Abstract
The proton momentum distribution of $^{3}\mathrm{He}$ has been determined up to momenta of 310 MeV/c by use of the reaction $^{3}\mathrm{He}(e, {e}^{\ensuremath{'}}p)$. The experimental missing-energy resolution, $\ensuremath{\delta}{E}_{m}=1.2$ MeV, was sufficient to separate the two- and three-body breakup channels. Results for the three-body disintegration have been obtained up to missing-energy values of 80 MeV. The resulting spectral function is compared to the predictions of Faddeev and variational calculations.
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