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[1211] | 1 | %\subsection{The escaping particle and coherent effects \editor{Gunter}} |
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| 2 | |
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| 3 | When a nucleon other than the incident particle leaves the nucleus, |
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| 4 | the ground state of the nucleus changes. The energy of the outgoing |
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| 5 | particle cannot be such that the total mass of the new nucleus would |
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| 6 | be below its ground state mass. To avoid this, we reduce the energy of |
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| 7 | an outgoing nucleons by the mass-difference of old and new nucleus. |
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| 8 | |
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| 9 | Furthermore, the momentum of the final exited nucleus derived from |
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| 10 | energy momentum balance may be such that its mass is below its ground |
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| 11 | state mass. In this case, we arbitrarily scale the momenta of all |
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| 12 | outgoing particles by a factor derived from the mass of the nucleus |
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| 13 | and the mass of the system of outgoing particles. |
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| 14 | |
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