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Revision: 1.1, Wed Oct 22 13:58:52 2003 UTC (20 years, 11 months ago) by jones
Branch point for: MAIN
Initial revision

	subroutine target_init(using_Eloss,using_Coulomb,the_cent,thp_cent,
     >              Pp_cent,Mh2,ebeam,Pe_cent)

	implicit none
	include 'constants.inc'
	include 'target.inc'

	integer	i
	real*8 the_cent, thp_cent, Pp_cent, Mh2, ebeam, energy
	real*8 Pe_cent
	real*8 za2, fc
	logical	using_Eloss, using_Coulomb

	real*8 zero
	parameter (zero=0.0d0)	!double precision zero for subroutines calls.

! The radiation length of the target

	targ.L1 = log(184.15) - log(targ.Z)/3.0
	targ.L2 = log(1194.) - 2.*log(targ.Z)/3.0
	if(targ.Z.eq.1)then
	  targ.L1=5.31
	  targ.L2=6.144
	endif
	za2 = (targ.Z*alpha)**2
	fc = za2*(1.202+za2*(-1.0369+za2*1.008/(za2+1)))

! ... The radiation length, in both g/cm2 and cm; For H,D,4He, using
! ... PDB values (1999), other calculated directly from Tsai formula
! ... (For 4He, the Tsai formula is 10% lower).

	if (nint(targ.A).eq.1) then
	  targ.X0 = 61.28
	else if (nint(targ.A).eq.2) then
	  targ.X0 = 122.4
	else if (nint(targ.A).eq.4) then
	  targ.X0 = 94.32
	else if (nint(targ.A).eq.3) then
	  write(6,*) 'Using Tsai formula for He-3 radiation length!!! (is there a better value?)'
	  targ.X0 = 716.405*targ.A/targ.Z/(targ.Z*(targ.L1-fc)+targ.L2)
	else
	  targ.X0 = 716.405*targ.A/targ.Z/(targ.Z*(targ.L1-fc)+targ.L2)
	endif
	targ.X0_cm = targ.X0/targ.rho

! ... 'Average' ionization losses (MOST PROBABLE, REALLY).  Printed out by simc
! ... (so ave or m.p. are both OK), and Ebeam_vertex_ave (which should be m.p.)

	energy = ebeam
	call trip_thru_target (1,zero,energy,zero,targ.Eloss(1).ave,
     >                         targ.teff(1).ave,Me,4)
	energy = sqrt(Pe_cent**2+Me2)
	call trip_thru_target (2,zero,energy,the_cent,targ.Eloss(2).ave,
     >                         targ.teff(2).ave,Me,4)
	energy = sqrt(Pp_cent**2 + Mh2)
	call trip_thru_target (3,zero,energy,thp_cent,targ.Eloss(3).ave,
     >                         targ.teff(3).ave,sqrt(Mh2),4)
	if (.not.using_Eloss) then
	  do i = 1, 3
	    targ.Eloss(i).ave = 0.0
	  enddo
	endif

! ... Coulomb potential energy (NB All of the following are positive)

	if (using_Coulomb) then
	  targ.Coulomb.ave=6./5.*(targ.Z-1.)*alpha*hbarc/(1.18*targ.A**(1./3.))
	  targ.Coulomb_constant = 5./12. * targ.Coulomb.ave
	  targ.Coulomb.min = targ.Coulomb_constant * 2.0
	  targ.Coulomb.max = targ.Coulomb_constant * 3.0
	else
	  targ.Coulomb.ave = 0.0
	  targ.Coulomb_constant = 0.0
	  targ.Coulomb.min = 0.0
	  targ.Coulomb.max = 0.0
	endif

	return
	end

!----------------------------------------------------------------------

	subroutine limits_init(H)

	implicit none
	include 'simulate.inc'
	include 'radc.inc'
	include 'histograms.inc'

	integer i
	real*8 r
	real*8 Ebeam_min, Ebeam_max
	real*8 t1,t2			!temp. variables.
	real*8 slop_Coulomb, slop_Ebeam, slop_Ee, slop_Ep
	record /cuts/ the_phys, thp_phys, z, pp
	record /histograms/ H

!-----------------------------------------------------------------------
! RECORDS store information relating to various quantities at several
! 'STATES' in event description:
! (of course, not all qties are _recorded_ in each of these stages)
!
!	orig.*		qties are TRUE qties but before ANY radiation
!	vertex.*	qties are those used to determine spec fn and sigcc
!			weighting, so TRUE qties before tails 2,3 radiated
!	recon.*		qties are defined AT the spectrometers, AFTER being
!			run through the single arm montecarlos
!
!	main.SP.*	qties are defined AT the spectrometers, so TRUE
!			qties AFTER any modifications due to non-radiative
!			interaction with the target (this includes Coulomb
!			accel/decel of initial/final electron)
!	main.FP.*	spect. focal plane values-if using spect. model
!	main.RECON.*	qties are defined AT the spectrometers, AFTER being
!			run through the single arm montecarlos
!
! Note that in the absence of radiation, GEN=VERTEX
! Note that if a spectrometer is not used, RECON=SP, FP is empty.
! Note that the generated qties we have to compare with gen limits later
! are unaffected by radiation in tail1, so equal to vertex qties.
!
!
! EDGES on event qties at any stage can be derived from these cuts, by taking
! the transformations (and associated uncertainties) between each stage into
! account. The general usefulness of defining these edges is to improve
! efficiency --> provide checks at intermediate stages to allow us to abort
! an event early, and provide some foreknowledge in generation routines of
! what will make it to the end. We must be certain that these derived EDGES
! are wide enough that the events making it through the cuts don't come
! uncomfortably close to them.
!
!	SPedge.*	Limits at spectrometer = Acceptance + slop
!	edge.*		Limits after interaction = SPedge + musc or eloss
!						 = VERTEXedge + coulomb + rad.
!	VERTEXedge.*	Limits at vertex (from energy conservation).
!	gen.*		Generation limits.
!
! SLOPS
!	slop.MC.*	Due to spectrometer resolution (spectrometer MC).
!	slop_*		Slop in calculated physics quantities (from spect.
!			resolution + range of eloss/coulomb/...
!
!----------------------------------------------------------------------

