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Phys. Rev. C 69, 034604 (2004) [15 pages]

Analysis of polarized 16O(e⃗,ep⃗) observables within the relativistic distorted wave impulse approximation

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M. C. Martínez1, J. R. Vignote2, J. A. Caballero1, T. W. Donnelly3, E. Moya de Guerra4, and J. M. Udías2
1Departamento de Física Atómica, Molecular y Nuclear, Universidad de Sevilla, Apartado Postal 1065, E-41080 Sevilla, Spain
2Departamento de Física Atómica, Molecular y Nuclear, Universidad Complutense de Madrid, E-28040 Madrid, Spain
3Center for Theoretical Physics, Laboratory for Nuclear Science and Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
4Instituto de Estructura de la Materia, CSIC, Serrano 123, E-28006 Madrid, Spain

Received 22 September 2003; published 12 March 2004

Recoil nucleon transferred polarization observables in coincidence quasielastic electron scattering are studied within the relativistic distorted wave impulse approximation. Results for response functions and polarization asymmetries are discussed for proton knockout from p1∕2, p3∕2, and s1∕2 shells in 16O. The impact of spinor distortion is examined by comparing the fully relativistic calculation with results obtained by projecting out the negative-energy components. In particular, a careful analysis of effects linked to the description of the bound and scattered relativistic nucleon wave functions is presented. The high sensitivity of some polarization observables to the dynamical enhancement of the lower components, already shown within the relativistic plane wave impulse approximation, is proven to be maintained in the relativistic distorted wave approach. Semi-relativistic approaches based on the effective momentum approximation are also studied. Finally, comparison with experimental data and a brief analysis of effects linked to medium modified form factors is presented.

© 2004 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.69.034604
DOI:
10.1103/PhysRevC.69.034604
PACS:
25.30.Rw, 14.20.Gk, 24.10.Jv, 24.30.Gd