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DC Field | Value | Language |
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dc.contributor.author | Noji, S. | - |
dc.contributor.author | Zegers, R.G.T. | - |
dc.contributor.author | Austin, S.M. | - |
dc.contributor.author | Baugher, T. | - |
dc.contributor.author | Bazin, D. | - |
dc.contributor.author | Brown, A.B. | - |
dc.contributor.author | Campbell, C.M. | - |
dc.contributor.author | Cole, A.L. | - |
dc.contributor.author | Doster, H.J. | - |
dc.contributor.author | Gade, A. | - |
dc.contributor.author | Guess, C.J. | - |
dc.contributor.author | Gupta, S. | - |
dc.contributor.author | Hitt, G.W. | - |
dc.contributor.author | Langer, G. | - |
dc.contributor.author | Lipschutz, S. | - |
dc.contributor.author | Lunderberg, E. | - |
dc.contributor.author | Meharchand, R. | - |
dc.contributor.author | Meisel, Z. | - |
dc.contributor.author | Perdikakis, G. | - |
dc.contributor.author | Pereira, J. | - |
dc.contributor.author | Recchia, F. | - |
dc.contributor.author | Schatz, H. | - |
dc.contributor.author | Scott, M. | - |
dc.contributor.author | Stroberg, S.R. | - |
dc.contributor.author | Sullivan, C. | - |
dc.contributor.author | Valdez, L. | - |
dc.contributor.author | Walz, C. | - |
dc.contributor.author | Weisshaar, D. | - |
dc.contributor.author | William, S.J. | - |
dc.contributor.author | Wimmer, K. | - |
dc.date.accessioned | 2016-11-22T07:21:35Z | - |
dc.date.available | 2016-11-22T07:21:35Z | - |
dc.date.issued | 2016-11-22 | - |
dc.identifier.uri | http://localhost:8080/xmlui/handle/123456789/550 | - |
dc.description.abstract | The Gamow-Teller strength in the β+ direction to Sc46 was extracted via the Ti46(t,He3+γ) reaction at 115MeV/u. The γ-ray coincidences served to precisely measure the very weak Gamow-Teller transition to a final state at 991 keV. Although this transition is weak, it is crucial for accurately estimating electron-capture rates in astrophysical scenarios with relatively low stellar densities and temperatures, such as presupernova stellar evolution. Shell-model calculations with different effective interactions in the pf shell-model space do not reproduce the experimental Gamow-Teller strengths, which is likely due to sd-shell admixtures. Calculations in the quasiparticle random phase approximation that are often used in astrophysical simulations also fail to reproduce the experimental Gamow-Teller strength distribution, leading to strongly overestimated electron-capture rates. Because reliable theoretical predictions of Gamow-Teller strengths are important for providing astrophysical electron-capture reaction rates for a broad set of nuclei in the lower pf shell, we conclude that further theoretical improvements are required to match astrophysical needs. | en_US |
dc.language.iso | en_US | en_US |
dc.subject | Electron-capture | en_US |
dc.subject | Random phase approximations | en_US |
dc.subject | Stellar evolutions | en_US |
dc.subject | Astrophysical simulations | en_US |
dc.subject | Shells (structures) | en_US |
dc.title | β+ Gamow-teller transition strengths from Ti 46 and stellar electron-capture rates | en_US |
dc.type | Article | en_US |
Appears in Collections: | Year-2014 |
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