Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni

Proton-emission branches of the 10+ isomer in the Tz=−1 nucleus 54Ni have been imaged with the active target and time projection chamber (ACTAR TPC) in an experiment conducted at the Grand Accélérateur National d'Ions Lourds (GANIL). The completed decay scheme allows derivation of the reduced t...
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Autor*in:	D. Rudolph [verfasserIn] B. Blank [verfasserIn] J. Giovinazzo [verfasserIn] T. Roger [verfasserIn] H. Alvarez-Pol [verfasserIn] A. Arokia Raj [verfasserIn] P. Ascher [verfasserIn] M. Caamaño-Fresco [verfasserIn] L. Caceres [verfasserIn] D.M. Cox [verfasserIn] B. Fernández-Domínguez [verfasserIn] J. Lois-Fuentes [verfasserIn] M. Gerbaux [verfasserIn] S. Grévy [verfasserIn] G.F. Grinyer [verfasserIn] O. Kamalou [verfasserIn] B. Mauss [verfasserIn] A. Mentana [verfasserIn] J. Pancin [verfasserIn] J. Pibernat [verfasserIn] J. Piot [verfasserIn] O. Sorlin [verfasserIn] C. Stodel [verfasserIn] J.-C. Thomas [verfasserIn] M. Versteegen [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2022

Schlagwörter:	54Ni Nuclear shell model Isospin symmetry Electromagnetic decay E4 transition Effective charges

Übergeordnetes Werk:	In: Physics Letters B - Elsevier, 2015, 830(2022), Seite 137144-
Übergeordnetes Werk:	volume:830 ; year:2022 ; pages:137144-

Links:	Link aufrufen Link aufrufen Link aufrufen Journal toc

DOI / URN:	10.1016/j.physletb.2022.137144

Katalog-ID:	DOAJ028995961

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520			\|a Proton-emission branches of the 10+ isomer in the Tz=−1 nucleus 54Ni have been imaged with the active target and time projection chamber (ACTAR TPC) in an experiment conducted at the Grand Accélérateur National d'Ions Lourds (GANIL). The completed decay scheme allows derivation of the reduced transition strengths, B(E2;10+→8+) and B(E4;10+→6+), for the two competing γ-ray transitions. By means of a comparison with their well-known ‘mirror transitions’ in Tz=+1 54Fe, and aided by a variety of shell-model calculations in the fp model space, effective charges for E4 transitions near N=Z 56Ni can be deduced: επ≈1.40 and εν≈0.30. Mirror-energy differences are explored with various shell-model interactions and isospin-symmetry breaking terms.
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allfields	10.1016/j.physletb.2022.137144 doi (DE-627)DOAJ028995961 (DE-599)DOAJea965b7c5d4143adbb904f0362e74d03 DE-627 ger DE-627 rakwb eng QC1-999 D. Rudolph verfasserin aut Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Proton-emission branches of the 10+ isomer in the Tz=−1 nucleus 54Ni have been imaged with the active target and time projection chamber (ACTAR TPC) in an experiment conducted at the Grand Accélérateur National d'Ions Lourds (GANIL). The completed decay scheme allows derivation of the reduced transition strengths, B(E2;10+→8+) and B(E4;10+→6+), for the two competing γ-ray transitions. By means of a comparison with their well-known ‘mirror transitions’ in Tz=+1 54Fe, and aided by a variety of shell-model calculations in the fp model space, effective charges for E4 transitions near N=Z 56Ni can be deduced: επ≈1.40 and εν≈0.30. Mirror-energy differences are explored with various shell-model interactions and isospin-symmetry breaking terms. 54Ni Nuclear shell model Isospin symmetry Electromagnetic decay E4 transition Effective charges Physics B. Blank verfasserin aut J. Giovinazzo verfasserin aut T. Roger verfasserin aut H. Alvarez-Pol verfasserin aut A. Arokia Raj verfasserin aut P. Ascher verfasserin aut M. Caamaño-Fresco verfasserin aut L. Caceres verfasserin aut D.M. Cox verfasserin aut B. Fernández-Domínguez verfasserin aut J. Lois-Fuentes verfasserin aut M. Gerbaux verfasserin aut S. Grévy verfasserin aut G.F. Grinyer verfasserin aut O. Kamalou verfasserin aut B. Mauss verfasserin aut A. Mentana verfasserin aut J. Pancin verfasserin aut J. Pibernat verfasserin aut J. Piot verfasserin aut O. Sorlin verfasserin aut C. Stodel verfasserin aut J.-C. Thomas verfasserin aut M. Versteegen verfasserin aut In Physics Letters B Elsevier, 2015 830(2022), Seite 137144- (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:830 year:2022 pages:137144- https://doi.org/10.1016/j.physletb.2022.137144 kostenfrei https://doaj.org/article/ea965b7c5d4143adbb904f0362e74d03 kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269322002787 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 830 2022 137144-
