TABLE OF CONTENTS
- 1. lowPhotonAnalysis/lowPhotonAnalysis
- 1.1. lowPhotonAnalysis/outputEvents
- 1.2. lowPhotonAnalysis/outputEvents_onlyFree
- 1.3. lowPhotonAnalysis/FissumOutput
- 1.4. lowPhotonAnalysis/KruscheOutput
- 1.5. lowPhotonAnalysis/KruscheAnalyse_cut
- 1.6. lowPhotonAnalysis/TwoPiOutput
- 1.7. lowPhotonAnalysis/photonAnalyse
- 1.8. lowPhotonAnalysis/pi0gamma_analysis
- 1.9. lowPhotonAnalysis/pi0gamma_momcut
- 1.10. lowPhotonAnalysis/pi0gamma_masscut
- 1.11. lowPhotonAnalysis/pi0gamma_mombin
- 1.12. lowPhotonAnalysis/pi0gamma_massres_sigma
- 1.13. lowPhotonAnalysis/pi0gamma_massres_tau
- 1.14. lowPhotonAnalysis/Ekin_pi0_cut
- 1.15. lowPhotonAnalysis/eta_analysis
- 1.16. lowPhotonAnalysis/MissingMass_analysis
- 1.17. lowPhotonAnalysis/DoOutChannels
- 1.18. lowPhotonAnalysis/readinput
- 2. /LowPhotonAnalysis
- 2.1. LowPhotonAnalysis/analyze_Photon
- 2.2. LowPhotonAnalysis/photonFS_Analyse
- 2.3. LowPhotonAnalysis/pi0gamma_analyze
- 2.4. LowPhotonAnalysis/pi0gamma_dsigma_dm.dat
- 2.5. LowPhotonAnalysis/pi0gamma_dsigma_dp.dat
- 2.6. LowPhotonAnalysis/pi0gamma_dsigma_dE.dat
- 2.7. LowPhotonAnalysis/pi0gamma_dsigma_dEkin.dat
- 2.8. LowPhotonAnalysis/OmegaExcitFunc_pi0gamma.dat
- 2.9. LowPhotonAnalysis/kruscheAnalyse
- 2.9.1. kruscheAnalyse/KruscheAnalyse.dat
- 2.9.2. kruscheAnalyse/KruscheAnalyse_prelim.dat
- 2.9.3. kruscheAnalyse/get_deltaE
- 2.9.4. kruscheAnalyse/get_EPion
- 2.10. LowPhotonAnalysis/fissumAnalyse
- 2.11. LowPhotonAnalysis/etaAnalyse
- 2.12. LowPhotonAnalysis/twoPi_output
- 2.13. LowPhotonAnalysis/sigmaMomEEEE.dat
- 2.14. LowPhotonAnalysis/sigmaRadiusEEEE.dat
- 2.15. LowPhotonAnalysis/sigmadm_mom_EEEE_ZZZ.dat
- 2.16. LowPhotonAnalysis/twoPi_output_hist
- 2.17. LowPhotonAnalysis/massInv_TwoPi
/LowPhotonAnalysis [ Modules ]
NAME
module LowPhotonAnalysis
PURPOSE
Includes analysis routines for photon induced runs
lowPhotonAnalysis/outputEvents [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
logical,save :: outputEvents=.false.
PURPOSE
If .true. then all events are printed to file.
lowPhotonAnalysis/outputEvents_onlyFree [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
logical,save :: outputEvents_onlyFree=.false.
PURPOSE
If outputEvents=.true. then only particles which may leave the nucleus, i.e. may become "free", are printed to file.
lowPhotonAnalysis/FissumOutput [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
logical,save :: FissumOutput=.false.
PURPOSE
If .true. then we perform an analysis as in PRC 53,#3 pages 1278 ff. (1996) Produces dsigma/dOmega/dT_pi for pi^+
lowPhotonAnalysis/KruscheOutput [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
logical,save :: KruscheOutput=.false.
