Tensor force role in β decays analyzed within the Gogny-interaction shell model

B. Dai, B. S. Hu, Y. Z. Ma, J. G. Li, S. M. Wang, C. W. Johnson, F. R. Xu

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Abstract

Background: The half-life of the famous C14β decay is anomalously long, with different mechanisms: the tensor force, cross-shell mixing, and three-body forces, proposed to explain the cancellations that lead to a small transition matrix element. Purpose: We revisit and analyze the role of the tensor force for the β decay of C14 as well as of neighboring isotopes. Methods: We add a tensor force to the Gogny interaction, and derive an effective Hamiltonian for shell-model calculations. The calculations were carried out in a p-sd model space to investigate cross-shell effects. Furthermore, we decompose the wave functions according to the total orbital angular momentum L in order to analyze the effects of the tensor force and cross-shell mixing. Results: The inclusion of the tensor force significantly improves the shell-model calculations of the β-decay properties of carbon isotopes. In particular, the anomalously slow β decay of C14 can be explained by the isospin T=0 part of the tensor force, which changes the components of N14 with the orbital angular momentum L=0,1, and results in a dramatic suppression of the Gamow-Teller transition strength. At the same time, the description of other nearby β decays are improved. Conclusions: Decomposition of wave function into L components illuminates how the tensor force modifies nuclear wave functions, in particular suppression of β-decay matrix elements. Cross-shell mixing also has a visible impact on the β-decay strength. Inclusion of the tensor force does not seem to significantly change, however, binding energies of the nuclei within the phenomenological interaction.

Original languageEnglish
Article number064327
JournalPhysical Review C
Volume103
Issue number6
DOIs
StatePublished - Jun 2021
Externally publishedYes

Funding

This work has been supported by the National Key Research and Development Program of China under Grant No. 2018YFA0404401; the National Natural Science Foundation of China under Grants No. 11835001, 11921006, and 12035001; China Postdoctoral Science Foundation under Grant No. BX20200136; the State Key Laboratory of Nuclear Physics and Technology, Peking University under Grant No. NPT2020ZZ01; by the U.S. Department of Energy, Office of Science, Office of Nuclear Physics, under Award No. DE-FG02-03ER41272, and by the CUSTIPEN (China-U.S. Theory Institute for Physics with Exotic Nuclei) funded by the U.S. Department of Energy, Office of Science under Award No. DE-SC0009971. We acknowledge the High-Performance Computing Platform of Peking University for providing computational resources.

FundersFunder number
U.S. Department of Energy
Office of Science
Nuclear PhysicsDE-SC0009971, DE-FG02-03ER41272
National Natural Science Foundation of China12035001, 11835001, 11921006
China Postdoctoral Science FoundationBX20200136
National Key Research and Development Program of China2018YFA0404401
State Key Laboratory of Nuclear Physics and Technology, Peking UniversityNPT2020ZZ01

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