spelling	10.1016/j.physletb.2022.137144 doi (DE-627)DOAJ028995961 (DE-599)DOAJea965b7c5d4143adbb904f0362e74d03 DE-627 ger DE-627 rakwb eng QC1-999 D. Rudolph verfasserin aut Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Proton-emission branches of the 10+ isomer in the Tz=−1 nucleus 54Ni have been imaged with the active target and time projection chamber (ACTAR TPC) in an experiment conducted at the Grand Accélérateur National d'Ions Lourds (GANIL). The completed decay scheme allows derivation of the reduced transition strengths, B(E2;10+→8+) and B(E4;10+→6+), for the two competing γ-ray transitions. By means of a comparison with their well-known ‘mirror transitions’ in Tz=+1 54Fe, and aided by a variety of shell-model calculations in the fp model space, effective charges for E4 transitions near N=Z 56Ni can be deduced: επ≈1.40 and εν≈0.30. Mirror-energy differences are explored with various shell-model interactions and isospin-symmetry breaking terms. 54Ni Nuclear shell model Isospin symmetry Electromagnetic decay E4 transition Effective charges Physics B. Blank verfasserin aut J. Giovinazzo verfasserin aut T. Roger verfasserin aut H. Alvarez-Pol verfasserin aut A. Arokia Raj verfasserin aut P. Ascher verfasserin aut M. Caamaño-Fresco verfasserin aut L. Caceres verfasserin aut D.M. Cox verfasserin aut B. Fernández-Domínguez verfasserin aut J. Lois-Fuentes verfasserin aut M. Gerbaux verfasserin aut S. Grévy verfasserin aut G.F. Grinyer verfasserin aut O. Kamalou verfasserin aut B. Mauss verfasserin aut A. Mentana verfasserin aut J. Pancin verfasserin aut J. Pibernat verfasserin aut J. Piot verfasserin aut O. Sorlin verfasserin aut C. Stodel verfasserin aut J.-C. Thomas verfasserin aut M. Versteegen verfasserin aut In Physics Letters B Elsevier, 2015 830(2022), Seite 137144- (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:830 year:2022 pages:137144- https://doi.org/10.1016/j.physletb.2022.137144 kostenfrei https://doaj.org/article/ea965b7c5d4143adbb904f0362e74d03 kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269322002787 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 830 2022 137144-
allfields_unstemmed	10.1016/j.physletb.2022.137144 doi (DE-627)DOAJ028995961 (DE-599)DOAJea965b7c5d4143adbb904f0362e74d03 DE-627 ger DE-627 rakwb eng QC1-999 D. Rudolph verfasserin aut Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Proton-emission branches of the 10+ isomer in the Tz=−1 nucleus 54Ni have been imaged with the active target and time projection chamber (ACTAR TPC) in an experiment conducted at the Grand Accélérateur National d'Ions Lourds (GANIL). The completed decay scheme allows derivation of the reduced transition strengths, B(E2;10+→8+) and B(E4;10+→6+), for the two competing γ-ray transitions. By means of a comparison with their well-known ‘mirror transitions’ in Tz=+1 54Fe, and aided by a variety of shell-model calculations in the fp model space, effective charges for E4 transitions near N=Z 56Ni can be deduced: επ≈1.40 and εν≈0.30. Mirror-energy differences are explored with various shell-model interactions and isospin-symmetry breaking terms. 54Ni Nuclear shell model Isospin symmetry Electromagnetic decay E4 transition Effective charges Physics B. Blank verfasserin aut J. Giovinazzo verfasserin aut T. Roger verfasserin aut H. Alvarez-Pol verfasserin aut A. Arokia Raj verfasserin aut P. Ascher verfasserin aut M. Caamaño-Fresco verfasserin aut L. Caceres verfasserin aut D.M. Cox verfasserin aut B. Fernández-Domínguez verfasserin aut J. Lois-Fuentes verfasserin aut M. Gerbaux verfasserin aut S. Grévy verfasserin aut G.F. Grinyer verfasserin aut O. Kamalou verfasserin aut B. Mauss verfasserin aut A. Mentana verfasserin aut J. Pancin verfasserin aut J. Pibernat verfasserin aut J. Piot verfasserin aut O. Sorlin verfasserin aut C. Stodel verfasserin aut J.