Gamow-Teller strengths in 24Na using the 24Mg(t,3He) reaction at 115 AMeV
| dc.creator | Howard, M. E. | |
| dc.creator | Zegers, R. G. T. | |
| dc.creator | Austin, Sam M. | |
| dc.creator | Bazin, D. | |
| dc.creator | Brown, B. A. | |
| dc.creator | Cole, A. L. | |
| dc.creator | Davids, B. | |
| dc.creator | Famiano, M. | |
| dc.creator | Fujita, Y. | |
| dc.creator | Gade, A. | |
| dc.creator | Galaviz, D. | |
| dc.creator | Hitt, G. W. | |
| dc.creator | Matos, M. | |
| dc.creator | Reitzner, S. D. | |
| dc.creator | Samanta, C. | |
| dc.creator | Schradin, L. J. | |
| dc.creator | Shimbara, Y. | |
| dc.creator | Smith, E. E. | |
| dc.creator | Simenel, C. | |
| dc.date | 2008-07-15 | |
| dc.date.accessioned | 2026-07-07T11:44:49Z | |
| dc.date.available | 2026-07-07T11:44:49Z | |
| dc.description | Gamow-Teller transitions from 24Mg to 24Na were studied via the (t,3He) reaction at 115 AMeV using a secondary triton beam produced via fast fragmentation of 150 AMeV 16O ions. Compared to previous (t,3He) experiments at this energy that employed a primary alpha beam, the secondary beam intensity is improved by about a factor of five. Despite the large emittance of the secondary beam, an excitation-energy resolution of ~200 keV is achieved. A good correspondence is found between the extracted Gamow-Teller strength distribution and those available from other charge-exchange probes. Theoretical calculations using the newly developed USDA and USDB sd-shell model interactions reproduce the data well. | |
| dc.description | 10 pages, 3 figures | |
| dc.identifier | https://arxiv.org/abs/0807.2402 | |
| dc.identifier | http://arxiv.org/abs/0807.2402 | |
| dc.identifier | Phys.Rev.C78:047302,2008 | |
| dc.identifier | doi:10.1103/PhysRevC.78.047302 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/201688 | |
| dc.subject | Nuclear Experiment | |
| dc.title | Gamow-Teller strengths in 24Na using the 24Mg(t,3He) reaction at 115 AMeV | |
| dc.type | text |