6533b7dbfe1ef96bd12713f7

RESEARCH PRODUCT

Measurements of the induced polarization in the quasi-elastic A(e,e′p→) process in non-coplanar kinematics

Concettina SfientiM. HeiligS. StrauchM. HoekT. BreceljRonald GilmanT. KolarJ. MüllerHarald MerkelS. ŠIrcaS. ŠIrcaPatrick AchenbachIvica FriščićU. MüllerD. IzraeliS. KegelJ. PochodzallaR. SpreckelsAnselm EsserMichaela ThielL. DebenjakJ. BeričičD. G. MiddletonJ. LichtenstadtGuy RonD. BosnarAdi AshkenaziI. YaronM. OlivenboimS. ŠTajnerM. SchothI. KoroverA. WeberHartmuth ArenhövelCarlotta GiustiB. S. SchlimmeE. ClineF. SchulzM. O. DistlerM. MihovilovičM. MihovilovičM. MihovilovičEliahu CohenE. PiasetzkyR. BöhmIsrael MardorS.j. PaulP. KlagY. KohlA. Tyukin

subject

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsPlane (geometry)ScatteringShell (structure)7. Clean energy01 natural sciencesInduced polarizationp-processMomentumTransverse planeDeuterium0103 physical sciencesAtomic physics010306 general physics

description

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 p miss and the “off-coplanarity” angle ϕ p q between the scattering and reaction planes. For the full 360° range in ϕ p q , both the normal ( P y ) and, for the first time, the transverse ( P x ) components of the induced polarization were measured with respect to the coordinate system associated with the scattering plane. P x vanishes in coplanar kinematics, however in non-coplanar kinematics, it is on the same scale as P y . We find that the dependence on ϕ p q is sine-like for P x and cosine-like for P y . For carbon, the magnitude of the induced polarization is especially large when protons are knocked out from the p 3 / 2 shell at very small p miss . For the deuteron, the induced polarization is near zero at small | p miss | , and its magnitude increases with | p miss | . 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.

https://doi.org/10.1016/j.physletb.2020.135984