Coulomb energy differences in t = 1 mirror rotational bands in (50)Fe and (50)Cr
Gamma rays from the N = Z-2 nucleus (50)Fe have been observed, establishing the rotational ground state band up to the state J(pi) = 11+ at 6.994 MeV excitation energy. The experimental Coulomb energy differences, obtained by comparison with the isobaric analog states in its mirror (50)Cr, confirm t...
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creator | Lenzi, S M Mărginean, N Napoli, D R Ur, C A Zuker, A P de Angelis, G Algora, A Axiotis, M Bazzacco, D Belcari, N Bentley, M A Bizzeti, P G Bizzeti-Sona, A Brandolini, F von Brentano, P Bucurescu, D Cameron, J A Chandler, C De Poli, M Dewald, A Eberth, H Farnea, E Gadea, A Garces-Narro, J Gelletly, W Grawe, H Isocrate, R Joss, D T Kalfas, C A Klug, T Lampman, T Lunardi, S Martínez, T Martínez-Pinedo, G Menegazzo, R Nyberg, J Podolyak, Z Poves, A Ribas, R V Rossi Alvarez, C Rubio, B Sánchez-Solano, J Spolaore, P Steinhardt, T Thelen, O Tonev, D Vitturi, A von Oertzen, W Weiszflog, M |
description | Gamma rays from the N = Z-2 nucleus (50)Fe have been observed, establishing the rotational ground state band up to the state J(pi) = 11+ at 6.994 MeV excitation energy. The experimental Coulomb energy differences, obtained by comparison with the isobaric analog states in its mirror (50)Cr, confirm the qualitative interpretation of the backbending patterns in terms of successive alignments of proton and neutron pairs. A quantitative agreement with experiment has been achieved by exact shell model calculations, incorporating the differences in radii along the yrast bands, and properly renormalizing the Coulomb matrix elements in the pf model space. |
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The experimental Coulomb energy differences, obtained by comparison with the isobaric analog states in its mirror (50)Cr, confirm the qualitative interpretation of the backbending patterns in terms of successive alignments of proton and neutron pairs. A quantitative agreement with experiment has been achieved by exact shell model calculations, incorporating the differences in radii along the yrast bands, and properly renormalizing the Coulomb matrix elements in the pf model space.</description><identifier>ISSN: 0031-9007</identifier><identifier>EISSN: 1079-7114</identifier><identifier>PMID: 11580500</identifier><language>eng</language><publisher>United States: American Physical Society</publisher><ispartof>Physical review letters, 2001-09, Vol.87 (12), p.122501-122501</ispartof><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0001-7539-388X ; 0000-0001-5477-6021</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/11580500$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink><backlink>$$Uhttps://in2p3.hal.science/in2p3-00011010$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Lenzi, S M</creatorcontrib><creatorcontrib>Mărginean, N</creatorcontrib><creatorcontrib>Napoli, D R</creatorcontrib><creatorcontrib>Ur, C A</creatorcontrib><creatorcontrib>Zuker, A P</creatorcontrib><creatorcontrib>de Angelis, G</creatorcontrib><creatorcontrib>Algora, A</creatorcontrib><creatorcontrib>Axiotis, M</creatorcontrib><creatorcontrib>Bazzacco, D</creatorcontrib><creatorcontrib>Belcari, N</creatorcontrib><creatorcontrib>Bentley, M A</creatorcontrib><creatorcontrib>Bizzeti, P G</creatorcontrib><creatorcontrib>Bizzeti-Sona, A</creatorcontrib><creatorcontrib>Brandolini, F</creatorcontrib><creatorcontrib>von Brentano, P</creatorcontrib><creatorcontrib>Bucurescu, D</creatorcontrib><creatorcontrib>Cameron, J A</creatorcontrib><creatorcontrib>Chandler, C</creatorcontrib><creatorcontrib>De Poli, M</creatorcontrib><creatorcontrib>Dewald, A</creatorcontrib><creatorcontrib>Eberth, H</creatorcontrib><creatorcontrib>Farnea, E</creatorcontrib><creatorcontrib>Gadea, A</creatorcontrib><creatorcontrib>Garces-Narro, J</creatorcontrib><creatorcontrib>Gelletly, W</creatorcontrib><creatorcontrib>Grawe, H</creatorcontrib><creatorcontrib>Isocrate, R</creatorcontrib><creatorcontrib>Joss, D T</creatorcontrib><creatorcontrib>Kalfas, C A</creatorcontrib><creatorcontrib>Klug, T</creatorcontrib><creatorcontrib>Lampman, T</creatorcontrib><creatorcontrib>Lunardi, S</creatorcontrib><creatorcontrib>Martínez, T</creatorcontrib><creatorcontrib>Martínez-Pinedo, G</creatorcontrib><creatorcontrib>Menegazzo, R</creatorcontrib><creatorcontrib>Nyberg, J</creatorcontrib><creatorcontrib>Podolyak, Z</creatorcontrib><creatorcontrib>Poves, A</creatorcontrib><creatorcontrib>Ribas, R V</creatorcontrib><creatorcontrib>Rossi Alvarez, C</creatorcontrib><creatorcontrib>Rubio, B</creatorcontrib><creatorcontrib>Sánchez-Solano, J</creatorcontrib><creatorcontrib>Spolaore, P</creatorcontrib><creatorcontrib>Steinhardt, T</creatorcontrib><creatorcontrib>Thelen, O</creatorcontrib><creatorcontrib>Tonev, D</creatorcontrib><creatorcontrib>Vitturi, A</creatorcontrib><creatorcontrib>von Oertzen, W</creatorcontrib><creatorcontrib>Weiszflog, M</creatorcontrib><title>Coulomb energy differences in t = 1 mirror rotational bands in (50)Fe and (50)Cr</title><title>Physical review letters</title><addtitle>Phys Rev Lett</addtitle><description>Gamma rays from the N = Z-2 nucleus (50)Fe have been observed, establishing the rotational ground state band up to the state J(pi) = 11+ at 6.994 MeV excitation energy. The experimental Coulomb energy differences, obtained by comparison with the isobaric analog states in its mirror (50)Cr, confirm the qualitative interpretation of the backbending patterns in terms of successive alignments of proton and neutron pairs. 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The experimental Coulomb energy differences, obtained by comparison with the isobaric analog states in its mirror (50)Cr, confirm the qualitative interpretation of the backbending patterns in terms of successive alignments of proton and neutron pairs. A quantitative agreement with experiment has been achieved by exact shell model calculations, incorporating the differences in radii along the yrast bands, and properly renormalizing the Coulomb matrix elements in the pf model space.</abstract><cop>United States</cop><pub>American Physical Society</pub><pmid>11580500</pmid><tpages>1</tpages><orcidid>https://orcid.org/0000-0001-7539-388X</orcidid><orcidid>https://orcid.org/0000-0001-5477-6021</orcidid></addata></record> |
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title | Coulomb energy differences in t = 1 mirror rotational bands in (50)Fe and (50)Cr |
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