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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=175984"><dc:title>Measurement of the helicity-dependent response in quasi-elastic proton knockout from $^{40}$Ca</dc:title><dc:creator>Kolar,	Tim	(Avtor)
	</dc:creator><dc:creator>Mihovilovič,	Miha	(Avtor)
	</dc:creator><dc:creator>Požun,	Matej	(Avtor)
	</dc:creator><dc:creator>Širca,	Simon	(Avtor)
	</dc:creator><dc:subject>nuclear physics</dc:subject><dc:subject>nuclear structure</dc:subject><dc:subject>electron scattering</dc:subject><dc:subject>final-state interactions</dc:subject><dc:subject>nuclear optical potential</dc:subject><dc:subject>polarized electron scattering</dc:subject><dc:subject>beam helicity asymmetry</dc:subject><dc:description>The role of the electron-helicity-dependent cross-section term and the structure function $f'_{01}$ in the quasi-elastic $A(\overrightarrow{e}, e' p)$ process was studied. The $f'_{01}$  was measured for proton knockout from the $1\mathrm{d}_{3/2}$ shell in $^{40}$Ca via the $^{40}$Ca$(\overrightarrow{e}, e' p)^{39} K_{g. s.}$  reaction, leaving the residual nucleus in a well-defined state. It requires a longitudinally polarized electron beam and out-of-plane proton detection. This structure function vanishes in the absence of final-state interactions (FSI) involving the ejected proton. Presented are the dependencies of $f'_{01}$ on the missing momentum (closely related to the initial proton’s Fermi momentum) and the angle between the knocked-out proton and the virtual photon momenta. The role of the spin-orbit interaction in FSI through the $\overrightarrow{L}\cdot \overrightarrow{S}$ term in a nuclear optical potential is discussed.</dc:description><dc:date>2025</dc:date><dc:date>2025-11-17 11:27:26</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>175984</dc:identifier><dc:language>sl</dc:language></rdf:Description></rdf:RDF>
