Bulletin of the American Physical Society
5th Joint Meeting of the APS Division of Nuclear Physics and the Physical Society of Japan
Volume 63, Number 12
Tuesday–Saturday, October 23–27, 2018; Waikoloa, Hawaii
Session 1WCB: Nuclear Fission Turns 80 II |
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Chair: Ramona Vogt, Lawrence Livermore National Laboratory Room: Hilton Kohala 2 |
Tuesday, October 23, 2018 11:00AM - 11:30AM |
1WCB.00001: Fission of fermium isotopes using Langevin calculations Invited Speaker: Yoshihiro Aritomo Fragment mass distributions in the fission of 246,264Fm at low excitation energies are studied using the three-dimensional Langevin equations with potential energy landscape of the two-centershell model. After overcoming the 1st saddle point, the large-amplitude shape motion along a specific shape degrees of freedom is found in the 2nd minimum of the potential energy landscape due to the nature of the friction tensor in the Langevin equation. The 2nd-saddle points are found at two positions which links to the compact-symmetric scission and elongated-asymmetric scission, respectively, and they are located at both ends of the shape motion in the 2nd minimum. Height of the mass-symmetric 2nd saddle point relative to the asymmetric saddle point decreases toward heavier Fm isotopes. It was shown that not only the structure of the potential energy landscape but also the wide-range directive uctuation of nuclear shape have a crucial role to understand the mechanism of the sharp transition of mass asymmetry. |
Tuesday, October 23, 2018 11:30AM - 12:00PM |
1WCB.00002: Survey of current US fission experiments Invited Speaker: Fredrik Tovesson As we approach the 80th anniversary of the discovery of nuclear fission, one might reasonably expect that there is little new information to be learned in this mature field. In reality, however, there is still a strong desire to advance our understanding of fission, which has led to a resurgence in fission experiments over the last decade. This is driven both by scientific curiosity, the role of fission in astrophysical processes, and the need for accurate and precise nuclear data for technology. As theoretical models of fission start to be more predictive and truly incorporate correlations, new experiments are essential for testing and validation purposes. |
Tuesday, October 23, 2018 12:00PM - 12:30PM |
1WCB.00003: Measurement of high-energy prompt fission gamma rays in 235U(nth,f) Invited Speaker: Tatsuhiko Ogawa We have measured the energy spectrum of prompt gamma-rays produced in thermal-neutron induced fission of 235U, up to 20 MeV. The measurement was performed at the PF1B beamline of the Institut Laue Langevin using a detection system composed of two multi-wire proportional counters (MWPCs) and two LaBr3(Ce) scintillation detectors (thickness: 12.7 cm and radius: 15.9 cm), placed on the opposite sides of the 235U target facing the neutron beam. The large LaBr3(Ce) scintillation detectors were employed to achieve high detection efficiency at high energy. The target thickness was 117 mg/cm2, and the neutron flux at the target position amounted to 1.0x108 neutrons/cm2/s. The gamma-rays from fission fragments, intercepted by the LaBr3(Ce) detectors were recorded in coincidence with fragments detected in the MWPCs, for the total duration of 437 hours. By unfolding the response of LaBr3(Ce) scintillation detectors, the gamma-ray energy spectrum was obtained. The resulting raw gamma-ray energy spectrum shows an exponential decline up to 10 MeV, with humps at 4 MeV and 6 MeV, similar to the spectrum from spontaneous fission of 252Cf in earlier studies. Above 10 MeV, the spectrum exhibits a broad bump that we tentatively attribute to the giant dipole resonance. Compared to the literature data for prompt gamma-rays from the thermal neutron induced fission of actinides, whose energy spectra are known only up to 8 MeV, we have significantly increased the sensitivity and revealed the structure of the spectrum between 10 and 20 MeV. Our approach would open new studies on the structure of neutron-rich fission fragments as well as lead to better understanding of fission mechanism. |
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