1995
DOI: 10.1103/physrevc.52.1216
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Inclusive electron scattering onH3andHe

Abstract: InClusive electron scattering data on 3He and 3H are analyzed under full treatment of the final state interactions (FSI) using realistic nucleon-nucleon forces. The data are well described. We use two different methods, one where we calculate the pd and ppn breakup contributions separately and another one which is related to the optical theorem for Compton scattering. Both rely on precise solutions of Faddeev-like equations and agree perfectly. The importance of FSI and the inclusion of total isospin T= 3/2 fo… Show more

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Cited by 28 publications
(58 citation statements)
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“…The rather tedious but known steps to evaluate the overlaps between momentum vector states with shifted vector arguments and our partial wave projected basis states as well as the six fold integration can be carried through analytically with the techniques presented in [69]. Results for various partial wave projected matrix elements can be found in [51,73,101,107]. As an example the expression in (234) results for an…”
Section: The Performancementioning
confidence: 99%
See 3 more Smart Citations
“…The rather tedious but known steps to evaluate the overlaps between momentum vector states with shifted vector arguments and our partial wave projected basis states as well as the six fold integration can be carried through analytically with the techniques presented in [69]. Results for various partial wave projected matrix elements can be found in [51,73,101,107]. As an example the expression in (234) results for an…”
Section: The Performancementioning
confidence: 99%
“…We refrain to quote again the simpler equations given in [48][49][50][51]73] valid for NN forces only. The more complex equations are necessary since for light nuclei [26,74] and few-nucleon scattering processes [18] 3N forces are mandatory.…”
Section: Formalism In the Faddeev Schemementioning
confidence: 99%
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“…It is worth noting that i) the inclusion of the final state interaction (FSI), between the knocked out nucleon and the spectator pair, ii) the meson exchange currents, iii) the relativistic corrections and iv) the presence of the ∆ in the bound-state, are still open problems for the inclusive polarized responses of the three-nucleon system. As far as the first topic is concerned, that only for unpolarized cross sections refined calculations including FSI are available [10,11], exhibiting large FSI effects at very low momentum transfer (Q 2 < 0.1 (GeV /c) 2 ), while at Q 2 > 0.25 (GeV /c) 2 PWIA calculations are able to give a good description of the experimental data at the qe peak, both for the unpolarized longitudinal and transverse response functions [12,13].…”
Section: Introductionmentioning
confidence: 99%