Total cross-section for photoelectric effect

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| Geant 3.16  |               GEANT User's Guide              | PHYS230  ##
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Author(s) : L.Urban Submitted: 26.10.84 Origin : Same Revised: 17.12.92

Subroutines

                    +--------------------------------+
                    |CALL GPHOTI  |
                    +--------------------------------+
                                  

GPHOTI calculates the total cross-section for the photoelectric effect. It tabulates the mean free path, lambda= ((1)/(Sigma)) (in cm), as a function of the medium and the energy [bib-STOR]. It calls the function GPHSIG for the total cross-section. The energy binning is set within the array ELOW (COMMON CGMULO) in the routine GPHYSI. GPHOTI is called at initialization time by GPHYSI.

                VALUE = GPHSIG(Z,EGAM)
                                  

GPHSIG calculates the total cross-section for the photoelectric effect of a photon with energy EGAM in material with atomic number Z. It is called by GPHOTI.

Method

The mean free path, lambda, for a photon to interact via photoelectric effect is given by

    lambda =((1)/ (sum ))  (in cm)                                     (1)

where sum , the macroscopic cross-sectioni, for an element is given as

    sum  =((Nrhosigma(Z, E     ))/(A))  in (1/cm)                      (2)
                          gamma

and for a compound or a mixture

    sum  =((Nrho sim sigma(Z ,E      ))/(sim p A )) = Nrhosim (w /A )* rho(Z ,E     )(3)
                            i  gamma          i i               i  i        i  gamma

where

  N         Avogadro's number
  Z(Z )     atomic number (of i'th component) of the medium
     i
  A(A )     atomic number (of i'th component) of the medium
     i
  rho       density
  sigma     total cross-section
  p         proportion by number of the i'th element in
   i        the material (p   ' w / A  wherew  the corresponding
                           i     i   i       i
            proportion by weight).

For 5<=Z< =100 the binding energy of the inner shells have been parameterized as:

            2                    3
    E (Z) =Z  (A + B Z+ C Z + D Z )  MeV                               (4)
     i          i   i    i 2   i

where, i= K,L ,L are as following: I II

   +------+------------------------------------------------------------
   |      |              |             |               |              |
   +------+------A-------+------B------+-------C-------+------D-------+
   |      |              |             |               |              |
   | K    |  0.66644e-5  | 0.22077e-6  |  -0.32552e-8  | 0.18199e-10  |
   | L    | -0.29179e-6  | 0.87983e-7  | - 0.12589e-8  | 0.69602e-11  |
   |  I   |              |             |               |              |
   | L    | -0.68606e-6  | 0.10078e-6  |  -0.14496e-8  | 0.78809e-11  |
   +--II--+--------------+-------------+---------------+--------------+
   |      |
                                  

Then the cross-section of the photoeletric effect can be parameterized as:

                                                                 2
                               (p /Z) +p X +p  +p Z +(p / X)+p  Z
                                 1      2    3   2     5 3    6
                                 +p (Z/X) +(p / X )+ (p Z )
                                   7         8         9
                                       2             2          3
                                 +p  (Z /X) +p  (Z/ X )+ p  (1/X )if  E>E (Z)
                  alpha beta       10         11          12             k
    sigma(Z, E)= Z     X    {  (p  /Z) +p  X +p                   if E  

    X =m/ E  ;  sigma in barn/atom                                     (6)

The fit was made over 301 data points chosen between 5<=Z< =100 and 10keV< =E<=50 MeV. The values of the parameters are put in the DATA statement within the function GPHSIG which compute the formula (4) in barn/atom. The accuracy of the fit is estimated to be Deltasigma/sigma<=25% near to the peaks, and Deltasigma/ sigma<=10% elsewhere.