Nuclear density dependence of polarization transfer in quasi-elastic ${\rm A}(\vec{e},e' \vec{p})$ reactions (2311.01935v3)
Abstract: The ratio of the transverse and longitudinal component of polarization transfer to protons in the quasi-elastic $(\vec{e}, e{\prime} \vec{p}\,)$ reaction, $P{\prime}_x/P{\prime}_z$, is sensitive to the proton's electromagnetic form factor ratio, $G_E/G_M$. To explore density-dependent in-medium modifications, a comparison of polarization transfer ratios involving protons from distinct nuclear shells, each with different local nuclear densities, has been proposed. In this study, we present such comparisons between four shells, $1s_{1/2}$, $1p_{3/2}$ in ${12}\mathrm{C}$ and $1d_{3/2}$, $2s_{1/2}$ in ${40}\mathrm{Ca}$. In an effort to account for other many-body effects that may differ between shells, we use a state-of-the-art relativistic distorted-wave impulse-approximation (RDWIA) calculation and present the double ratios, $(P{\prime}x/P{\prime}_z){\rm Data}/(P{\prime}x/P{\prime}_z){\rm RDWIA}$ as well as the super ratios, $\left[(P{\prime}x/P{\prime}_z){\rm A}/(P{\prime}x/P{\prime}_z){\rm B}\right]{\rm Data}/\left[(P{\prime}_x/P{\prime}_z){\rm A}/(P{\prime}x/P{\prime}_z){\rm B}\right]_{\rm RDWIA}$, for chosen shells A and B, as a function of effective local nuclear densities. We find that double ratios for individual shells show a dependence on the probed effective nuclear densities. Studying the ratios, we observed a systematic variation between pairs of higher- and lower-density shells.
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