3 C Nothing important has been changed here. A few 'garbage' has been
4 C cleaned up here, like common block HIJJET3 for the sea quark strings
5 C which were originally created to implement the DPM scheme which
6 C later was abadoned in the final version. The lines which operate
7 C on these data are also deleted in the program.
11 C There are some changes in the program: subroutine HARDJET is now
12 C consolidated with HIJHRD. HARDJET is used to re-initiate PYTHIA
13 C for the triggered hard processes. Now that is done altogether
14 C with other normal hard processes in modified JETINI. In the new
15 C version one calls JETINI every time one calls HIJHRD. In the new
16 C version the effect of the isospin of the nucleon on hard processes,
17 C especially direct photons is correctly considered.
18 C For A+A collisions, one has to initilize pythia
19 C separately for each type of collisions, pp, pn,np and nn,
20 C or hp and hn for hA collisions. In JETINI we use the following
21 C catalogue for different types of collisions:
23 C h+A: h+p (I_TYPE=1), h+n (I_TYPE=2)
24 C A+h: p+h (I_TYPE=1), n+h (I_TYPE=2)
25 C A+A: p+p (I_TYPE=1), p+n (I_TYPE=2), n+p (I_TYPE=3), n+n (I_TYPE=4)
26 C*****************************************************************
30 C Last modification on January 5, 1998. Two misstakes are corrected in
31 C function G. A Misstake in the subroutine Parton is also corrected.
32 C (These are pointed out by Ysushi Nara).
35 C Last modifcation on April 10, 1996. To conduct final
36 C state radiation, PYTHIA reorganize the two scattered
37 C partons and their final momenta will be a little
38 C different. The summed total momenta of the partons
39 C from the final state radiation are stored in HINT1(26-29)
40 C and HINT1(36-39) which are little different from
41 C HINT1(21-24) and HINT1(41-44).
45 C Last modfication on September 11, 1995. When HIJING and
46 C PYTHIA are initialized, the shadowing is evaluated at
47 C b=0 which is the maximum. This will cause overestimate
48 C of shadowing for peripheral interactions. To correct this
49 C problem, shadowing is set to zero when initializing. Then
50 C use these maximum cross section without shadowing as a
51 C normalization of the Monte Carlo. This however increase
52 C the computing time. IHNT2(16) is used to indicate whether
53 C the sturcture function is called for (IHNT2(16)=1) initialization
54 C or for (IHNT2(16)=0)normal collisions simulation
56 C Last modification on Aagust 28, 1994. Two bugs associate
57 C with the impact parameter dependence of the shadowing is
61 c Last modification on October 14, 1994. One bug is corrected
62 c in the direct photon production option in subroutine
63 C HIJHRD.( this problem was reported by Jim Carroll and Mike Beddo).
64 C Another bug associated with keeping the decay history
65 C in the particle information is also corrected.(this problem
66 C was reported by Matt Bloomer)
69 C Last modification on July 15, 1994. The option to trig on
70 C heavy quark production (charm IHPR2(18)=0 or beauty IHPR2(18)=1)
71 C is added. To do this, set IHPR2(3)=3. For inclusive production,
