* $Id$ C********************************************************************* SUBROUTINE LUXDIF_HIJING(NC,NJET,KFL,ECM,CHI,THE,PHI) C...Purpose: to give the angular orientation of events. #include "lujets_hijing.inc" #include "ludat1_hijing.inc" #include "ludat2_hijing.inc" C...Charge. Factors depending on polarization for QED case. QF=KCHG(KFL,1)/3. POLL=1.-PARJ(131)*PARJ(132) POLD=PARJ(132)-PARJ(131) IF(MSTJ(102).LE.1.OR.MSTJ(109).EQ.1) THEN HF1=POLL HF2=0. HF3=PARJ(133)**2 HF4=0. C...Factors depending on flavour, energy and polarization for QFD case. ELSE SFF=1./(16.*PARU(102)*(1.-PARU(102))) SFW=ECM**4/((ECM**2-PARJ(123)**2)**2+(PARJ(123)*PARJ(124))**2) SFI=SFW*(1.-(PARJ(123)/ECM)**2) AE=-1. VE=4.*PARU(102)-1. AF=SIGN(1.,QF) VF=AF-4.*QF*PARU(102) HF1=QF**2*POLL-2.*QF*VF*SFI*SFF*(VE*POLL-AE*POLD)+ & (VF**2+AF**2)*SFW*SFF**2*((VE**2+AE**2)*POLL-2.*VE*AE*POLD) HF2=-2.*QF*AF*SFI*SFF*(AE*POLL-VE*POLD)+2.*VF*AF*SFW*SFF**2* & (2.*VE*AE*POLL-(VE**2+AE**2)*POLD) HF3=PARJ(133)**2*(QF**2-2.*QF*VF*SFI*SFF*VE+(VF**2+AF**2)* & SFW*SFF**2*(VE**2-AE**2)) HF4=-PARJ(133)**2*2.*QF*VF*SFW*(PARJ(123)*PARJ(124)/ECM**2)* & SFF*AE ENDIF C...Mass factor. Differential cross-sections for two-jet events. SQ2=SQRT(2.) QME=0. IF(MSTJ(103).GE.4.AND.IABS(MSTJ(101)).LE.1.AND.MSTJ(102).LE.1.AND. &MSTJ(109).NE.1) QME=(2.*ULMASS_HIJING(KFL)/ECM)**2 IF(NJET.EQ.2) THEN SIGU=4.*SQRT(1.-QME) SIGL=2.*QME*SQRT(1.-QME) SIGT=0. SIGI=0. SIGA=0. SIGP=4. C...Kinematical variables. Reduce four-jet event to three-jet one. ELSE IF(NJET.EQ.3) THEN X1=2.*P(NC+1,4)/ECM X2=2.*P(NC+3,4)/ECM ELSE ECMR=P(NC+1,4)+P(NC+4,4)+SQRT((P(NC+2,1)+P(NC+3,1))**2+ & (P(NC+2,2)+P(NC+3,2))**2+(P(NC+2,3)+P(NC+3,3))**2) X1=2.*P(NC+1,4)/ECMR X2=2.*P(NC+4,4)/ECMR ENDIF C...Differential cross-sections for three-jet (or reduced four-jet). XQ=(1.-X1)/(1.-X2) CT12=(X1*X2-2.*X1-2.*X2+2.+QME)/SQRT((X1**2-QME)*(X2**2-QME)) ST12=SQRT(1.-CT12**2) IF(MSTJ(109).NE.1) THEN SIGU=2.*X1**2+X2**2*(1.+CT12**2)-QME*(3.+CT12**2-X1-X2)- & QME*X1/XQ+0.5*QME*((X2**2-QME)*ST12**2-2.*X2)*XQ SIGL=(X2*ST12)**2-QME*(3.-CT12**2-2.5*(X1+X2)+X1*X2+QME)+ & 0.5*QME*(X1**2-X1-QME)/XQ+0.5*QME*((X2**2-QME)*CT12**2-X2)*XQ SIGT=0.5*(X2**2-QME-0.5*QME*(X2**2-QME)/XQ)*ST12**2 SIGI=((1.-0.5*QME*XQ)*(X2**2-QME)*ST12*CT12+QME*(1.-X1-X2+ & 0.5*X1*X2+0.5*QME)*ST12/CT12)/SQ2 SIGA=X2**2*ST12/SQ2 SIGP=2.*(X1**2-X2**2*CT12) C...Differential cross-sect for scalar gluons (no mass or QFD effects). ELSE SIGU=2.*(2.-X1-X2)**2-(X2*ST12)**2 SIGL=(X2*ST12)**2 SIGT=0.5*SIGL SIGI=-(2.-X1-X2)*X2*ST12/SQ2 SIGA=0. SIGP=0. ENDIF ENDIF C...Upper bounds for differential cross-section. HF1A=ABS(HF1) HF2A=ABS(HF2) HF3A=ABS(HF3) HF4A=ABS(HF4) SIGMAX=(2.*HF1A+HF3A+HF4A)*ABS(SIGU)+2.*(HF1A+HF3A+HF4A)* &ABS(SIGL)+2.*(HF1A+2.*HF3A+2.*HF4A)*ABS(SIGT)+2.*SQ2* &(HF1A+2.*HF3A+2.*HF4A)*ABS(SIGI)+4.*SQ2*HF2A*ABS(SIGA)+ &2.*HF2A*ABS(SIGP) C...Generate angular orientation according to differential cross-sect. 100 CHI=PARU(2)*RLU_HIJING(0) CTHE=2.*RLU_HIJING(0)-1. PHI=PARU(2)*RLU_HIJING(0) CCHI=COS(CHI) SCHI=SIN(CHI) C2CHI=COS(2.*CHI) S2CHI=SIN(2.*CHI) THE=ACOS(CTHE) STHE=SIN(THE) C2PHI=COS(2.*(PHI-PARJ(134))) S2PHI=SIN(2.*(PHI-PARJ(134))) SIG=((1.+CTHE**2)*HF1+STHE**2*(C2PHI*HF3-S2PHI*HF4))*SIGU+ &2.*(STHE**2*HF1-STHE**2*(C2PHI*HF3-S2PHI*HF4))*SIGL+ &2.*(STHE**2*C2CHI*HF1+((1.+CTHE**2)*C2CHI*C2PHI-2.*CTHE*S2CHI* &S2PHI)*HF3-((1.+CTHE**2)*C2CHI*S2PHI+2.*CTHE*S2CHI*C2PHI)*HF4)* &SIGT-2.*SQ2*(2.*STHE*CTHE*CCHI*HF1-2.*STHE*(CTHE*CCHI*C2PHI- &SCHI*S2PHI)*HF3+2.*STHE*(CTHE*CCHI*S2PHI+SCHI*C2PHI)*HF4)*SIGI+ &4.*SQ2*STHE*CCHI*HF2*SIGA+2.*CTHE*HF2*SIGP IF(SIG.LT.SIGMAX*RLU_HIJING(0)) GOTO 100 RETURN END