2009
DOI: 10.1103/physrevc.80.024611
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Calculation of nuclear reaction cross sections on excited nuclei with the coupled-channels method

Abstract: We calculate nuclear cross sections on excited nuclei in the fast neutron energy range. We partition the whole process into two contributions: the direct reaction part and the compound nuclear reactions. A coupled-channels method is used for calculating the direct transition of the nucleus from the initial excited state, which is a member of the ground-state rotational band, to the final ground and excited low-lying levels. This process is strongly affected by the channel coupling. The compound nuclear reactio… Show more

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Cited by 26 publications
(22 citation statements)
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References 34 publications
(35 reference statements)
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“…These results indicate that the compound formation cross sections shown in Fig. 3 of [1] for the ground and first excited states should be closer together in a fully converged calculation. The values for the nonadiabatic to adiabatic ratios of Fig.…”
Section: B Rare-earth Nucleimentioning
confidence: 88%
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“…These results indicate that the compound formation cross sections shown in Fig. 3 of [1] for the ground and first excited states should be closer together in a fully converged calculation. The values for the nonadiabatic to adiabatic ratios of Fig.…”
Section: B Rare-earth Nucleimentioning
confidence: 88%
“…We employ the definition of Edmonds [21] for the rotation matrices D I MK (ω), where ω = (α, β, γ) represents the set of Euler angles required to rotate the space-fixed axes of the deformed target into the body-fixed axes 1 . Eq.…”
Section: B the Adiabatic Approximation For Rigid Rotorsmentioning
confidence: 99%
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“…In this context, partial cross sections feeding the ground states or isomers are particularly crucial in certain cases of the s-process nucleosynthesis [1][2][3], or of astrophysical environments such as neutron stars or supernovae where reactions on the isomeric states can occur [4,5].…”
Section: Introductionmentioning
confidence: 99%
“…The CoH 3 code included discrete level information for the first 47 levels, up to the 11.32-MeV 2 + state in 20 Ne. Because neon is a deformed nucleus (β 2 = 0.73 for 20 Ne and β 2 = 0.63 for 22 Ne), the CoH 3 code used a HauserFeshbach calculation, including transmission coefficients obtained from a coupled-channels calculation [18]. Although CoH 3 reproduced the data more accurately than TALYS, the discrepancy between the CoH 3 calculation and data is most likely due to the use of the spherical Koning-Delaroche potential in the coupled-channels calculation.…”
mentioning
confidence: 99%