SUBROUTINE PHOPRE(IPARR,WT,NEUDAU,NCHARB)
C.----------------------------------------------------------------------
C.
C.    PHOTOS:   Photon radiation in decays
C.
C.    Purpose:  Order (alpha) radiative corrections  are  generated  in
C.              the decay of the IPPAR-th particle in the HEP-like
C.              common /PHOEVT/.  Photon radiation takes place from one
C.              of the charged daughters of the decaying particle IPPAR
C.              WT is calculated, eventual rejection will be performed
C.              later after inclusion of interference weight.
C.
C.    Input Parameter:    IPPAR:  Pointer   to   decaying  particle  in
C.                                /PHOEVT/ and the common itself,
C.
C.    Output Parameters:  Common  /PHOEVT/, either  with  or  without a
C.                                photon(s) added.
C.                        WT      weight of the configuration 
C.
C.    Author(s):  Z. Was, B. van Eijk             Created at:  26/11/89
C.                                                Last Update: 26/05/93
C.
C.----------------------------------------------------------------------
      IMPLICIT NONE
      DOUBLE PRECISION MINMAS,MPASQR,MCHREN
      DOUBLE PRECISION BETA,EPS,DEL1,DEL2,DATA
      REAL*8 PHOCHA,PHOSPI,PHORAN,PHOCOR,MASSUM
      INTEGER IP,IPARR,IPPAR,I,J,ME,NCHARG,NEUPOI,NLAST,THEDUM
      INTEGER IDABS,IDUM
      INTEGER NCHARB,NEUDAU
      REAL*8 WT
      INTEGER NMXPHO
      PARAMETER (NMXPHO=10000)
      INTEGER IDPHO,ISTPHO,JDAPHO,JMOPHO,NEVPHO,NPHO
      REAL*8 PPHO,VPHO
      COMMON/PHOEVT/NEVPHO,NPHO,ISTPHO(NMXPHO),IDPHO(NMXPHO),
     &JMOPHO(2,NMXPHO),JDAPHO(2,NMXPHO),PPHO(5,NMXPHO),VPHO(4,NMXPHO)
      LOGICAL CHKIF
      COMMON/PHOIF/CHKIF(NMXPHO)
      INTEGER CHAPOI(NMXPHO)
      DOUBLE PRECISION MCHSQR,MNESQR
      REAL*8 PNEUTR
      COMMON/PHOMOM/MCHSQR,MNESQR,PNEUTR(5)
      DOUBLE PRECISION COSTHG,SINTHG
      REAL*8 XPHMAX,XPHOTO
      COMMON/PHOPHS/XPHMAX,XPHOTO,COSTHG,SINTHG
      REAL*8 ALPHA,XPHCUT
      COMMON/PHOCOP/ALPHA,XPHCUT
      INTEGER IREP
      REAL*8 PROBH,CORWT,XF
      COMMON/PHOPRO/PROBH,CORWT,XF,IREP
C--
      IPPAR=IPARR
C--   Store pointers for cascade treatement...
      IP=IPPAR
      NLAST=NPHO
      IDUM=1
C--
C--   Check decay multiplicity..
      IF (JDAPHO(1,IP).EQ.0) RETURN
C--
C--   Loop over daughters, determine charge multiplicity
   10 NCHARG=0
      IREP=0
      MINMAS=0.D0
      MASSUM=0.D0
      DO 20 I=JDAPHO(1,IP),JDAPHO(2,IP)
C--
C--
C--   Exclude marked particles, quarks and gluons etc...
        IDABS=ABS(IDPHO(I))
        IF (CHKIF(I-JDAPHO(1,IP)+3)) THEN
          IF (PHOCHA(IDPHO(I)).NE.0) THEN
            NCHARG=NCHARG+1
            IF (NCHARG.GT.NMXPHO) THEN
              DATA=NCHARG
              CALL PHOERR(1,'PHOTOS',DATA)
            ENDIF
            CHAPOI(NCHARG)=I
          ENDIF
          MINMAS=MINMAS+PPHO(5,I)**2
        ENDIF
        MASSUM=MASSUM+PPHO(5,I)
   20 CONTINUE
      IF (NCHARG.NE.0) THEN
C--
C--   Check that sum of daughter masses does not exceed parent mass
        IF ((PPHO(5,IP)-MASSUM)/PPHO(5,IP).GT.2.D0*XPHCUT) THEN
C--
C--   Order  charged  particles  according  to decreasing mass, this  to
C--   increase efficiency (smallest mass is treated first).
