Symmetric fission in the neutron-induced fission of Fm255
R.C. Ragaini, E.K. Hulet, R. W. Lougheed, J. F. Wild
Abstract
R.C. Ragaini, E.K. Hulet, R. W. Lougheed, J. F. Wild
Abstract
The kinetic energy distributions of coincident fission fragments from the thermal-neutron-induced fission of $^{255}\mathrm{Fm}$ and $^{251}\mathrm{Cf}$ have been measured with phosphorus-diffused silicon detectors. The most probable values for the postneutron total kinetic energy are 192.5\ifmmode\pm\else\textpm\fi{}2.9 MeV for $^{255}\mathrm{Fm}$ and 182.1\ifmmode\pm\else\textpm\fi{}2.7 MeV for $^{251}\mathrm{Cf}$. Fragment mass distributions were calculated without applying neutron emission corrections. The resultant mass and kinetic energy distributions for $^{255}\mathrm{Fm}$ indicate a predominantly asymmetric mass division combined with appreciable symmetric fission. Fragment pairs near mass symmetry were found to be unusually energetic, which is a characteristic shared with symmetric fission in $^{257}\mathrm{Fm}$ and $^{258}\mathrm{Fm}$. These results are well described by the two-center model of fission. Thermal-neutron-induced fission cross sections were measured as 3400\ifmmode\pm\else\textpm\fi{}170 b for $^{255}\mathrm{Fm}$ and 4800 \ifmmode\pm\else\textpm\fi{} 250 b for $^{251}\mathrm{Cf}$.[NUCLEAR REACTIONS, FISSION $^{255}\mathrm{Fm}(n,f)$, $^{251}\mathrm{Cf}(n,f)$, $E=0.025$ eV; measured $\ensuremath{\sigma}$, fragment $E$; deduced fragment masses.]
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The kinetic energy distributions of coincident fission fragments from the thermal-neutron-induced fission of $^{255}\mathrm{Fm}$ and $^{251}\mathrm{Cf}$ have been measured with phosphorus-diffused silicon detectors. The most probable values for the postneutron total kinetic energy are 192.5\ifmmode\pm\else\textpm\fi{}2.9 MeV for $^{255}\mathrm{Fm}$ and 182.1\ifmmode\pm\else\textpm\fi{}2.7 MeV for $^{251}\mathrm{Cf}$. Fragment mass distributions were calculated without applying neutron emission corrections. The resultant mass and kinetic energy distributions for $^{255}\mathrm{Fm}$ indicate a predominantly asymmetric mass division combined with appreciable symmetric fission. Fragment pairs near mass symmetry were found to be unusually energetic, which is a characteristic shared with symmetric fission in $^{257}\mathrm{Fm}$ and $^{258}\mathrm{Fm}$. These results are well described by the two-center model of fission. Thermal-neutron-induced fission cross sections were measured as 3400\ifmmode\pm\else\textpm\fi{}170 b for $^{255}\mathrm{Fm}$ and 4800 \ifmmode\pm\else\textpm\fi{} 250 b for $^{251}\mathrm{Cf}$.[NUCLEAR REACTIONS, FISSION $^{255}\mathrm{Fm}(n,f)$, $^{251}\mathrm{Cf}(n,f)$, $E=0.025$ eV; measured $\ensuremath{\sigma}$, fragment $E$; deduced fragment masses.]
Key concepts: Fission, Physics, Kinetic energy, Neutron, Nuclear physics, Neutron emission, Energy (signal processing), Neutron temperature