cSampMol.f File Reference

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Functions/Subroutines
subroutine	csampmol (mediax, teta, cond)
subroutine	csampmol0 (mediax, teta, cond)
subroutine	cxaic2 (mediax, xc2)
subroutine	cmolexpb (mediax, expb)
subroutine	cprescatcalc

Function/Subroutine Documentation

cmolexpb()

subroutine cmolexpb	(	type(xsmedia), intent(in)	mediax,
		real*8	expb
	)

Definition at line 201 of file cSampMol.f.

References d0.

Referenced by csampmol0().

!            compute exp(b) of Moliere's scattering theory.
!            epPreScatCalc must have been called beforehand for 
!            each scattering.
      use modxsecmedia
      implicit none
#include "Zglobalc.h"
#include "Ztrack.h"
#include "Ztrackv.h"

      
!      type(epmedia):: mediax ! input. media
      type(xsmedia),intent(in):: mediax
      real*8 expb   ! output. exp(b) of Moliere's theory.

      real*8  gbeta2, beta2, massratio2
      common /zcmedia/ gbeta2, beta2, massratio2
      
      real(8):: sum, alfai2, temp
      integer::i 

      if( beta2 > 0.99 ) then  ! beta > 0.995 --> regards 1
         sum = mediax%MoliereExpb
      else
         sum =0.
!         temp = (cTrack.p.charge/137.0)**2/beta2
         temp = (trackbefmove%p%charge/137.0)**2/beta2
         do i = 1,  mediax%noOfElem

            alfai2 = mediax%elem(i)%Z**2 *temp

            sum = sum +
     *       mediax%elem(i)%No *
     *       mediax%elem(i)%Z**0.3333*(mediax%elem(i)%Z + 1.d0)
     *       / (1.d0 + 3.327d0*alfai2)
         enddo
         sum = 6702.d0 *sum/mediax%A
      endif
!      expb = sum *Move.dx * cTrack.p.charge**2 /beta2
      expb = sum *intinfarray(processno)%thickness/10. *
     *   trackbefmove%p%charge**2 /beta2
     

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cprescatcalc()

subroutine cprescatcalc

(

)

Definition at line 246 of file cSampMol.f.

References d0, kelec, and masele.

Referenced by csampmol0().

!           compute g* beta^2,  beta^2, (Me/M)^2
      implicit none
#include "Zglobalc.h"
#include "Zmass.h"
#include "Zcode.h"
#include "Ztrack.h"
#include "Ztrackv.h"

      real*8  gbeta2, beta2, massratio2
      common /zcmedia/  gbeta2, beta2,  massratio2

      real(8):: g1, g2, g

!      g1 = cTrack.p.fm.p(4)/cTrack.p.mass
      g1 = trackbefmove%p%fm%p(4)/trackbefmove%p%mass
!      g2 = Move.Track.p.fm.p(4)/cTrack.p.mass
      g2 = movedtrack%p%fm%p(4)/trackbefmove%p%mass
      beta2 = 1.d0 - 1.d0/g1/g2   !        < beta^2>
!      gbeta2=(g1 - 1.d0/g1) * (g2 - 1.d0/g2)   ! < (g*beta^2)^2 >
!      gbeta2 =( sqrt(g1*g2)*beta2)**2
      gbeta2 =g1*g2*(beta2)**2
!      if(gbeta2 == 0.) then
!         g = (g1+ g2)/2.
!         gbeta2 = (g-1.d0/g)**2
!      endif

!      if(cTrack.p.code == kelec) then
      if(trackbefmove%p%code == kelec) then
         massratio2= 1.
      else
!         massratio2= (masele/cTrack.p.mass)**2 ! (me/m)^2
         massratio2= (masele/trackbefmove%p%mass)**2 ! (me/m)^2
      endif

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csampmol()

subroutine csampmol	(	type(xsmedia), intent(in)	mediax,
		real(8), intent(out)	teta,
		integer, intent(out)	cond
	)

Definition at line 7 of file cSampMol.f.

References csampmol0(), d0, false, rndc(), and true.

Referenced by cmulscat().

      use modxsecmedia
      implicit none
!        Moliere theory of multiple scattering angle.
!        with improvement by Bethe.  rejection factor sqrt(sin teta/teta)
!        is included 
!        
!        The other is the next factor which need not be applied ?
!         exp(Bxc2/16.) rejection may be tried. We use Moliere when Bxc2 <1
!         So, if this rejection is to be tried, 
!         since for Bxc2=1, exp(..)=1.064 so the rejection for
!         smaller Bxc2 must be done by
!         u <  exp(Bxc2/16)/1.064. 
!      Define next for this correction;
!cccc # define REJBYEXPBXC2
!               For Pb, 1GeV e, there is no difference with this correction
!         of without this correction.
!     
!#include "Zglobalc.h"
!#include "Zmass.h"
!#include "Ztrack.h"
!#include "Ztrackv.h"
      
