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Shell-model studies of the astrophysical mirror rp-reactions $^{34}$S (p,y) $^{35}$ C1 and $^{34g,m}$ C1(py)$^{35}Ar

The two mirror rp-reactions $^{34}$S (p,y) $^{35}$ C1 and $^{34g,m}$ C1(py)$^{35}$Ar were studied via a shell-model approach. At energies in the resonance region near the proton- emission threshold many negative-parity states appear. We present results of calculations in a full (0+1)hω model space w...

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Detalles Bibliográficos
Autores principales: Richter, W A, Brown, B Alex, Longland, R, Wrede, C, Fry, C
Lenguaje:eng
Publicado: CERN 2019
Acceso en línea:http://cds.cern.ch/record/2669073
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author Richter, W A
Brown, B Alex
Longland, R
Wrede, C
Fry, C
author_facet Richter, W A
Brown, B Alex
Longland, R
Wrede, C
Fry, C
author_sort Richter, W A
collection CERN
description The two mirror rp-reactions $^{34}$S (p,y) $^{35}$ C1 and $^{34g,m}$ C1(py)$^{35}$Ar were studied via a shell-model approach. At energies in the resonance region near the proton- emission threshold many negative-parity states appear. We present results of calculations in a full (0+1)hω model space which addresses this problem. Energies, spectroscopic factors and proton-decay widths are calculated for input into the reaction rates. Comparisons are also made with a recent experimental determination of the reaction rate for the first reaction. The thermonuclear $^{34g,m}$C1(py)$^{35}$Ar reaction rates are unknown because of a lack of experimental data. The rates for transitions from the ground state of $^{34}$C1 as well as from the isomeric first excited state of $^{34}$C1 are explicitly calculated taking into account the relative populations of the two states.
id oai-inspirehep.net-1726631
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2019
publisher CERN
record_format invenio
spelling oai-inspirehep.net-17266312019-09-30T06:29:59Zhttp://cds.cern.ch/record/2669073engRichter, W ABrown, B AlexLongland, RWrede, CFry, CShell-model studies of the astrophysical mirror rp-reactions $^{34}$S (p,y) $^{35}$ C1 and $^{34g,m}$ C1(py)$^{35}ArThe two mirror rp-reactions $^{34}$S (p,y) $^{35}$ C1 and $^{34g,m}$ C1(py)$^{35}$Ar were studied via a shell-model approach. At energies in the resonance region near the proton- emission threshold many negative-parity states appear. We present results of calculations in a full (0+1)hω model space which addresses this problem. Energies, spectroscopic factors and proton-decay widths are calculated for input into the reaction rates. Comparisons are also made with a recent experimental determination of the reaction rate for the first reaction. The thermonuclear $^{34g,m}$C1(py)$^{35}$Ar reaction rates are unknown because of a lack of experimental data. The rates for transitions from the ground state of $^{34}$C1 as well as from the isomeric first excited state of $^{34}$C1 are explicitly calculated taking into account the relative populations of the two states.CERNoai:inspirehep.net:17266312019
spellingShingle Richter, W A
Brown, B Alex
Longland, R
Wrede, C
Fry, C
Shell-model studies of the astrophysical mirror rp-reactions $^{34}$S (p,y) $^{35}$ C1 and $^{34g,m}$ C1(py)$^{35}Ar
title Shell-model studies of the astrophysical mirror rp-reactions $^{34}$S (p,y) $^{35}$ C1 and $^{34g,m}$ C1(py)$^{35}Ar
title_full Shell-model studies of the astrophysical mirror rp-reactions $^{34}$S (p,y) $^{35}$ C1 and $^{34g,m}$ C1(py)$^{35}Ar
title_fullStr Shell-model studies of the astrophysical mirror rp-reactions $^{34}$S (p,y) $^{35}$ C1 and $^{34g,m}$ C1(py)$^{35}Ar
title_full_unstemmed Shell-model studies of the astrophysical mirror rp-reactions $^{34}$S (p,y) $^{35}$ C1 and $^{34g,m}$ C1(py)$^{35}Ar
title_short Shell-model studies of the astrophysical mirror rp-reactions $^{34}$S (p,y) $^{35}$ C1 and $^{34g,m}$ C1(py)$^{35}Ar
title_sort shell-model studies of the astrophysical mirror rp-reactions $^{34}$s (p,y) $^{35}$ c1 and $^{34g,m}$ c1(py)$^{35}ar
url http://cds.cern.ch/record/2669073
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