In electron microbeam techniques, the particle beam is focused on the mater
ial to be analysed. When the election beam enters the target, the electrons
give rise to ionization processes producing secondary electrons and photon
s, the latter being used to characterize the material. As a consequence, a
detailed description of the photon diffusion requires the solution of two c
oupled equations describing respectively electron and photon diffusion. The
approach considering two transport equations, even if formally correct, is
almost unaffordable because of the high mathematical complexity of the ele
ctron transport equation. In this article, an alternative approach is sugge
sted which is based on the use of an approximate solution for the electron
transport using the Fokker-Planck equation [5]. The resulting electron dist
ribution, computed analytically as a solution of the above equation, is ver
y similar to the ionization distribution and is used as the source term in
the Boltzmann transport equation describing the photon diffusion in the mat
erial. The 3D photon transport equation for unpolarised photons with this s
ource term is solved to obtain a detailed description of the photon fluores
cence from a homogeneous slab.