101. Measurement of polarization-transfer to bound protons in carbon and its virtuality dependence
- Author
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A1 Collaboration, Izraeli, D., Brecelj, T., Achenbach, P., Ashkenazi, A., Böhm, R., Cohen, E. O., Distler, M. O., Esser, A., Gilman, R., Kolar, T., Korover, I., Lichtenstadt, J., Mardor, I., Merkel, H., Mihovilovič, M., Müller, U., Olivenboim, M., Piasetzky, E., Ron, G., Schlimme, B. S., Schoth, M., Sfienti, C., Širca, S., Štajner, S., Strauch, S., Thiel, M., Weber, A., and Yaron, I.
- Subjects
Nuclear Experiment - Abstract
We measured the ratio $P_{x}/P_{z}$ of the transverse to longitudinal components of polarization transferred from electrons to bound protons in $^{12}\mathrm{C}$ by the $^{12}\mathrm{C}(\vec{e},e'\vec{p})$ process at the Mainz Microtron (MAMI). We observed consistent deviations from unity of this ratio normalized to the free-proton ratio, $(P_{x}/P_{z})_{^{12}\mathrm{C}}/(P_{x}/P_{z})_{^{1}\mathrm{H}}$, for both $s$- and $p$-shell knocked out protons, even though they are embedded in averaged local densities that differ by about a factor of two. The dependence of the double ratio on proton virtuality is similar to the one for knocked out protons from $^{2}\mathrm{H}$ and $^{4}\mathrm{He}$, suggesting a universal behavior. It further implies no dependence on average local nuclear density.
- Published
- 2017
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