72 C one should reset HIPR1(10)=0.0. One can also trig larger pt
73 C QQbar production by giving HIPR1(10) a nonvanishing value.
74 C The mass of the heavy quark in the calculation of the cross
75 C section (HINT1(59)--HINT1(65)) is given by HIPR1(7) (the
76 C default is the charm mass D=1.5). We also include a separate
77 C K-factor for heavy quark and direct photon production by
80 C Last modification on May 24, 1994. The option to
81 C retain the information of all particles including those
82 C who have decayed is IHPR(21)=1 (default=0). KATT(I,3) is
83 C added to contain the line number of the parent particle
84 C of the current line which is produced via a decay.
85 C KATT(I,4) is the status number of the particle: 11=particle
86 C which has decayed; 1=finally produced particle.
89 C Last modification on May 24, 1994( in HIJSFT when valence quark
90 C is quenched, the following error is corrected. 1.2*IHNT2(1) -->
91 C 1.2*IHNT2(1)**0.333333, 1.2*IHNT2(3) -->1.2*IHNT(3)**0.333333)
94 C Last modification on March 16, 1994 (heavy flavor production
95 C processes MSUB(81)=1 MSUB(82)=1 have been switched on,
96 C charm production is the default, B-quark option is
97 C IHPR2(18), when it is switched on, charm quark is
101 C Last modification on March 23, 1994 (an error is corrected
102 C in the impact parameter dependence of the jet cross section)
104 C Last modification Oct. 1993 to comply with non-vax
107 C*********************************************
108 C LAST MODIFICATION April 5, 1991
109 CQUARK DISTRIBUTIOIN (1-X)**A/(X**2+C**2/S)**B
110 C(A=HIPR1(44),B=HIPR1(46),C=HIPR1(45))
111 C STRING FLIP, VENUS OPTION IHPR2(15)=1,IN WHICH ONE CAN HAVE ONE AND
112 C TWO COLOR CHANGES, (1-W)**2,W*(1-W),W*(1-W),AND W*2, W=HIPR1(18),
113 C AMONG PT DISTRIBUTION OF SEA QUARKS IS CONTROLLED BY HIPR1(42)
115 C gluon jets can form a single string system
117 C initial state radiation is included
119 C all QCD subprocesses are included
121 c direct particles production is included(currently only direct
124 C Effect of high P_T trigger bias on multiple jets distribution
126 C******************************************************************
128 C Heavy Ion Jet INteraction Generator *
130 C X. N. Wang and M. Gyulassy *
131 C Lawrence Berkeley Laboratory *
133 C******************************************************************
135 C******************************************************************
136 C NFP(K,1),NFP(K,2)=flavor of q and di-q, NFP(K,3)=present ID of *
137 C proj, NFP(K,4) original ID of proj. NFP(K,5)=colli status(0=no,*
138 C 1=elastic,2=the diffrac one in single-diffrac,3= excited string.*
139 C |NFP(K,6)| is the total # of jet production, if NFP(K,6)<0 it *
140 C can not produce jet anymore. NFP(K,10)=valence quarks scattering*
141 C (0=has not been,1=is going to be, -1=has already been scattered *
142 C NFP(k,11) total number of interactions this proj has suffered *
143 C PP(K,1)=PX,PP(K,2)=PY,PP(K,3)=PZ,PP(K,4)=E,PP(K,5)=M(invariant *
144 C mass), PP(K,6,7),PP(K,8,9)=transverse momentum of quark and *
145 C diquark,PP(K,10)=PT of the hard scattering between the valence *
146 C quarks; PP(K,14,15)=the mass of quark,diquark. *
