subroutine DOGevolvep0(xin,qin,p2in,ip2in,pdf) include 'parmsetup.inc' real*8 xin,qin,q2in,p2in,pdf(-6:6),xval(45),qcdl4,qcdl5 real*8 upv,dnv,usea,dsea,str,chm,bot,top,glu character*16 name(nmxset) integer nmem(nmxset),ndef(nmxset),mmem common/NAME/name,nmem,ndef,mmem integer ns save call DOPHO1(xin,qin,upv,dnv,usea,dsea,str,chm,bot,glu) pdf(-6)= 0.0d0 pdf(6)= 0.0d0 pdf(-5)= bot pdf(5 )= bot pdf(-4)= chm pdf(4 )= chm pdf(-3)= str pdf(3 )= str pdf(-2)= usea pdf(2 )= upv pdf(-1)= dsea pdf(1 )= dnv pdf(0 )= glu return ccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc entry DOGevolvep1(xin,qin,p2in,ip2in,pdf) call DOPHO2(xin,qin,upv,dnv,usea,dsea,str,chm,bot,glu) pdf(-6)= 0.0d0 pdf(6)= 0.0d0 pdf(-5)= bot pdf(5 )= bot pdf(-4)= chm pdf(4 )= chm pdf(-3)= str pdf(3 )= str pdf(-2)= usea pdf(2 )= upv pdf(-1)= dsea pdf(1 )= dnv pdf(0 )= glu return ccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc entry DOGread(nset) read(1,*)nmem(nset),ndef(nset) return c ccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc entry DOGalfa(alfas,qalfa) call getnset(iset) call GetOrderAsM(iset,iord) call Getlam4M(iset,imem,qcdl4) call Getlam5M(iset,imem,qcdl5) call aspdflib(alfas,Qalfa,iord,qcdl5) return c ccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc entry DOGinit(Eorder,Q2fit) return c ccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc entry DOGpdf(mem) imem = mem return c 1000 format(5e13.5) end ccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc SUBROUTINE DOPHO1(DX,DQ,DUV,DDV,DUB,DDB,DSB,DCB,DBB,DGL) C******************************************************************** C* * C* Parametrization of parton distribution functions * C* in the photon (LO analysis) - asymptotic solution of AP eq.! * C* * C* authors: D.Duke and H.Owens (DO) * C* /Phys.Rev. D26 (1982) 1600/ * C* * C* Prepared by: * C* Krzysztof Charchula, DESY * C* bitnet: F1PCHA@DHHDESY3 * C* decnet: 13313::CHARCHULA * C* * C* Modified by: * C* H. Plothow-Besch/CERN-PPE * C* * C******************************************************************** C implicit real*8 (a-h,o-z) double precision + CQ(5), + DX,DQ,DUV,DDV,DUB,DDB,DSB,DCB,DBB,DGL PARAMETER (ALPEM=7.29927D-3, PI=3.141592D0) PARAMETER (ALAM=0.2D0) DATA CQ/0.33333D0,0.66666D0,0.33333D0,0.66666D0,0.33333D0/ C Q2 = DQ*DQ ALAM2=ALAM**2 FQ=ALPEM/(2.*PI)*LOG(Q2/ALAM2) C C...gluons POMG=0.194*(1.-DX)**1.03/(DX**0.97) DGL=POMG*FQ C C...quarks POM1=(1.81-1.67*DX+2.16*DX**2) POM2=DX**0.7/(1.-0.4*LOG(1.-DX)) POM3=38.D-4*(1.-DX)**1.82/(DX**1.18) DDB=(CQ(1)**2*POM1*POM2+POM3)*FQ DDV=DDB DUB=(CQ(2)**2*POM1*POM2+POM3)*FQ DUV=DUB DSB=(CQ(3)**2*POM1*POM2+POM3)*FQ DCB=(CQ(4)**2*POM1*POM2+POM3)*FQ DBB=(CQ(5)**2*POM1*POM2+POM3)*FQ RETURN END ccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc SUBROUTINE DOPHO2(DX,DQ,DUV,DDV,DUB,DDB,DSB,DCB,DBB,DGL) C******************************************************************** C* * C* Parametrization of parton distribution functions * C* in the photon (LO analysis) - asymptotic solution of AP eq.! * C* * C* authors: D.Duke and H.Owens (DO) * C* /Phys.Rev. D26 (1982) 1600/ * C* * C* Prepared by: * C* Krzysztof Charchula, DESY * C* bitnet: F1PCHA@DHHDESY3 * C* decnet: 13313::CHARCHULA * C* * C* Modified by: * C* H. Plothow-Besch/CERN-PPE * C* * C******************************************************************** C implicit real*8 (a-h,o-z) double precision + CQ(5), + DX,DQ,DUV,DDV,DUB,DDB,DSB,DCB,DBB,DGL PARAMETER (ALPEM=7.29927D-3,PI=3.141592D0) PARAMETER (ALAM=0.4D0) DATA CQ/0.33333D0,0.66666D0,0.33333D0,0.66666D0,0.33333D0/ C Q2 = DQ*DQ ALAM2=ALAM**2 FQ=ALPEM/(2.*PI)*LOG(Q2/ALAM2) C C...gluons POMG=0.194*(1.-DX)**1.03/(DX**0.97) DGL=POMG*FQ C C...quarks POM1=(1.81-1.67*DX+2.16*DX**2) POM2=DX**0.7/(1.-0.4*LOG(1.-DX)) POM3=38.D-4*(1.-DX)**1.82/(DX**1.18) DDB=(CQ(1)**2*POM1*POM2+POM3)*FQ DDV=DDB DUB=(CQ(2)**2*POM1*POM2+POM3)*FQ DUV=DUB DSB=(CQ(3)**2*POM1*POM2+POM3)*FQ DCB=(CQ(4)**2*POM1*POM2+POM3)*FQ DBB=(CQ(5)**2*POM1*POM2+POM3)*FQ RETURN END ccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc