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Influence of the odd neutron on the fragment characteristics in the photofission of 235U
Institution:1. IEK-5 Photovoltaik, Forschungszentrum Jülich GmbH, D-52425 Jülich, Germany;2. Institute of Materials Science, TU Darmstadt, D-64287 Darmstadt, Germany;3. Evonik Industries AG, CREAVIS-Science to Business, D-45722 Marl, Germany;1. Département de radiothérapie, centre Georges-François-Leclerc, 1, rue du Professeur-Marion, BP 77980, 21079 Dijon cedex, France;2. Département de radiologie, centre Georges-François-Leclerc, 1, rue du Professeur-Marion, 21079 Dijon cedex, France;3. Département de médecine nucléaire, centre Georges-François-Leclerc, 1, rue du Professeur-Marion, 21079 Dijon cedex, France;1. Research Center for Electron Photon Science (ELPH), Tohoku University, Sendai 982-0826, Japan;2. Department of Physics, Yamagata University, Yamagata 990-8560, Japan;3. Department of Physics, Tohoku University, Sendai 980-8578, Japan;4. Department of Information Science, Tohoku Gakuin University, Sendai 981-3193, Japan;5. Department of Physics, University of Tokyo, Tokyo 113-0033, Japan;6. Institute of Particle and Nuclear Studies, High Energy Accelerator Research Organization (KEK), Tsukuba 305-0801, Japan
Abstract:Cumulative and independent post-neutron product yields were measured for the photofission on 235U with 6.5, 7.0, and 8.4 MeV bremsstrahlung, applying γ-spectrometric methods on catcherfoils and pneumatically transported 235U-samples. The independent yields for the heavy (A = 128–149) fragments were deduced. Post-neutron mass and isotonic yield distributions were studied together with the elemental yield distributions and the proton odd-even effect. The mass distribution shows about an equal yield for the mass regions around A = 134 (N = 82) and A = 142 (N = 86–88). The proton odd-even effect for the fission of this odd-A nucleus remains at a constant value δp = 25% in the studied compound nucleus excitation energy region, indicating that the odd neutron does not influence the energy transfer between the different degrees of freedom during the descent from saddle to scission point in a substantial way.
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