PURPOSE
If .true. then we perform an analysis as in EPJA22 347-351 (2004)
lowPhotonAnalysis/KruscheAnalyse_cut [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
real, save :: KruscheAnalyse_cut=0. ! GeV
PURPOSE
Value of the cut for the deltaE cut in EPJA22 347-351 (2004).
lowPhotonAnalysis/TwoPiOutput [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
logical,save :: TwoPiOutput = .false.
PURPOSE
If .true. then we perform an analysis for 2pi production, including statistics for the mass of the pi-pi pair.
lowPhotonAnalysis/photonAnalyse [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
logical,save :: photonAnalyse=.false.
PURPOSE
Special analysis for final state photons
lowPhotonAnalysis/pi0gamma_analysis [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
logical, save :: pi0gamma_analysis = .false.
PURPOSE
Do analysis of pi0 gamma pairs (dsigma/dm), to reconstruct invariant mass spectrum of omega mesons.
lowPhotonAnalysis/pi0gamma_momcut [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
real, save :: pi0gamma_momcut = 0.5
PURPOSE
Cut on the absolute omega three momentum in GeV, being applied to the pi0 gamma spectrum.
lowPhotonAnalysis/pi0gamma_masscut [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
real, dimension(1:2), save :: pi0gamma_masscut = (/0.,2./)
PURPOSE
Cuts on the pi0-gamma invariant mass in GeV, being applied to all pi0-gamma spectra (except the mass spectrum). First component is lower limit, second component is upper limit.
lowPhotonAnalysis/pi0gamma_mombin [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
real, save :: pi0gamma_mombin = 0.050
PURPOSE
Bin size for the pi0 gamma momenentum spectrum in GeV.
lowPhotonAnalysis/pi0gamma_massres_sigma [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
real, save :: pi0gamma_massres_sigma = 0.025
PURPOSE
Sigma parameter for the exp. resolution smearing (width of the Gauss or Novosibirsk function in GeV). See also pi0gamma_massres_tau.
lowPhotonAnalysis/pi0gamma_massres_tau [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
real, save :: pi0gamma_massres_tau = -0.090
PURPOSE
Skewness parameter tau of the Novosibirsk function (for exp. resolution smearing). See also pi0gamma_massres_sigma.
lowPhotonAnalysis/Ekin_pi0_cut [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
real, save :: Ekin_pi0_cut = 0.
PURPOSE
Cut on the kinetic energy of neutral pions in the pi0gamma_analysis. Only pions with kinetic energies larger than this cutoff are used for the analysis.
lowPhotonAnalysis/eta_analysis [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
logical, save :: eta_analysis = .false.
PURPOSE
Do analysis of eta mesons
lowPhotonAnalysis/MissingMass_analysis [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
logical, save :: MissingMass_analysis = .false.
PURPOSE
Do analysis of missing mass distributions for 1 nucleon and 2 nucleon final states
lowPhotonAnalysis/DoOutChannels [ Global module-variables ]
[ Top ] [ lowPhotonAnalysis ] [ Global module-variables ]
SOURCE
logical, save :: DoOutChannels = .false.
PURPOSE
switch on/off: reporting of all final state channels
lowPhotonAnalysis/readinput [ Subroutines ]
[ Top ] [ lowPhotonAnalysis ] [ Subroutines ]
NAME
subroutine readinput
INPUTS
NONE
OUTPUT
NONE
PURPOSE
This subroutine reads out the jobcard "photonAnalysis". Only called once to initialize the module.