! ... get slop values for the difference between orig and recon
! ... SPECTROMETER quantities (recon inaccuracies due to the montecarlos)

	if (using_E_arm_montecarlo) then
	  if (electron_arm.eq.1) then
	    slop.MC.e.delta.used = slop_param_d_HMS
	    slop.MC.e.yptar.used = slop_param_t_HMS
	    slop.MC.e.xptar.used = slop_param_p_HMS
	  else if (electron_arm.eq.2) then
	    slop.MC.e.delta.used = slop_param_d_SOS
	    slop.MC.e.yptar.used = slop_param_t_SOS
	    slop.MC.e.xptar.used = slop_param_p_SOS
	  else if (electron_arm.eq.3) then
	    slop.MC.e.delta.used = slop_param_d_HRSR
	    slop.MC.e.yptar.used = slop_param_t_HRSR
	    slop.MC.e.xptar.used = slop_param_p_HRSR
	  else if (electron_arm.eq.4) then
	    slop.MC.e.delta.used = slop_param_d_HRSL
	    slop.MC.e.yptar.used = slop_param_t_HRSL
	    slop.MC.e.xptar.used = slop_param_p_HRSL
	  endif
	endif
	if (using_P_arm_montecarlo) then
	  if (hadron_arm.eq.1) then
	    slop.MC.p.delta.used = slop_param_d_HMS
	    slop.MC.p.yptar.used = slop_param_t_HMS
	    slop.MC.p.xptar.used = slop_param_p_HMS
	  else if (hadron_arm.eq.2) then
	    slop.MC.p.delta.used = slop_param_d_SOS
	    slop.MC.p.yptar.used = slop_param_t_SOS
	    slop.MC.p.xptar.used = slop_param_p_SOS
	  else if (hadron_arm.eq.3) then
	    slop.MC.p.delta.used = slop_param_d_HRSR
	    slop.MC.p.yptar.used = slop_param_t_HRSR
	    slop.MC.p.xptar.used = slop_param_p_HRSR
	  else if (hadron_arm.eq.4) then
	    slop.MC.p.delta.used = slop_param_d_HRSL
	    slop.MC.p.yptar.used = slop_param_t_HRSL
	    slop.MC.p.xptar.used = slop_param_p_HRSL
	  endif
	endif

! ... Add slop to SPedges.  Used as input to final edge.*.*.* and to
! ... calculate minimum/maximum theta_phys for extreme_trip_thru_target.

	SPedge.e.delta.min = SPedge.e.delta.min - slop.MC.e.delta.used
	SPedge.e.delta.max = SPedge.e.delta.max + slop.MC.e.delta.used
	SPedge.e.yptar.min = SPedge.e.yptar.min - slop.MC.e.yptar.used
	SPedge.e.yptar.max = SPedge.e.yptar.max + slop.MC.e.yptar.used
	SPedge.e.xptar.min = SPedge.e.xptar.min - slop.MC.e.xptar.used
	SPedge.e.xptar.max = SPedge.e.xptar.max + slop.MC.e.xptar.used
	SPedge.p.delta.min = SPedge.p.delta.min - slop.MC.p.delta.used
	SPedge.p.delta.max = SPedge.p.delta.max + slop.MC.p.delta.used
	SPedge.p.yptar.min = SPedge.p.yptar.min - slop.MC.p.yptar.used
	SPedge.p.yptar.max = SPedge.p.yptar.max + slop.MC.p.yptar.used
	SPedge.p.xptar.min = SPedge.p.xptar.min - slop.MC.p.xptar.used
	SPedge.p.xptar.max = SPedge.p.xptar.max + slop.MC.p.xptar.used

! Compute TRUE edges -- distortions in the target come into play

	edge.e.E.min = (1.+SPedge.e.delta.min/100.)*spec.e.P +
     >		targ.Coulomb.min - dE_edge_test
	edge.e.E.max = (1.+SPedge.e.delta.max/100.)*spec.e.P +
     >		targ.Coulomb.max + dE_edge_test
	pp.min = (1.+SPedge.p.delta.min/100.)*spec.p.P - dE_edge_test
	pp.max = (1.+SPedge.p.delta.max/100.)*spec.p.P + dE_edge_test
	pp.min = max(0.001d0,pp.min)  !avoid p=0 (which can lead to div by zero)(
	edge.p.E.min = sqrt(pp.min**2 + Mh2)
	edge.p.E.max = sqrt(pp.max**2 + Mh2)

! ... extreme theta_e,theta_p,z values for extreme_trip_thru_target.
	the_phys.max = acos( (spec.e.cos_th-spec.e.sin_th*SPedge.e.yptar.max)/
     >		sqrt(1.+SPedge.e.yptar.max**2+SPedge.e.xptar.max**2) )
	the_phys.min = acos( (spec.e.cos_th-spec.e.sin_th*SPedge.e.yptar.min)/
     >		sqrt(1.+SPedge.e.yptar.min**2) )
	thp_phys.max = acos( (spec.p.cos_th-spec.p.sin_th*SPedge.p.yptar.max)/
     >		sqrt(1.+SPedge.p.yptar.max**2+SPedge.p.xptar.max**2) )
	thp_phys.min = acos( (spec.p.cos_th-spec.p.sin_th*SPedge.p.yptar.min)/
     >		sqrt(1.+SPedge.p.yptar.min**2) )
	z.min = -0.5*targ.length
	z.max =  0.5*targ.length
	call extreme_trip_thru_target(Ebeam, the_phys, thp_phys, edge.e.E,
     >                                pp, z, Mh)
	if (.not.using_Eloss) then
	  do i = 1, 3
	    targ.Eloss(i).min = 0.0
	    targ.Eloss(i).max = 0.0
	  enddo
	endif

	if (.not.mc_smear) then
	  targ.musc_max(1)=0.
	  targ.musc_max(2)=0.
	  targ.musc_max(3)=0.
	endif

