Lifetime Measurements of Excited States in ^{172}Pt and the Variation of Quadrupole Transition Strength with Angular Momentum
Lifetimes of the first excited 2^{+} and 4^{+} states in the extremely neutron-deficient nuclide ^{172}Pt have been measured for the first time using the recoil-distance Doppler shift and recoil-decay tagging techniques. An unusually low value of the ratio B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_...
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creator | Cederwall, B Doncel, M Aktas, Ö Ertoprak, A Liotta, R Qi, C Grahn, T Cullen, D M Hodge, D Giles, M Stolze, S Badran, H Braunroth, T Calverley, T Cox, D M Fang, Y D Greenlees, P T Hilton, J Ideguchi, E Julin, R Juutinen, S Raju, M Kumar Li, H Liu, H Matta, S Modamio, V Pakarinen, J Papadakis, P Partanen, J Petrache, C M Rahkila, P Ruotsalainen, P Sandzelius, M Sarén, J Scholey, C Sorri, J Subramaniam, P Taylor, M J Uusitalo, J Valiente-Dobón, J J |
description | Lifetimes of the first excited 2^{+} and 4^{+} states in the extremely neutron-deficient nuclide ^{172}Pt have been measured for the first time using the recoil-distance Doppler shift and recoil-decay tagging techniques. An unusually low value of the ratio B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+})=0.55(19) was found, similar to a handful of other such anomalous cases observed in the entire Segré chart. The observation adds to a cluster of a few extremely neutron-deficient nuclides of the heavy transition metals with neutron numbers N≈90-94 featuring the effect. No theoretical model calculations reported to date have been able to explain the anomalously low B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+}) ratios observed in these cases. Such low values cannot, e.g., be explained within the framework of the geometrical collective model or by algebraic approaches within the interacting boson model framework. It is proposed that the group of B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+}) ratios in the extremely neutron-deficient even-even W, Os, and Pt nuclei around neutron numbers N≈90-94 reveal a quantum phase transition from a seniority-conserving structure to a collective regime as a function of neutron number. Although a system governed by seniority symmetry is the only theoretical framework for which such an effect may naturally occur, the phenomenon is highly unexpected for these nuclei that are not situated near closed shells. |
doi_str_mv | 10.1103/PhysRevLett.121.022502 |
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An unusually low value of the ratio B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+})=0.55(19) was found, similar to a handful of other such anomalous cases observed in the entire Segré chart. The observation adds to a cluster of a few extremely neutron-deficient nuclides of the heavy transition metals with neutron numbers N≈90-94 featuring the effect. No theoretical model calculations reported to date have been able to explain the anomalously low B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+}) ratios observed in these cases. Such low values cannot, e.g., be explained within the framework of the geometrical collective model or by algebraic approaches within the interacting boson model framework. It is proposed that the group of B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+}) ratios in the extremely neutron-deficient even-even W, Os, and Pt nuclei around neutron numbers N≈90-94 reveal a quantum phase transition from a seniority-conserving structure to a collective regime as a function of neutron number. Although a system governed by seniority symmetry is the only theoretical framework for which such an effect may naturally occur, the phenomenon is highly unexpected for these nuclei that are not situated near closed shells.</description><identifier>ISSN: 0031-9007</identifier><identifier>EISSN: 1079-7114</identifier><identifier>DOI: 10.1103/PhysRevLett.121.022502</identifier><identifier>PMID: 30085703</identifier><language>eng</language><publisher>United States: American Physical Society</publisher><subject>Nuclear Experiment ; Physics</subject><ispartof>Physical review letters, 2018-07, Vol.121 (2), p.022502-022502</ispartof><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0003-2300-2626 ; 0000-0002-8335-452X</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,27903,27904</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/30085703$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://hal.science/hal-01839665$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Cederwall, B</creatorcontrib><creatorcontrib>Doncel, M</creatorcontrib><creatorcontrib>Aktas, Ö</creatorcontrib><creatorcontrib>Ertoprak, A</creatorcontrib><creatorcontrib>Liotta, R</creatorcontrib><creatorcontrib>Qi, C</creatorcontrib><creatorcontrib>Grahn, T</creatorcontrib><creatorcontrib>Cullen, D