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Phys. Rev. C 37, 231–238 (1988)

High momentum components in nuclei

Abstract
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M. Avan, A. Baldit, J. Castor, M. El Zoubidi, J. Fargeix, H. Fonvieille, P. Force, J. L. Guelou, B. Harradi, and G. Landaud
Laboratoire de Physique Corpusculaire, Université de Clermont II, 63170 Aubiere, France

J. P. Didelez and F. Reide
Institut de Physique Nucléaire, 91406 Orsay, France

M. Bernheim, A. Gerard, A. Magnon, C. Marchand, J. Morgenstern, J. Picard, and and P. Vernin
Departement de Physique Nucléaire, Centre d’Etudes Nucléaires de Saclay, Gif-sur-Yvette, France

H. Jackson
Argonne National Laboratory, Argonne, Illinois

Received 22 April 1987; published in the issue dated January 1988

To clarify the analysis of our existing backward proton scattering data in terms of high momentum components in nuclei, we have measured exclusive cross sections for the backward energetic protons in coincidence with the γ rays emitted by the target. At 200 MeV incident proton energy, the mass distribution of the residual nuclei from a 28Si target suggests a single scattering reaction on a nucleon of the target. We have also performed large momentum transfer electron scattering on 12C and 58Ni using a 640 MeV electron beam. These data analyzed within the quasi-two-body scaling approach display a scaling regime identical to the one previously observed for the protons. Both of these features give credence to the ‘‘single scattering,’’ basic assumption in the quasi-two-body scaling theory. The experimental momentum distribution is in good agreement with several theoretical predictions which include short range correlations.

© 1988 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.37.231
DOI:
10.1103/PhysRevC.37.231
PACS:
25.30.Fj, 25.40.-h, 25.40.Gr, 25.90.+k