SUBROUTINE NSD C----------------------------------------------------------------------- C N(ON) S(INGLE) D(IFFRACTION CASE) C C SETS PARAMETERS FOR HDPM IN CASE OF NON-SINGLE-DIFFRACTION EVENT C THIS SUBROUTINE IS CALLED FROM HDPM C----------------------------------------------------------------------- IMPLICIT DOUBLE PRECISION (A-H,O-Z) *KEEP,INTER. COMMON /INTER/ AVCH,AVCH3,DC0,DLOG,DMLOG,ECMDIF,ECMDPM,ELAB, * FNEUT,FNEUT2,GNU,PLAB,POSC2,POSC3,POSN2,POSN3, * RC3TO2,S,SEUGF,SEUGP,SLOG,SLOGSQ,SMLOG, * WIDC2,WIDC3,WIDN2,WIDN3,YCM,YY0,ZN, * IDIF,ITAR DOUBLE PRECISION AVCH,AVCH3,DC0,DLOG,DMLOG,ECMDIF,ECMDPM,ELAB, * FNEUT,FNEUT2,GNU,PLAB,POSC2,POSC3,POSN2,POSN3, * RC3TO2,S,SEUGF,SEUGP,SLOG,SLOGSQ,SMLOG, * WIDC2,WIDC3,WIDN2,WIDN3,YCM,YY0,ZN INTEGER IDIF,ITAR *KEEP,RUNPAR. COMMON /RUNPAR/ FIXHEI,THICK0,HILOECM,HILOELB, * STEPFC,NRRUN,NSHOW,PATAPE,MONIIN, * MONIOU,MDEBUG,NUCNUC, * CETAPE, * SHOWNO,ISHW,NOPART,NRECS,NBLKS,MAXPRT,NDEBDL, * N1STTR,MDBASE, * DEBDEL,DEBUG,FDECAY,FEGS,FIRSTI,FIXINC,FIXTAR, * FIX1I,FMUADD,FNKG,FPRINT,FDBASE * ,GHEISH,GHESIG COMMON /RUNPAC/ DSN,HOST,USER DOUBLE PRECISION FIXHEI,THICK0,HILOECM,HILOELB REAL STEPFC INTEGER NRRUN,NSHOW,PATAPE,MONIIN,MONIOU,MDEBUG,NUCNUC, * SHOWNO,ISHW,NOPART,NRECS,NBLKS,MAXPRT,NDEBDL, * N1STTR,MDBASE INTEGER CETAPE CHARACTER*79 DSN CHARACTER*20 HOST,USER LOGICAL DEBDEL,DEBUG,FDECAY,FEGS,FIRSTI,FIXINC,FIXTAR, * FIX1I,FMUADD,FNKG,FPRINT,FDBASE * ,GHEISH,GHESIG *KEND. C----------------------------------------------------------------------- IF ( DEBUG ) WRITE(MDEBUG,*) 'NSD :' C CENTRAL RAPIDITY DENSITY ( RHO ) FOR NSD REACTION C PARAMETRISATION SEE CAPDEVIELLE,J.PHYS.G:NUCL.PHYS.16(1990)1539 EQ.7 IF ( ECMDPM .LE. 680.D0 ) THEN DC0 = 0.82D0 * (S**0.107D0) ELSE DC0 = 0.64D0 * (S**0.126D0) ENDIF C THERE ARE 3 ENERGY DEPENDENT FORMULAS FOR AVERAGE CHARGED C MULTIPLICITY ( AVCH0 ); C PARAMETRISATIONS SEE CAPDEVIELLE,J.PHYS.G:NUCL.PHYS.16(1990)1539 EQ.8 IF ( ECMDPM .LE. 187.5D0 ) THEN AVCH0 = 0.57D0 + 0.584D0 * SLOG + 0.127D0 * SLOGSQ ELSEIF ( ECMDPM .LT. 945.5D0 ) THEN AVCH0 = -6.55D0 + 6.89D0 * S**0.131D0 ELSE AVCH0 = 3.4D0 * S**0.17D0 ENDIF C MINIMUM AVERAGE CHARGED MULTIPLICITY IS 1 AVCH0 = MAX( 1.D0, AVCH0 ) C EXCESS OF CHARGED PARTICLES WHICH COME FROM AIR TARGET IF ( ECMDPM .LE. 137.D0 ) THEN AVCH3 = 0.57D0 * AVCH0 * (GNU - 1.D0) ELSE AVCH3 = 0.5D0 * AVCH0 * (GNU - 1.D0) ENDIF C AVERAGE NUMBER OF ALL CHARGED AVCH = AVCH0 + AVCH3 C THE FOLOWING PROCEDURE IS TO PRODUCE PHOTONS FROM UNKNOWN NEUTRAL C DECAYS FOLLOWING CORRELATION WITH CHARGED PARTICLES BASED ON PHOTON C EXCESS AT COLLIDER EXPERIMENTS. SEUGP IS C PARAMETRISATION OF UA5: ANSORGE ET AL., Z.PHYS.C43 (1989) 75 IF ( ECMDPM .LE. 103.D0 ) THEN SEUGP = -1.27D0 + 0.52D0 * SLOG + 0.148D0 * SLOGSQ ELSE C PROBLEM OF THE RISE OF THE UNKNOWN ETA PRODUCTION CROSS SECTION C IS SOLVED WITH THOUW'S PARAMETRISATION OF UA5 DATA: SEUGP = -18.7D0 + 11.55D0 * S**0.1195D0 ENDIF SEUGP = MAX( 0.5D0, SEUGP ) IF ( DEBUG ) WRITE(MDEBUG,100) * SNGL(DC0),SNGL(AVCH0),SNGL(AVCH3),SNGL(AVCH),SNGL(SEUGP) 100 FORMAT(' NSD : DC0,AVCH0,AVCH3,AVCH,SEUGP=',5F12.7) C CENTER OF GAUSSIAN FOR CHARGED SECONDARIES 1ST AND 2ND STRING C NEEDED FOR SOME CALCULATION ; FINAL POSITION CALCULATED LATER POSC2 = 0.146D0 * SMLOG + 0.072D0 C WIDTH OF GAUSSIAN FOR CHARGED SECONDARIES 1ST AND 2ND STRING WIDC2 = 0.12D0 * SMLOG + 0.18D0 IF ( GNU .LE. 1.D0 ) THEN POSC3 = 0.D0 WIDC3 = 1.D0 ELSE C CENTER OF GAUSSIAN 3RD STRING (TARGET CONTRIB. FOR PROJECTILE-AIR) POSC3 = 3.D0 - 2.575D0 * EXP( -0.081756452D0 * GNU ) C WIDTH OF GAUSSIAN FOR 3RD STRING WIDC3 = 1.2338466D0 + 0.078969916D0 * LOG(GNU) ENDIF IF ( DEBUG ) WRITE(MDEBUG,110) * SNGL(POSC2),SNGL(WIDC2),SNGL(POSC3),SNGL(WIDC3) 110 FORMAT(' NSD : POSC2,WIDC2,POSC3,WIDC3=',4F12.7) RETURN END