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 language | English |
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Article number | 064327 |
Journal | Physical Review C |
Volume | 103 |
Issue number | 6 |
DOIs | |
State | Published - Jun 2021 |
Externally published | Yes |
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.
Funders | Funder number |
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U.S. Department of Energy | |
Office of Science | |
Nuclear Physics | DE-SC0009971, DE-FG02-03ER41272 |
National Natural Science Foundation of China | 12035001, 11835001, 11921006 |
China Postdoctoral Science Foundation | BX20200136 |
National Key Research and Development Program of China | 2018YFA0404401 |
State Key Laboratory of Nuclear Physics and Technology, Peking University | NPT2020ZZ01 |