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Total cross-section for e e annihilation

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| Geant 3.16  |               GEANT User's Guide              | PHYS350  ##
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Author(s) : L.Urban Submitted: 26.10.84 Origin : Same Revised: 19.12.92

Subroutines

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                    |CALL GANNII  |
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GANNII tabulates the mean free path at initialization time as a function of the medium and of the energy (see JMATE data structure). The energy binning is set within the array ELOW (common block /GCMULO/) in the routine GPHYSI. GANNII is called from GPHYSI.

Method

The mean free path, lambda, for a positron to interact via annihilation is

    lambda =((1)/ (sum ))= ((A)/(Nrhosigma(Z,E)))                      (1)

where

sum
macroscopic cross-section (in 1/cm)
N
Avogadro's number
Z,A
atomic number and weight of the medium
rho
density of the medium
sigma(Z,E)
total annihilation cross-section per atom.

For the annihilation cross-section the formula of Heitler is used. The total cross-section is given by [bib-EGS3], [bib-HEIT]:

                       2                    2                  2                       2                            2
    sigma(Z, E)= ((Zpir )/(gamma+1))[((gamma +4gamma+1)/ (gamma -1))ln(gamma+sqrt(gamma - 1))-((gamma+3)/(sqrt(gamma  -1)))](2)
                       0

where r is the classical radius of the electron and gamma= E/m. In the 0

case of a compound/mixture the effective atomic number and weight (evaluated in GSMIXT are used in computing the cross-section. This treatment of the compounds/mixtures is correct in those processes where the cross-section depends on the atomic number Z linearly (annihilation, Moeller and Bhabha scattering, Compton scattering).