Non-resonant direct p- and d-wave neutron capture by 12C
| dc.creator | Kikuchi, T. | |
| dc.creator | Nagai, Y. | |
| dc.creator | Suzuki, T. S. | |
| dc.creator | Shima, T. | |
| dc.creator | Kii, T. | |
| dc.creator | Igashira, M. | |
| dc.creator | Mengoni, A. | |
| dc.creator | Otsuka, T. | |
| dc.date | 1998-02-17 | |
| dc.date.accessioned | 2026-07-07T11:11:34Z | |
| dc.date.available | 2026-07-07T11:11:34Z | |
| dc.description | Discrete gamma-rays from the neutron capture state of 13C to its low-lying bound states have been measured using pulsed neutrons at En = 550 keV. The partial capture cross sections have been determined to be 1.7+/-0.5, 24.2+/-1.0, 2.0+/-0.4 and 1.0+/-0.4 microb for the ground (1/2-), first (1/2+), second (3/2-) and third (5/2+) excited states, respectively. From a comparison with theoretical predictions based on the non-resonant direct radiative capture mechanism, we could determine the spectroscopic factor for the 1/2+ state to be 0.80 +/- 0.04, free from neutron-nucleus interaction ambiguities in the continuum. In addition we have detected the contribution of the non-resonant d-wave capture component in the partial cross sections for transitions leading to the 1/2- and 3/2- states. While the s-wave capture dominates at En < 100 keV, the d-wave component turns out to be very important at higher energies. From the present investigation the 12C(n,gamma)13C reaction rate is obtained for temperatures in the range 10E+7 - 10E+10 K. | |
| dc.description | Accepted for publication in Phys. Rev. C. - 16 pages + 8 figures | |
| dc.identifier | https://arxiv.org/abs/nucl-th/9802051 | |
| dc.identifier | http://arxiv.org/abs/nucl-th/9802051 | |
| dc.identifier | Phys.Rev.C57:2724-2730,1998 | |
| dc.identifier | doi:10.1103/PhysRevC.57.2724 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/191140 | |
| dc.subject | Nuclear Theory | |
| dc.title | Non-resonant direct p- and d-wave neutron capture by 12C | |
| dc.type | text |