |
599 | ENDIF | |
600 | ||
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 | |
603 | KFLO(1)=K(N+1,2) | |
604 | KFLO(2)=K(N+2,2) | |
605 | K(N+1,1)=K(N+3,1) | |
606 | K(N+1,2)=K(N+3,2) | |
607 | DO 500 J=1,5 | |
608 | PV(1,J)=P(N+1,J)+P(N+2,J) | |
609 | 500 P(N+1,J)=P(N+3,J) | |
610 | PV(1,5)=PMR | |
611 | N=N+1 | |
612 | NP=0 | |
613 | NQ=2 | |
614 | PS=0. | |
615 | MSTJ(93)=2 | |
616 | PSQ=ULMASS_HIJING(KFLO(1)) | |
617 | MSTJ(93)=2 | |
618 | PSQ=PSQ+ULMASS_HIJING(KFLO(2)) | |
619 | MMAT=11 | |
620 | GOTO 180 | |
621 | ENDIF | |
622 | ||
623 | C...Boost back for rapidly moving particle. | |
624 | 510 N=N+ND | |
625 | IF(MBST.EQ.1) THEN | |
626 | DO 520 J=1,3 | |
627 | 520 BE(J)=P(IP,J)/P(IP,4) | |
628 | GA=P(IP,4)/P(IP,5) | |
629 | DO 540 I=NSAV+1,N | |
630 | BEP=BE(1)*P(I,1)+BE(2)*P(I,2)+BE(3)*P(I,3) | |
631 | DO 530 J=1,3 | |
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) | |
634 | ENDIF | |
635 | ||
636 | C...Fill in position of decay vertex. | |
637 | DO 560 I=NSAV+1,N | |
638 | DO 550 J=1,4 | |
639 | 550 V(I,J)=VDCY(J) | |
640 | 560 V(I,5)=0. | |
641 | ||
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 | |
644 | K(NSAV+1,1)=3 | |
645 | K(NSAV+2,1)=3 | |
646 | K(NSAV+3,1)=3 | |
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) | |
653 | MSTJ(92)=-(NSAV+1) | |
654 | ELSEIF(MSTJ(23).GE.1.AND.MMAT.EQ.4) THEN | |
655 | K(NSAV+2,1)=3 | |
656 | K(NSAV+3,1)=3 | |
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) | |
661 | MSTJ(92)=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 | |
664 | K(NSAV+1,1)=3 | |
665 | K(NSAV+2,1)=3 | |
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) | |
670 | MSTJ(92)=NSAV+1 | |
671 | ELSEIF(MSTJ(23).GE.1.AND.MMAT.EQ.33.AND.IABS(K(NSAV+2,2)).EQ.21) | |
672 | &THEN | |
673 | K(NSAV+1,1)=3 | |
674 | K(NSAV+2,1)=3 | |
675 | K(NSAV+3,1)=3 | |
676 | KCP=LUCOMP_HIJING(K(NSAV+1,2)) | |
677 | KQP=KCHG(KCP,2)*ISIGN(1,K(NSAV+1,2)) | |
678 | JCON=4 | |
679 | IF(KQP.LT.0) JCON=5 | |
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) | |
684 | MSTJ(92)=NSAV+1 | |
685 | ELSEIF(MSTJ(23).GE.1.AND.MMAT.EQ.33) THEN | |
686 | K(NSAV+1,1)=3 | |
687 | K(NSAV+3,1)=3 | |
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) | |
692 | MSTJ(92)=NSAV+1 | |
693 | ENDIF | |
694 | ||
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 | |
698 | K(IP,4)=NSAV+1 | |
699 | K(IP,5)=N | |
700 | ||
701 | RETURN | |
702 | END |