	edge.e.E.min = edge.e.E.min + targ.Eloss(2).min
	edge.e.E.max = edge.e.E.max + targ.Eloss(2).max
	edge.p.E.min = edge.p.E.min + targ.Eloss(3).min
	edge.p.E.max = edge.p.E.max + targ.Eloss(3).max
	edge.e.yptar.min = SPedge.e.yptar.min - targ.musc_max(2)
	edge.e.yptar.max = SPedge.e.yptar.max + targ.musc_max(2)
	edge.e.xptar.min = SPedge.e.xptar.min - targ.musc_max(2)
	edge.e.xptar.max = SPedge.e.xptar.max + targ.musc_max(2)
	edge.p.yptar.min = SPedge.p.yptar.min - targ.musc_max(3)
	edge.p.yptar.max = SPedge.p.yptar.max + targ.musc_max(3)
	edge.p.xptar.min = SPedge.p.xptar.min - targ.musc_max(3)
	edge.p.xptar.max = SPedge.p.xptar.max + targ.musc_max(3)

! Edges on values of Em and Pm BEFORE reconstruction. Need to apply slop to
! take into account all transformations from ORIGINAL TRUE values to
! RECONSTRUCTED TRUE values --> that includes: (a) reconstruction slop on
! spectrometer values (b) variation in the beam energy (c) difference between
! actual losses and the corrections made for them

! ... Save the 'measured' beam energy, which will be used in recon.

	Ebeam_vertex_ave = Ebeam + targ.Coulomb.ave - targ.Eloss(1).ave

! ... Calculate slop in energies and momenta.

	Ebeam_max = Ebeam + dEbeam/2. - targ.Eloss(1).min + targ.Coulomb.max
	Ebeam_min = Ebeam - dEbeam/2. - targ.Eloss(1).max + targ.Coulomb.min
	slop_Coulomb = targ.Coulomb.max - targ.Coulomb.ave
	slop_Ebeam = dEbeam/2. + slop_Coulomb
	slop_Ee = slop.MC.e.delta.used/100.*spec.e.P + slop_Coulomb
	r = sqrt(edge.p.E.max**2 - Mh2)
	slop_Ep = sqrt( (r + slop.MC.p.delta.used/100.*spec.p.P)**2 + Mh2 ) -
     >		edge.p.E.max
	slop_Ebeam = slop_Ebeam + (targ.Eloss(1).max-targ.Eloss(1).min)
	slop_Ee = slop_Ee + (targ.Eloss(2).max-targ.Eloss(2).min)
	slop_Ep = slop_Ep + (targ.Eloss(3).max-targ.Eloss(3).min)

	if (doing_heavy) then		! 'reconstructed' Em cuts.
	  slop.total.Em.used = slop_Ebeam + slop_Ee + slop_Ep + dE_edge_test
	  edge.Em.min = cuts.Em.min - slop.total.Em.used
	  edge.Em.max = cuts.Em.max + slop.total.Em.used
	  edge.Em.min = max(0.d0,edge.Em.min)
	endif

! Edges on Em, Pm, etc... VERTEXedge.* values are vertex limits.  edge.* values
! are limits at spectrometer (after eloss and e'/hadron radiation).  Remember
! that min/max values are initialized to wide open values in STRUCTURES.
! Need edge.Em to limit radiated photon energies.
! Need VERTEXedge.Em for calulating limits on radiatied photons.
! Need VERTEXedge.Pm for A(e,e'p) only (for generation limits on Ee', Ep').
! Note that Pm_theory(*).min/max might allow for positive and negative Pm,
! or it could have positive only.  We want *.Pm.min to be zero if zero is
! allowed, so we have to check for Pm_theory.min being negative.

! For (e,e'p), need Trec (for A-1 system) in order to set radiation limits.
! Calculate Trec max from limits on Pm (since P of recoiling A-1 system is Pm).
! For pions, want Trec to be T of recoiling nucleon (the struck nucleon).
! Can only get limits from general energy conservation, and can only get
! upper limit, since the lower limit is determined by the allowed radiation,
! which is not calculated yet (and needs Trec to be calculated).

! For (e,e'pi) and (e,e'K), there are two 'recoil' systems.  Trec is the
! spectator (A-1) recoil system.  Trec_struck is the recoiling baryon
! from the 'struck' nucleon (i.e. the neutron from pi+ production from a 
! proton, and the hyperon from the kaon production).

! Get radiation limits.  In all cases, total energy conservation gives
! the primary limit. The doing_heavy case has a second condition.  Radiated
! photons change Em from the vertex value to the measured value.  They also
! change Pm, which can modify Trec.  So the max. change in Em is for a
! minimum generated Em (VERTEXedge.Em.min) that ends up as a maximum measured Em
! (edge.Em.max), with slop to take into account the modification to Trec.

	if (doing_hyd_elast) then
	  VERTEXedge.Em.min = 0.0
	  VERTEXedge.Em.max = 0.0
	  VERTEXedge.Pm.min = 0.0
	  VERTEXedge.Pm.max = 0.0
	  VERTEXedge.Trec.min = 0.0
	  VERTEXedge.Trec.max = 0.0
	  Egamma_tot_max = Ebeam_max + targ.M - edge.e.E.min - edge.p.E.min

	else if (doing_deuterium) then
	  VERTEXedge.Em.min = Mp + Mn - targ.M		!2.2249 MeV, I hope.
	  VERTEXedge.Em.max = Mp + Mn - targ.M
	  if (Pm_theory(1).min .le. 0.0 .and. Pm_theory(1).max .ge. 0.0) then 
	    VERTEXedge.Pm.min = 0.0
	  else
	    VERTEXedge.Pm.min = Pm_theory(1).min
	  endif
	  VERTEXedge.Pm.max = max(abs(Pm_theory(1).min),abs(Pm_theory(1).max))
	  VERTEXedge.Trec.min=sqrt(targ.Mrec**2+VERTEXedge.Pm.min**2)-targ.Mrec
	  VERTEXedge.Trec.max=sqrt(targ.Mrec**2+VERTEXedge.Pm.max**2)-targ.Mrec
	  Egamma_tot_max = Ebeam_max + targ.Mtar_struck - VERTEXedge.Em.min -
     >		edge.e.E.min - edge.p.E.min - VERTEXedge.Trec.min