lowPhotonAnalysis/lowPhotonAnalysis [ Namelists ]
NAME
NAMELIST /lowPhotonAnalysis/
PURPOSE
Includes the switches:
- outputEvents
- outputEvents_onlyFree
- KruscheOutput
- KruscheAnalyse_cut
- FissumOutput
- photonAnalyse
- TwoPiOutput
- pi0gamma_analysis
- pi0gamma_momcut
- pi0gamma_masscut
- pi0gamma_mombin
- pi0gamma_massres_sigma
- pi0gamma_massres_tau
- Ekin_pi0_cut
- eta_analysis
- MissingMass_analysis
- DoOutChannels
LowPhotonAnalysis/analyze_Photon [ Subroutines ]
[ Top ] [ LowPhotonAnalysis ] [ Subroutines ]
NAME
subroutine analyze_Photon(Parts,finalFlag)
INPUTS
- type(particle), dimension(:,:) :: Parts -- particle vector
- logical, :: finalFlag -- .true. if it is the last call for one specific energy, therefore final output must be made.
OUTPUT
NONE
PURPOSE
Main routine for the analysis. Calls all subroutines.
LowPhotonAnalysis/photonFS_Analyse [ Subroutines ]
[ Top ] [ LowPhotonAnalysis ] [ Subroutines ]
NAME
subroutine photonFS_Analyse(Parts)
INPUTS
- type(particle), target, dimension(:,:) :: Parts --- particle vector
- logical, finalFlag -- .true. if it is the last call for one specific energy, therefore final output must be made.
OUTPUT
if "outputEvents" is true:
* Prints all events to a file called 'FinalEvents.dat' * Events stemming from omega, rho or phi production are printed to seperate files 'FinalEvents.rho.dat', ...
if "photonAnalyse" is true:
* Produces files called Photons_m2_vs_m3*.dat and Photons_dsigma_dm*.dat. * The first one contains the distribution of the invariant mass of all 3 gamma combinations vs the inv. mass of all 2gamma combinations. * The second one contains the cross section dSigma/dm vs the mass of 3 gammas.
PURPOSE
Groups all final state particles into events and writes them to file
LowPhotonAnalysis/pi0gamma_analyze [ Subroutines ]
[ Top ] [ LowPhotonAnalysis ] [ Subroutines ]
NAME
subroutine pi0gamma_analyze(Parts)
INPUTS
OUTPUT
- Produces an invariant mass spectrum of all pi0 gamma pairs in the final state and writes it to a file called 'pi0gamma_dsigma_dm.dat'
LowPhotonAnalysis/pi0gamma_dsigma_dm.dat [ Output files ]
[ Top ] [ LowPhotonAnalysis ] [ Output files ]
NAME
file pi0gamma_dsigma_dm.dat
PURPOSE
Pi0-gamma invariant-mass spectrum in microbarn/GeV/A.
LowPhotonAnalysis/pi0gamma_dsigma_dp.dat [ Output files ]
[ Top ] [ LowPhotonAnalysis ] [ Output files ]
NAME
file pi0gamma_dsigma_dp.dat
PURPOSE
Pi0-gamma momentum spectrum in microbarn/GeV/A.
LowPhotonAnalysis/pi0gamma_dsigma_dE.dat [ Output files ]
[ Top ] [ LowPhotonAnalysis ] [ Output files ]
NAME
file pi0gamma_dsigma_dE.dat
PURPOSE
Pi0-gamma energy spectrum in microbarn/GeV/A.
LowPhotonAnalysis/pi0gamma_dsigma_dEkin.dat [ Output files ]
[ Top ] [ LowPhotonAnalysis ] [ Output files ]
NAME
file pi0gamma_dsigma_dEkin.dat
PURPOSE
Pi0-gamma kinetic energy spectrum in microbarn/GeV/A.
LowPhotonAnalysis/OmegaExcitFunc_pi0gamma.dat [ Output files ]
[ Top ] [ LowPhotonAnalysis ] [ Output files ]
NAME
file OmegaExcitFunc_pi0gamma.dat
PURPOSE
Contains the omega excitation function, i.e. the energy-dependent inclusive omega photo-production cross section, as observed through the decay into pi0-gamma. In contrast to OmegaExcitFunc.dat, this does include FSI effects.
