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Shape coexistence revealed in the $$N=Z$$ N = Z isotope $$^{72}$$ 72 Kr through inelastic scattering
The European Physical Journal A ( IF 2.6 ) Pub Date : 2020-06-03 , DOI: 10.1140/epja/s10050-020-00171-3
K. Wimmer , T. Arici , W. Korten , P. Doornenbal , J.-P. Delaroche , M. Girod , J. Libert , T. R. Rodríguez , P. Aguilera , A. Algora , T. Ando , H. Baba , B. Blank , A. Boso , S. Chen , A. Corsi , P. Davies , G. de Angelis , G. de France , D. T. Doherty , J. Gerl , R. Gernhäuser , T. Goigoux , D. Jenkins , G. Kiss , S. Koyama , T. Motobayashi , S. Nagamine , M. Niikura , S. Nishimura , A. Obertelli , D. Lubos , V. H. Phong , B. Rubio , E. Sahin , T. Y. Saito , H. Sakurai , L. Sinclair , D. Steppenbeck , R. Taniuchi , V. Vaquero , R. Wadsworth , J. Wu , M. Zielinska

The \(N=Z=36\) nucleus \(^{72}\)Kr has been studied by inelastic scattering at intermediate energies. Two targets, \(^{9}\)Be and \(^{197}\)Au, were used to extract the nuclear deformation length, \(\delta _\text {N}\), and the reduced E2 transition probability, B(E2). The previously unknown non-yrast \(2^+\) and \(4^+\) states as well as a new candidate for the octupole \(3^-\) state have been observed in the scattering on the Be target and placed in the level scheme based on \(\gamma -\gamma \) coincidences. The second \(2^+\) state was also observed in the scattering on the Au target and the \(B(E2;\;2^+_2 \rightarrow 0^+_1)\) value could be determined for the first time. Analyzing the results in terms of a two-band mixing model shows clear evidence for a oblate-prolate shape coexistence and can be explained by a shape change from an oblate ground state to prolate deformed yrast band from the first \(2^+\) state. This interpretation is corroborated by beyond mean field calculations using the Gogny D1S interaction.

中文翻译:

通过非弹性散射,在$ N = Z $$ N = Z同位素$$ ^ {72} $$ 72 Kr中揭示了形状共存

\(N = Z = 36 \)\(^ {72} \)氪已经研究了非弹性散射在中间能量。使用两个目标\(^ {9} \) Be和\(^ {197} \) Au来提取核变形长度\(\ delta _ \ text {N} \)和简化后的E 2转移概率BE 2)。在Be目标和目标上的散射中观察到了以前未知的非剧烈的\(2 ^ + \)\(4 ^ + \)状态以及八极\(3 ^-\)状态的新候选对象。根据\(\ gamma-\ gamma \)巧合放置在级别方案中。第二在金靶上的散射中也观察到\(2 ^ + \)状态,并且可以首次确定\(B(E2; \; 2 ^ + _ 2 \ rightarrow 0 ^ + _ 1)\)值。用两频带混合模型分析结果显示了扁圆形形状共存的明确证据,并且可以通过从第一\(2 ^ + \)从扁圆形基态到扁形变形的yrast带的形状变化来解释。州。使用Gogny D1S交互进行的超出平均范围的计算证实了这种解释。
更新日期:2020-06-03
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