Abstract
The first measurements of the induced proton polarization for the reaction are reported. The experiment was performed at quasifree kinematics for energy and momentum transfer (294 MeV, 756 MeV/c) and sampled a missing momentum range of 0–250 MeV/c. The induced polarization arises from final-state interactions and for these kinematics is dominated by the real part of the spin-orbit optical potential. The distorted-wave impulse approximation provides good agreement with data for the shell. The data for the continuum suggest that both the shell and underlying configurations contribute.
- Received 29 July 1997
DOI:https://doi.org/10.1103/PhysRevLett.80.456
©1998 American Physical Society