147 C******************************************************************
149 C****************************************************************
153 C****************************************************************
154 SUBROUTINE HIJING(FRAME,BMIN0,BMAX0)
156 DIMENSION SCIP(300,300),RNIP(300,300),SJIP(300,300),JTP(3),
157 & IPCOL(90000),ITCOL(90000)
159 #include "hiparnt.inc"
161 #include "hijcrdn.inc"
162 #include "himain1.inc"
163 #include "himain2.inc"
164 #include "histrng.inc"
165 #include "hijjet1.inc"
166 #include "hijjet2.inc"
167 #include "hijjet4.inc"
169 #include "lujets_hijing.inc"
170 #include "ludat1_hijing.inc"
173 BMAX=MIN(BMAX0,HIPR1(34)+HIPR1(35))
175 IF(IHNT2(1).LE.1 .AND. IHNT2(3).LE.1) THEN
177 BMAX=2.5*SQRT(HIPR1(31)*0.1/HIPR1(40))
179 C ********HIPR1(31) is in mb =0.1fm**2
180 C*******THE FOLLOWING IS TO SELECT THE COORDINATIONS OF NUCLEONS
181 C BOTH IN PROJECTILE AND TARGET NUCLEAR( in fm)
186 IF(IHNT2(1).LE.1) GO TO 14
192 C ********choose theta from uniform cos(theta) distr
193 PHI=RLU_HIJING(0)*2.0*HIPR1(40)
194 C ********choose phi form uniform phi distr 0 to 2*pi
195 YP(1,KP)=R*SX*COS(PHI)
196 YP(2,KP)=R*SX*SIN(PHI)
198 IF(HIPR1(29).EQ.0.0) GO TO 10
200 DNBP1=(YP(1,KP)-YP(1,KP2))**2
201 DNBP2=(YP(2,KP)-YP(2,KP2))**2
202 DNBP3=(YP(3,KP)-YP(3,KP2))**2
203 DNBP=DNBP1+DNBP2+DNBP3
204 IF(DNBP.LT.HIPR1(29)*HIPR1(29)) GO TO 5
205 C ********two neighbors cannot be closer than
211 IF(YP(3,I).GT.YP(3,J)) GO TO 12
223 C******************************
227 IF(IHNT2(3).LE.1) GO TO 24
233 C ********choose theta from uniform cos(theta) distr
234 PHI=RLU_HIJING(0)*2.0*HIPR1(40)
235 C ********chose phi form uniform phi distr 0 to 2*pi
236 YT(1,KT)=R*SX*COS(PHI)
237 YT(2,KT)=R*SX*SIN(PHI)
239 IF(HIPR1(29).EQ.0.0) GO TO 20
241 DNBT1=(YT(1,KT)-YT(1,KT2))**2
242 DNBT2=(YT(2,KT)-YT(2,KT2))**2
243 DNBT3=(YT(3,KT)-YT(3,KT2))**2
244 DNBT=DNBT1+DNBT2+DNBT3
245 IF(DNBT.LT.HIPR1(29)*HIPR1(29)) GO TO 15
246 C ********two neighbors cannot be closer than
252 IF(YT(3,I).LT.YT(3,J)) GO TO 22
264 C********************
269 WRITE(6,*) 'infinite loop happened in HIJING'
278 C ********Initialize for a new event
288 C**** BB IS THE ABSOLUTE VALUE OF IMPACT PARAMETER,BB**2 IS
289 C RANDOMLY GENERATED AND ITS ORIENTATION IS RANDOMLY SET
290 C BY THE ANGLE PHI FOR EACH COLLISION.******************
292 BB=SQRT(BMIN**2+RLU_HIJING(0)*(BMAX**2-BMIN**2))
293 PHI=2.0*HIPR1(40)*RLU_HIJING(0)
302 B2=(YP(1,JP)+BBX-YT(1,JT))**2+(YP(2,JP)+BBY-YT(2,JT))**2
303 R2=B2*HIPR1(40)/HIPR1(31)/0.1
304 C ********mb=0.1*fm, YP is in fm,HIPR1(31) is in mb
305 RRB1=MIN((YP(1,JP)**2+YP(2,JP)**2)
306 & /1.2**2/REAL(IHNT2(1))**0.6666667,1.0)
307 RRB2=MIN((YT(1,JT)**2+YT(2,JT)**2)
308 & /1.2**2/REAL(IHNT2(3))**0.6666667,1.0)
309 APHX1=HIPR1(6)*4.0/3.0*(IHNT2(1)**0.3333333-1.0)
311 APHX2=HIPR1(6)*4.0/3.0*(IHNT2(3)**0.3333333-1.0)
313 HINT1(18)=HINT1(14)-APHX1*HINT1(15)
314 & -APHX2*HINT1(16)+APHX1*APHX2*HINT1(17)
315 IF(IHPR2(14).EQ.0.OR.
316 & (IHNT2(1).EQ.1.AND.IHNT2(3).EQ.1)) THEN
317 GS=1.0-EXP(-(HIPR1(30)+HINT1(18))*ROMG(R2)/HIPR1(31))
319 IF(RANTOT.GT.GS) GO TO 70
322 GSTOT_0=2.0*(1.0-EXP(-(HIPR1(30)+HINT1(18))