-C. Thomas verfasserin aut M. Versteegen verfasserin aut In Physics Letters B Elsevier, 2015 830(2022), Seite 137144- (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:830 year:2022 pages:137144- https://doi.org/10.1016/j.physletb.2022.137144 kostenfrei https://doaj.org/article/ea965b7c5d4143adbb904f0362e74d03 kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269322002787 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 830 2022 137144-
allfieldsGer	10.1016/j.physletb.2022.137144 doi (DE-627)DOAJ028995961 (DE-599)DOAJea965b7c5d4143adbb904f0362e74d03 DE-627 ger DE-627 rakwb eng QC1-999 D. Rudolph verfasserin aut Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Proton-emission branches of the 10+ isomer in the Tz=−1 nucleus 54Ni have been imaged with the active target and time projection chamber (ACTAR TPC) in an experiment conducted at the Grand Accélérateur National d'Ions Lourds (GANIL). The completed decay scheme allows derivation of the reduced transition strengths, B(E2;10+→8+) and B(E4;10+→6+), for the two competing γ-ray transitions. By means of a comparison with their well-known ‘mirror transitions’ in Tz=+1 54Fe, and aided by a variety of shell-model calculations in the fp model space, effective charges for E4 transitions near N=Z 56Ni can be deduced: επ≈1.40 and εν≈0.30. Mirror-energy differences are explored with various shell-model interactions and isospin-symmetry breaking terms. 54Ni Nuclear shell model Isospin symmetry Electromagnetic decay E4 transition Effective charges Physics B. Blank verfasserin aut J. Giovinazzo verfasserin aut T. Roger verfasserin aut H. Alvarez-Pol verfasserin aut A. Arokia Raj verfasserin aut P. Ascher verfasserin aut M. Caamaño-Fresco verfasserin aut L. Caceres verfasserin aut D.M. Cox verfasserin aut B. Fernández-Domínguez verfasserin aut J. Lois-Fuentes verfasserin aut M. Gerbaux verfasserin aut S. Grévy verfasserin aut G.F. Grinyer verfasserin aut O. Kamalou verfasserin aut B. Mauss verfasserin aut A. Mentana verfasserin aut J. Pancin verfasserin aut J. Pibernat verfasserin aut J. Piot verfasserin aut O. Sorlin verfasserin aut C. Stodel verfasserin aut J.-C. Thomas verfasserin aut M. Versteegen verfasserin aut In Physics Letters B Elsevier, 2015 830(2022), Seite 137144- (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:830 year:2022 pages:137144- https://doi.org/10.1016/j.physletb.2022.137144 kostenfrei https://doaj.org/article/ea965b7c5d4143adbb904f0362e74d03 kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269322002787 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 830 2022 137144-
allfieldsSound	10.1016/j.physletb.2022.137144 doi (DE-627)DOAJ028995961 (DE-599)DOAJea965b7c5d4143adbb904f0362e74d03 DE-627 ger DE-627 rakwb eng QC1-999 D. Rudolph verfasserin aut Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni 2022 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Proton-emission branches of the 10+ isomer in the Tz=−1 nucleus 54Ni have been imaged with the active target and time projection chamber (ACTAR TPC) in an experiment conducted at the Grand Accélérateur National d'Ions Lourds (GANIL). The completed decay scheme allows derivation of the reduced transition strengths, B(E2;10+→8+) and B(E4;10+→6+), for the two competing γ-ray transitions. By means of a comparison with their well-known ‘mirror transitions’ in Tz=+1 54Fe, and aided by a variety of shell-model calculations in the fp model space, effective charges for E4 transitions near N=Z 56Ni can be deduced: επ≈1.40 and εν≈0.30. Mirror-energy differences are explored with various shell-model interactions and isospin-symmetry breaking terms. 