Decay and Fission Hindrance of Two- and Four-Quasiparticle K Isomers in ^{254}Rf
Two isomers decaying by electromagnetic transitions with half-lives of 4.7(1.1) and 247(73) μs have been discovered in the heavy ^{254}Rf nucleus. The observation of the shorter-lived isomer was made possible by a novel application of a digital data acquisition system. The isomers were interpreted a...
Ausführliche Beschreibung
Autor*in: |
Dracoulis, G D [verfasserIn] |
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Englisch |
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2015 |
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Übergeordnetes Werk: |
Enthalten in: Physical review letters - Ridge, NY : American Physical Society, 1958, 115(2015), 13 |
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Übergeordnetes Werk: |
volume:115 ; year:2015 ; number:13 |
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Katalog-ID: |
OLC196929597X |
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520 | |a Two isomers decaying by electromagnetic transitions with half-lives of 4.7(1.1) and 247(73) μs have been discovered in the heavy ^{254}Rf nucleus. The observation of the shorter-lived isomer was made possible by a novel application of a digital data acquisition system. The isomers were interpreted as the K^{π}=8^{-}, ν^{2}(7/2^{+}[624],9/2^{-}[734]) two-quasineutron and the K^{π}=16^{+}, 8^{-}ν^{2}(7/2^{+}[624],9/2^{-}[734])⊗8^{-}π^{2}(7/2^{-}[514],9/2^{+}[624]) four-quasiparticle configurations, respectively. Surprisingly, the lifetime of the two-quasiparticle isomer is more than 4 orders of magnitude shorter than what has been observed for analogous isomers in the lighter N=150 isotones. The four-quasiparticle isomer is longer lived than the ^{254}Rf ground state that decays exclusively by spontaneous fission with a half-life of 23.2(1.1) μs. The absence of sizable fission branches from either of the isomers implies unprecedented fission hindrance relative to the ground state. | ||
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700 | 1 | |a Rogers, A M |4 oth | |
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700 | 1 | |a David, H M |4 oth | |
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700 | 1 | |a Stolze, S |4 oth | |
700 | 1 | |a Seweryniak, D |4 oth | |
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700 | 1 | |a Khoo, T L |4 oth | |
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700 | 1 | |a Alcorta, M |4 oth | |
700 | 1 | |a Qiu, Y |4 oth | |
700 | 1 | |a Zhu, S |4 oth | |
700 | 1 | |a Chen, J |4 oth | |
700 | 1 | |a Fallon, P |4 oth | |
700 | 1 | |a Greenlees, P T |4 oth | |
700 | 1 | |a Savard, G |4 oth | |
700 | 1 | |a Ahmad, I |4 oth | |
700 | 1 | |a Hartley, D J |4 oth | |
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700 | 1 | |a Hoffman, C R |4 oth | |
700 | 1 | |a Kwarsick, J T |4 oth | |
700 | 1 | |a Gregorich, K E |4 oth | |
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PQ20160211 (DE-627)OLC196929597X (DE-599)GBVOLC196929597X (PRQ)p594-a4a6734ca32dfd794d6180ac3f0946cb0dafaccc599e1661238b476307d43260 (KEY)0009201020150000115001300000decayandfissionhindranceoftwoandfourquasiparticlek DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk Dracoulis, G D verfasserin aut Decay and Fission Hindrance of Two- and Four-Quasiparticle K Isomers in ^{254}Rf 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Two isomers decaying by electromagnetic transitions with half-lives of 4.7(1.1) and 247(73) μs have been discovered in the heavy ^{254}Rf nucleus. The observation of the shorter-lived isomer was made possible