Abstract

The axial charge in the weak nucleon axial vector current has been precisely determined by measuring the alignment correlation terms in the $\ensuremath{\beta}$-ray angular distributions of the purely spin aligned mirror pair nuclei ${}^{12}\mathrm{B}{(I}^{\ensuremath{\pi}}{=1}^{+}{,T}_{1/2}=20.2 \mathrm{ms})$ and ${}^{12}\mathrm{N}{(I}^{\ensuremath{\pi}}{=1}^{+}{,T}_{1/2}=11.0 \mathrm{ms}).$ The axial charge was determined to be $y=4.96\ifmmode\pm\else\textpm\fi{}0.09$ $(\mathrm{stat}.)\ifmmode\pm\else\textpm\fi{}0.05$ $(\mathrm{syst}.)$ at a 90% confidence level. The previously obtained data in the year 1996 was reanalyzed to be added to the present result. The combined result is $y=4.90\ifmmode\pm\else\textpm\fi{}0.10$ at a 90% confidence level. The axial charge is enhanced as much as $(72\ifmmode\pm\else\textpm\fi{}4)%$ from the impulse approximation model calculated value ${y}_{\mathrm{IA}}=2.85.$ Calculations using the impulse approximation with the soft-$\ensuremath{\pi}$ contribution ${y}_{\mathrm{th}}=4.15$ explain the data quite well but not completely. If we introduce the in-medium mass renormalization the unexplained part of the experimental result corresponds to an in nuclear-medium nucleon mass reduction of $(16\ifmmode\pm\else\textpm\fi{}4)%$ at a 90% confidence level relative to the free nucleon mass, at the place where the decaying nucleon resides.

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