	else if (doing_heavy) then
	  VERTEXedge.Pm.min=1.d10
	  VERTEXedge.Pm.max=-1.d10
	  do i = 1, nrhoPm
	    if (Pm_theory(i).min .le. 0.0 .and. Pm_theory(i).max .ge. 0.0) then 
	      t1 = 0.0
	    else
	      t1 = Pm_theory(1).min
	    endif
	    t2=max(abs(Pm_theory(i).min),abs(Pm_theory(i).max))
	    VERTEXedge.Pm.min = min(VERTEXedge.Pm.min,t1)
	    VERTEXedge.Pm.max = max(VERTEXedge.Pm.max,t2)
	  enddo
	  VERTEXedge.Em.min = E_Fermi
	  VERTEXedge.Em.max = 1.d10
	  VERTEXedge.Trec.min=sqrt(targ.Mrec**2+VERTEXedge.Pm.min**2)-targ.Mrec
	  VERTEXedge.Trec.max=sqrt(targ.Mrec**2+VERTEXedge.Pm.max**2)-targ.Mrec

! Radiation gives reconstructed Em larger than the true Em, so apply
! limits on measured Em to vertex Em + Egamma.
	  t1 = Ebeam_max + targ.Mtar_struck - VERTEXedge.Em.min -
     >		edge.e.E.min - edge.p.E.min - VERTEXedge.Trec.min
	  t2 = (edge.Em.max - VERTEXedge.Em.min) +
     >		(VERTEXedge.Trec.max - VERTEXedge.Trec.min)
	  Egamma_tot_max = min(t1,t2)

! ... Note that we check the hardwired_rad and using_rad flags here, instead of
! ... waiting until the end as in the other cases.  This is because doing_heavy
! ... uses Egamma_tot_max in calculation of VERTEXedge.Em.min/max limits.
	  if (hardwired_rad) Egamma_tot_max = Egamma_gen_max
	  if (.not.using_rad) Egamma_tot_max = 0.0
          VERTEXedge.Em.min = max(VERTEXedge.Em.min,edge.Em.min-Egamma_tot_max)
          VERTEXedge.Em.max = min(VERTEXedge.Em.max,edge.Em.max)

	else if (doing_hydpi .or. doing_hydkaon .or. doing_hyddvcs) then
	  VERTEXedge.Em.min = 0.0
	  VERTEXedge.Em.max = 0.0
	  VERTEXedge.Pm.min = 0.0
	  VERTEXedge.Pm.max = 0.0
	  VERTEXedge.Trec.min = 0.	!T_recoil for A-1 system.
	  VERTEXedge.Trec.max = 0.
	  VERTEXedge.Trec_struck.min = 0.
	  VERTEXedge.Trec_struck.max = Ebeam_max + targ.Mtar_struck - targ.Mrec_struck -
     >		edge.e.E.min - edge.p.E.min
	  Egamma_tot_max = Ebeam_max + targ.Mtar_struck - targ.Mrec_struck -
     >		edge.e.E.min - edge.p.E.min - VERTEXedge.Trec_struck.min

	else if (doing_deutpi .or. doing_deutkaon .or. doing_deutdvcs) then
	  VERTEXedge.Em.min = Mp + Mn - targ.M		!2.2249 MeV, I hope.
	  VERTEXedge.Em.max = Mp + Mn - targ.M
	  VERTEXedge.Pm.min = 0.0
	  VERTEXedge.Pm.max = pval(nump)
	  VERTEXedge.Trec.min = sqrt(targ.Mrec**2+VERTEXedge.Pm.min**2)-targ.Mrec
	  VERTEXedge.Trec.max = sqrt(targ.Mrec**2+VERTEXedge.Pm.max**2)-targ.Mrec
	  VERTEXedge.Trec_struck.min = 0.0
	  VERTEXedge.Trec_struck.max = Ebeam_max + targ.Mtar_struck - targ.Mrec_struck -
     >		edge.e.E.min - edge.p.E.min - VERTEXedge.Em.min -
     >		VERTEXedge.Trec.min
	  Egamma_tot_max = Ebeam_max + targ.Mtar_struck - targ.Mrec_struck -
     >		edge.e.E.min - edge.p.E.min - VERTEXedge.Em.min -
     >		VERTEXedge.Trec.min - VERTEXedge.Trec_struck.min

	else if (doing_hepi .or. doing_hekaon .or. doing_hedvcs) then
	  VERTEXedge.Em.min = targ.Mtar_struck + targ.Mrec - targ.M !*IF CORRECT Mrec!!!
!	  VERTEXedge.Em.max = eval(nume)
	  VERTEXedge.Em.max = 100.0	!temp. for generate_he_em
	  VERTEXedge.Pm.min = 0.0
	  VERTEXedge.Pm.max = pval(nump)
	  VERTEXedge.Trec.min = sqrt(targ.Mrec**2+VERTEXedge.Pm.min**2)-targ.Mrec
	  VERTEXedge.Trec.max = sqrt(targ.Mrec**2+VERTEXedge.Pm.max**2)-targ.Mrec
	  VERTEXedge.Trec_struck.min = 0.0
	  VERTEXedge.Trec_struck.max = Ebeam_max + targ.Mtar_struck -
     >		targ.Mrec_struck - edge.e.E.min - edge.p.E.min
	  Egamma_tot_max = Ebeam_max + targ.Mtar_struck -
     >		targ.Mrec_struck - edge.e.E.min - edge.p.E.min -
     >		VERTEXedge.Trec_struck.min - VERTEXedge.Em.min

	endif

	if (doing_kaon .or. doing_pion .or. doing_dvcs) then
	  write(6,*) 'E_bind =',VERTEXedge.Em.min,'MeV in limits_init (QF only)'
	endif

