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[1208] | 1 | \section{MC procedure.} |
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| 2 | |
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| 3 | The evaporation model algorithm consists |
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| 4 | from repeating steps of binary break-ups of |
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| 5 | the excited nuclear fragments: |
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| 6 | \begin{enumerate} |
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| 7 | \item Create a nuclear fragment: assign atomic mass number $A$, electrical |
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| 8 | charge $Z$, fragment four vector $P_0$, fragment excitation energy $E^{*}$ and |
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| 9 | fragment angular momentum $\vec{L}_0$; |
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| 10 | \item Calculate the probabilities of break-up channels and |
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| 11 | sample a channel; |
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| 12 | \item Sample evaporated fragment $b$ kinetic energy at rest of decaying fragment; |
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| 13 | \item Assuming isotropical evaporated fragments distribution, sample |
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| 14 | its flay off angles at rest of decaying fragment $b$; |
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| 15 | \item boost the evaporated and residual fragment momenta into observer frame. |
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| 16 | \item Calculate residual fragment atomic mass number $A_f$, electrical |
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| 17 | charge $Z_f$, fragment four vector $P_f$, fragment excitation energy |
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| 18 | $E_f^{*}$ and |
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| 19 | fragment angular momentum $\vec{L}_f$; |
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| 20 | \item Repeat this procedure starting from step (2) |
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| 21 | until no more fragment (the probabilities of break-up channels |
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| 22 | equal zero) can be evaporated. |
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| 23 | \end{enumerate} |
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