The12C(n,n′)3αCross Section up to 60 MeV
Author:
Affiliation:
1. Los Alamos National Laboratory, P.O. Box 1663, Los Alamos, New Mexico 87545
Publisher
Informa UK Limited
Subject
Nuclear Energy and Engineering
Link
https://www.tandfonline.com/doi/pdf/10.13182/NSE84-A17144
Reference20 articles.
1. J. LACHKAR, F. COCU, G. HAOUT, P. LeFLOCH, Y. PATIN, and J. SIGAUD, “An Evaluation of the Neutron Induced Scattering, Reaction and Photo-Production Cross Sections of Carbon,” NEANDC (E) 168 “L,” INDC (FR)-7/L, Service Physique Nucléaire Bruyéres-le-Chatel (1975).
2. Improved predictions of neutron detection efficiency resulting from new measurements of 12C(n,p) and 12C(n,d) reactions at 56 MeV
3. A compilation of n-p and n-C cross sections and their use in a Monte Carlo program to calculate the neutron detection efficiency in plastic scintillator in the energy range 1–300 MeV
4. Study of the reaction 12C(n, 3α)n from threshold to En = 35 MeV
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1. Neutron-induced light charged particle production in carbon at 96 MeV;Nuclear Physics A;2005-01
2. Evaluation of neutron cross sections of carbon-12 for energies up to 80 MeV;J NUCL SCI TECHNOL;1997
3. Evaluation of Neutron Cross Sections of Carbon-12 for Energies up to 80MeV;Journal of Nuclear Science and Technology;1997-02
4. Calculation and Evaluation of Cross Sections and Kerma Factors for Neutrons up to 100 MeV on Carbon;Nuclear Science and Engineering;1996-05
5. Intermediate-State Structure in the 12C(n,n3α) and 16O(n,n4α) Breakup Induced by 22.5 and 25.4 MeV Neutrons;Nuclear Data for Science and Technology;1992
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