! ... override calculated limits with hardwired value if desired.
	if (hardwired_rad) Egamma_tot_max = Egamma_gen_max
	if (.not.using_rad) Egamma_tot_max = 0.0
	if (doing_tail(1)) Egamma1_max = Egamma_tot_max
	if (doing_tail(2)) Egamma2_max = Egamma_tot_max
	if (doing_tail(3)) Egamma3_max = Egamma_tot_max
! mkj new
	if (doing_pion .and. which_pion .eq. 3) then
	  VERTEXedge.Em.min = max(VERTEXedge.Em.min,edge.Em.min)
	  VERTEXedge.Em.max = min(VERTEXedge.Em.max,edge.Em.max)
	endif
! mkj new

! ... compute edge on summed _generated_ energies based on predicted VERTEX
! ... and TRUE values of Em (Ee'+Ep' for doing_heavy, Ee' for pion/kaon,
! ... Ee' for D(e,e'p), not used for hydrogen elastic.)

	if (doing_hyd_elast) then	!NO generated energies.
	  gen.sumEgen.min = 0.0
	  gen.sumEgen.max = 0.0

	else if (doing_heavy) then	!generated TOTAL (e+p) energy limits.
	  gen.sumEgen.max = Ebeam_max + targ.Mtar_struck - VERTEXedge.Trec.min - VERTEXedge.Em.min
	  gen.sumEgen.min = Ebeam_min + targ.Mtar_struck - VERTEXedge.Trec.max - VERTEXedge.Em.max - Egamma1_max 
! ... Secondary limits for sumEgen when generating electron + proton.
	  gen.sumEgen.max = min(gen.sumEgen.max,edge.e.E.max+edge.p.E.max+Egamma_tot_max)
	  gen.sumEgen.min = max(gen.sumEgen.min,edge.e.E.min+edge.p.E.min)
c mkj new
	else if (doing_pion .and. which_pion .eq. 3) then
	  gen.sumEgen.max = Ebeam_max + targ.Mtar_struck -
     >		 edge.p.E.min - VERTEXedge.Em.min
	  gen.sumEgen.min = Ebeam_min + targ.Mtar_struck -
     >		edge.p.E.max - VERTEXedge.Trec.max - VERTEXedge.Em.max - Egamma1_max 
	  gen.sumEgen.max = edge.e.E.max
	  gen.sumEgen.min = edge.e.E.min
	  write(6,*) 'gen.sumEgen.max,gen.sumEgen.min',gen.sumEgen.max,gen.sumEgen.min
c	  gen.sumEgen.max = min(gen.sumEgen.max,edge.e.E.max+edge.p.E.max)
c	  gen.sumEgen.min = max(gen.sumEgen.min,edge.e.E.min+edge.p.E.min)
c mkj new
	else				!generated ELECTRON energy limits.

	  if (doing_deuterium) then
	    gen.sumEgen.max = Ebeam_max + targ.Mtar_struck - VERTEXedge.Em.min -
     >		edge.p.E.min - VERTEXedge.Trec.min
	    gen.sumEgen.min = Ebeam_min + targ.Mtar_struck - VERTEXedge.Em.max -
     >		edge.p.E.max - VERTEXedge.Trec.max - Egamma_tot_max

	  else if (doing_hydpi .or. doing_hydkaon .or. doing_hyddvcs) then
	    gen.sumEgen.max = Ebeam_max + targ.Mtar_struck - targ.Mrec_struck -
     >		edge.p.E.min - VERTEXedge.Trec_struck.min
	    gen.sumEgen.min = Ebeam_min + targ.Mtar_struck - targ.Mrec_struck -
     >		edge.p.E.max - VERTEXedge.Trec_struck.max - Egamma_tot_max

	  else if (doing_deutpi.or.doing_hepi.or.doing_deutkaon.or.
     >  	 doing_hekaon.or.doing_deutdvcs.or.doing_hedvcs) then
	    gen.sumEgen.max = Ebeam_max + targ.Mtar_struck - targ.Mrec_struck -
     >		edge.p.E.min - VERTEXedge.Trec_struck.min - VERTEXedge.Em.min -
     >		VERTEXedge.Trec.min
	    gen.sumEgen.min = Ebeam_min + targ.Mtar_struck - targ.Mrec_struck -
     >		edge.p.E.max - VERTEXedge.Trec_struck.max - VERTEXedge.em.max -
     >		VERTEXedge.Trec.max - Egamma_tot_max

	  endif
! ... Secondary limits for sumEgen when only generating electron.
	  gen.sumEgen.max = min(gen.sumEgen.max, edge.e.E.max+Egamma2_max)
	  gen.sumEgen.min = max(gen.sumEgen.min, edge.e.E.min)
	endif

	gen.sumEgen.min = gen.sumEgen.min - dE_edge_test
	gen.sumEgen.max = gen.sumEgen.max + dE_edge_test
	gen.sumEgen.min = max(0.d0,gen.sumEgen.min)

! ... E arm GENERATION limits from sumEgen.
! ... Not used for doing_hyd_elast, but define for the hardwired histograms.

	if (doing_hyd_elast) then
	  gen.e.E.min = edge.e.E.min
	  gen.e.E.max = edge.e.E.max + Egamma2_max
	else if(doing_deuterium.or.doing_pion.or.doing_kaon.or.doing_dvcs) then
	  gen.e.E.min = gen.sumEgen.min
	  gen.e.E.max = gen.sumEgen.max
	else if (doing_heavy) then
	  gen.e.E.min = gen.sumEgen.min - edge.p.E.max - Egamma3_max
	  gen.e.E.max = gen.sumEgen.max - edge.p.E.min
	endif
! ... Apply limits from direct comparison to acceptance.
	gen.e.E.min = max(gen.e.E.min, edge.e.E.min)
	gen.e.E.max = min(gen.e.E.max, edge.e.E.max + Egamma2_max)

	gen.e.delta.min = (gen.e.E.min/spec.e.P-1.)*100.
	gen.e.delta.max = (gen.e.E.max/spec.e.P-1.)*100.
	gen.e.yptar.min = edge.e.yptar.min
	gen.e.yptar.max = edge.e.yptar.max
	gen.e.xptar.min = edge.e.xptar.min
	gen.e.xptar.max = edge.e.xptar.max