by a novel application of a digital data acquisition system. The isomers were interpreted as the K^{π}=8^{-}, ν^{2}(7/2^{+}[624],9/2^{-}[734]) two-quasineutron and the K^{π}=16^{+}, 8^{-}ν^{2}(7/2^{+}[624],9/2^{-}[734])⊗8^{-}π^{2}(7/2^{-}[514],9/2^{+}[624]) four-quasiparticle configurations, respectively. Surprisingly, the lifetime of the two-quasiparticle isomer is more than 4 orders of magnitude shorter than what has been observed for analogous isomers in the lighter N=150 isotones. The four-quasiparticle isomer is longer lived than the ^{254}Rf ground state that decays exclusively by spontaneous fission with a half-life of 23.2(1.1) μs. The absence of sizable fission branches from either of the isomers implies unprecedented fission hindrance relative to the ground state. Hota, S S oth Bernstein, L A oth Back, B B oth Esker, N E oth Rogers, A M oth Wiens, A oth Baartman, B oth David, H M oth Gates, J M oth Carpenter, M P oth Konki, J oth Stolze, S oth Seweryniak, D oth Cromaz, M oth Khoo, T L oth Macchiavelli, A O oth Chiara, C J oth Gothe, O R oth Hauschild, K oth Nair, C oth Doherty, D T oth Albers, M oth Lauritsen, T oth Clark, R M oth Campbell, C M oth Ruotsalainen, P oth Kondev, F G oth Rissanen, J oth Alcorta, M oth Qiu, Y oth Zhu, S oth Chen, J oth Fallon, P oth Greenlees, P T oth Savard, G oth Ahmad, I oth Hartley, D J oth Janssens, R V F oth Mudder, P R oth Greene, J P oth Bertone, P F oth Hoffman, C R oth Kwarsick, J T oth Gregorich, K E oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 115(2015), 13 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:115 year:2015 number:13 http://www.ncbi.nlm.nih.gov/pubmed/26451549 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 115 2015 13 |
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PQ20160211 (DE-627)OLC196929597X (DE-599)GBVOLC196929597X (PRQ)p594-a4a6734ca32dfd794d6180ac3f0946cb0dafaccc599e1661238b476307d43260 (KEY)0009201020150000115001300000decayandfissionhindranceoftwoandfourquasiparticlek DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk Dracoulis, G D verfasserin aut Decay and Fission Hindrance of Two- and Four-Quasiparticle K Isomers in ^{254}Rf 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Two isomers decaying by electromagnetic transitions with half-lives of 4.7(1.1) and 247(73) μs have been discovered in the heavy ^{254}Rf nucleus. The observation of the shorter-lived isomer was made possible by a novel application of a digital data acquisition system. The isomers were interpreted as the K^{π}=8^{-}, ν^{2}(7/2^{+}[624],9/2^{-}[734]) two-quasineutron and the K^{π}=16^{+}, 8^{-}ν^{2}(7/2^{+}[624],9/2^{-}[734])⊗8^{-}π^{2}(7/2^{-}[514],9/2^{+}[624]) four-quasiparticle configurations, respectively. Surprisingly, the lifetime of the two-quasiparticle isomer is more than 4 orders of magnitude shorter than what has been observed for analogous isomers in the lighter N=150 isotones. The four-quasiparticle isomer is longer lived than the ^{254}Rf ground state that decays exclusively by spontaneous fission with a half-life of 23.2(1.1) μs. The absence of sizable fission branches from either of the isomers implies unprecedented fission hindrance relative to the ground state. Hota, S S oth Bernstein, L A oth Back, B B oth Esker, N E oth Rogers, A M oth Wiens, A oth Baartman, B oth David, H M oth Gates, J M oth Carpenter, M P oth Konki, J oth Stolze, S oth Seweryniak, D oth Cromaz, M oth Khoo, T L oth Macchiavelli, A O oth Chiara, C J oth Gothe, O R oth Hauschild, K oth Nair, C oth Doherty, D T oth Albers, M oth Lauritsen, T oth Clark, R M oth Campbell, C M oth Ruotsalainen, P