2020
DOI: 10.1007/978-3-030-58082-7_3
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CoH3: The Coupled-Channels and Hauser-Feshbach Code

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Cited by 17 publications
(13 citation statements)
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“…The fission probabilities P f (E) for the first and second chances are calculated with the CoH 3 code [67]. The fission parameters, such as the fission barrier, curvature, and level density, are adjusted to reproduce the evaluated fission cross section of 235 U.…”
Section: Extrapolating To the Second Chance Fissionmentioning
confidence: 99%
“…The fission probabilities P f (E) for the first and second chances are calculated with the CoH 3 code [67]. The fission parameters, such as the fission barrier, curvature, and level density, are adjusted to reproduce the evaluated fission cross section of 235 U.…”
Section: Extrapolating To the Second Chance Fissionmentioning
confidence: 99%
“…However, the nuclear reaction codes that were employed to create the photonuclear data library -EM-PIRE [72,73], TALYS [74], CCONE [75], and CoH 3 [76] -have implemented relatively simple pre-equilibrium models for photonuclear reactions. In some cases, the exciton model for a neutron-induced reaction is considered as a surrogate for the photo-induced precompound process, and the initial configuration of 1p-0h or 2p-1h is assumed.…”
Section: Pre-equilibrium Particle Emissionmentioning
confidence: 99%
“…The modern Hauser-Feshbach nuclear reaction codes, EMPIRE [72,73], TALYS [74], CCONE [75], and CoH 3 [76], which are often utilized for nucleon-induced reaction calculations, are also capable of calculating photo-induced reaction cross sections. As a result, they are widely used in the evaluation of general purpose nuclear data libraries, and are combined with the advancedcapabilities utility codes to create ENDF-6 format data files.…”
Section: B Nuclear Reaction Codes For Photonuclear Data Evaluationmentioning
confidence: 99%
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“…The modern Hauser-Feshbach nuclear reaction codes such as EMPIRE [8], TALYS [9], CCONE [10], and CoH3 [11], used to calculate photo-induced reaction crosssections, also call for testing in a wide range of atomic masses and energies. Although at present there is a sufficient dataset on the experimental cross-sections in the GDR energy region [12,13], the use of the data on singleor two-particle reactions only, precludes testing various theoretical concepts, because the results of calculations by different models (e.g., nuclear level density LD 1-6 computation in the TALYS1.95 code) differ from each other only slightly.…”
Section: Introductionmentioning
confidence: 99%