LowPhotonAnalysis/kruscheAnalyse [ Subroutines ]
[ Top ] [ LowPhotonAnalysis ] [ Subroutines ]
NAME
subroutine kruscheAnalyse(Parts,finalFlag)
PURPOSE
Evaluates the cross section for pi^0 production in the same way as Krusche in EPJA 22, 347 (2004)
INPUTS
- type(particle), dimension(:,:) :: Parts -- particle vector
- logical, finalFlag -- .true. if it is the last call for one specific energy, therefore final output must be made.
OUTPUT
- See 'KruscheAnalyse.dat' for Xsections and delta(E) histograms are given in 'deltaE_E_gamma_'//realToChar4(energy_gamma)//'_GeV.dat'
kruscheAnalyse/KruscheAnalyse.dat [ Output files ]
[ Top ] [ kruscheAnalyse ] [ Output files ]
NAME
file KruscheAnalyse.dat
PURPOSE
Evaluate the cross section for pi^0 production in the same way as Krusche in EPJA 22, 347 (2004).
PURPOSE
Columns:
- 1 : E_gamma [Gev]
- 2 : sigma pi0 [mb]
- 3 : sigma pi0 after cut [mb]
- 4 : error sigma pi0 [mb]
- 5 : error sigma pi0 after cut [mb]
kruscheAnalyse/KruscheAnalyse_prelim.dat [ Output files ]
[ Top ] [ kruscheAnalyse ] [ Output files ]
NAME
file KruscheAnalyse_prelim.dat
PURPOSE
Same as KruscheAnalyse.dat, but output is written afer each run and not only the averaged result after each energy.
kruscheAnalyse/get_deltaE [ Subroutines ]
[ Top ] [ kruscheAnalyse ] [ Subroutines ]
NAME
real function get_deltaE(part)
PURPOSE
Evaluates for a given particle "delta E" according to eq. 4 in arXiv:nucl-ex/0406002v1 (June 2004).
INPUTS
- type(particle), intent(in) :: part
kruscheAnalyse/get_EPion [ Subroutines ]
[ Top ] [ kruscheAnalyse ] [ Subroutines ]
NAME
real function get_EPion(E_gamma)
PURPOSE
Evaluates the energy of a pion in the CM-frame of a gamma Nucleon collision.
INPUTS
- real:: E_gamma -- Energy of gamma in GeV in frame where nucleon rests
LowPhotonAnalysis/fissumAnalyse [ Subroutines ]
[ Top ] [ LowPhotonAnalysis ] [ Subroutines ]
NAME
subroutine fissumAnalyse(Parts,finalFlag)
PURPOSE
Evaluates the cross section for pi^+ production in the same binnings as Fissum PRC 53,3 pages 1278ff. (19996)
INPUTS
- type(particle), dimension(:,:) :: Parts -- particle vector
- logical :: finalFlag -- .true. if it is the last call for one specific energy, therefore final output must be made.
OUTPUT
LowPhotonAnalysis/etaAnalyse [ Subroutines ]
[ Top ] [ LowPhotonAnalysis ] [ Subroutines ]
NAME
subroutine etaAnalyse(Parts,finalFlag)
PURPOSE
...
INPUTS
- type(particle), dimension(:,:) :: Parts -- particle vector
- logical :: finalFlag -- .true. if it is the last call for one specific energy, therefore final output must be made.
OUTPUT
NOTES
the inclusive production cross sections are averaged over the different runs.
LowPhotonAnalysis/twoPi_output [ Subroutines ]
[ Top ] [ LowPhotonAnalysis ] [ Subroutines ]
NAME
subroutine twoPi_output(Parts, finalFlag,elab)
INPUTS
- type(particle), dimension(:,:) :: Parts -- particle vector
- logical :: finalFlag -- .true. if it is the last call for one specific & energy, therefore final output must be made.
- real, optional :: elab
OUTPUT
NONE
PURPOSE
Makes output for two-pion production processes. Writes to the following files:
- Total cross sections for pi pi production : "twoPi_Total.dat"
- dsigma/dm : "sigmadm*.dat"
- dsigma/dp "sigmaMom*.dat"
- dsigma/dm/dp "sigmadm_mom*.dat"
where * is the given energy elab or the photon energy if elab is not present.
