Received: January 30, 2021
Accepted: May 25, 2021
Published Online: August 31, 2021
Keywords:
Ternary fission, Pre-existence probability, Relative yield, Excitation energy
Ternary decay is comparatively a rare phenomenon. The yield distribution for the thermal neutron-induced fission of 236U was investigated within the Temperature-dependent Relativistic Mean Field (TRMF) approach and statistical theory. Binding energy obtained from TRMF for the ground state and at a specific temperature is used to evaluate the fragment excitation energy, which is needed to calculate the nuclear level density. Using the ternary convolution, the yield for α-accompanied fission of 236U* is calculated. Initial results are presented which shows a maximum yield for the fragment pair Tc + Ag +α. Further, the ternary pre-existence probability for the spontaneous fission of 236U was studied considering fixed third fragments of α,10Be and 14C using the area of the overlapping region. No significant change in the yield distribution was observed when fragment deformations are considered. However, the heavy group for the probable pair remains as 132Sn with a change in mass number of the lighter fragment.
The unstable nuclei undergo radioactive decay by emitting radiations such as α, β and γ. Nuclear fission is another important process in which the nucleus splits into particles spontaneously or through induced processes along with the release of energy. When the excitation energy of the fragments is smaller, no neutrons are emitted and the phenomenon is known as cold fission. In such processes, one of the fragments was found to be associated with the closed-shell nuclei.
Ternary fission is an exotic decay mode in which the parent system splits into three fragments, and can be used as a probe to study the nuclear structure information. α accompanied fission is mostly observed as the light charged particle accompanied fission with its energy spectrum from 6 to 40 MeV. The size of the third particle varies from neutron to the case of true ternary fission in which the three fission fragments are of equal mass. Light particles such as H, Li, Be, and C were also observed in the spontaneous fission of various parent systems.
The experimental investigation [1] for the neutron-induced fission of 235U indicated the presence of one α-particle per 250 fissions. Further Tsien et al., [2] studied the mass and kinetic energy of fission fragments in the tripartition of 235U. Mostly the third particle was observed perpendicular to the other two heavier masses. In addition, the authors reported the quadripartition of the uranium
The unstable nuclei undergo radioactive decay by emitting radiations such as α, β and γ. Nuclear fission is another important process in which the nucleus splits into particles spontaneously or through induced processes along with the release of energy. When the excitation energy of the fragments is smaller, no neutrons are emitted and the phenomenon is known as cold fission. In such processes, one of the fragments was found to be associated with the closed-shell nuclei.
Ternary fission is an exotic decay mode in which the parent system splits into three fragments, and can be used as a probe to study the nuclear structure information. α accompanied fission is mostly observed as the light charged particle accompanied fission with its energy spectrum from 6 to 40 MeV. The size of the third particle varies from neutron to the case of true ternary fission in which the three fission fragments are of equal mass. Light particles such as H, Li, Be, and C were also observed in the spontaneous fission of various parent systems.
The experimental investigation [1] for the neutron-induced fission of 235U indicated the presence of one α-particle per 250 fissions. Further Tsien et al., [2] studied the mass and kinetic energy of fission fragments in the tripartition of 235U. Mostly the third particle was observed perpendicular to the other two heavier masses. In addition, the authors reported the quadripartition of the uranium