We present a new formulation of one of the major radiative corrections to the weak charge of the proton—that arising from the axial-vector hadron part of the γZ box diagram, ℜe□γZA. This formulation, based on dispersion relations, relates the γZ contributions to moments of the F₃γZ interference structure function. It has a clear connection to the pioneering work of Marciano and Sirlin, and enables a systematic approach to improved numerical precision. Using currently available data, the total correction from all intermediate states is ℜe□γZA=0.004 4(4) at zero energy, which shifts the theoretical estimate of the proton weak charge from 0.071 3(8) to 0.070 5(8). The energy dependence of this result, which is vital for interpreting the Qweak ...
We examine the interference γZ box corrections to parity-violating elastic electron–proton scatterin...
The weak charge of the proton has been determined for the first time via a high precision electron-p...
The Qweak collaboration at Jefferson Lab made the first direct measurement of the proton\u27s weak c...
Precision measurements offer important, low-energy tests of the Standard Model. The Qweak and (propo...
We present a new dispersive formulation of the γZ box radiative corrections to weak charges of bound...
We present a comprehensive analysis of γZ interference corrections to the weak charge of the proton ...
We use dispersion relations to evaluate the γZ box contribution to parity-violating electron scatter...
We present a comprehensive analysis of gamma-Z interference corrections to the weak charge of the pr...
The possibility of measuring the parity-violating asymmetry in Møller scattering with sufficient acc...
The possibility of measuring the parity-violating asymmetry in Møller scattering with sufficient acc...
We generalize forward real Compton amplitude to the case of the interference of the electromagnetic ...
The Qweak experiment at Jefferson Laboratory will make a 4% measurement of the proton's weak charge,...
The relativistic quark models study the hadronic systems in terms of the constituent quarks by using...
The Unitary and analytic model of nucleon electromagnetic structure, describing all existing nucleon...
In neutral current e"#+-#p deep inelastic scattering events the exchanged electroweak boson bet...
We examine the interference γZ box corrections to parity-violating elastic electron–proton scatterin...
The weak charge of the proton has been determined for the first time via a high precision electron-p...
The Qweak collaboration at Jefferson Lab made the first direct measurement of the proton\u27s weak c...
Precision measurements offer important, low-energy tests of the Standard Model. The Qweak and (propo...
We present a new dispersive formulation of the γZ box radiative corrections to weak charges of bound...
We present a comprehensive analysis of γZ interference corrections to the weak charge of the proton ...
We use dispersion relations to evaluate the γZ box contribution to parity-violating electron scatter...
We present a comprehensive analysis of gamma-Z interference corrections to the weak charge of the pr...
The possibility of measuring the parity-violating asymmetry in Møller scattering with sufficient acc...
The possibility of measuring the parity-violating asymmetry in Møller scattering with sufficient acc...
We generalize forward real Compton amplitude to the case of the interference of the electromagnetic ...
The Qweak experiment at Jefferson Laboratory will make a 4% measurement of the proton's weak charge,...
The relativistic quark models study the hadronic systems in terms of the constituent quarks by using...
The Unitary and analytic model of nucleon electromagnetic structure, describing all existing nucleon...
In neutral current e"#+-#p deep inelastic scattering events the exchanged electroweak boson bet...
We examine the interference γZ box corrections to parity-violating elastic electron–proton scatterin...
The weak charge of the proton has been determined for the first time via a high precision electron-p...
The Qweak collaboration at Jefferson Lab made the first direct measurement of the proton\u27s weak c...