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Effects of the nuclear structure of fission fragments on the high-energy prompt fission gamma-ray spectrum in U-235(n(th), f)

机译:裂变片段核结构对U-235的高能促进裂变γ射线光谱的影响(N(TH),F)

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摘要

The prompt fission gamma-ray energy spectrum for cold-neutron-induced fission of U-235 was measured in the energy range E-gamma = 0.8-20 MeV, by gaining a factor of about 10(5) in statistics compared to the measurements performed so far. The spectrum exhibits local bump structures at E-gamma approximate to 4 MeV and approximate to 6 MeV, and also a broad one at approximate to 15 MeV. In order to understand the origins of these bumps, the gamma-ray spectra were calculated using a statistical Hauser-Feshbach model, taking into account the deexcitation of all the possible primary fission fragments. It is shown that the bump at approximate to 4 MeV is created by the transitions between the discrete levels in the fragments around Sn-132, and the bump at approximate to 6 MeV mostly comes from the complementary light fragments. It is also indicated that a limited number of nuclides, which have high-spin states at low excitation energies, can contribute to the bump structure around E-gamma approximate to 15 MeV, induced by the transition feeding into the low-lying high-spin states.
机译:在与测量相比,通过在统计量增加约10(5)个统计量度,测量用于冷中子诱导的U-235的U-235诱导裂变的U-235诱导的U-235诱导裂变的促进裂变伽马射线能谱到目前为止表演。光谱在E-GAMMA近似为4MeV并近似为6meV,以及近15MeV的局部凸块结构。为了理解这些凸块的起源,使用统计的Hauser-Feshbach模型计算伽马射线光谱,考虑到所有可能的主要裂变片段的脱释。结果表明,近似到4MeV的凸块由SN-132周围的片段中的离散水平之间的过渡产生,并且近似到6meV的凸块主要来自互补的光片段。还表明,在低励磁能量下具有高旋转状态的有限数量的核素可以有助于E-GAMMA近似为15meV的凸块结构,该过渡进入低洼的高旋转诱导状态。

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  • 来源
    《Physical review, C》 |2019年第4期|共7页
  • 作者单位

    Japan Atom Energy Agcy Adv Sci Res Ctr Tokai Ibaraki 3191195 Japan;

    Japan Atom Energy Agcy Adv Sci Res Ctr Tokai Ibaraki 3191195 Japan;

    Japan Atom Energy Agcy Adv Sci Res Ctr Tokai Ibaraki 3191195 Japan;

    Japan Atom Energy Agcy Adv Sci Res Ctr Tokai Ibaraki 3191195 Japan;

    Japan Atom Energy Agcy Adv Sci Res Ctr Tokai Ibaraki 3191195 Japan;

    Japan Atom Energy Agcy Nucl Sci &

    Engn Ctr Tokai Ibaraki 3191195 Japan;

    Inst Laue Langevin F-38000 Grenoble France;

    Inst Laue Langevin F-38000 Grenoble France;

    Inst Laue Langevin F-38000 Grenoble France;

    European Commiss Joint Res Ctr B-2440 Geel Belgium;

    Univ Bordeaux CNRS IN2P3 CENBG 19 Chemin Solarium F-33175 Gradignan France;

    Univ Bordeaux CNRS IN2P3 CENBG 19 Chemin Solarium F-33175 Gradignan France;

    Univ Bordeaux CNRS IN2P3 CENBG 19 Chemin Solarium F-33175 Gradignan France;

    Univ Bordeaux CNRS IN2P3 CENBG 19 Chemin Solarium F-33175 Gradignan France;

    Univ Paris Sud Ctr Sci Nucl &

    Sci Mat F-91405 Orsay France;

    Univ Paris Sud Ctr Sci Nucl &

    Sci Mat F-91405 Orsay France;

    Chinese Acad Sci Inst Modern Phys Lanzhou 730000 Gansu Peoples R China;

    Kyoto Univ Inst Integrated Radiat &

    Nucl Sci Kumatori Osaka 5904094 Japan;

    Kyoto Univ Inst Integrated Radiat &

    Nucl Sci Kumatori Osaka 5904094 Japan;

    Kyoto Univ Inst Integrated Radiat &

    Nucl Sci Kumatori Osaka 5904094 Japan;

    Lund Univ Dept Phys S-22100 Lund Sweden;

    Los Alamos Natl Lab Theoret Div Los Alamos NM 87545 USA;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 原子核物理学、高能物理学;
  • 关键词

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