Point-by-Point model description of average prompt neutron data as a function of total kinetic energy of fission fragments
The experimental data of average prompt neutron multiplicity as a function of total kinetic energy of fragments <ν>(TKE) exhibit, especially in the case of 252Cf(SF), different slopes dTKE/dν and different behaviours at low TKE values. The Point-by-Point (PbP) model can describe these differen...
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| Format: | Article |
| Language: | English |
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EDP Sciences
2013-03-01
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| Series: | EPJ Web of Conferences |
| Online Access: | http://dx.doi.org/10.1051/epjconf/20134207007 |
| _version_ | 1828139173203148800 |
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| author | Tudora A. |
| author_facet | Tudora A. |
| author_sort | Tudora A. |
| collection | DOAJ |
| description | The experimental data of average prompt neutron multiplicity as a function of total kinetic energy of fragments <ν>(TKE) exhibit, especially in the case of 252Cf(SF), different slopes dTKE/dν and different behaviours at low TKE values. The Point-by-Point (PbP) model can describe these different behaviours. The higher slope dTKE/dν and the flattening of <ν> at low TKE exhibited by a part of experimental data sets is very well reproduced when the PbP multi-parametric matrix ν(A,TKE) is averaged over a double distribution Y(A,TKE). The lower slope and the almost linear behaviour over the entire TKE range exhibited by other data sets is well described when the same matrix ν(A,TKE) is averaged over a single distribution Y(A). In the case of average prompt neutron energy in SCM as a function of TKE, different dTKE/dε slopes are also obtained by averaging the same PbP matrix ε(A,TKE) over Y(A,TKE) and over Y(A). The results are exemplified for three fissioning systems benefiting of experimental data as a function of TKE: 252Cf(SF), 235U(nth,f) and 239Pu(nth,f). In the case of 234U(n,f) for the first time it was possible to calculate <ν>(TKE) and <ε>(TKE) at many incident energies by averaging the PbP multi-parametric matrices over the experimental Y(A,TKE) distributions recently measured at IRMM for 14 incident energies in the range 0.3-5 MeV. The results revealed that the slope dTKE/dν does not vary with the incident energy and the flattening of <ν> at low TKE values is more pronounced at low incident energies. The average model parameters dependences on TKE resulted from the PbP treatment allow the use of the most probable fragmentation approach, having the great advantage to provide results at many TKE values in a very short computing time compared to PbP and Monte Carlo treatments. |
| first_indexed | 2024-04-11T18:49:49Z |
| format | Article |
| id | doaj.art-80afe21c93894a649e769e0dcaee1de7 |
| institution | Directory Open Access Journal |
| issn | 2100-014X |
| language | English |
| last_indexed | 2024-04-11T18:49:49Z |
| publishDate | 2013-03-01 |
| publisher | EDP Sciences |
| record_format | Article |
| series | EPJ Web of Conferences |
| spelling | doaj.art-80afe21c93894a649e769e0dcaee1de72022-12-22T04:08:29ZengEDP SciencesEPJ Web of Conferences2100-014X2013-03-01420700710.1051/epjconf/20134207007Point-by-Point model description of average prompt neutron data as a function of total kinetic energy of fission fragmentsTudora A.The experimental data of average prompt neutron multiplicity as a function of total kinetic energy of fragments <ν>(TKE) exhibit, especially in the case of 252Cf(SF), different slopes dTKE/dν and different behaviours at low TKE values. The Point-by-Point (PbP) model can describe these different behaviours. The higher slope dTKE/dν and the flattening of <ν> at low TKE exhibited by a part of experimental data sets is very well reproduced when the PbP multi-parametric matrix ν(A,TKE) is averaged over a double distribution Y(A,TKE). The lower slope and the almost linear behaviour over the entire TKE range exhibited by other data sets is well described when the same matrix ν(A,TKE) is averaged over a single distribution Y(A). In the case of average prompt neutron energy in SCM as a function of TKE, different dTKE/dε slopes are also obtained by averaging the same PbP matrix ε(A,TKE) over Y(A,TKE) and over Y(A). The results are exemplified for three fissioning systems benefiting of experimental data as a function of TKE: 252Cf(SF), 235U(nth,f) and 239Pu(nth,f). In the case of 234U(n,f) for the first time it was possible to calculate <ν>(TKE) and <ε>(TKE) at many incident energies by averaging the PbP multi-parametric matrices over the experimental Y(A,TKE) distributions recently measured at IRMM for 14 incident energies in the range 0.3-5 MeV. The results revealed that the slope dTKE/dν does not vary with the incident energy and the flattening of <ν> at low TKE values is more pronounced at low incident energies. The average model parameters dependences on TKE resulted from the PbP treatment allow the use of the most probable fragmentation approach, having the great advantage to provide results at many TKE values in a very short computing time compared to PbP and Monte Carlo treatments.http://dx.doi.org/10.1051/epjconf/20134207007 |
| spellingShingle | Tudora A. Point-by-Point model description of average prompt neutron data as a function of total kinetic energy of fission fragments EPJ Web of Conferences |
| title | Point-by-Point model description of average prompt neutron data as a function of total kinetic energy of fission fragments |
| title_full | Point-by-Point model description of average prompt neutron data as a function of total kinetic energy of fission fragments |
| title_fullStr | Point-by-Point model description of average prompt neutron data as a function of total kinetic energy of fission fragments |
| title_full_unstemmed | Point-by-Point model description of average prompt neutron data as a function of total kinetic energy of fission fragments |
| title_short | Point-by-Point model description of average prompt neutron data as a function of total kinetic energy of fission fragments |
| title_sort | point by point model description of average prompt neutron data as a function of total kinetic energy of fission fragments |
| url | http://dx.doi.org/10.1051/epjconf/20134207007 |
| work_keys_str_mv | AT tudoraa pointbypointmodeldescriptionofaveragepromptneutrondataasafunctionoftotalkineticenergyoffissionfragments |