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《中国物理C》(英文)编辑部
2024年10月30日

Multi-modal calculations of prompt fission neutrons from 238U(n, f) at low induced energy

  • Properties of prompt fission neutrons from 238U(n, f) are calculated for incident neutron energies below 6 MeV using the multi-modal model, including the prompt fission neutron spectrum, the average prompt fission neutron multiplicity, and the prompt fission neutron multiplicity as a function of the fission fragment mass υ(A) (usually named “sawtooth” data) The three most dominant fission modes are taken into account. The model parameters are determined on the basis of experimental fission fragment data. The predicted results are in good agreement with the experimental data.
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  • [1] Kerdraon D, Billebaud A, Brissot R et al. Prog. Nucl. Energy, 2003, 42(1): 112 Kornilov N V, Hambsch F J, Fabry I. In Proceedings of the International Conference on Nuclear Data for Science and Technology. Bern: EPD Science, 2007. 3873 Terrell J. Phys. Rev., 1959, 113(2): 5274 Madland D G, Nix J R. Nucl. Sci. Eng., 1982, 81(2): 2135 Vladuca G, Tudora A. Computer Physics Communications, 2000, 125(1-3): 2216 Marten H, Ruben A, Seeliger D. IAEA-INDC (NDS), 1989, 220: 2457 Browne J C, Dietrich F S. Phys. Rev. C, 1974, 10(6): 25458 Madland D G, LaBauve R J, Nix J R. IAEA-INDC(NDS), 1989, 220: 2599 Tudora A, Morillon B, Hambsch F J et al. Nucl. Phys. A, 2005, 756(1-2): 17610 WANG Fu-Cheng, HU Ji-Min. J Phys. G: Nucl. Part. Phys., 1989, 15(6): 82911 Knitter H H, Hambsch F J, Jorgensen C B et al. Z. Naturf., 1987, 42a: 78612 Brosa U, Grossmann S, Muller A. Phys. Rep., 1990, 197(4): 16713 Schillebeeckx P, Wagemans C, Deruytter A et al. Nucl. Phys. A, 1992, 545(3): 62314 FAN T S, HU J M, BAO S L. Nucl. Phys. A, 1995, 591(2): 16115 FAN T S, HU J M, BAO S L. HEPNP, 1996, 20(2): 187 (in Chinese)16 Demattè L, Wagemans C, Barthéléy R et al. Nucl. Phys. A,1997, 617(3): 33117 Ohsava T, Hayashi H, Ohtani Y. In Proceedings of the International Conference on Nuclear Data for Science and Technology, ICTP Trieste, Italy. (Italian Physical Society, Bologna), 1997. 36518 Ohsawa T, Horiguchi T, Hayashi H. Nucl. Phys. A, 1999, 653(1): 1719 Ohsawa T, Horiguchi T, Mitsuhashi M. Nucl. Phys. A, 2000, 665(1): 320 Ohsawa T J. Nucl. Radiochem. Sci., 2002, 3(1): 9321 Hambsch F J, Oberstedt S, Vladuca G et al. Nucl. Phys. A, 2002, 709(1-4): 8522 Hambsch F J, Oberstedt S, Tudora A et al. Nucl. Phys. A, 2003, 726(3-4): 24823 Hambsch F J, Tudora A, Vladuca G et al. Annals of Nuclear Energy, 2005, 32(10): 103224 Vladuca G, Tudora A. Annals of Nuclear Energy, 2001, 28(16): 164325 ZHENG N, DING Y, ZHONG C L et al. Chin. Phys. B, 2009, 18(4): 126 ZHENG N, FAN T S, DING Y et al. Chin. Phys. C (HEP NP), 2010, 34(1): 4927 Weisskopf V F. Rev. Mod. Phys., 1957, 29(2): 17428 Frehaut J. IAEA INDC (NDS), 1989, 220: 9929 Vives F, Hambsch F J, Bax H et al. Nucl. Phys. A, 2000, 662(1-3): 6330 Reisdorf W, Unik J P, Griffin H C et al. Nucl. Phys. A, 1971, 177(2): 33731 Dilg W, Schantl W, Vonach H. Nucl. Phys. A, 1973, 217(2): 26932 Plyaskin V I, Kosilov R A. Physics of Atomic Nuclei, 2000, 63(5): 75233 Baba M, Wakabayashi H, Ishikawa M et al. IAEA-INDC (NDS),1989, 220: 14934 Boykov G S, Dmitriev V D, Kudyaev G A et al. Annals of Nuclear Energy, 1994, 21(10): 58535 www-nds.iaea.org/exfor/, Experimental Nuclear Reaction Data (EXFOR) Database (2010), entry numbers: 14215003, 20075002, 20490002, 21135006, 23054006, 32606002,40342002, 40429003, 40665002
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ZHENG Na, ZHONG Chun-Lai and FAN Tie-Shuan. Multi-modal calculations of prompt fission neutrons from 238U(n, f) at low induced energy[J]. Chinese Physics C, 2011, 35(10): 930-934. doi: 10.1088/1674-1137/35/10/008
ZHENG Na, ZHONG Chun-Lai and FAN Tie-Shuan. Multi-modal calculations of prompt fission neutrons from 238U(n, f) at low induced energy[J]. Chinese Physics C, 2011, 35(10): 930-934.  doi: 10.1088/1674-1137/35/10/008 shu
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Received: 2010-12-28
Revised: 1900-01-01
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Multi-modal calculations of prompt fission neutrons from 238U(n, f) at low induced energy

Abstract: Properties of prompt fission neutrons from 238U(n, f) are calculated for incident neutron energies below 6 MeV using the multi-modal model, including the prompt fission neutron spectrum, the average prompt fission neutron multiplicity, and the prompt fission neutron multiplicity as a function of the fission fragment mass υ(A) (usually named “sawtooth” data) The three most dominant fission modes are taken into account. The model parameters are determined on the basis of experimental fission fragment data. The predicted results are in good agreement with the experimental data.

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