Comparative study of ${}^6$He $\beta$-decay based on different similarity-renormalization-group evolved chiral interactions

TL;DR

This study compares the effects of different SRG-evolved chiral interactions on the ${}^6$He $eta$-decay Gamow-Teller matrix element, highlighting the importance of consistent two-body current evolution and interaction model dependence.

Contribution

It provides a comparative analysis of ${}^6$He $eta$-decay using SRG-evolved chiral interactions from different EFT formulations, emphasizing the impact of interaction choice and SRG evolution on results.

Findings

Significant $ ext{SRG}$-dependence of two-body current contributions.

Strong dependence of one-pion-exchange currents on interaction models.

Need for consistent SRG evolution of currents for reliable estimates.

Abstract

We report on a study of the Gamow-Teller matrix element contributing to ${}^6$He $\beta$-decay with similarity renormalization group (SRG) versions of momentum- and configuration-space two-nucleon interactions. These interactions are derived from two different formulations of chiral effective field theory ($\chi$EFT) -- without and with the explicit inclusion of $\Delta$-isobars. We consider evolution parameters $\Lambda_{\rm SRG}$ in the range between 1.2 and 2.0 fm$^{-1}$ and, for the $\Delta$-less case, also the unevolved (bare) interaction. The axial current contains one- and two-body terms, consistently derived at tree level (no loops) in the two distinct $\chi$EFT formulations we have adopted here. The ${}^6$He and ${}^6$Li ground-state wave functions are obtained from hyperspherical-harmonics (HH) solutions of the nuclear many-body problem. In $A\,$=$\,6$ systems, the HH method is limited at present to treat only two-body interactions and non-SRG evolved currents. Our results exhibit a significant dependence on $\Lambda_{\text{SRG}}$ of the contributions associated with two-body currents, suggesting that a consistent SRG-evolution of these is needed in order to obtain reliable estimates. We also show that the contributions from one-pion-exchange currents depend strongly on the model (chiral) interactions and on the momentum- or configuration-space cutoffs used to regularize them. These results might prove helpful in clarifying the origin of the sign difference recently found in No-Core-Shell-Model and Quantum Monte Carlo calculations of the ${}^6$He Gamow-Teller matrix element.