! ... P arm GENERATION limits from sumEgen.  Not used for any case
! ... except doing_heavy, but need to define for code that writes out limits.

	if (doing_hyd_elast.or.doing_deuterium.or.doing_pion.or.
     >      doing_kaon.or.doing_dvcs) then
	  gen.p.E.min = edge.p.E.min
	  gen.p.E.max = edge.p.E.max + Egamma3_max
	else if (doing_heavy)then
	  gen.p.E.min = gen.sumEgen.min - edge.e.E.max - Egamma2_max
	  gen.p.E.max = gen.sumEgen.max - edge.e.E.min
	endif
! ... Apply limits from direct comparison to acceptance.
        gen.p.E.min = max(gen.p.E.min, edge.p.E.min)
        gen.p.E.max = min(gen.p.E.max, edge.p.E.max + Egamma3_max)

	gen.p.delta.min = (sqrt(gen.p.E.min**2-Mh2)/spec.p.P-1.)*100.
	gen.p.delta.max = (sqrt(gen.p.E.max**2-Mh2)/spec.p.P-1.)*100.
	gen.p.yptar.min = edge.p.yptar.min
	gen.p.yptar.max = edge.p.yptar.max
	gen.p.xptar.min = edge.p.xptar.min
	gen.p.xptar.max = edge.p.xptar.max

! Axis specs for the diagnostic histograms
	H.gen.e.delta.min =  gen.e.delta.min
	H.gen.e.yptar.min =  gen.e.yptar.min
	H.gen.e.xptar.min = -gen.e.xptar.max
	H.gen.e.delta.bin = (gen.e.delta.max-gen.e.delta.min)/float(nHbins)
	H.gen.e.yptar.bin = (gen.e.yptar.max-gen.e.yptar.min)/float(nHbins)
	H.gen.e.xptar.bin = (gen.e.xptar.max-gen.e.xptar.min)/float(nHbins)
	H.gen.p.delta.min =  gen.p.delta.min
	H.gen.p.yptar.min =  gen.p.yptar.min
	H.gen.p.xptar.min = -gen.p.xptar.max
	H.gen.p.delta.bin = (gen.p.delta.max-gen.p.delta.min)/float(nHbins)
	H.gen.p.yptar.bin = (gen.p.yptar.max-gen.p.yptar.min)/float(nHbins)
	H.gen.p.xptar.bin = (gen.p.xptar.max-gen.p.xptar.min)/float(nHbins)
	H.gen.Em.min = VERTEXedge.Em.min
	H.gen.Em.bin = (max(100.d0,VERTEXedge.Em.max) - VERTEXedge.Em.min)/float(nHbins)
	H.gen.Pm.min = VERTEXedge.Pm.min
	H.gen.Pm.bin = (max(100.d0,VERTEXedge.Pm.max) - VERTEXedge.Pm.min)/float(nHbins)

	H.geni.e.delta.min = H.gen.e.delta.min
	H.geni.e.yptar.min = H.gen.e.yptar.min
	H.geni.e.xptar.min = H.gen.e.xptar.min
	H.geni.e.delta.bin = H.gen.e.delta.bin
	H.geni.e.yptar.bin = H.gen.e.yptar.bin
	H.geni.e.xptar.bin = H.gen.e.xptar.bin
	H.geni.p.delta.min = H.gen.p.delta.min
	H.geni.p.yptar.min = H.gen.p.yptar.min
	H.geni.p.xptar.min = H.gen.p.xptar.min
	H.geni.p.delta.bin = H.gen.p.delta.bin
	H.geni.p.yptar.bin = H.gen.p.yptar.bin
	H.geni.p.xptar.bin = H.gen.p.xptar.bin
	H.geni.Em.min = H.gen.Em.min
	H.geni.Em.bin = H.gen.Em.bin
	H.geni.Pm.min = H.gen.Pm.min
	H.geni.Pm.bin = H.gen.Pm.bin

	H.RECON.e.delta.min = H.gen.e.delta.min
	H.RECON.e.yptar.min = H.gen.e.yptar.min
	H.RECON.e.xptar.min = H.gen.e.xptar.min
	H.RECON.e.delta.bin = H.gen.e.delta.bin
	H.RECON.e.yptar.bin = H.gen.e.yptar.bin
	H.RECON.e.xptar.bin = H.gen.e.xptar.bin
	H.RECON.p.delta.min = H.gen.p.delta.min
	H.RECON.p.yptar.min = H.gen.p.yptar.min
	H.RECON.p.xptar.min = H.gen.p.xptar.min
	H.RECON.p.delta.bin = H.gen.p.delta.bin
	H.RECON.p.yptar.bin = H.gen.p.yptar.bin
	H.RECON.p.xptar.bin = H.gen.p.xptar.bin
	H.RECON.Em.min = H.gen.Em.min
	H.RECON.Em.bin = H.gen.Em.bin
	H.RECON.Pm.min = H.gen.Pm.min
	H.RECON.Pm.bin = H.gen.Pm.bin

	return
	end

!------------------------------------------------------------------------

	subroutine radc_init

	implicit none
	include 'simulate.inc'
	include 'radc.inc'
	include 'brem.inc'

