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通过电荷交换减法二次随机相位近似计算\(^{48}Ca\)和\(^{78}Ni\)中的伽莫夫-泰勒强度

Gamow-Teller Strength in ^{48}Ca and ^{78}Ni with the Charge-Exchange Subtracted Second Random-Phase Approximation.

作者信息

Gambacurta D, Grasso M, Engel J

机构信息

INFN-LNS, Laboratori Nazionali del Sud, 95123 Catania, Italy.

Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.

出版信息

Phys Rev Lett. 2020 Nov 20;125(21):212501. doi: 10.1103/PhysRevLett.125.212501.

DOI:10.1103/PhysRevLett.125.212501
PMID:33274967
Abstract

We develop a fully self-consistent subtracted second random-phase approximation for charge-exchange processes with Skyrme energy-density functionals. As a first application, we study Gamow-Teller excitations in the doubly magic nucleus ^{48}Ca, the lightest double-β emitter that could be used in an experiment, and in ^{78}Ni, the single-beta-decay rate of which is known. The amount of Gamow-Teller strength below 20 or 30 MeV is considerably smaller than in other energy-density-functional calculations and agrees better with experiment in ^{48}Ca, as does the beta-decay rate in ^{78}Ni. These important results, obtained without ad hoc quenching factors, are due to the presence of two-particle-two-hole configurations. Their density progressively increases with excitation energy, leading to a long high-energy tail in the spectrum, a fact that may have implications for the computation of nuclear matrix elements for neutrinoless double-β decay in the same framework.

摘要

我们针对采用斯凯瑞能量密度泛函的电荷交换过程,开发了一种完全自洽的减法二次随机相位近似方法。作为首个应用,我们研究了双幻核(^{48}Ca)(可用于实验的最轻双β衰变发射体)以及(^{78}Ni)(其单β衰变率已知)中的伽莫夫-泰勒激发。低于20或30兆电子伏特的伽莫夫-泰勒强度比其他能量密度泛函计算结果小得多,并且在(^{48}Ca)中与实验结果的吻合度更高,(^{78}Ni)中的β衰变率也是如此。这些重要结果在没有特设猝灭因子的情况下获得,归因于两粒子两空穴组态的存在。它们的密度随激发能逐渐增加,导致谱中出现长长的高能尾部,这一事实可能对在同一框架下计算无中微子双β衰变的核矩阵元有影响。

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