oth Kondev, F G oth Rissanen, J oth Alcorta, M oth Qiu, Y oth Zhu, S oth Chen, J oth Fallon, P oth Greenlees, P T oth Savard, G oth Ahmad, I oth Hartley, D J oth Janssens, R V F oth Mudder, P R oth Greene, J P oth Bertone, P F oth Hoffman, C R oth Kwarsick, J T oth Gregorich, K E oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 115(2015), 13 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:115 year:2015 number:13 http://www.ncbi.nlm.nih.gov/pubmed/26451549 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 115 2015 13 |
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PQ20160211 (DE-627)OLC196929597X (DE-599)GBVOLC196929597X (PRQ)p594-a4a6734ca32dfd794d6180ac3f0946cb0dafaccc599e1661238b476307d43260 (KEY)0009201020150000115001300000decayandfissionhindranceoftwoandfourquasiparticlek DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk Dracoulis, G D verfasserin aut Decay and Fission Hindrance of Two- and Four-Quasiparticle K Isomers in ^{254}Rf 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Two isomers decaying by electromagnetic transitions with half-lives of 4.7(1.1) and 247(73) μs have been discovered in the heavy ^{254}Rf nucleus. The observation of the shorter-lived isomer was made possible by a novel application of a digital data acquisition system. The isomers were interpreted as the K^{π}=8^{-}, ν^{2}(7/2^{+}[624],9/2^{-}[734]) two-quasineutron and the K^{π}=16^{+}, 8^{-}ν^{2}(7/2^{+}[624],9/2^{-}[734])⊗8^{-}π^{2}(7/2^{-}[514],9/2^{+}[624]) four-quasiparticle configurations, respectively. Surprisingly, the lifetime of the two-quasiparticle isomer is more than 4 orders of magnitude shorter than what has been observed for analogous isomers in the lighter N=150 isotones. The four-quasiparticle isomer is longer lived than the ^{254}Rf ground state that decays exclusively by spontaneous fission with a half-life of 23.2(1.1) μs. The absence of sizable fission branches from either of the isomers implies unprecedented fission hindrance relative to the ground state. Hota, S S oth Bernstein, L A oth Back, B B oth Esker, N E oth Rogers, A M oth Wiens, A oth Baartman, B oth David, H M oth Gates, J M oth Carpenter, M P oth Konki, J oth Stolze, S oth Seweryniak, D oth Cromaz, M oth Khoo, T L oth Macchiavelli, A O oth Chiara, C J oth Gothe, O R oth Hauschild, K oth Nair, C oth Doherty, D T oth Albers, M oth Lauritsen, T oth Clark, R M oth Campbell, C M oth Ruotsalainen, P oth Kondev, F G oth Rissanen, J oth Alcorta, M oth Qiu, Y oth Zhu, S oth Chen, J oth Fallon, P oth Greenlees, P T oth Savard, G oth Ahmad, I oth Hartley, D J oth Janssens, R V F oth Mudder, P R oth Greene, J P oth Bertone, P F oth Hoffman, C R oth Kwarsick, J T oth Gregorich, K E oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 115(2015), 13 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:115 year:2015 number:13 http://www.ncbi.nlm.nih.gov/pubmed/26451549 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 115 2015 13 |
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PQ20160211 (DE-627)OLC196929597X (DE-599)GBVOLC196929597X (PRQ)p594-a4a6734ca32dfd794d6180ac3f0946cb0dafaccc599e1661238b476307d43260 (KEY)0009201020150000115001300000decayandfissionhindranceoftwoandfourquasiparticlek DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk Dracoulis, G D verfasserin aut Decay and Fission Hindrance of Two- and Four-Quasiparticle K Isomers in ^{254}Rf 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Two isomers decaying by electromagnetic transitions with half-lives of 4.7(1.1) and 247(73) μs have been discovered in the heavy ^{254}Rf nucleus. The