!      type(epmedia):: mediax  ! input. media 
      type(xsmedia),intent(in):: mediax 
      real(8),intent(out)::teta !  sampled spatial angle in radian.
      integer,intent(out)::cond !  0 ok. non-0. Moliere theory not applicable
      integer::icon
      real(8):: u
      logical ok

      real*8  b, xc2, bxc2
      common /zmoliere/ b, xc2, bxc2

#ifdef REJBYEXPBXC2
      real(8):: expbxc2
#endif      
      ok = .false.
      cond = 0
      do while (.not. ok)
         call csampmol0(mediax, teta, icon)
         if( icon == 0 ) then !  Moliere
            call rndc(u)
!                
#ifdef REJBYEXPBXC2
            expbxc2 = exp(bxc2/16.0d0)/1.064d0  !   needed???
#endif
!
            if(teta < 0.5d0 ) then 
!                       sin(teta) /teta = (teta - teta^3/6)/teta
!                      = 1- teta^2/6.  max error  0.054 %
               ok = u**2 < (1.0d0- teta**2/6.0d0)
#ifdef REJBYEXPBXC2
!                    needed ???
               if(ok) then 
                  call rndc(u)
                  ok =  u < expbxc2
               endif
#endif
            elseif( teta < 3.1415 ) then
               ok = u**2 < sin(teta)/teta
#ifdef REJBYEXPBXC2
               if(ok) then 
                  call rndc(u)
                  ok =  u < expbxc2
               endif
#endif
            else
               ok = .false.
            endif
         elseif( icon == 1) then  !  GS
!             rejeciton not needed; GS is used
            ok =.true.
         else  ! should use Gaussian
            ok =.true.
            cond = 1
         endif
      enddo

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csampmol0()

subroutine csampmol0	(	type(xsmedia), intent(in)	mediax,
		real(8), intent(out)	teta,
		integer, intent(out)	cond
	)

Definition at line 88 of file cSampMol.f.

References cmolexpb(), cprescatcalc(), cxaic2(), and d0.

Referenced by csampmol().

      use modxsecmedia
      use cmodsampmolreduceda
      implicit none
!        Moliere theory of multiple scattering angle.
!        with improvement by Bethe.
!#include "Zglobalc.h"
!#include "Zmass.h"
!#include "Ztrack.h"
!#include "Ztrackv.h"

!      type(epmedia):: mediax  ! input. media 
      type(xsmedia),intent(in):: mediax

      real(8),intent(out)::teta !  sampled spatial angle in radian.
      integer,intent(out)::cond !  0 ok.  Moliere used
                                !  1 ok.  G.S is used.
                                !  2 n.g  Gauss should be used.

      real*8  b, xc2, bxc2
      common /zmoliere/ b, xc2, bxc2

      real*8  gbeta2, beta2, massratio2
      common /zcmedia/  gbeta2, beta2,  massratio2

      
!     *********************
      real*8  expb
      real(8):: sb,  tetasq

      call cprescatcalc  ! get g*beta^2, beta^2, (Me/M)^2 in Zcmdeia
!          get Xc^2
      call cxaic2(mediax,   xc2)
!           we don't get xa2 but directly get exp(b)
      call cmolexpb(mediax,   expb)
      sb =log(expb)  ! 
!///////////
!      write(*,'(a, 1p,6g14.5)')
!     *  ' sb ', sb, beta2, Move.dt, Move.dl, cTrack.p.fm.p(4),
!     *          Move.track.p.fm.p(4)
!//////////////
!          B -log(B) = b  
!///      if(sb .lt. 3.395d0) then
      if(sb .lt. 1.5d0) then
!         Moliere theory cannot be appliled; use Gaussian later
!         (almost no scattering)
         cond = 2
      else
         call cmolblogb(sb, b)  !  B
         bxc2 = b*xc2
         if(bxc2 > 1.0d0) then
!             normally this happens for low E, which stops soon
!             B  so not serious.
!               use GS method ? --> cond=1
            cond =2   ! use Gauss at present
         else
            call csampmolreduceda(b, tetasq, cond)
            if( cond == 0 ) then   ! now alwasy cond=0
               teta = sqrt(tetasq *bxc2)
            endif
!///////////
!      write(*,'(a, i2, 1p,9g14.5)')
!     *  'B ', cond, sb,beta2,B, Move.dt, Move.dl, cTrack.p.fm.p(4), 
!     *        Move.track.p.fm.p(4),  Bxc2, teta
!//////////////
         endif
      endif

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cxaic2()

subroutine cxaic2	(	type(xsmedia), intent(in)	mediax,
		real*8	xc2
	)

Definition at line 157 of file cSampMol.f.

References d0, and kelec.

Referenced by csampmol0().

!       compute xc2 of Moliere's theory of scattring.
!      epPreScatCalc must have been called beforehand for 
!      each scattering.
      use modxsecmedia
      implicit none
#include "Zglobalc.h"
#include "Ztrack.h"
#include "Ztrackv.h"
#include "Zcode.h"

      
!      type(epmedia):: mediax ! input. media
      type(xsmedia),intent(in):: mediax

      real*8 xc2   ! output. Xc^2 in radian^2

      real*8  gbeta2, beta2, massratio2
      common /zcmedia/ gbeta2, beta2, massratio2


!
!      integeral 0 to leng of  1/(beta**4 E**2)
!      is approximated as  leng/(beta1**2 gamma1 beta2**2 gamma2)
!      Note: bata**2 *gamma = gamma - 1/gamma
!


!      if( cTrack.p.code == kelec) then
      if( trackbefmove%p%code == kelec) then
         xc2 = mediax%MoliereForXc2
      else
!         xc2 = 0.6011d0*cTrack.p.charge**2 * massratio2 *
         xc2 = 0.6011d0*trackbefmove%p%charge**2 * massratio2 *
     *     mediax%Z2/mediax%A 
      endif
!         Move.dx is for EPICS. 
!      xc2 = xc2*Move.dx/gbeta2  ! dx is in g/cm2. no need to consider rhoc.
                                ! real length is dx/(rho*rhoc)
!       thickness is kg/m2;*  1000/10000 = 1/10  g/cm2
      xc2 = xc2*intinfarray(processno)%thickness/10./gbeta2  ! 

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