          IF (NCHARG.GT.1) CALL PHOOMA(1,NCHARG,CHAPOI)
C--
   30       CONTINUE
            DO 70 J=1,3
   70       PNEUTR(J)=-PPHO(J,CHAPOI(NCHARG))
            PNEUTR(4)=PPHO(5,IP)-PPHO(4,CHAPOI(NCHARG))
C--
C--   Calculate  invariant  mass of 'neutral' etc. systems
          MPASQR=PPHO(5,IP)**2
          MCHSQR=PPHO(5,CHAPOI(NCHARG))**2
          IF ((JDAPHO(2,IP)-JDAPHO(1,IP)).EQ.1) THEN
            NEUPOI=JDAPHO(1,IP)
            IF (NEUPOI.EQ.CHAPOI(NCHARG)) NEUPOI=JDAPHO(2,IP)
            MNESQR=PPHO(5,NEUPOI)**2
            PNEUTR(5)=PPHO(5,NEUPOI)
          ELSE
            MNESQR=PNEUTR(4)**2-PNEUTR(1)**2-PNEUTR(2)**2-PNEUTR(3)**2
            MNESQR=MAX(MNESQR,MINMAS-MCHSQR)
            PNEUTR(5)=SQRT(MNESQR)
          ENDIF
C--
C--   Determine kinematical limit...
          XPHMAX=(MPASQR-(PNEUTR(5)+PPHO(5,CHAPOI(NCHARG)))**2)/MPASQR
C--
C--   Photon energy fraction...
          CALL PHOENE(MPASQR,MCHREN,BETA,IDPHO(CHAPOI(NCHARG)))
C--
C--   Energy fraction not too large (very seldom) ? Define angle.
          IF ((XPHOTO.LT.XPHCUT).OR.(XPHOTO.GT.XPHMAX)) THEN
C--
C--   No radiation was accepted, check  for more daughters  that may ra-
C--   diate and correct radiation probability...
            NCHARG=NCHARG-1
            IF (NCHARG.GT.0) THEN
              IREP=IREP+1
              GOTO 30
            ENDIF
          ELSE
C--
C--   Angle is generated  in  the  frame defined  by  charged vector and
C--   PNEUTR, distribution is taken in the infrared limit...
            EPS=MCHREN/(1.D0+BETA)
C--
C--   Calculate sin(theta) and cos(theta) from interval variables
            DEL1=(2.D0-EPS)*(EPS/(2.D0-EPS))**PHORAN(THEDUM)
            DEL2=2.D0-DEL1
            COSTHG=(1.D0-DEL1)/BETA
            SINTHG=SQRT(DEL1*DEL2-MCHREN)/BETA
C--
C--   Determine spin of  particle and construct code  for matrix element
            ME=2.D0*PHOSPI(IDPHO(CHAPOI(NCHARG)))+1.D0
C--
C--   Weighting procedure with 'exact' matrix element, reconstruct kine-
C--   matics for photon, neutral and charged system and update /PHOEVT/.
C--   Find pointer to the first component of 'neutral' system
      DO  I=JDAPHO(1,IP),JDAPHO(2,IP)
        IF (I.NE.CHAPOI(NCHARG)) THEN
          NEUDAU=I
          GOTO 51
        ENDIF
      ENDDO
C--
C--   Pointer not found...
      DATA=NCHARG
      CALL PHOERR(5,'PHOKIN',DATA)
 51   CONTINUE
      NCHARB=CHAPOI(NCHARG)
      NCHARB=NCHARB-JDAPHO(1,IP)+3
      NEUDAU=NEUDAU-JDAPHO(1,IP)+3
        WT=PHOCOR(MPASQR,MCHREN,ME)

          ENDIF
        ELSE
          DATA=PPHO(5,IP)-MASSUM
          CALL PHOERR(10,'PHOTOS',DATA)
        ENDIF
      ENDIF
C--
      RETURN
      END