Erratum: New Perspectives on Spectroscopic Factor Quenching from Reactions [Phys. Rev. Lett. 131, 212503 (2023)]

Figure 1

Angular distributions for (a) ${}^{34}\mathrm{Ar}(p,d){}^{33}\mathrm{Ar}(\mathrm{g}.\mathrm{s}.)$, (b) ${}^{36}\mathrm{Ar}(p,d){}^{35}\mathrm{Ar}(\mathrm{g}.\mathrm{s}.)$, and (c) ${}^{46}\mathrm{Ar}(p,d){}^{45}\mathrm{Ar}(\mathrm{g}.\mathrm{s}.)$ at $33A\mathrm{MeV}$. All theoretical distributions have been scaled to reproduce the data from Ref. [2], and the scaling factors are the extracted SFs (shown in Table 1). The uncertainties result from both theoretical (obtained sampling the true KDUQ posterior distribution [1]) and experimental errors.

Figure 2

Ratio of the SF extracted from data and the shell model SF as a function of the asymmetry of the nucleus $\mathrm{\Delta }S=S_n-S_p$. The blue error bars correspond to the SFs extracted from the transfer data (see Table 1) and the red ones to the SFs extracted from the knockout data (see Table III of the Letter). Each error bar shows the $1\sigma$ and $2\sigma$ uncertainties. The shaded area corresponds to the $1\sigma$ uncertainties of a linear fit of the transfer (blue) and knockout (red) error bars.