Only for photon induced events also dsigm/dr is available in file 'sigmaRadius*.dat'
Here r is the radius of the production point of the measured pi pi pair.
NOTES
If you want to use this routine for non photon-induced events, then you must provide "elab"!!!
LowPhotonAnalysis/sigmaMomEEEE.dat [ Output files ]
[ Top ] [ LowPhotonAnalysis ] [ Output files ]
NAME
file sigmaMomEEEE.dat, EEEE= energy of the incoming photon in MeV
PURPOSE
The files are produced in the runs with eventtype=3=LowPhoton They show xsec (microbarn) for the __two-pion events__ versus pion momentum (GeV)
Columns:
- #1: momentum (absolute value of the pion 3-momentum)
- #2: PiMinus (xsec fo pi- )
- #3: PiNull (xsec fo pi0 )
- #4: PiPlus (xsec fo pi+ )
LowPhotonAnalysis/sigmaRadiusEEEE.dat [ Output files ]
[ Top ] [ LowPhotonAnalysis ] [ Output files ]
NAME
file sigmaRadiusEEEE.dat, EEEE= energy of the incoming photon in MeV
PURPOSE
The files are produced in the runs with eventtype=3=LowPhoton They show xsec (microbarn) for the __two-pion events__ versus radius of the nucleus for various final states
Columns:
- #1: radius[fm]
- #2: baryon density[fm^-3]
- #3: dsigma/dRadius (1:6) [10^-6 b/fm/A]
- #4: xsec for PiNull PiNull [microbarn]
- #5 xsec for PiNull PiPlus
- #6 xsec for piNull piMinus
- #7 xsec for piPlus piMinus
- #8 xsec for PiPlus PiPlus
- #9 xsec for piMinus piMinus
LowPhotonAnalysis/sigmadm_mom_EEEE_ZZZ.dat [ Output files ]
[ Top ] [ LowPhotonAnalysis ] [ Output files ]
NAME
file sigmadm_mom_EEEE_ZZZ.dat, EEEE= energy of the incoming photon in MeV ZZZ = channel (predefined two-photon final state)
PURPOSE
The files are produced in the runs with eventtype=3=LowPhoton They show xsec (microbarn) for the __two-pion events__ versus pion momentum for various final states
Columns:
- #1: mass [GeV] = invariant mass of the two outgoing pions
- #2: momentum [GeV]
- #3: dsigma/dm/dp [10^-6 b/GeV^2/A]
LowPhotonAnalysis/twoPi_output_hist [ Subroutines ]
[ Top ] [ LowPhotonAnalysis ] [ Subroutines ]
NAME
subroutine twoPi_output_hist(Parts,finalFlag)
PURPOSE
Makes dsigma/dm output for two-pion production processes.
INPUTS
- type(particle), dimension(:,:) :: Parts -- particle vector
- logical :: finalFlag -- .true. if it is the last call for one specific
energy, therefore final output must be made.
OUTPUT
Writes to the following files:
- twopi_dsigma_dm_"energy_gamma"_MeV.dat'
"energy_gamma" is the photon energy
LowPhotonAnalysis/massInv_TwoPi [ Subroutines ]
[ Top ] [ LowPhotonAnalysis ] [ Subroutines ]
NAME
function massInv_TwoPi(p,q,chargep,chargeq) Result(m)
INPUTS
- real, dimension(1:3) :: p
- real, dimension(1:3) :: q
- integer :: chargep
- integer :: chargeq
PURPOSE
Evaluates invariant mass of two pions with momentum p,q and charge chargep,chargeq
OUTPUT
real :: m -- m=SQRT((p+q)*(p+q)) where p and q are the 4-vectors
NOTES
real, parameter :: massPiZero=0.138 real, parameter :: massPiCharged=0.138