Comparison of recoil polarization in the $^{12}{\rm C}(\vec{e},{e}'\vec{p})$ process for protons extracted from $s$ and $p$ shell

T. Kolar,S. Paul, T. Brecelj,P. Achenbach,R. Böhm,D. Bosnar,E. O. Cohen,M. O. Distler,A. Esser,C. Giusti,M. Hoek,D. Izraeli,S. Kegel, Y. Kohl,I. Korover,J. Lichtenstadt,I. Mardor,H. Merkel, M. Mihovilovič,J. Müller,U. Müller, M. Olivenboim, E. Piasetzky, J. Pochodzalla, B. S. Schlimme, C. Sfienti, S. Širca, R. Spreckels,S. Štajner,M. Thiel,A. Weber,I. Yaron, for the A Collaboration

arxiv(2020)

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摘要
We present first measurements of the double ratio of the polarization transfer components $(P^{\prime}_{\!x} \!/ P^{\prime}_{\!z} )_p/ (P^{\prime}_{\!x} \!/ P^{\prime}_{\!z} )_s$ for knock-out protons from $s$ and $p$ shells in $^{12}{\rm C}$ measured by the $^{12}{\rm C}(\vec{e},{e}'\vec{p}\,)$ reaction in quasi-elastic kinematics. The data are compared to theoretical predictions in relativistic distorted-wave impulse approximation. Our results show that differences between $s$- and $p$-shell protons, observed when compared at the same initial momentum (missing momentum) largely disappear when the comparison is done at the same proton virtuality. We observe no density-dependent medium modifications for protons from $s$ and $p$ shells with the same virtuality in spite of the large differences in the respective nuclear densities.
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