observation of the shorter-lived isomer was made possible by a novel application of a digital data acquisition system. The isomers were interpreted as the K^{π}=8^{-}, ν^{2}(7/2^{+}[624],9/2^{-}[734]) two-quasineutron and the K^{π}=16^{+}, 8^{-}ν^{2}(7/2^{+}[624],9/2^{-}[734])⊗8^{-}π^{2}(7/2^{-}[514],9/2^{+}[624]) four-quasiparticle configurations, respectively. Surprisingly, the lifetime of the two-quasiparticle isomer is more than 4 orders of magnitude shorter than what has been observed for analogous isomers in the lighter N=150 isotones. The four-quasiparticle isomer is longer lived than the ^{254}Rf ground state that decays exclusively by spontaneous fission with a half-life of 23.2(1.1) μs. The absence of sizable fission branches from either of the isomers implies unprecedented fission hindrance relative to the ground state. Hota, S S oth Bernstein, L A oth Back, B B oth Esker, N E oth Rogers, A M oth Wiens, A oth Baartman, B oth David, H M oth Gates, J M oth Carpenter, M P oth Konki, J oth Stolze, S oth Seweryniak, D oth Cromaz, M oth Khoo, T L oth Macchiavelli, A O oth Chiara, C J oth Gothe, O R oth Hauschild, K oth Nair, C oth Doherty, D T oth Albers, M oth Lauritsen, T oth Clark, R M oth Campbell, C M oth Ruotsalainen, P oth Kondev, F G oth Rissanen, J oth Alcorta, M oth Qiu, Y oth Zhu, S oth Chen, J oth Fallon, P oth Greenlees, P T oth Savard, G oth Ahmad, I oth Hartley, D J oth Janssens, R V F oth Mudder, P R oth Greene, J P oth Bertone, P F oth Hoffman, C R oth Kwarsick, J T oth Gregorich, K E oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 115(2015), 13 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:115 year:2015 number:13 http://www.ncbi.nlm.nih.gov/pubmed/26451549 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 115 2015 13 |
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PQ20160211 (DE-627)OLC196929597X (DE-599)GBVOLC196929597X (PRQ)p594-a4a6734ca32dfd794d6180ac3f0946cb0dafaccc599e1661238b476307d43260 (KEY)0009201020150000115001300000decayandfissionhindranceoftwoandfourquasiparticlek DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk Dracoulis, G D verfasserin aut Decay and Fission Hindrance of Two- and Four-Quasiparticle K Isomers in ^{254}Rf 2015 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier Two isomers decaying by electromagnetic transitions with half-lives of 4.7(1.1) and 247(73) μs have been discovered in the heavy ^{254}Rf nucleus. The observation of the shorter-lived isomer was made possible by a novel application of a digital data acquisition system. The isomers were interpreted as the K^{π}=8^{-}, ν^{2}(7/2^{+}[624],9/2^{-}[734]) two-quasineutron and the K^{π}=16^{+}, 8^{-}ν^{2}(7/2^{+}[624],9/2^{-}[734])⊗8^{-}π^{2}(7/2^{-}[514],9/2^{+}[624]) four-quasiparticle configurations, respectively. Surprisingly, the lifetime of the two-quasiparticle isomer is more than 4 orders of magnitude shorter than what has been observed for analogous isomers in the lighter N=150 isotones. The four-quasiparticle isomer is longer lived than the ^{254}Rf ground state that decays exclusively by spontaneous fission with a half-life of 23.2(1.1) μs. The absence of sizable fission branches from either of the isomers implies unprecedented fission hindrance relative to the ground state. Hota, S S oth Bernstein, L A oth Back, B B oth Esker, N E oth Rogers, A M oth Wiens, A oth Baartman, B oth David, H M oth Gates, J M oth Carpenter, M P oth Konki, J oth Stolze, S oth Seweryniak, D oth Cromaz, M oth Khoo, T L oth Macchiavelli, A O oth Chiara, C J oth Gothe, O R oth Hauschild, K oth Nair, C oth Doherty, D T oth Albers, M