323 & /HIPR1(31)/2.0*ROMG(0.0)))
325 GS=1.0-EXP(-(HIPR1(30)+HINT1(18))/HIPR1(31)*ROMG(R2))
326 GSTOT=2.0*(1.0-SQRT(1.0-GS))
327 RANTOT=RLU_HIJING(0)*GSTOT_0
328 IF(RANTOT.GT.GSTOT) GO TO 70
329 IF(RANTOT.GT.GS) THEN
332 C ********perform elastic collisions
336 SJIP(JP,JT)=HINT1(18)
341 C ********total number interactions proj and targ has
346 & (IHNT2(1).EQ.1.AND.IHNT2(3).EQ.1)) GO TO 60
351 C ********At large impact parameter, there maybe no
352 C interaction at all. For NN collision
353 C repeat the event until interaction happens
355 IF(IHPR2(3).NE.0) THEN
356 NHARD=1+INT(RLU_HIJING(0)*(NCOLT-1)+0.5)
357 NHARD=MIN(NHARD,NCOLT)
362 IF(IHPR2(9).EQ.1) THEN
363 NMINI=1+INT(RLU_HIJING(0)*(NCOLT-1)+0.5)
364 NMINI=MIN(NMINI,NCOLT)
368 C ********Specifying the location of the hard and
369 C minijet if they are enforced by user
373 IF(SCIP(JP,JT).EQ.-1.0) GO TO 200
374 NFP(JP,11)=NFP(JP,11)+1
375 NFT(JT,11)=NFT(JT,11)+1
376 IF(NFP(JP,5).LE.1 .AND. NFT(JT,5).GT.1) THEN
379 ELSE IF(NFP(JP,5).GT.1 .AND. NFT(JT,5).LE.1) THEN
382 ELSE IF(NFP(JP,5).LE.1 .AND. NFT(JT,5).LE.1) THEN
386 ELSE IF(NFP(JP,5).GT.1 .AND. NFT(JT,5).GT.1) THEN
392 C*****************************************************************
393 IF(IHPR2(8).EQ.0 .AND. IHPR2(3).EQ.0) GO TO 160
394 C ********When IHPR2(8)=0 no jets are produced
395 IF(NFP(JP,6).LT.0 .OR. NFT(JT,6).LT.0) GO TO 160
396 C ********jets can not be produced for (JP,JT)
397 C because not enough energy avaible for
400 HINT1(18)=SJIP(JP,JT)
401 TT=ROMG(R2)*HINT1(18)/HIPR1(31)
402 TTS=HIPR1(30)*ROMG(R2)/HIPR1(31)
404 IF(IHPR2(3).NE.0 .AND. JP.EQ.JPHARD .AND. JT.EQ.JTHARD) THEN
406 CALL HIJHRD(JP,JT,0,JFLG,0)
416 IF(ABS(HINT1(46)).GT.HIPR1(11).AND.JFLG.EQ.2) NFP(JP,7)=1
417 IF(ABS(HINT1(56)).GT.HIPR1(11).AND.JFLG.EQ.2) NFT(JT,7)=1
418 IF(MAX(ABS(HINT1(46)),ABS(HINT1(56))).GT.HIPR1(11).AND.
419 & JFLG.GE.3) IASG(NSG,3)=1
423 HINT1(20+I05)=HINT1(40+I05)
424 HINT1(30+I05)=HINT1(50+I05)
427 IF(IHPR2(8).EQ.0) GO TO 160
428 RRB1=MIN((YP(1,JP)**2+YP(2,JP)**2)/1.2**2
429 & /REAL(IHNT2(1))**0.6666667,1.0)
430 RRB2=MIN((YT(1,JT)**2+YT(2,JT)**2)/1.2**2
431 & /REAL(IHNT2(3))**0.6666667,1.0)
432 APHX1=HIPR1(6)*4.0/3.0*(IHNT2(1)**0.3333333-1.0)
434 APHX2=HIPR1(6)*4.0/3.0*(IHNT2(3)**0.3333333-1.0)
436 HINT1(65)=HINT1(61)-APHX1*HINT1(62)
437 & -APHX2*HINT1(63)+APHX1*APHX2*HINT1(64)
438 TTRIG=ROMG(R2)*HINT1(65)/HIPR1(31)
440 C ********subtract the trigger jet from total number
441 C of jet production to be done since it has
442 C already been produced here
443 XR1=-ALOG(EXP(-TTRIG)+RLU_HIJING(0)*(1.0-EXP(-TTRIG)))
445 XR1=XR1-ALOG(RLU_HIJING(0))
446 IF(XR1.LT.TTRIG) GO TO 106
449 XR=XR-ALOG(RLU_HIJING(0))
450 IF(XR.LT.TT-TTRIG) GO TO 107
454 C ********create a hard interaction with specified P_T
456 IF(IHPR2(9).EQ.1.AND.JP.EQ.JPMINI.AND.JT.EQ.JTMINI) GO TO 110
457 C ********create at least one pair of mini jets
460 IF(IHPR2(8).GT.0 .AND.RNIP(JP,JT).LT.EXP(-TT)*
461 & (1.0-EXP(-TTS))) GO TO 160
462 C ********this is the probability for no jet production
463 110 XR=-ALOG(EXP(-TT)+RLU_HIJING(0)*(1.0-EXP(-TT)))
465 XR=XR-ALOG(RLU_HIJING(0))
466 IF(XR.LT.TT) GO TO 111
467 112 NJET=MIN(NJET,IHPR2(8))
