TABLE OF CONTENTS
- 1. /baryonWidthVacuum
- 1.1. baryonWidthVacuum/getAngularMomentum_baryon
- 1.2. baryonWidthVacuum/interactionRadius
- 1.3. baryonWidthVacuum/srts_srt_switch
- 1.4. baryonWidthVacuum/deltaRho_cutoff
- 1.5. baryonWidthVacuum/meson_cutoff
- 1.6. baryonWidthVacuum/baryon_cutoff
- 1.7. baryonWidthVacuum/use_cutoff
- 1.8. baryonWidthVacuum/Delta_width
- 1.9. baryonWidthVacuum/getParameters
- 1.10. baryonWidthVacuum/readInput
- 1.11. baryonWidthVacuum/BaryonWidthVacuum
- 1.12. baryonWidthVacuum/monopoleFormfactor
- 1.13. baryonWidthVacuum/vacuumWidth
- 1.14. baryonWidthVacuum/stableFinalState
- 1.15. baryonWidthVacuum/Delta_Dmitriev
- 1.16. baryonWidthVacuum/Delta_Moniz
- 1.17. baryonWidthVacuum/Delta_Verwest
- 1.18. baryonWidthVacuum/Delta_Bass
- 1.19. baryonWidthVacuum/semistableFinalState
- 1.20. baryonWidthVacuum/rho_AB_Integrand
- 1.21. baryonWidthVacuum/rhoDeltaFinalState
- 1.21.1. rhoDeltaFinalState/deltaRho
/baryonWidthVacuum [ Modules ]
NAME
module baryonWidthVacuum
NOTES
Module which calculates the partial and full widths of the baryon resonances in dependence of their mass. Their pole mass is given by their mass in 'particleProperties' and the widths at this pole mass as well. Everything corresponds to the vacuum situation. The resulting width is therefore always the width in vacuum! As mass of the resonance we use the four-vector definition: p_mu p^mu= mass**2 Prescription according to Manley et al. Phys. Rev. D45 (1992) 4002.
baryonWidthVacuum/interactionRadius [ Global module-variables ]
[ Top ] [ baryonWidthVacuum ] [ Global module-variables ]
SOURCE
real, parameter, public :: interactionRadius = 1./hbarc
PURPOSE
interaction radius for Blatt-Weisskopf functions: r = 1fm
baryonWidthVacuum/srts_srt_switch [ Global module-variables ]
[ Top ] [ baryonWidthVacuum ] [ Global module-variables ]
SOURCE
logical, parameter, public :: srts_srt_switch=.false.
PURPOSE
Modifies the width according to S. Leupold's definition of the width, one especially has to exchange s against sqrt(s) in the denominator of Formula 2.76 of Effenbergers Phd
baryonWidthVacuum/deltaRho_cutoff [ Global module-variables ]
[ Top ] [ baryonWidthVacuum ] [ Global module-variables ]
SOURCE
real, save :: deltaRho_cutoff=0.85
PURPOSE
baryonWidthVacuum/meson_cutoff [ Global module-variables ]
[ Top ] [ baryonWidthVacuum ] [ Global module-variables ]
SOURCE
real, save :: meson_cutoff=1.6
PURPOSE
baryonWidthVacuum/baryon_cutoff [ Global module-variables ]
[ Top ] [ baryonWidthVacuum ] [ Global module-variables ]
SOURCE
real, save :: baryon_cutoff=2.0
PURPOSE
- Cut off parameter for the decay of a resonance into an unstable baryon
and a meson. * Units of GeV
baryonWidthVacuum/use_cutoff [ Global module-variables ]
[ Top ] [ baryonWidthVacuum ] [ Global module-variables ]
SOURCE
logical, save :: use_cutoff = .true.
PURPOSE
- Switch on and off the use of cut off parameters.
