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Proton and $\gamma$- partial widths of astrophysically important states of $^{30}$S studied by the $\beta$-delayed decay of $^{31}$Ar
Resonances just above the proton threshold in $^{30}$S affect the $^{29}$P$(p,\gamma)^{30}$S reaction under astrophysical conditions. The ($p,\gamma$)-reaction rate is currently determined indirectly and depends on the properties of the relevant resonances. We present here a method for finding the r...
Autores principales: | , , , , , , , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2013
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevC.87.055808 http://cds.cern.ch/record/1525846 |
_version_ | 1780929268681801728 |
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author | Koldste, G.T. Blank, B. Borge, M.J.G. Briz, J.A. Carmona-Gallardo, M. Fraile, L.M. Fynbo, H.O.U. Giovinazzo, J. Johansen, J.G. Jokinen, A. Jonson, B. Kurturkian-Nieto, T. Kusk, J.H. Nilsson, T. Perea, A. Pesudo, V. Picado, E. Riisager, K. Saastamoinen, A. Tengblad, O. Thomas, J.C. Van de Walle, J. |
author_facet | Koldste, G.T. Blank, B. Borge, M.J.G. Briz, J.A. Carmona-Gallardo, M. Fraile, L.M. Fynbo, H.O.U. Giovinazzo, J. Johansen, J.G. Jokinen, A. Jonson, B. Kurturkian-Nieto, T. Kusk, J.H. Nilsson, T. Perea, A. Pesudo, V. Picado, E. Riisager, K. Saastamoinen, A. Tengblad, O. Thomas, J.C. Van de Walle, J. |
author_sort | Koldste, G.T. |
collection | CERN |
description | Resonances just above the proton threshold in $^{30}$S affect the $^{29}$P$(p,\gamma)^{30}$S reaction under astrophysical conditions. The ($p,\gamma$)-reaction rate is currently determined indirectly and depends on the properties of the relevant resonances. We present here a method for finding the ratio between the proton- and $\gamma$- partial widths of resonances in $^{30}$S. The widths are determined from the $\beta -2p$ and $\beta -p-\gamma$-decay of $^{31}$Ar, which is produced at ISOLDE, CERN. Experimental limits on the ratio between the proton- and $\gamma$- partial widths for astrophysical relevant levels in $^{30}$S have been found for the first time. A level at 4689.2(24)keV is identified in the $\gamma$-spectrum, and an upper limit on the $\Gamma_{p}/\Gamma_{\gamma}$ ratio of 0.26 (95% C.L.) is found. In the two-proton spectrum two levels at 5227(3)keV and 5847(4)keV are identified. These levels were previously seen to $\gamma$-decay and upper limits on the $\Gamma_{\gamma}/\Gamma_{p}$ ratio of 0.5 and 9, respectively, (95% C.L.) are found, where the latter differs from previous calculations. |
id | cern-1525846 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2013 |
record_format | invenio |
spelling | cern-15258462021-12-07T07:49:58Zdoi:10.1103/PhysRevC.87.055808http://cds.cern.ch/record/1525846engKoldste, G.T.Blank, B.Borge, M.J.G.Briz, J.A.Carmona-Gallardo, M.Fraile, L.M.Fynbo, H.O.U.Giovinazzo, J.Johansen, J.G.Jokinen, A.Jonson, B.Kurturkian-Nieto, T.Kusk, J.H.Nilsson, T.Perea, A.Pesudo, V.Picado, E.Riisager, K.Saastamoinen, A.Tengblad, O.Thomas, J.C.Van de Walle, J.Proton and $\gamma$- partial widths of astrophysically important states of $^{30}$S studied by the $\beta$-delayed decay of $^{31}$ArNuclear Physics - ExperimentResonances just above the proton threshold in $^{30}$S affect the $^{29}$P$(p,\gamma)^{30}$S reaction under astrophysical conditions. The ($p,\gamma$)-reaction rate is currently determined indirectly and depends on the properties of the relevant resonances. We present here a method for finding the ratio between the proton- and $\gamma$- partial widths of resonances in $^{30}$S. The widths are determined from the $\beta -2p$ and $\beta -p-\gamma$-decay of $^{31}$Ar, which is produced at ISOLDE, CERN. Experimental limits on the ratio between the proton- and $\gamma$- partial widths for astrophysical relevant levels in $^{30}$S have been found for the first time. A level at 4689.2(24)keV is identified in the $\gamma$-spectrum, and an upper limit on the $\Gamma_{p}/\Gamma_{\gamma}$ ratio of 0.26 (95% C.L.) is