468 IF(IHPR2(8).LT.0) NJET=ABS(IHPR2(8))
469 C ******** Determine number of mini jet production
473 CALL HIJHRD(JP,JT,JOUT,JFLG,1)
474 C ********JFLG=1 jets valence quarks, JFLG=2 with
475 C gluon jet, JFLG=3 with q-qbar prod for
476 C (JP,JT). If JFLG=0 jets can not be produced
477 C this time. If JFLG=-1, error occured abandon
478 C this event. JOUT is the total hard scat for
480 IF(JFLG.EQ.0) GO TO 160
482 IF(IHPR2(10).NE.0) WRITE(6,*) 'error occured in HIJHRD'
486 IF(ABS(HINT1(46)).GT.HIPR1(11).AND.JFLG.EQ.2) NFP(JP,7)=1
487 IF(ABS(HINT1(56)).GT.HIPR1(11).AND.JFLG.EQ.2) NFT(JT,7)=1
488 IF(MAX(ABS(HINT1(46)),ABS(HINT1(56))).GT.HIPR1(11).AND.
489 & JFLG.GE.3) IASG(NSG,3)=1
490 C ******** jet with PT>HIPR1(11) will be quenched
493 CALL HIJSFT(JP,JT,JOUT,IERROR)
495 IF(IHPR2(10).NE.0) WRITE(6,*) 'error occured in HIJSFT'
499 C ********conduct soft scattering between JP and JT
504 C********perform jet quenching for jets with PT>HIPR1(11)**********
506 IF((IHPR2(8).NE.0.OR.IHPR2(3).NE.0).AND.IHPR2(4).GT.0.AND.
507 & IHNT2(1).GT.1.AND.IHNT2(3).GT.1) THEN
509 IF(NFP(I,7).EQ.1) CALL QUENCH(I,1)
512 IF(NFT(I,7).EQ.1) CALL QUENCH(I,2)
515 IF(IASG(ISG,3).EQ.1) CALL QUENCH(ISG,3)
519 C**************fragment all the string systems in the following*****
521 C********N_ST is where particle information starts
522 C********N_STR+1 is the number of strings in fragmentation
523 C********the number of strings before a line is stored in K(I,4)
524 C********IDSTR is id number of the string system (91,92 or 93)
526 IF(IHPR2(20).NE.0) THEN
528 CALL HIJFRG(ISG,3,IERROR)
529 IF(MSTU(24).NE.0 .OR.IERROR.GT.0) THEN
532 IF(IHPR2(10).NE.0) THEN
533 call LULIST_HIJING(1)
534 WRITE(6,*) 'error occured, repeat the event'
538 C ********Check errors
542 IF(IHPR2(21).EQ.0) THEN
543 CALL LUEDIT_HIJING(2)
546 IF(K(N_ST,2).LT.91.OR.K(N_ST,2).GT.93) GO TO 351
551 IF(FRAME.EQ.'LAB') THEN
554 C ******** boost back to lab frame(if it was in)
558 IF(K(I,2).EQ.IDSTR) THEN
567 IF(K(I,3).EQ.0 .OR. K(K(I,3),2).EQ.IDSTR) THEN
570 KATT(NATT,3)=NATT-I+K(I,3)+N_STR-K(K(I,3),4)
572 C ****** identify the mother particle
584 C ********Fragment the q-qbar jets systems *****
589 DO 400 J_JTP=1,JTP(NTP)
590 CALL HIJFRG(J_JTP,NTP,IERROR)
591 IF(MSTU(24).NE.0 .OR. IERROR.GT.0) THEN
594 IF(IHPR2(10).NE.0) THEN
595 call LULIST_HIJING(1)
596 WRITE(6,*) 'error occured, repeat the event'
600 C ********check errors
606 IF(NTP.EQ.2) NFTP=10+NFT(J_JTP,5)
608 IF(IHPR2(21).EQ.0) THEN
609 CALL LUEDIT_HIJING(2)
610 ELSE IF (NFTP.EQ. 3 .OR. NFTP .EQ. 13) THEN
612 IF(K(N_ST,2).LT.91.OR.K(N_ST,2).GT.93) GO TO 381
616 IF(FRAME.EQ.'LAB') THEN
619 C ******** boost back to lab frame(if it was in)
623 IF(K(I,2).EQ.IDSTR) THEN
632 IF(K(I,3).EQ.0 .OR. K(K(I,3),2).EQ.IDSTR) THEN
635 KATT(NATT,3)=NATT-I+K(I,3)+N_STR-K(K(I,3),4)
637 C ****** identify the mother particle
650 C ********Fragment the q-qq related string systems
658 PATT(NATT,1)=PDR(I,1)
659 PATT(NATT,2)=PDR(I,2)
660 PATT(NATT,3)=PDR(I,3)
661 PATT(NATT,4)=PDR(I,4)
669 C ********store the direct-produced particles
671 DENGY=EATT/(IHNT2(1)*HINT1(6)+IHNT2(3)*HINT1(7))-1.0
672 IF(ABS(DENGY).GT.HIPR1(43).AND.IHPR2(20).NE.0
673 & .AND.IHPR2(21).EQ.0) THEN
674 IF(IHPR2(10).NE.0) WRITE(6,*) 'Energy not conserved, repeat the
676 C call LULIST_HIJING(1)