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[1208] | 1 | \section{MC procedure.} |
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| 2 | |
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| 3 | \hspace{1.0em}The Monte Carlo procedure of calculation of characteristics of |
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| 4 | fission fragments can be outlined as follows: |
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| 5 | \begin{itemize} |
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| 6 | \item Select fission mode (symmetric or asymmetric). |
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| 7 | Sample atomic number $A_f$ of a fission |
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| 8 | fragment according to experimentaly defined distribution, which consists |
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| 9 | from the "symmetrical" and "asymmetrical" parts; |
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| 10 | \item For choosen $A_f$ randomly in accordance with |
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| 11 | Gaussian distribution and the experimentaly defined |
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| 12 | dispersion and average |
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| 13 | select the fragment charge $Z_f$; |
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| 14 | \item For |
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| 15 | choosen $A_f, Z_f$ sample |
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| 16 | the kinetic energy of fragments |
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| 17 | according to the Gaussian |
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| 18 | distribution |
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| 19 | with experimentaly defined average values |
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| 20 | and dispersions; |
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| 21 | \item Applying energy conservation and using fragment ground state masses |
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| 22 | calculate excitation energy of fragments and share it between fragments |
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| 23 | assuming that fragments have equal temperatures; |
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| 24 | \item Calculate absolute value of the c.m. |
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| 25 | fragment momentum (non-relativistic kinematics |
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| 26 | is used) and sample fragment flay off angles assuming isotropical |
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| 27 | angular distribution of fragments; |
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| 28 | \item Perform evaporation for the excited fragments. |
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| 29 | \end{itemize} |
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