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C. M. Spaltro; Th. S. Bauer; H. P. Blok; T. Botto; E. Cisbani; R. De Leo; G. E. Dodge; R. Ent; S. Frullani; F. Garibaldi; W. Gloeckle; J. Golak; M. N. Harakeh; M. Iodice; E. Jans; H. Kamada; W. J. Kasdorp; C. Kormanyos; L. Lapikas; A. Misiejuk; S. I. Nagorny; G. J. Nooren; C. J. G. Onderwater; R. Perrino; M. van Sambeek; R. Skibiski; R. Starink; G. van der Steenhoven; J. Tjon; M. A. van Uden; G. M. Urciuoli; H. de Vries; H. Witaa; M. Yeomans
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2002
Thomas Jefferson National Accelerator Facility, Newport News, VA (United States). Funding organisation: USDOE Office of Energy Research (ER) (United States)2002
AbstractAbstract
[en] The cross section for the 3He(e,e(prime)d)p reaction has been measured as a function of the missing momentum pm in (q,omega)-constant kinematics at beam energies of 370 and 576 MeV for values of the three-momentum transfer q of 412, 504 and 604 MeV/c. The L(+ TT), T and LT structure functions have been separated for q=412 and 504 MeV/c. The data are compared to three-body Faddeev calculations, including meson-exchange currents (MEC), and to calculations based on a covariant diagrammatic expansion. The influence of final-state interactions and meson-exchange currents is discussed. The pm-dependence of the data is reasonably well described by all calculations. However, the most advanced Faddeev calculations, which employ the AV18 nucleon-nucleon interaction and include MEC, overestimate the measured cross sections, especially the longitudinal part, and at the larger values of q. The diagrammatic approach gives a fair description of the cross section, but under (over)estimates the longitudinal (transverse) structure function
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Source
JLAB-PHY--02-42; DOE/ER--40150-2316
Record Type
Journal Article
Journal
Nuclear Physics. A; ISSN 0375-9474; ; v. 706(3-4); p. 403-417
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