Physics Letters B (Dec 2020)
Measurements of the induced polarization in the quasi-elastic A(e,e′p→) process in non-coplanar kinematics
- S.J. Paul,
- T. Kolar,
- T. Brecelj,
- P. Achenbach,
- H. Arenhövel,
- A. Ashkenazi,
- J. Beričič,
- R. Böhm,
- D. Bosnar,
- E. Cline,
- E.O. Cohen,
- L. Debenjak,
- M.O. Distler,
- A. Esser,
- I. Friščić,
- R. Gilman,
- C. Giusti,
- M. Heilig,
- M. Hoek,
- D. Izraeli,
- S. Kegel,
- P. Klag,
- Y. Kohl,
- 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,
- S. Strauch,
- M. Thiel,
- A. Tyukin,
- A. Weber,
- I. Yaron
Affiliations
- S.J. Paul
- School of Physics and Astronomy, Tel Aviv University, Tel Aviv 69978, Israel; Corresponding author.
- T. Kolar
- Jožef Stefan Institute, 1000 Ljubljana, Slovenia
- T. Brecelj
- Jožef Stefan Institute, 1000 Ljubljana, Slovenia
- 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
- 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
- L. Debenjak
- Jožef Stefan Institute, 1000 Ljubljana, Slovenia
- 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
- Y. Kohl
- 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
- 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
-
Vol. 811
p. 135984
Abstract
We report measurements of the induced polarization P→ of protons knocked out from 2H and 12C via the A(e,e′p→) reaction. We have studied the dependence of P→ on two kinematic variables: the missing momentum pmiss and the “off-coplanarity” angle ϕpq between the scattering and reaction planes. For the full 360° range in ϕpq, both the normal (Py) and, for the first time, the transverse (Px) components of the induced polarization were measured with respect to the coordinate system associated with the scattering plane. Px vanishes in coplanar kinematics, however in non-coplanar kinematics, it is on the same scale as Py.We find that the dependence on ϕpq is sine-like for Px and cosine-like for Py. For carbon, the magnitude of the induced polarization is especially large when protons are knocked out from the p3/2 shell at very small pmiss. For the deuteron, the induced polarization is near zero at small |pmiss|, and its magnitude increases with |pmiss|. For both nuclei such behavior is reproduced qualitatively by theoretical results, driven largely by the spin-orbit part of the final-state interactions. However, for both nuclei, sizeable discrepancies exist between experiment and theory.