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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...
Autores principales: | , , , , |
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Lenguaje: | eng |
Publicado: |
CERN
2019
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Acceso en línea: | http://cds.cern.ch/record/2669073 |
_version_ | 1780962237468377088 |
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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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