- These cut-offs are necessary when working with dispersion relations to deduce the real part.
baryonWidthVacuum/Delta_width [ Global module-variables ]
[ Top ] [ baryonWidthVacuum ] [ Global module-variables ]
SOURCE
integer, save :: Delta_width = 1
PURPOSE
Select a parametrization for the Delta width:
- 1 = Manley (GiBUU default, cf. Manley/Saleski, Phys. Rev. D 45, 1992)
- 2 = Dmitriev (Dmitriev/Sushkov/Gaarde, Nucl. Phys. A 459, 1986)
- 3 = Moniz (Koch/Moniz/Ohtsuka, Ann. of Phys. 154, 1984)
- 4 = Verwest (Phys. Lett. B 83, 1979)
- 5 = UrQMD (Bass et al., Prog. Part. Nucl. Phys. 41, 1998)
baryonWidthVacuum/getParameters [ Subroutines ]
[ Top ] [ baryonWidthVacuum ] [ Subroutines ]
NAME
subroutine getParameters(a,b,c,flag)
PURPOSE
return the values of ...
baryonWidthVacuum/readInput [ Subroutines ]
[ Top ] [ baryonWidthVacuum ] [ Subroutines ]
NAME
subroutine readInput
PURPOSE
Reads input in jobcard out of namelist "BaryonWidthVacuum".
baryonWidthVacuum/BaryonWidthVacuum [ Namelists ]
[ Top ] [ baryonWidthVacuum ] [ Namelists ]
NAME
NAMELIST /BaryonWidthVacuum/
PURPOSE
Includes the input switches:
baryonWidthVacuum/monopoleFormfactor [ Functions ]
[ Top ] [ baryonWidthVacuum ] [ Functions ]
NAME
real function monopoleFormfactor(mass,pole,lambda)
PURPOSE
...
baryonWidthVacuum/vacuumWidth [ Subroutines ]
[ Top ] [ baryonWidthVacuum ] [ Subroutines ]
NAME
function vacuumWidth (mass, partID, ratio, rho_AB_atPole) result (gammaTotal)
PURPOSE
This routine calculates the total vacuum decay width of a baryonic resonance, i.e. the sum of all partial decay widths, and the branching ratios for each channel as a function of the offshell mass (m^2 = p_mu p^mu). Parameters taken from Manley et al. Phys. Rev. D45 (1992) 4002 and PDG. The mass dependence of the resonances is treated according to Manley.
INPUTS
OUTPUT
- real, dimension(1:nDecays) :: ratio -- branching ratio = partial width / full width for all 2 body decay channels of the baryons
- real, dimension(1:nDecays) :: rho_AB_atPole -- rho_ab(poleMass) of specific decay channel according Effenberger Dr. thesis, eq 2.76
- real :: gammaTotal -- full width in GeV
baryonWidthVacuum/stableFinalState [ Subroutines ]
[ Top ] [ baryonWidthVacuum ] [ Subroutines ]
NAME
subroutine stableFinalState (mass, poleMass, mass1, mass2, L, partialWidth_pole, partialWidth_mass, rho_AB_Pole)
PURPOSE
calculate the partial width for the decay into two stable particles. Manley et al. Phys. Rev. D45 (1992) 4002.
NOTES
decay only allowed if:
INPUTS
- integer :: L -- Angular Momentum
- real :: polemass -- pole mass of mother resonance
- real :: mass -- mass of mother resonance
- real :: mass1 -- mass of first decay product
- real :: mass2 -- mass of second decay product
- real :: partialWidth_pole -- partial width of decayChannel at pole mass
OUTPUT
- real :: partialWidth_mass -- partial width at real mass
- real :: rho_AB_Pole -- Equation 2.76 of Effe Dr. evaluated at pole
baryonWidthVacuum/Delta_Dmitriev [ Subroutines ]
[ Top ] [ baryonWidthVacuum ] [ Subroutines ]
NAME
subroutine Delta_Dmitriev (mass, partialWidth_pole, partialWidth_mass, rho_AB_pole)
PURPOSE
Calculate the Delta width according to: Dmitriev/Sushkov/Gaarde, Nucl. Phys. A 459 (1986) 503-524
INPUTS
- real :: mass -- mass of mother resonance
- real :: partialWidth_pole -- partial width of decayChannel at pole mass
OUTPUT
- real :: partialWidth_mass -- partial width at real mass
- real :: rho_AB_Pole -- rho_ab as defined in eq. (2.75) of Effenberger PhD evaluated at pole
baryonWidthVacuum/Delta_Moniz [ Subroutines ]
[ Top ] [ baryonWidthVacuum ] [ Subroutines ]
NAME
subroutine Delta_Moniz (mass, partialWidth_pole, partialWidth_mass, rho_AB_pole)
PURPOSE
Calculate the Delta width according to: Koch/Moniz/Ohtsuka, Ann. of Phys. 154 (1984) 99
INPUTS
- real :: mass -- mass of mother resonance
- real :: partialWidth_pole -- partial width of decayChannel at pole mass
OUTPUT
- real :: partialWidth_mass -- partial width at real mass
- real :: rho_AB_Pole -- rho_ab as defined in eq. (2.75) of Effenberger PhD evaluated at pole
baryonWidthVacuum/Delta_Verwest [ Subroutines ]
[ Top ] [ baryonWidthVacuum ] [ Subroutines ]
NAME
subroutine Delta_Verwest (mass, partialWidth_pole, partialWidth_mass, rho_AB_pole)
PURPOSE
Calculate the Delta width according to: B.J. Verwest, Phys. Lett. B 83 (1979) 161.