M</creatorcontrib><creatorcontrib>Hodge, D</creatorcontrib><creatorcontrib>Giles, M</creatorcontrib><creatorcontrib>Stolze, S</creatorcontrib><creatorcontrib>Badran, H</creatorcontrib><creatorcontrib>Braunroth, T</creatorcontrib><creatorcontrib>Calverley, T</creatorcontrib><creatorcontrib>Cox, D M</creatorcontrib><creatorcontrib>Fang, Y D</creatorcontrib><creatorcontrib>Greenlees, P T</creatorcontrib><creatorcontrib>Hilton, J</creatorcontrib><creatorcontrib>Ideguchi, E</creatorcontrib><creatorcontrib>Julin, R</creatorcontrib><creatorcontrib>Juutinen, S</creatorcontrib><creatorcontrib>Raju, M Kumar</creatorcontrib><creatorcontrib>Li, H</creatorcontrib><creatorcontrib>Liu, H</creatorcontrib><creatorcontrib>Matta, S</creatorcontrib><creatorcontrib>Modamio, V</creatorcontrib><creatorcontrib>Pakarinen, J</creatorcontrib><creatorcontrib>Papadakis, P</creatorcontrib><creatorcontrib>Partanen, J</creatorcontrib><creatorcontrib>Petrache, C M</creatorcontrib><creatorcontrib>Rahkila, P</creatorcontrib><creatorcontrib>Ruotsalainen, P</creatorcontrib><creatorcontrib>Sandzelius, M</creatorcontrib><creatorcontrib>Sarén, J</creatorcontrib><creatorcontrib>Scholey, C</creatorcontrib><creatorcontrib>Sorri, J</creatorcontrib><creatorcontrib>Subramaniam, P</creatorcontrib><creatorcontrib>Taylor, M J</creatorcontrib><creatorcontrib>Uusitalo, J</creatorcontrib><creatorcontrib>Valiente-Dobón, J J</creatorcontrib><title>Lifetime Measurements of Excited States in ^{172}Pt and the Variation of Quadrupole Transition Strength with Angular Momentum</title><title>Physical review letters</title><addtitle>Phys Rev Lett</addtitle><description>Lifetimes of the first excited 2^{+} and 4^{+} states in the extremely neutron-deficient nuclide ^{172}Pt have been measured for the first time using the recoil-distance Doppler shift and recoil-decay tagging techniques. An unusually low value of the ratio B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+})=0.55(19) was found, similar to a handful of other such anomalous cases observed in the entire Segré chart. The observation adds to a cluster of a few extremely neutron-deficient nuclides of the heavy transition metals with neutron numbers N≈90-94 featuring the effect. No theoretical model calculations reported to date have been able to explain the anomalously low B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+}) ratios observed in these cases. Such low values cannot, e.g., be explained within the framework of the geometrical collective model or by algebraic approaches within the interacting boson model framework. It is proposed that the group of B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+}) ratios in the extremely neutron-deficient even-even W, Os, and Pt nuclei around neutron numbers N≈90-94 reveal a quantum phase transition from a seniority-conserving structure to a collective regime as a function of neutron number. 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An unusually low value of the ratio B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+})=0.55(19) was found, similar to a handful of other such anomalous cases observed in the entire Segré chart. The observation adds to a cluster of a few extremely neutron-deficient nuclides of the heavy transition metals with neutron numbers N≈90-94 featuring the effect. No theoretical model calculations reported to date have been able to explain the anomalously low B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+}) ratios observed in these cases. Such low values cannot, e.g., be explained within the framework of the geometrical collective model or by algebraic approaches within the interacting boson model framework. It is proposed that the group of B(E2:4_{1}^{+}→2_{1}^{+})/B(E2:2_{1}^{+}→0_{gs}^{+}) ratios in the extremely neutron-deficient even-even W, Os, and Pt nuclei around neutron numbers N≈90-94 reveal a quantum phase transition from a seniority-conserving structure to a collective regime as a function of neutron number. Although a system governed by seniority symmetry is the only theoretical framework for which such an effect may naturally occur, the phenomenon is highly unexpected for these nuclei that are not situated near closed shells.</abstract><cop>United States</cop><pub>American Physical Society</pub><pmid>30085703</pmid><doi>10.1103/PhysRevLett.121.022502</doi><tpages>1</tpages><orcidid>https://orcid.org/0000-0003-2300-2626</orcidid><orcidid>https://orcid.org/0000-0002-8335-452X</orcidid></addata></record> |
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title | Lifetime Measurements of Excited States in ^{172}Pt and the Variation of Quadrupole Transition Strength with Angular Momentum |
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