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PENELOPE 2003 - OECD Nuclear Energy Agency

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Chapter 3<br />

Electron and positron interactions<br />

In this chapter we consider the interactions of fast electrons and positrons of kinetic<br />

energy E with matter. For the sake of simplicity, we start by assuming that the particles<br />

move in a single-element medium of atomic number Z and density ρ, with N atoms per<br />

unit volume. The extension to compounds, and mixtures, is normally done on the<br />

basis of the additivity approximation, i.e. the molecular DCS is approximated as the<br />

incoherent sum of the atomic DCSs of all the atoms in a molecule.<br />

E<br />

θ<br />

E<br />

E<br />

E−W<br />

θ<br />

θ s<br />

E s<br />

= W−U i<br />

Elastic scattering<br />

I nelastic scattering<br />

W<br />

E +<br />

E<br />

θ<br />

E−W<br />

E<br />

E −<br />

θ −<br />

θ +<br />

Bremsstrahlung emission<br />

P o sitro n annih ilatio n<br />

Figure 3.1: Basic interactions of electrons and positrons with matter.

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