English

Exploring $\beta$ decay and $\beta$-delayed neutron emission in exotic $^{46,47}$Cl isotopes

Nuclear Experiment 2025-08-12 v2

Abstract

In this paper, β\beta^- and β\beta-delayed neutron decays of 46,47^{46,47}Cl are reported from an experiment carried out at the National Superconducting Cyclotron Laboratory using the Beta Counting System. The half-lives of both 46^{46}Cl and 47^{47}Cl were extracted. Based on the delayed γ\gamma-ray transitions observed, the level structure of N=28N = 28 46^{46}Ar was determined. Completely different sets of excited states above the first 2+2^+ state in 46^{46}Ar were populated in the 46^{46}Cl β0n\beta0n and 47^{47}Cl β1n\beta1n decay channels. Two new γ\gamma-ray transitions in 47^{47}Ar were identified from the very weak 47^{47}Cl β0n\beta0n decay. Furthermore, 46^{46}Cl β1n\beta1n and 47^{47}Cl β2n\beta2n were also observed to yield different population patterns for levels in 45^{45}Ar, including states of different parities. The experimental results allow us to address some of the open questions related to the delayed neutron emission process. For isotopes with large neutron excess and high QβQ_{\beta} values, delayed neutron emission remains an important decay mode and can be utilized as a powerful spectroscopic tool. Experimental results were compared with shell-model calculations using the FSU and VMUV_{MU} effective interactions.

Keywords

Cite

@article{arxiv.2502.19378,
  title  = {Exploring $\beta$ decay and $\beta$-delayed neutron emission in exotic $^{46,47}$Cl isotopes},
  author = {Vandana Tripathi and B. Longfellow and A. Volya and E. Rubino and C. Benetti and J. F. Perello and S. L. Tabor and S. N. Liddick and P. C. Bender and M. P. Carpenter and J. J. Carroll and A. Chester and C. J. Chiara and K. Childers and B. R. Clark and B. P. Crider and J. T. Harke and R. Jain and S. Luitel and M. J. Mogannam and T. H. Ogunbeku and A. L. Richard and S. Saha and O. A. Shehu and R. Unz and Y. Xiao and Yiyi Zhu},
  journal= {arXiv preprint arXiv:2502.19378},
  year   = {2025}
}