1. Measurements of the electron-helicity asymmetry in the quasi-elastic Process
- Author
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Kolar, T., Paul, S.J., Achenbach, P., Arenhövel, H., Ashkenazi, A., Beričič, J., Böhm, R., Bosnar, D., Brecelj, T., Cline, E., Cohen, E.O., Distler, M.O., Esser, A., Friščić, I., Gilman, R., Giusti, C., Heilig, M., Hoek, M., Izraeli, D., Kegel, S., Klag, P., Korover, I., Lichtenstadt, J., Mardor, I., Merkel, H., Middleton, D.G., Mihovilovič, M., Müller, J., Müller, U., Olivenboim, M., Piasetzky, E., Pochodzalla, J., Ron, G., Schlimme, B.S., Schoth, M., Schulz, F., Sfienti, C., Širca, S., Spreckels, R., Štajner, S., Stöttinger, Y., Strauch, S., Thiel, M., Tyukin, A., Weber, A., and Yaron, I.
- Abstract
We present measurements of the electron helicity asymmetry in quasi-elastic proton knockout from $^{2}$H and $^{12}$C nuclei by polarized electrons. This asymmetry depends on the fifth structure function, is antisymmetric with respect to the scattering plane, and vanishes in the absence of final-state interactions, and thus it provides a sensitive tool for their study. Our kinematics cover the full range in off-coplanarity angle ϕpq, with a polar angle θpq coverage up to about 8°. The missing energy resolution enabled us to determine the asymmetries for knock-out resulting in different states of the residual $^{11}$B system. We find that the helicity asymmetry for p-shell knockout from $^{12}$C depends on the final state of the residual system and is relatively large (up to ≈0.16), especially at low missing momentum. It is considerably smaller (up to ≈0.01) for s-shell knockout from both $^{12}$C and $^{2}$H. The data for $^{2}$H are in very good agreement with theoretical calculations, while the predictions for $^{12}$C exhibit differences with respect to the data.
- Published
- 2022