54Ni Nuclear shell model Isospin symmetry Electromagnetic decay E4 transition Effective charges Physics B. Blank verfasserin aut J. Giovinazzo verfasserin aut T. Roger verfasserin aut H. Alvarez-Pol verfasserin aut A. Arokia Raj verfasserin aut P. Ascher verfasserin aut M. Caamaño-Fresco verfasserin aut L. Caceres verfasserin aut D.M. Cox verfasserin aut B. Fernández-Domínguez verfasserin aut J. Lois-Fuentes verfasserin aut M. Gerbaux verfasserin aut S. Grévy verfasserin aut G.F. Grinyer verfasserin aut O. Kamalou verfasserin aut B. Mauss verfasserin aut A. Mentana verfasserin aut J. Pancin verfasserin aut J. Pibernat verfasserin aut J. Piot verfasserin aut O. Sorlin verfasserin aut C. Stodel verfasserin aut J.-C. Thomas verfasserin aut M. Versteegen verfasserin aut In Physics Letters B Elsevier, 2015 830(2022), Seite 137144- (DE-627)266015360 (DE-600)1466612-1 18732445 nnns volume:830 year:2022 pages:137144- https://doi.org/10.1016/j.physletb.2022.137144 kostenfrei https://doaj.org/article/ea965b7c5d4143adbb904f0362e74d03 kostenfrei http://www.sciencedirect.com/science/article/pii/S0370269322002787 kostenfrei https://doaj.org/toc/0370-2693 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2014 GBV_ILN_2025 GBV_ILN_2034 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2064 GBV_ILN_2111 GBV_ILN_2153 GBV_ILN_2336 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 830 2022 137144-
language	English
source	In Physics Letters B 830(2022), Seite 137144- volume:830 year:2022 pages:137144-
sourceStr	In Physics Letters B 830(2022), Seite 137144- volume:830 year:2022 pages:137144-
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	54Ni Nuclear shell model Isospin symmetry Electromagnetic decay E4 transition Effective charges Physics
isfreeaccess_bool	true
container_title	Physics Letters B
authorswithroles_txt_mv	D. Rudolph @@aut@@ B. Blank @@aut@@ J. Giovinazzo @@aut@@ T. Roger @@aut@@ H. Alvarez-Pol @@aut@@ A. Arokia Raj @@aut@@ P. Ascher @@aut@@ M. Caamaño-Fresco @@aut@@ L. Caceres @@aut@@ D.M. Cox @@aut@@ B. Fernández-Domínguez @@aut@@ J. Lois-Fuentes @@aut@@ M. Gerbaux @@aut@@ S. Grévy @@aut@@ G.F. Grinyer @@aut@@ O. Kamalou @@aut@@ B. Mauss @@aut@@ A. Mentana @@aut@@ J. Pancin @@aut@@ J. Pibernat @@aut@@ J. Piot @@aut@@ O. Sorlin @@aut@@ C. Stodel @@aut@@ J.-C. Thomas @@aut@@ M. Versteegen @@aut@@
publishDateDaySort_date	2022-01-01T00:00:00Z
hierarchy_top_id	266015360
id	DOAJ028995961
language_de	englisch
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Rudolph</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2022</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Proton-emission branches of the 10+ isomer in the Tz=−1 nucleus 54Ni have been imaged with the active target and time projection chamber (ACTAR TPC) in an experiment conducted at the Grand Accélérateur National d'Ions Lourds (GANIL). The completed decay scheme allows derivation of the reduced transition strengths, B(E2;10+→8+) and B(E4;10+→6+), for the two competing γ-ray transitions. By means of a comparison with their well-known ‘mirror transitions’ in Tz=+1 54Fe, and aided by a variety of shell-model calculations in the fp model space, effective charges for E4 transitions near N=Z 56Ni can be deduced: επ≈1.40 and εν≈0.30. 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callnumber-first	Q - Science
author	D. Rudolph
spellingShingle	D. Rudolph misc QC1-999 misc 54Ni misc Nuclear shell model misc Isospin symmetry misc Electromagnetic decay misc E4 transition misc Effective charges misc Physics Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni
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topic_title	QC1-999 Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni 54Ni Nuclear shell model Isospin symmetry Electromagnetic decay E4 transition Effective charges
topic	misc QC1-999 misc 54Ni misc Nuclear shell model misc Isospin symmetry misc Electromagnetic decay misc E4 transition misc Effective charges misc Physics
topic_unstemmed	misc QC1-999 misc 54Ni misc Nuclear shell model misc Isospin symmetry misc Electromagnetic decay misc E4 transition misc Effective charges misc Physics
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title	Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni
