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<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/"><rdf:Description rdf:about="https://repozitorij.uni-lj.si/IzpisGradiva.php?id=124741"><dc:title>Measurement of recoil proton polarization in the $\mathrm{^{12}C(\vec e, e' \vec p)}$ process at large virtualities</dc:title><dc:creator>Kolar,	Tim	(Avtor)
	</dc:creator><dc:creator>Širca,	Simon	(Mentor)
	</dc:creator><dc:subject>polarized electron beam</dc:subject><dc:subject>electron-proton scattering</dc:subject><dc:subject>lepton-induced reactions</dc:subject><dc:subject>nuclear shell model</dc:subject><dc:subject>polarimetry</dc:subject><dc:subject>magnetic charged-particle spectrometers</dc:subject><dc:description>Electron scattering experiments of the A$(\vec{e},e'\vec{p})$ type involving degrees of freedom related to the polarization of the particles are a rich source of information about the proton structure, both when embedded inside nucleus or when it is free (A=$^1$H). This was established by numerous experiments which were conducted on $^1$H, $^2$H, $^4$He, $^{12}$C, and $^{16}$O targets. These measurements presented the results, typically, as a function of momentum transfer squared or missing momentum. Only recently a new variable, called virtuality, has become a more popular choice. This is mainly due to the fact that the polarization transfer component ratio normalized with the same ratio for hydrogen, $\mathrm{(P'_x/P'_z)_A/(P'_x/P'_z)_{^1H}}$, which can be related to the change of electromagnetic form-factor ratio, $\mathrm{G^p_E/G^p_M}$, of the bound proton, exhibits universal behavior once it is considered as a function of virtuality, regardless of which target nucleus is used. 

This work presents the first measurement of the polarization transfer components in the A$(\vec{e},e'\vec{p})$ process in quasi-elastic kinematics for protons of similar virtualities that were knocked out from the s$_{1/2}$ and p$_{3/2}$ shells in $^{12}$C. With this experiment we wanted to exploit the predicted difference between the local nuclear densities exhibited by protons when bound in s$_{1/2}$ and p$_{3/2}$ shells to study possible density-dependent in-medium modifications of proton's electromagnetic form factors. Within the uncertainties of our measurements we observed no such modification and found a relatively good agreement between experimental results and the predicted polarization components calculated in relativistic distorted-wave impulse approximation (RDWIA).</dc:description><dc:date>2021</dc:date><dc:date>2021-02-13 08:15:02</dc:date><dc:type>Doktorsko delo/naloga</dc:type><dc:identifier>124741</dc:identifier><dc:language>sl</dc:language></rdf:Description></rdf:RDF>