oth Lauritsen, T oth Clark, R M oth Campbell, C M oth Ruotsalainen, P oth Kondev, F G oth Rissanen, J oth Alcorta, M oth Qiu, Y oth Zhu, S oth Chen, J oth Fallon, P oth Greenlees, P T oth Savard, G oth Ahmad, I oth Hartley, D J oth Janssens, R V F oth Mudder, P R oth Greene, J P oth Bertone, P F oth Hoffman, C R oth Kwarsick, J T oth Gregorich, K E oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 115(2015), 13 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:115 year:2015 number:13 http://www.ncbi.nlm.nih.gov/pubmed/26451549 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 115 2015 13 |
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Dracoulis, G D @@aut@@ Hota, S S @@oth@@ Bernstein, L A @@oth@@ Back, B B @@oth@@ Esker, N E @@oth@@ Rogers, A M @@oth@@ Wiens, A @@oth@@ Baartman, B @@oth@@ David, H M @@oth@@ Gates, J M @@oth@@ Carpenter, M P @@oth@@ Konki, J @@oth@@ Stolze, S @@oth@@ Seweryniak, D @@oth@@ Cromaz, M @@oth@@ Khoo, T L @@oth@@ Macchiavelli, A O @@oth@@ Chiara, C J @@oth@@ Gothe, O R @@oth@@ Hauschild, K @@oth@@ Nair, C @@oth@@ Doherty, D T @@oth@@ Albers, M @@oth@@ Lauritsen, T @@oth@@ Clark, R M @@oth@@ Campbell, C M @@oth@@ Ruotsalainen, P @@oth@@ Kondev, F G @@oth@@ Rissanen, J @@oth@@ Alcorta, M @@oth@@ Qiu, Y @@oth@@ Zhu, S @@oth@@ Chen, J @@oth@@ Fallon, P @@oth@@ Greenlees, P T @@oth@@ Savard, G @@oth@@ Ahmad, I @@oth@@ Hartley, D J @@oth@@ Janssens, R V F @@oth@@ Mudder, P R @@oth@@ Greene, J P @@oth@@ Bertone, P F @@oth@@ Hoffman, C R @@oth@@ Kwarsick, J T @@oth@@ Gregorich, K E @@oth@@ |
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Decay and Fission Hindrance of Two- and Four-Quasiparticle K Isomers in ^{254}Rf |
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Decay and Fission Hindrance of Two- and Four-Quasiparticle K Isomers in ^{254}Rf |
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decay and fission hindrance of two- and four-quasiparticle k isomers in ^{254}rf |
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Decay and Fission Hindrance of Two- and Four-Quasiparticle K Isomers in ^{254}Rf |
abstract |
Two isomers decaying by electromagnetic transitions with half-lives of 4.7(1.1) and 247(73) μs have been discovered in the heavy ^{254}Rf nucleus. The observation of the shorter-lived isomer was made possible by a novel application of a digital data acquisition system. The isomers were interpreted as the K^{π}=8^{-}, ν^{2}(7/2^{+}[624],9/2^{-}[734]) two-quasineutron and the K^{π}=16^{+}, 8^{-}ν^{2}(7/2^{+}[624],9/2^{-}[734])⊗8^{-}π^{2}(7/2^{-}[514],9/2^{+}[624]) four-quasiparticle configurations, respectively. Surprisingly, the lifetime of the two-quasiparticle isomer is more than 4 orders of magnitude shorter than what has been observed for analogous isomers in the lighter N=150 isotones. The four-quasiparticle isomer is longer lived than the ^{254}Rf ground state that decays exclusively by spontaneous fission with a half-life of 23.2(1.1) μs. The absence of sizable fission branches from either of the isomers implies unprecedented fission hindrance relative to the ground state. |
abstractGer |
Two isomers decaying by electromagnetic transitions with half-lives of 4.7(1.1) and 247(73) μs have been discovered in the heavy ^{254}Rf nucleus. The observation of the shorter-lived isomer was made possible by a novel application of a digital data acquisition system. The isomers were interpreted as the K^{π}=8^{-}, ν^{2}(7/2^{+}[624],9/2^{-}[734]) two-quasineutron and the K^{π}=16^{+}, 8^{-}ν^{2}(7/2^{+}[624],9/2^{-}[734])⊗8^{-}π^{2}(7/2^{-}[514],9/2^{+}[624]) four-quasiparticle configurations, respectively. Surprisingly, the lifetime of the two-quasiparticle isomer is more than 4 orders of magnitude shorter than what has been observed for analogous isomers in the lighter N=150 isotones. The four-quasiparticle isomer is longer lived than the ^{254}Rf ground state that decays exclusively by spontaneous fission with a half-life of 23.2(1.1) μs. The absence of sizable fission branches from either of the isomers implies unprecedented fission hindrance relative to the ground state. |
