* $Id$ C********************************************************************* SUBROUTINE LUBOEI_HIJING(NSAV) C...Purpose: to modify event so as to approximately take into account C...Bose-Einstein effects according to a simple phenomenological C...parametrization. IMPLICIT DOUBLE PRECISION(D) #include "lujets_hijing.inc" #include "ludat1_hijing.inc" DIMENSION DPS(4),KFBE(9),NBE(0:9),BEI(100) DATA KFBE/211,-211,111,321,-321,130,310,221,331/ C...Boost event to overall CM frame. Calculate CM energy. IF((MSTJ(51).NE.1.AND.MSTJ(51).NE.2).OR.N-NSAV.LE.1) RETURN DO 100 J=1,4 100 DPS(J)=0. DO 120 I=1,N IF(K(I,1).LE.0.OR.K(I,1).GT.10) GOTO 120 DO 110 J=1,4 110 DPS(J)=DPS(J)+P(I,J) 120 CONTINUE CALL LUDBRB_HIJING(0,0,0.,0.,-DPS(1)/DPS(4),-DPS(2)/DPS(4), &-DPS(3)/DPS(4)) PECM=0. DO 130 I=1,N 130 IF(K(I,1).GE.1.AND.K(I,1).LE.10) PECM=PECM+P(I,4) C...Reserve copy of particles by species at end of record. NBE(0)=N+MSTU(3) DO 160 IBE=1,MIN(9,MSTJ(51)) NBE(IBE)=NBE(IBE-1) DO 150 I=NSAV+1,N IF(K(I,2).NE.KFBE(IBE)) GOTO 150 IF(K(I,1).LE.0.OR.K(I,1).GT.10) GOTO 150 IF(NBE(IBE).GE.MSTU(4)-MSTU(32)-5) THEN CALL LUERRM_HIJING(11 $ ,'(LUBOEI_HIJING:) no more memory left in LUJETS_HIJING') RETURN ENDIF NBE(IBE)=NBE(IBE)+1 K(NBE(IBE),1)=I DO 140 J=1,3 140 P(NBE(IBE),J)=0. 150 CONTINUE 160 CONTINUE C...Tabulate integral for subsequent momentum shift. DO 210 IBE=1,MIN(9,MSTJ(51)) IF(IBE.NE.1.AND.IBE.NE.4.AND.IBE.LE.7) GOTO 180 IF(IBE.EQ.1.AND.MAX(NBE(1)-NBE(0),NBE(2)-NBE(1),NBE(3)-NBE(2)). &LE.1) GOTO 180 IF(IBE.EQ.4.AND.MAX(NBE(4)-NBE(3),NBE(5)-NBE(4),NBE(6)-NBE(5), &NBE(7)-NBE(6)).LE.1) GOTO 180 IF(IBE.GE.8.AND.NBE(IBE)-NBE(IBE-1).LE.1) GOTO 180 IF(IBE.EQ.1) PMHQ=2.*ULMASS_HIJING(211) IF(IBE.EQ.4) PMHQ=2.*ULMASS_HIJING(321) IF(IBE.EQ.8) PMHQ=2.*ULMASS_HIJING(221) IF(IBE.EQ.9) PMHQ=2.*ULMASS_HIJING(331) QDEL=0.1*MIN(PMHQ,PARJ(93)) IF(MSTJ(51).EQ.1) THEN NBIN=MIN(100,NINT(9.*PARJ(93)/QDEL)) BEEX=EXP(0.5*QDEL/PARJ(93)) BERT=EXP(-QDEL/PARJ(93)) ELSE NBIN=MIN(100,NINT(3.*PARJ(93)/QDEL)) ENDIF DO 170 IBIN=1,NBIN QBIN=QDEL*(IBIN-0.5) BEI(IBIN)=QDEL*(QBIN**2+QDEL**2/12.)/SQRT(QBIN**2+PMHQ**2) IF(MSTJ(51).EQ.1) THEN BEEX=BEEX*BERT BEI(IBIN)=BEI(IBIN)*BEEX ELSE BEI(IBIN)=BEI(IBIN)*EXP(-(QBIN/PARJ(93))**2) ENDIF 170 IF(IBIN.GE.2) BEI(IBIN)=BEI(IBIN)+BEI(IBIN-1) C...Loop through particle pairs and find old relative momentum. 180 DO 200 I1M=NBE(IBE-1)+1,NBE(IBE)-1 I1=K(I1M,1) DO 200 I2M=I1M+1,NBE(IBE) I2=K(I2M,1) Q2OLD=MAX(0.,(P(I1,4)+P(I2,4))**2-(P(I1,1)+P(I2,1))**2-(P(I1,2)+ &P(I2,2))**2-(P(I1,3)+P(I2,3))**2-(P(I1,5)+P(I2,5))**2) QOLD=SQRT(Q2OLD) C...Calculate new relative momentum. IF(QOLD.LT.0.5*QDEL) THEN QMOV=QOLD/3. ELSEIF(QOLD.LT.(NBIN-0.1)*QDEL) THEN RBIN=QOLD/QDEL IBIN=RBIN RINP=(RBIN**3-IBIN**3)/(3*IBIN*(IBIN+1)+1) QMOV=(BEI(IBIN)+RINP*(BEI(IBIN+1)-BEI(IBIN)))* & SQRT(Q2OLD+PMHQ**2)/Q2OLD ELSE QMOV=BEI(NBIN)*SQRT(Q2OLD+PMHQ**2)/Q2OLD ENDIF Q2NEW=Q2OLD*(QOLD/(QOLD+3.*PARJ(92)*QMOV))**(2./3.) C...Calculate and save shift to be performed on three-momenta. HC1=(P(I1,4)+P(I2,4))**2-(Q2OLD-Q2NEW) HC2=(Q2OLD-Q2NEW)*(P(I1,4)-P(I2,4))**2 HA=0.5*(1.-SQRT(HC1*Q2NEW/(HC1*Q2OLD-HC2))) DO 190 J=1,3 PD=HA*(P(I2,J)-P(I1,J)) P(I1M,J)=P(I1M,J)+PD 190 P(I2M,J)=P(I2M,J)-PD 200 CONTINUE 210 CONTINUE C...Shift momenta and recalculate energies. DO 230 IM=NBE(0)+1,NBE(MIN(9,MSTJ(51))) I=K(IM,1) DO 220 J=1,3 220 P(I,J)=P(I,J)+P(IM,J) 230 P(I,4)=SQRT(P(I,5)**2+P(I,1)**2+P(I,2)**2+P(I,3)**2) C...Rescale all momenta for energy conservation. PES=0. PQS=0. DO 240 I=1,N IF(K(I,1).LE.0.OR.K(I,1).GT.10) GOTO 240 PES=PES+P(I,4) PQS=PQS+P(I,5)**2/P(I,4) 240 CONTINUE FAC=(PECM-PQS)/(PES-PQS) DO 260 I=1,N IF(K(I,1).LE.0.OR.K(I,1).GT.10) GOTO 260 DO 250 J=1,3 250 P(I,J)=FAC*P(I,J) P(I,4)=SQRT(P(I,5)**2+P(I,1)**2+P(I,2)**2+P(I,3)**2) 260 CONTINUE C...Boost back to correct reference frame. CALL LUDBRB_HIJING(0,0,0.,0.,DPS(1)/DPS(4),DPS(2)/DPS(4),DPS(3) $ /DPS(4)) RETURN END