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1%\subsection{Pauli blocking simulation\editor{Gunter}}
2
3The cross sections used in this model are cross sections for free particles. In
4the nucleus these cross sections are reduced to effective cross sections by
5Pauli-blocking due to Fermi statistics.
6
7 For nucleons created by a collision, ie. an inelastic
8scattering or from decay, we check that all secondary nucleons occupy a state
9allowed by Fermi statistics. We assume that the nucleus in its ground state and
10all states below Fermi energy are occupied. All secondary nucleons  therefore
11must have a momentum $p_i$ above local Fermi momentum $p_F(r)$, i.e.
12\begin{equation}
13p_i > p_F^{max}(r).
14\end{equation}
15
16If any of the nucleons of the collision has a momentum below the local Fermi
17momentum, then the collision is Pauli blocked.  The reaction products are
18discarded, and the original particles continue the cascade.
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