abstract_unstemmed |
Two isomers decaying by electromagnetic transitions with half-lives of 4.7(1.1) and 247(73) μs have been discovered in the heavy ^{254}Rf nucleus. The observation of the shorter-lived isomer was made possible by a novel application of a digital data acquisition system. The isomers were interpreted as the K^{π}=8^{-}, ν^{2}(7/2^{+}[624],9/2^{-}[734]) two-quasineutron and the K^{π}=16^{+}, 8^{-}ν^{2}(7/2^{+}[624],9/2^{-}[734])⊗8^{-}π^{2}(7/2^{-}[514],9/2^{+}[624]) four-quasiparticle configurations, respectively. Surprisingly, the lifetime of the two-quasiparticle isomer is more than 4 orders of magnitude shorter than what has been observed for analogous isomers in the lighter N=150 isotones. The four-quasiparticle isomer is longer lived than the ^{254}Rf ground state that decays exclusively by spontaneous fission with a half-life of 23.2(1.1) μs. The absence of sizable fission branches from either of the isomers implies unprecedented fission hindrance relative to the ground state. |
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title_short |
Decay and Fission Hindrance of Two- and Four-Quasiparticle K Isomers in ^{254}Rf |
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Hota, S S Bernstein, L A Back, B B Esker, N E Rogers, A M Wiens, A Baartman, B David, H M Gates, J M Carpenter, M P Konki, J Stolze, S Seweryniak, D Cromaz, M Khoo, T L Macchiavelli, A O Chiara, C J Gothe, O R Hauschild, K Nair, C Doherty, D T Albers, M Lauritsen, T Clark, R M Campbell, C M Ruotsalainen, P Kondev, F G Rissanen, J Alcorta, M Qiu, Y Zhu, S Chen, J Fallon, P Greenlees, P T Savard, G Ahmad, I Hartley, D J Janssens, R V F Mudder, P R Greene, J P Bertone, P F Hoffman, C R Kwarsick, J T Gregorich, K E |
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Hota, S S Bernstein, L A Back, B B Esker, N E Rogers, A M Wiens, A Baartman, B David, H M Gates, J M Carpenter, M P Konki, J Stolze, S Seweryniak, D Cromaz, M Khoo, T L Macchiavelli, A O Chiara, C J Gothe, O R Hauschild, K Nair, C Doherty, D T Albers, M Lauritsen, T Clark, R M Campbell, C M Ruotsalainen, P Kondev, F G Rissanen, J Alcorta, M Qiu, Y Zhu, S Chen, J Fallon, P Greenlees, P T Savard, G Ahmad, I Hartley, D J Janssens, R V F Mudder, P R Greene, J P Bertone, P F Hoffman, C R Kwarsick, J T Gregorich, K E |
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The observation of the shorter-lived isomer was made possible by a novel application of a digital data acquisition system. The isomers were interpreted as the K^{π}=8^{-}, ν^{2}(7/2^{+}[624],9/2^{-}[734]) two-quasineutron and the K^{π}=16^{+}, 8^{-}ν^{2}(7/2^{+}[624],9/2^{-}[734])⊗8^{-}π^{2}(7/2^{-}[514],9/2^{+}[624]) four-quasiparticle configurations, respectively. Surprisingly, the lifetime of the two-quasiparticle isomer is more than 4 orders of magnitude shorter than what has been observed for analogous isomers in the lighter N=150 isotones. The four-quasiparticle isomer is longer lived than the ^{254}Rf ground state that decays exclusively by spontaneous fission with a half-life of 23.2(1.1) μs. 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