The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of the momentum transfer in the reaction H-2(e, e'p) have been measured at a four-momentum transfer squared of 0.2 (GeV/c)(2), for missing momenta between 160 and 220 MeV/c at an invariant mass of 1050 MeV. For a proper description of these data calculations that include a relativistic form of the nucleon current operator are favoured. The absolute 2H(e, e'p) cross-section data favour a covariant calculation over non-relativistic calculations with relativistic corrections
Using the covariant spectator theory and the transversity formalism, the unpolarized, coincidence cr...
Cross sections are presented for the reaction 2H(e,e′p)n for momentum transfers in the range 1.2≤Q2≤...
In a series of recent publications, a new approach to the non-relativistic reduction of the electrom...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
Using the covariant spectator theory and the transversity formalism, the unpolarized, coincidence cr...
Cross sections are presented for the reaction 2H(e,e′p)n for momentum transfers in the range 1.2≤Q2≤...
In a series of recent publications, a new approach to the non-relativistic reduction of the electrom...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The structure function R(LT) and the cross-section asymmetry A(phi) with respect to the direction of...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
The reaction (2)H(e, e'p) has been studied at an invariant mass W of 1050 MeV, i.e. well below the D...
Using the covariant spectator theory and the transversity formalism, the unpolarized, coincidence cr...
Cross sections are presented for the reaction 2H(e,e′p)n for momentum transfers in the range 1.2≤Q2≤...
In a series of recent publications, a new approach to the non-relativistic reduction of the electrom...