!--------------------------------------------------------------
!
! First, about those (mysterious) 2 main 'radiative option' flags ...
!
! The significance of RAD_FLAG:
!	 RAD_FLAG  = 0	.. use best available formulas, generate in
!			.. (ntail,Egamma) basis
!		   = 1	.. use BASICRAD only, generate in (ntail,Egamma)
!			.. basis
!		   = 2	.. use BASICRAD only, generate in (Egamma(1,2,3))
!			.. basis but prevent overlap of tails (bogus, note)
!		   = 3	.. use BASICRAD only, generate in (Egamma(1,2,3))
!			.. allowing radiation in all 3 directions
!			.. simultaneously
! The (ntail,Egamma) basis can be called the PEAKED basis since it allows
! only 3 photon directions. PEAKED_BASIS_FLAG is set to zero below when
! the peaked basis is being used, in this way we can conveniently tell
! the BASICRAD routine to use the full Egamma formula to generate the gamma
! energy whenever it's called.
!
! (See N. Makins' thesis, section 4.5.6, for more help on this point)
!
! The significance of EXTRAD_FLAG:
!	EXTRAD_FLAG = 1	.. use only BASIC external radiation formulas
!			.. (phi = 1)
!		    = 2	.. use BASIC ext rad formulas x phi
!		    = 3 .. use Friedrich approximation the way we always
!			.. have
!		    = 0 .. use DEFAULTS: 3 for RAD_FLAG = 0, 1 otherwise; note
!			   that the defaults mimic the hardwired 'settings'
!			   in SIMULATE, which doesnt read EXTRAD_FLAG
!			   but determines what to do based on RAD_FLAG
!--------------------------------------------------------------

! Check setting of EXTRAD_FLAG

	if (debug(2)) write(6,*)'radc_init: entering...'
	if (extrad_flag.eq.0) then
	  if (rad_flag.eq.0) then
	    extrad_flag = 3
	  else if (rad_flag.eq.1 .or. rad_flag.eq.2 .or. rad_flag.eq.3) then
	    extrad_flag = 1
	  endif
	else if (extrad_flag.lt.0) then
	  stop 'Imbecile! check your stupid setting of EXTRAD_FLAG'
	endif

! 'etatzai' parameter

	if (debug(4)) write(6,*)'radc_init: at 1'
	etatzai = (12.0+(targ.Z+1.)/(targ.Z*targ.L1+targ.L2))/9.0
	if (debug(4)) write(6,*)'radc_init: etatzai = ',etatzai

! Initialize brem flags (brem doesn't include the normal common blocks)
	produce_output = debug(1)
	exponentiate = use_expon
	include_hard = .true.
	calculate_spence = .true.

	if (debug(2)) write(6,*)'radc_init: ending...'
	return
	end

!---------------------------------------------------------------------

	subroutine radc_init_ev (main,vertex)

	implicit none
	include 'structures.inc'
	include 'radc.inc'

	integer		i
	real*8		r, Ecutoff, dsoft, dhard, dsoft_prime
	real*8		lambda_dave, schwinger, brem, bremos
	record /event_main/ main
	record /event/	vertex

! Note that calculate_central calls this with (main,ev) rather than
! (main,vertex).  Since these are just local variables, calling it vertex
! here does not cause any problem, and makes it easier to follow
! modifications to vertex.* variables in later calls.

	real*8 zero
	parameter (zero=0.0d0)	!double precision zero for subroutine calls.

! Compute some quantities that will be needed for rad corr on this event

! ... factor for limiting energy of external radiation along incident electron
!	etta = 1.0 + 2*vertex.ein*sin(vertex.e.theta/2.)**2/(targ.A*amu)
! ... moron move! let's can that etta factor ...

	etta = 1.0

! ... the bt's

	do i=1,2
	  bt(i) = etatzai*main.target.teff(i)
	enddo

! ... the lambda's (effective bt's for internal radiation)

	do i=1,3
	  lambda(i) = lambda_dave(i,1,doing_tail(3),vertex.Ein,vertex.e.E,vertex.p.E,
     >			vertex.p.P,vertex.e.theta)
	enddo
	rad_proton_this_ev = lambda(3).gt.0

! ... get the hard correction factor. don't care about Ecutoff! Just want dhard here

	Ecutoff = 450.
	if (intcor_mode.eq.0) then
	  r = schwinger(Ecutoff,vertex,.true.,dsoft,dhard)
	else
	  if (.not.use_offshell_rad) then
	    r = brem(vertex.Ein,vertex.e.E,Ecutoff,rad_proton_this_ev,dsoft,dhard,
     >		dsoft_prime)
	  else
	    r = bremos(Ecutoff, zero, zero, vertex.Ein, vertex.e.P*vertex.ue.x,
     >		vertex.e.P*vertex.ue.y, vertex.e.P*vertex.ue.z, zero, zero, zero,
     >		vertex.p.P*vertex.up.x, vertex.p.P*vertex.up.y, vertex.p.P*vertex.up.z,
     >		vertex.p.E, rad_proton_this_ev, dsoft, dhard, dsoft_prime)
	  endif
	endif
	hardcorfac = 1./(1.-dhard)
	g(4)=-dsoft_prime*Ecutoff+bt(1)+bt(2)

! ... initialize the parameters needed for our "basic" calculation

	call basicrad_init_ev (vertex.Ein,vertex.e.E,vertex.p.E)

! ... the relative magnitudes of the three tails (we may not need them)

	do i=1,3
	  frac(i) = g(i)/g(0)
	enddo

	return
	end

!-----------------------------------------------------------------------

	subroutine basicrad_init_ev (e1,e2,e3)

	implicit none
	include 'simulate.inc'
	include 'radc.inc'

	real*8 one
	parameter (one=1.)

	integer i
	real*8 e1,e2,e3,e(3),gamma

	if (debug(2)) write(6,*)'basicrad_init_ev: entering...'
	e(1) = e1
	e(2) = e2
	e(3) = e3

! bt's for internal + external
! ??? One possibility for shutting off tails 1 or
! 2 is to set g(1/2) = 0 here ... note that lambda(3) is set to 0 in
! lambda_dave at the moment, AND proton terms are removed from brem if proton
! radiation off. something analogous and similarly consistent would have to be
! done for the other tails, right now they're just nixed in generate_rad. also
! check ALL ntail.eq.0 checks in kinema constraint lines of generate_rad

	g(1) = lambda(1) + bt(1)
	g(2) = lambda(2) + bt(2)
	g(3) = lambda(3)
	g(0) = g(1)+g(2)+g(3)

! Internal constants

	c_int(1) = lambda(1)/(e(1)*e(2))**(lambda(1)/2.)
	c_int(2) = lambda(2)/(e(1)*e(2))**(lambda(2)/2.)

