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

被引:15
|
作者
Makii, H. [1 ]
Nishio, K. [1 ]
Hirose, K. [1 ]
Orlandi, R. [1 ]
Leguillon, R. [1 ]
Ogawa, T. [2 ]
Soldner, T. [3 ]
Koster, U. [3 ]
Pollitt, A. [3 ]
Hambsch, F-J [4 ]
Tsekhanovich, I [5 ]
Aiche, M. [5 ]
Czajkowski, S. [5 ]
Mathieu, L. [5 ]
Petrache, C. M. [6 ,7 ]
Astier, A. [6 ,7 ]
Guo, S. [8 ,9 ]
Ohtsuki, T. [10 ]
Sekimoto, S. [10 ]
Takamiya, K. [10 ]
Frost, R. J. W. [11 ]
Kawano, T. [12 ]
机构
[1] Japan Atom Energy Agcy, Adv Sci Res Ctr, Tokai, Ibaraki 3191195, Japan
[2] Japan Atom Energy Agcy, Nucl Sci & Engn Ctr, Tokai, Ibaraki 3191195, Japan
[3] Inst Laue Langevin, F-38000 Grenoble, France
[4] European Commiss, Joint Res Ctr, B-2440 Geel, Belgium
[5] Univ Bordeaux, CNRS, IN2P3, CENBG, 19 Chemin Solarium, F-33175 Gradignan, France
[6] Univ Paris Sud, Ctr Sci Nucl & Sci Mat, F-91405 Orsay, France
[7] CNRS, IN2P3, F-91405 Orsay, France
[8] Chinese Acad Sci, Inst Modern Phys, Lanzhou 730000, Gansu, Peoples R China
[9] Univ Chinese Acad Sci, Sch Nucl Sci & Technol, Beijing 100049, Peoples R China
[10] Kyoto Univ, Inst Integrated Radiat & Nucl Sci, Kumatori, Osaka 5904094, Japan
[11] Lund Univ, Dept Phys, S-22100 Lund, Sweden
[12] Los Alamos Natl Lab, Theoret Div, Los Alamos, NM 87545 USA
关键词
NEUTRON-INDUCED FISSION; MULTIMODAL ANALYSIS; EMISSION; MULTIPLICITY; FORMULA; MODELS; SYSTEM;
D O I
10.1103/PhysRevC.100.044610
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
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.
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页数:7
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