2021
DOI: 10.1140/epja/s10050-021-00434-7
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Neutron capture on $$^{16}$$O within the framework of RMF + ACCC + BCS for astrophysical simulations

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Cited by 3 publications
(3 citation statements)
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“…The cross section of neutron capture on 16 O mainly consists of three parts: direct capture, resonance, and the interference between the direct capture and the resonance. We have estimated these terms separately and found that the contribution from low-lying resonance to Maxwellian-averaged cross section (MACS) progressively increases as the energy goes beyond 70 keV, in which the resonant cross section takes the form of Breit-Wigner formula with an energy-dependent decay width [2,3].…”
Section: Introductionmentioning
confidence: 99%
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“…The cross section of neutron capture on 16 O mainly consists of three parts: direct capture, resonance, and the interference between the direct capture and the resonance. We have estimated these terms separately and found that the contribution from low-lying resonance to Maxwellian-averaged cross section (MACS) progressively increases as the energy goes beyond 70 keV, in which the resonant cross section takes the form of Breit-Wigner formula with an energy-dependent decay width [2,3].…”
Section: Introductionmentioning
confidence: 99%
“…Usually, the decay width of a resonant state is defined as a constant in textbooks and some references [4,5]. Except for a constant width, an energy-dependent width is also utilized in some works [6][7][8], including our former attempts [2,3]. There are two ways commonly used to obtain an energy-dependent width.…”
Section: Introductionmentioning
confidence: 99%
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