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Spaltro, C. M; Bauer, Th. S; Blok, H. P; Botto, T; Cisbani, E; De Leo, R; Dodge, G. E; Ent, R; Frullani, S; Garibaldi, F; Gloeckle, W; Golak, J; Harakeh, M. N; Iodice, M; Jans, E; Kamada, H; Kasdorp, W. J; Kormanyos, C; Lapikas, L; Misiejuk, A; Nagorny, S. I; Nooren, G. J; Onderwater, C. J. G; Perrino, R; van Sambeek, M; Skibinski, R; Starink, R; van der Steenhoven, G; Tjon, J; van Uden, M. A; Urciuoli, G. M; de Vries, H; Witala, H; Yeomans, M
01/2002Journal Article
Nucl.Phys.A706:403-417,2002 The cross section for the $^3$He(e, e$'$d)p reaction has been measured as a function of the missing momentum $p_m$ 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 \mevc. The L(+TT), T and LT structure functions have been separated for $q$ = 412 and 504 \mevc. 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 $p_m$-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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