Scaling function and nucleon momentum distribution

J. A. Caballero, M. B. Barbaro, A. N. Antonov, M. V. Ivanov, and T. W. Donnelly
Phys. Rev. C 81, 055502 – Published 18 May 2010

Abstract

Scaling studies of inclusive quasielastic electron scattering reactions have been used in the past as a basic tool to obtain information on the nucleon momentum distribution in nuclei. However, the connection between the scaling function, extracted from the analysis of cross-section data, and the spectral function only exists assuming very restricted approximations. We revisit the basic expressions involved in scaling studies and how they can be linked to the nucleon momentum distribution. In particular, the analysis applied in the past to the so-called scaling region, that is, negative values of the scaling variable y, is extended here to positive y, as a “universal” superscaling function has been extracted from the analysis of the separated longitudinal data. This leads to results that clearly differ from those based solely on the negative-y scaling region, providing new information on how the energy and momentum are distributed in the spectral function.

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  • Received 10 March 2010

DOI:https://doi.org/10.1103/PhysRevC.81.055502

©2010 American Physical Society

Authors & Affiliations

J. A. Caballero1,*, M. B. Barbaro2, A. N. Antonov3, M. V. Ivanov3, and T. W. Donnelly4

  • 1Departamento de Física Atómica, Molecular y Nuclear, Universidad de Sevilla, ES-41080 Sevilla, Spain
  • 2Dipartimento di Fisica Teorica, Università di Torino and INFN, Sezione di Torino, Via P. Giuria 1, I-10125 Torino, Italy
  • 3Institute for Nuclear Research and Nuclear Energy, Bulgarian Academy of Sciences, BG-1784 Sofia, Bulgaria
  • 4Center for Theoretical Physics, Laboratory for Nuclear Science and Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA

  • *jac@us.es

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Vol. 81, Iss. 5 — May 2010

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