Physics Letters B (Jan 2022)
Measurements of the electron-helicity asymmetry in the quasi-elastic A(e→,e′p) process
- T. Kolar,
- S.J. Paul,
- P. Achenbach,
- H. Arenhövel,
- A. Ashkenazi,
- J. Beričič,
- R. Böhm,
- D. Bosnar,
- T. Brecelj,
- E. Cline,
- E.O. Cohen,
- M.O. Distler,
- A. Esser,
- I. Friščić,
- R. Gilman,
- C. Giusti,
- M. Heilig,
- M. Hoek,
- D. Izraeli,
- S. Kegel,
- P. Klag,
- I. Korover,
- J. Lichtenstadt,
- I. Mardor,
- H. Merkel,
- D.G. Middleton,
- M. Mihovilovič,
- J. Müller,
- U. Müller,
- M. Olivenboim,
- E. Piasetzky,
- J. Pochodzalla,
- G. Ron,
- B.S. Schlimme,
- M. Schoth,
- F. Schulz,
- C. Sfienti,
- S. Širca,
- R. Spreckels,
- S. Štajner,
- Y. Stöttinger,
- S. Strauch,
- M. Thiel,
- A. Tyukin,
- A. Weber,
- I. Yaron
Affiliations
- T. Kolar
- School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel; Corresponding author.
- S.J. Paul
- School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel
- P. Achenbach
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- H. Arenhövel
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- A. Ashkenazi
- School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel
- J. Beričič
- Jožef Stefan Institute, 1000 Ljubljana, Slovenia
- R. Böhm
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- D. Bosnar
- Department of Physics, University of Zagreb, HR-10002 Zagreb, Croatia
- T. Brecelj
- Jožef Stefan Institute, 1000 Ljubljana, Slovenia
- E. Cline
- Rutgers, The State University of New Jersey, Piscataway, NJ 08855, USA
- E.O. Cohen
- School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel
- M.O. Distler
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- A. Esser
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- I. Friščić
- Department of Physics, University of Zagreb, HR-10002 Zagreb, Croatia
- R. Gilman
- Rutgers, The State University of New Jersey, Piscataway, NJ 08855, USA
- C. Giusti
- Dipartimento di Fisica, Università degli Studi di Pavia and INFN, Sezione di Pavia, via A. Bassi 6, I-27100 Pavia, Italy
- M. Heilig
- Universität Konstanz, Fachbereich Physik, Universitätsstraße 10, 78464 Konstanz, Germany
- M. Hoek
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- D. Izraeli
- School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel
- S. Kegel
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- P. Klag
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- I. Korover
- Department of Physics, NRCN, P.O. Box 9001, Beer-Sheva 84190, Israel; School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel
- J. Lichtenstadt
- School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel
- I. Mardor
- School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel; Soreq NRC, Yavne 81800, Israel
- H. Merkel
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- D.G. Middleton
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- M. Mihovilovič
- Faculty of Mathematics and Physics, University of Ljubljana, 1000 Ljubljana, Slovenia; Jožef Stefan Institute, 1000 Ljubljana, Slovenia; Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- J. Müller
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- U. Müller
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- M. Olivenboim
- School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel
- E. Piasetzky
- School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel
- J. Pochodzalla
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- G. Ron
- Racah Institute of Physics, Hebrew University of Jerusalem, Jerusalem 91904, Israel
- B.S. Schlimme
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- M. Schoth
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- F. Schulz
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- C. Sfienti
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- S. Širca
- Faculty of Mathematics and Physics, University of Ljubljana, 1000 Ljubljana, Slovenia; Jožef Stefan Institute, 1000 Ljubljana, Slovenia
- R. Spreckels
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- S. Štajner
- Jožef Stefan Institute, 1000 Ljubljana, Slovenia
- Y. Stöttinger
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- S. Strauch
- University of South Carolina, Columbia, SC 29208, USA
- M. Thiel
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- A. Tyukin
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- A. Weber
- Institut für Kernphysik, Johannes Gutenberg-Universität, 55099 Mainz, Germany
- I. Yaron
- School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel
- Journal volume & issue
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Vol. 824
p. 136798
Abstract
We present measurements of the electron helicity asymmetry in quasi-elastic proton knockout from 2H and 12C 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 11B system. We find that the helicity asymmetry for p-shell knockout from 12C 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 12C and 2H. The data for 2H are in very good agreement with theoretical calculations, while the predictions for 12C exhibit differences with respect to the data.