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The ${^3}He(e,e'd)p reaction in (q,omega)-constant kinematics

  • C.M. Spaltro
  • , Th.S. Bauer
  • , H.P. Blok
  • , T. Botto
  • , E. Cisbani
  • , R. De Leo
  • , G. Dodge
  • , R. Ent
  • , S. Frullani
  • , F. Garibaldi
  • , J. Glöckle
  • , J. Golak
  • , M. Iodice
  • , E. Jans
  • , H. Kamada
  • , W.J. Kadorp
  • , C. Kormanyos
  • , L. Lapikás*
  • , A. Misiejuk
  • , S.I. Nagorny
  • G.J.L. Nooren, Gerco Onderwater, R. Perrino, M. van Sambeek, R. Skibilski, R. Starink, M.A. van Uden, G.M. Urciouli, H. de Vries, H. Witala, D.M. Yeomans, M.N. Harakeh, G. van der Steenhoven, J. Tjon
*Corresponding author voor dit werk

    OnderzoeksoutputAcademicpeer review

    10 Citaten (Scopus)

    Samenvatting

    The cross section for the 3He(e,e′d)p reaction has been measured as a function of the missing momentum pm in (q,ω)-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.
    Originele taal-2English
    Pagina's (van-tot)403-417
    Aantal pagina's15
    TijdschriftNuclear Physics A
    Volume706
    DOI's
    StatusPublished - 2002

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