*	csa NOTE: GN says these masses s/b Mp!

	c_int(3) = lambda(3)/(Mp*e(3))**(lambda(3)/2.)
	do i = 1, 3
	  c_int(i) = c_int(i) * exp(-euler*lambda(i)) / gamma(one+lambda(i))
	enddo
	g_int = lambda(1) + lambda(2) + lambda(3)
	c_int(0) = c_int(1)*c_int(2) * g_int / lambda(1)/lambda(2)

! ... proton radiation could be off

	if (lambda(3).gt.0) c_int(0) = c_int(0) * c_int(3)/lambda(3)
	c_int(0) = c_int(0) * gamma(one+lambda(1)) * gamma(one+lambda(2))
     >		* gamma(one+lambda(3)) / gamma(one+g_int)

! External constants

	do i = 1, 2
	  c_ext(i) = bt(i)/e(i)**bt(i)/gamma(one+bt(i))
	enddo
	c_ext(3) = 0.0
	g_ext = bt(1) + bt(2)
	c_ext(0) = c_ext(1)*c_ext(2) * g_ext / bt(1)/bt(2)
	c_ext(0) = c_ext(0)*gamma(one+bt(1))*gamma(one+bt(2))/gamma(one+g_ext)

! Internal + external constants

	do i = 1, 2
	  c(i) = c_int(i) * c_ext(i) * g(i)/lambda(i)/bt(i)
     >		* gamma(one+lambda(i))*gamma(one+bt(i))/gamma(one+g(i))
	enddo
	c(3) = c_int(3)

! Finally, constant for combined tails

	c(0) = c(1)*c(2) * g(0)/g(1)/g(2)

! ... proton radiation could be off

	if (g(3).gt.0) c(0) = c(0) * c(3)/g(3)
	c(0)=c(0)*gamma(one+g(1))*gamma(one+g(2))*gamma(one+g(3))/gamma(one+g(0))
	c(4)=g(4)/(e1*e2)**g(4)/gamma(one+g(4))
	if(g(3).gt.0) c(4)=c(4)/e3**g(4)
	if (debug(2)) write(6,*)'basicrad_init_ev: ending...'
	return
	end

!----------------------------------------------------------------------
!	theory_init:
!
! Input spectral function(NOT called for H(e,e'p) or pion/kaon production!)
!
! Note: Some flags that existed in old A(e,e'p) code (e.g. DD's version)
! have been removed.  Code has been changed to correspond to the following
! settings for the old flags:
!	norm_Ji_tail = 0
!	doing_Ji_tail = 0
!	Em_start_Ji_tail = 0.
!	fixed_gamma = .true.

	subroutine theory_init(success)
	
	implicit none
	include 'simulate.inc'

	real*8 Pm_values(ntheorymax), absorption
	integer m,n,iok
	logical success

! ... open the file
	if ( nint(targ.A) .eq. 2) then
	  theory_file='h2.theory'
	else if ( nint(targ.A) .eq. 12) then
	  theory_file='c12.theory'
	else if ( nint(targ.A) .eq. 56) then
	  theory_file='fe56.theory'
	else if ( nint(targ.A) .eq. 197) then
	  theory_file='au197.theory'
	else
	  write(6,*) 'No Theory File (spectral function) for A = ',targ.A
	  write(6,*) 'Defaulting to c12.theory'
	  theory_file='c12.theory'
	endif
	open(unit=1,file=theory_file,status='old',readonly,shared,iostat=iok)

! ... read in the theory file
	read(1,*,err=40) nrhoPm, absorption, E_Fermi
	do m=1, nrhoPm
	  read(1,*,err=40) nprot_theory(m), Em_theory(m), Emsig_theory(m),
     >		bs_norm_theory(m)
	  nprot_theory(m) = nprot_theory(m) * absorption
	enddo
	read(1,*,err=40) Pm_values(1),theory(1,1)
	do m=1, nrhoPm
	  n=2
	  read(1,*,err=40,end=50) Pm_values(2),theory(m,2)
	  do while (Pm_values(n).gt.Pm_values(n-1))
	    n=n+1
	    read(1,*,err=40,end=50) Pm_values(n),theory(m,n)
	  enddo

! ........ figure out details of the Pm axes
50	  Pm_theory(m).n=n-1
	  Pm_theory(m).bin=Pm_values(2)-Pm_values(1)
	  Pm_theory(m).min=Pm_values(1)-Pm_theory(m).bin/2.
	  Pm_theory(m).max=Pm_values(Pm_theory(m).n)+Pm_theory(m).bin/2.
	  if (abs(Pm_theory(m).min+Pm_theory(m).bin*Pm_theory(m).n -
	1	Pm_theory(m).max) .gt. 0.1) then
		write(6,'(1x,''ERROR: theory_init found unequal Pm bins in distribution number '',i2,''!'')') m
		close(1)
		return
	  endif

! ........ prepare for the next loop
	  Pm_values(1) = Pm_values(n)
	  theory(m+1,1) = theory(m,n)
	enddo

! ... are we doing deuterium? (i.e. only using a 1D spectral function)
	doing_deuterium = nrhoPm.eq.1 .and. E_Fermi.lt.1.0

! ... renormalize the momentum distributions
	do m=1, nrhoPm
	  do n=1, Pm_theory(m).n
	    theory(m,n) = theory(m,n)/bs_norm_theory(m)
	  enddo
	enddo

! ... and calculate the integral of the Em distribution above E_Fermi to
! ... renormalize
	if (doing_heavy) then
	  do m=1, nrhoPm
	    Em_int_theory(m) = 1.
	    Em_int_theory(m) = (pi/2. + atan((Em_theory(m)-E_Fermi)/
     >		(0.5*Emsig_theory(m))))/pi
	  enddo
	endif

! ... we made it
	success=.true.
	close(1)
	return

! ... oops
40	continue
	write(6,*) 'ERROR: theory_init failed to read in the theory file'

	return
	end

Analyzer/Replay: Mark Jones, Documents: Stephen Wood
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