found. In the two-proton spectrum two levels at 5227(3)keV and 5847(4)keV are identified. These levels were previously seen to $\gamma$-decay and upper limits on the $\Gamma_{\gamma}/\Gamma_{p}$ ratio of 0.5 and 9, respectively, (95% C.L.) are found, where the latter differs from previous calculations.Resonances just above the proton threshold in 30S affect the 29P(p,γ)30S reaction under astrophysical conditions. The (p,γ)-reaction rate is currently determined indirectly and depends on the properties of the relevant resonances. We present here a method for finding the ratio between the proton and γ partial widths of resonances in 30S. The widths are determined from the β2p- and βpγ-decay of 31Ar, which is produced at the ISOLDE radioactive ion beam facility at the European research organization CERN. Experimental limits on the ratio between the proton and γ partial widths for astrophysical relevant levels in 30S have been found for the first time. A level at 4689.2(24)keV is identified in the γ spectrum, and an upper limit on the Γp/Γγ ratio of 0.26 (95% C.L.) is found. In the two-proton spectrum two levels at 5227(3)keV and 5847(4)keV are identified. These levels were previously seen to γ decay and upper limits on the Γγ/Γp ratio of 0.5 and 9, respectively, (95% C.L.) are found, where the latter differs from previous calculations.Resonances just above the proton threshold in 30S affect the 29P(p,gamma)30S reaction under astrophysical conditions. The (p,gamma)-reaction rate is currently determined indirectly and depends on the properties of the relevant resonances. We present here a method for finding the ratio between the proton and gamma partial widths of resonances in 30S. The widths are determined from the beta-2p and beta-p-gamma decay of 31Ar, which is produced at the ISOLDE facility at the European research organization CERN. Experimental limits on the ratio between the proton and gamma partial widths for astrophysical relevant levels in 30S have been found for the first time. A level at 4688(5) keV is identified in the gamma spectrum, and an upper limit on the proton to gamma width of 0.26 (95 % C.L.) is found. In the two-proton spectrum two levels at 5227(3) keV and 5847(4) keV are identified. These levels are previously seen to gamma decay and upper limits on the gamma to proton width of 0.5 and 9, respectively, (95 % C.L.) are found, where the latter differs from previous calculations.arXiv:1303.1940oai:cds.cern.ch:15258462013-03-11 |
spellingShingle | Nuclear Physics - Experiment Koldste, G.T. Blank, B. Borge, M.J.G. Briz, J.A. Carmona-Gallardo, M. Fraile, L.M. Fynbo, H.O.U. Giovinazzo, J. Johansen, J.G. Jokinen, A. Jonson, B. Kurturkian-Nieto, T. Kusk, J.H. Nilsson, T. Perea, A. Pesudo, V. Picado, E. Riisager, K. Saastamoinen, A. Tengblad, O. Thomas, J.C. Van de Walle, J. Proton and $\gamma$- partial widths of astrophysically important states of $^{30}$S studied by the $\beta$-delayed decay of $^{31}$Ar |
title | Proton and $\gamma$- partial widths of astrophysically important states of $^{30}$S studied by the $\beta$-delayed decay of $^{31}$Ar |
title_full | Proton and $\gamma$- partial widths of astrophysically important states of $^{30}$S studied by the $\beta$-delayed decay of $^{31}$Ar |
title_fullStr | Proton and $\gamma$- partial widths of astrophysically important states of $^{30}$S studied by the $\beta$-delayed decay of $^{31}$Ar |
title_full_unstemmed | Proton and $\gamma$- partial widths of astrophysically important states of $^{30}$S studied by the $\beta$-delayed decay of $^{31}$Ar |
title_short | Proton and $\gamma$- partial widths of astrophysically important states of $^{30}$S studied by the $\beta$-delayed decay of $^{31}$Ar |
title_sort | proton and $\gamma$- partial widths of astrophysically important states of $^{30}$s studied by the $\beta$-delayed decay of $^{31}$ar |
topic | Nuclear Physics - Experiment |
url | https://dx.doi.org/10.1103/PhysRevC.87.055808 http://cds.cern.ch/record/1525846 |
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