arXiv2025
Measurements of $β$-spectral shapes is an important way to examine the effective value of the weak axial coupling $g_{\rm A}$. These stu\ dies focus specifically on forbidden non-unique $β^-$ transitions, as only in these cases is the spectral shape directly sensitive to th\ e ratio $g_{\rm A}/g_{\rm V}$. Here, the value of the weak vector coupling constant, $g_{\rm V}$, is fixed at 1.0 according to the Conserve\ d Vector Current (CVC) hypothesis. In previous studies for the fourth-forbidden non-unique $β^-$ decays of $^{113}$Cd [J.~Kostensalo \textit{et al.}, Phys. Lett. B 822, 136652 (2021)] and $^{115}$In [A.~F. Leder \textit{et al.}, Phys. Rev. Lett. 129, 232502 \ (2022) and L. Pagnanini \textit{et al.}, Phys. Rev. Lett. 133, 122501 (2024)] a quenched value was determined for the ratio $g_{\rm A}/g_{\rm V}$ using $g_{\rm V}=1.0$. A notable exception is the recent measurement and analysis of the second-forbidden non-unique $\ β$-decay transition in $^{99}$Tc, performed by M. Paulsen \textit{et al.}, Phys. Rev. C 110, 05503(2024). Where an enhanced ratio $g_{\\ rm A}/g_{\rm V}=1.526(92)$ was suggested. To resolve this apparently contradictory situation with the effective value of $g_{\rm A}$, we hav\ e performed calculations based on the nuclear shell model (NSM) Hamiltonians glekpn, jj45pnb, and the MQPM approach with a careful considera\ tion of the small relativistic vector nuclear matrix element (sNME). The theoretical spectra were compared to the $^{99}$Tc $β$-decay sp\ ectrum by using the 4$π$ gold absorber with a Metallic Magnetic Calorimeter (MMC). In all cases, we found that the data matches well with \ reduced $g_{\rm A}$/$g_{\rm V}$ values of 1.0--1.2. Our result contradicts the previously reported measurement for $^{99}$Tc and instead sup\ ports a quenched axial coupling as reported for other isotopes.