Abstract:Background: Lifetimes of nuclear excited states in fission fragments have been studied in the past following isotope separation, thus giving access mainly to the fragments' daughters and only to long-lived isomeric states in the primary fragments. For the first time now, short-lived excited states in the primary fragments, produced in neutron-induced prompt fission of 235 U and 241 Pu, were studied within the EXILL&FATIMA campaign at the intense neutron-beam facility of the Institute Laue-Langevin in Grenoble.… Show more
“…For optimum efficiency the FATIMA detectors were placed as close as possible to the target, at 8.5 cm. Several results for lifetimes in the picosecond and nanosecond region have already been published from the EXILL&FATIMA campaign [22][23][24][25][26]. A more detailed description of the experimental setup can be found in Ref.…”
Excited states of the neutron-rich nucleus 148 Ce have been populated by neutron-induced fission of 235 U and 241 Pu samples. Their electromagnetic decays were studied by means of γ-ray coincidence spectroscopy with fast-timing capabilities. Lifetimes of the 2 + 1 and 4 + 1 states of 148 Ce were obtained and their E2 decay rates deduced. The B 4/2 = B(E2; 4 + 1 → 2 + 1)/B(E2; 2 + 1 → 0 + 1) ratio indicates that 148 Ce is a transitional nucleus while the N = 88/90 shape phase transition evolves into a gradual change of nuclear deformation for proton numbers Z < 60.
“…For optimum efficiency the FATIMA detectors were placed as close as possible to the target, at 8.5 cm. Several results for lifetimes in the picosecond and nanosecond region have already been published from the EXILL&FATIMA campaign [22][23][24][25][26]. A more detailed description of the experimental setup can be found in Ref.…”
Excited states of the neutron-rich nucleus 148 Ce have been populated by neutron-induced fission of 235 U and 241 Pu samples. Their electromagnetic decays were studied by means of γ-ray coincidence spectroscopy with fast-timing capabilities. Lifetimes of the 2 + 1 and 4 + 1 states of 148 Ce were obtained and their E2 decay rates deduced. The B 4/2 = B(E2; 4 + 1 → 2 + 1)/B(E2; 2 + 1 → 0 + 1) ratio indicates that 148 Ce is a transitional nucleus while the N = 88/90 shape phase transition evolves into a gradual change of nuclear deformation for proton numbers Z < 60.
“…At this energy, based on prompt fission fragment spectroscopy following the spontaneous fission of 248 Cm [7], a candidate transition was proposed to be the decay of the first 3 − state to the first 2 + state. However, the respective coincidences have not been observed following neutron-induced fission of 235 U [8] nor in the spontaneous fission of 252 Cf [9]. It should be noted though that there are three peaks visible, which have not been observed before, and they lie in the same energy range where the missing 3 − → 2 + transition is expected.…”
“…On the other hand, the recent experimental result of Ref. [13] beyond the neutron magic number N = 82 turn out to show a different nature in the structure evolution as compared to the neighboring Sn [14] and Xe [52] nuclides.…”
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