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1%\subsection{The escaping particle and coherent effects \editor{Gunter}}
2
3When a nucleon other than the incident particle leaves the nucleus,
4the ground state of the nucleus changes. The energy of the outgoing
5particle cannot be such that the total mass of the new nucleus would
6be below its ground state mass. To avoid this, we reduce the energy of
7an outgoing nucleons by the mass-difference  of old and new nucleus.
8
9Furthermore, the momentum of the final exited nucleus derived from
10energy momentum balance may be such that its mass is below its ground
11state mass. In this case, we arbitrarily scale the momenta of all
12outgoing particles by a factor derived from the mass of the nucleus
13and the mass of the system of outgoing particles.
14
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