INPUTS
- real :: mass -- mass of mother resonance
- real :: partialWidth_pole -- partial width of decayChannel at pole mass
OUTPUT
- real :: partialWidth_mass -- partial width at real mass
- real :: rho_AB_Pole -- rho_ab as defined in eq. (2.75) of Effenberger PhD evaluated at pole
baryonWidthVacuum/Delta_Bass [ Subroutines ]
[ Top ] [ baryonWidthVacuum ] [ Subroutines ]
NAME
subroutine Delta_Bass (mass, partialWidth_pole, partialWidth_mass, rho_AB_pole)
PURPOSE
Calculate the Delta width as used in UrQMD, cf.: Bass et al., Prog. Part. Nucl. Phys. 41 (1998) 255-369.
INPUTS
- real :: mass -- mass of mother resonance
- real :: partialWidth_pole -- partial width of decayChannel at pole mass
OUTPUT
- real :: partialWidth_mass -- partial width at real mass
- real :: rho_AB_Pole -- rho_ab as defined in eq. (2.75) of Effenberger PhD evaluated at pole
baryonWidthVacuum/semistableFinalState [ Subroutines ]
[ Top ] [ baryonWidthVacuum ] [ Subroutines ]
NAME
subroutine semistableFinalState (mass, polemass, idStable, idUnstable, L, partialWidth_pole, partialWidth_mass, rho_AB_Pole)
PURPOSE
Calculate the partial width for the decay into one stable and one unstable particle.
Calculates the partial width dependend on mass of a resonance decaying into one stable and one unstable decay product. According to Manley and Effenberger' Dr. Thesis equation 2.76.
INPUTS
- real :: mass -- mass of mother resonance
- real :: polemass -- polemass of mother resonance
- integer :: idUnstable -- ID of unstable decay product
- integer :: idStable -- ID of stable decay product
- integer :: L -- angular momentum of final state
- real :: partialWidth_pole -- partial width at pole of resonance
OUTPUT
- real :: partialWidth_mass -- partial width at real mass
- real :: rho_AB_Pole -- Equation 2.76 of Effe Dr. evaluated at pole
baryonWidthVacuum/rho_AB_Integrand [ Functions ]
[ Top ] [ baryonWidthVacuum ] [ Functions ]
NAME
real function rho_AB_Integrand(mu)
NOTES
This is the integrand of rho_ab(mu) in Effenbergers Dr.-Thesis, page 27, formula 2.76. Only in the case of only one unstable particle!
baryonWidthVacuum/rhoDeltaFinalState [ Subroutines ]
[ Top ] [ baryonWidthVacuum ] [ Subroutines ]
NAME
subroutine rhoDeltaFinalState(mass,poleMass,L,partialWidth_pole,partialWidth_mass,rho_AB_atPole)
PURPOSE
Calculate Resonance decays into delta and rho.
INPUTS
- integer :: L -- Angular Momentum
- real :: mass -- mass of resonance
- real :: partialWidth_pole -- partial widht of decayChannel at pole mass
- real :: poleMass -- pole mass of resonance
OUTPUT
- real :: partialWidth_mass -- partial width at real mass
- real :: rho_AB_atPole -- Equation 2.76 of Effe Dr. thesis evaluated at pole mass
rhoDeltaFinalState/deltaRho [ Functions ]
[ Top ] [ rhoDeltaFinalState ] [ Functions ]
NAME
function deltaRho (srts, ang, flag) result (integral)
NOTES
This routine calculates the integral of the Delta rho final state It calculates rho_AB as quoted in equation 2.76 in Effenbergers Dr. thesis