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title_full	Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni
author_sort	D. Rudolph
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author_browse	D. Rudolph B. Blank J. Giovinazzo T. Roger H. Alvarez-Pol A. Arokia Raj P. Ascher M. Caamaño-Fresco L. Caceres D.M. Cox B. Fernández-Domínguez J. Lois-Fuentes M. Gerbaux S. Grévy G.F. Grinyer O. Kamalou B. Mauss A. Mentana J. Pancin J. Pibernat J. Piot O. Sorlin C. Stodel J.-C. Thomas M. Versteegen
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title_sort	mirror symmetry at mass a = 54: e4 effective charges near doubly magic 56ni
callnumber	QC1-999
title_auth	Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni
abstract	Proton-emission branches of the 10+ isomer in the Tz=−1 nucleus 54Ni have been imaged with the active target and time projection chamber (ACTAR TPC) in an experiment conducted at the Grand Accélérateur National d'Ions Lourds (GANIL). The completed decay scheme allows derivation of the reduced transition strengths, B(E2;10+→8+) and B(E4;10+→6+), for the two competing γ-ray transitions. By means of a comparison with their well-known ‘mirror transitions’ in Tz=+1 54Fe, and aided by a variety of shell-model calculations in the fp model space, effective charges for E4 transitions near N=Z 56Ni can be deduced: επ≈1.40 and εν≈0.30. Mirror-energy differences are explored with various shell-model interactions and isospin-symmetry breaking terms.
abstractGer	Proton-emission branches of the 10+ isomer in the Tz=−1 nucleus 54Ni have been imaged with the active target and time projection chamber (ACTAR TPC) in an experiment conducted at the Grand Accélérateur National d'Ions Lourds (GANIL). The completed decay scheme allows derivation of the reduced transition strengths, B(E2;10+→8+) and B(E4;10+→6+), for the two competing γ-ray transitions. By means of a comparison with their well-known ‘mirror transitions’ in Tz=+1 54Fe, and aided by a variety of shell-model calculations in the fp model space, effective charges for E4 transitions near N=Z 56Ni can be deduced: επ≈1.40 and εν≈0.30. Mirror-energy differences are explored with various shell-model interactions and isospin-symmetry breaking terms.
abstract_unstemmed	Proton-emission branches of the 10+ isomer in the Tz=−1 nucleus 54Ni have been imaged with the active target and time projection chamber (ACTAR TPC) in an experiment conducted at the Grand Accélérateur National d'Ions Lourds (GANIL). The completed decay scheme allows derivation of the reduced transition strengths, B(E2;10+→8+) and B(E4;10+→6+), for the two competing γ-ray transitions. By means of a comparison with their well-known ‘mirror transitions’ in Tz=+1 54Fe, and aided by a variety of shell-model calculations in the fp model space, effective charges for E4 transitions near N=Z 56Ni can be deduced: επ≈1.40 and εν≈0.30. Mirror-energy differences are explored with various shell-model interactions and isospin-symmetry breaking terms.
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title_short	Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni
url	https://doi.org/10.1016/j.physletb.2022.137144 https://doaj.org/article/ea965b7c5d4143adbb904f0362e74d03 http://www.sciencedirect.com/science/article/pii/S0370269322002787 https://doaj.org/toc/0370-2693
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author2Str	B. Blank J. Giovinazzo T. Roger H. Alvarez-Pol A. Arokia Raj P. Ascher M. Caamaño-Fresco L. Caceres D.M. Cox B. Fernández-Domínguez J. Lois-Fuentes M. Gerbaux S. Grévy G.F. Grinyer O. Kamalou B. Mauss A. Mentana J. Pancin J. Pibernat J. Piot O. Sorlin C. Stodel J.-C. Thomas M. Versteegen
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up_date	2024-07-03T20:34:00.392Z
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Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni

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Mirror symmetry at mass A = 54: E4 effective charges near doubly magic 56Ni