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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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