Fission properties of233Th
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Cited by (25)
Measurement of fission products yields in the quasi-mono-energetic neutron-induced fission of <sup>232</sup>Th
2016, Nuclear Physics ACitation Excerpt :Similarly, the fission fragment yields data of neutron-deficient Th isotopes such as 220–229Th in the excitation energy range of the GDR region due to electromagnetic fission in inverse kinematics are available in Refs. [63–65]. From these data, it was observed that the yields of fission products are available in a wide range of neutron- [24–51] and bremsstrahlung- [52–62] induced fissions of 232Th. However, the fission product yields data within neutron energies of 8 to 14.8 MeV are available in limited way except our data at the neutron energies of 6.35, 8.53 and 10.09 MeV [50].
Mass distribution in the quasi-mono-energetic neutron-induced fission of <sup>238</sup>U
2013, Nuclear Physics ACitation Excerpt :In the literature, some data are available in the reactor neutron-induced fission of 232Th [21,22] and 238U [23,24]. However, fission yield data for various other mono-energetic neutron-induced fissions of 232Th [25–48] and 238U [48–73] are available in literature. On the other hand, yields of fission fragments in the excitation energy range of the GDR region due to electromagnetic fission in inverse kinematics [74–76] are available for neutron-deficient lighter actinides such as 220–229Th and 231–234U.
Mass and kinetic energy distributions for the photofission of <sup>232</sup>Th with 6.44 to 13.15 MeV bremsstrahlung
1993, Nuclear Physics, Section AFission fragment velocities, masses, and energies from <sup>232</sup>Th(n, f) in the resonance-energy region
1992, Nuclear Physics, Section AComparison of different methods for the determination of fission fragment velocity, mass, and energy distributions for <sup>232</sup>Th(n, f)
1989, Nuclear Inst. and Methods in Physics Research, A