To probe CP violation in the leptonic sector using GeV energy neutrino beams in current and future experiments using argon detectors, precise models of the complex underlying neutrino and antineutrino interactions are needed. The E12-14-012 experiment at Jefferson Lab Hall A was designed to perform a combined analysis of inclusive and exclusive electron scatterings on both argon (N = 22) and titanium (Z = 22) nuclei using GeV-energy electron beams. The measurement on titanium nucleus provides essential information to understand the neutrino scattering on argon, large contribution to which comes from scattering off neutrons. Here we report the first experimental study of electron-titanium scattering as double-differential cross section at be...
The electron (anti-)neutrino component of the T2K neutrino beam constitutes the largest background i...
The first direct measurement of electron neutrino quasielastic and quasielasticlike scattering on hy...
The E12-14-012 experiment, performed in Jefferson Lab Hall A, has collected exclusive electron-scatt...
To probe CP violation in the leptonic sector using GeV energy neutrino beams in current and future e...
To probe CP violation in the leptonic sector using GeV energy neutrino beams in current and future e...
To probeCPviolation in the leptonic sector usingGeVenergy neutrino beams in current and future exper...
The success of the ambitious programs of both long- and short-baseline neutrino-oscillation experime...
The success of the ambitious programs of both long- and short-baseline neutrino-oscillation experime...
The E12-14-012 experiment, performed in Jefferson Lab Hall A, has collected exclusive electron-scatt...
The E12-14-012 experiment performed at Jefferson Lab Hall A has collected inclusive electron-scatter...
The E12-14-012 experiment, performed in Jefferson Lab Hall A, has measured the (e,e′p) cross section...
Knowledge of neutrino cross sections is critical for understanding neutrino oscillation experiments....
We present the first measurement of the single-differential νe+¯νe charged-current inclusive cross s...
The E12-14-012 experiment, performed in Jefferson Lab Hall A, has measured the (e,e′p) cross section...
The electron (anti-)neutrino component of the T2K neutrino beam constitutes the largest background i...
The first direct measurement of electron neutrino quasielastic and quasielasticlike scattering on hy...
The E12-14-012 experiment, performed in Jefferson Lab Hall A, has collected exclusive electron-scatt...
To probe CP violation in the leptonic sector using GeV energy neutrino beams in current and future e...
To probe CP violation in the leptonic sector using GeV energy neutrino beams in current and future e...
To probeCPviolation in the leptonic sector usingGeVenergy neutrino beams in current and future exper...
The success of the ambitious programs of both long- and short-baseline neutrino-oscillation experime...
The success of the ambitious programs of both long- and short-baseline neutrino-oscillation experime...
The E12-14-012 experiment, performed in Jefferson Lab Hall A, has collected exclusive electron-scatt...
The E12-14-012 experiment performed at Jefferson Lab Hall A has collected inclusive electron-scatter...
The E12-14-012 experiment, performed in Jefferson Lab Hall A, has measured the (e,e′p) cross section...
Knowledge of neutrino cross sections is critical for understanding neutrino oscillation experiments....
We present the first measurement of the single-differential νe+¯νe charged-current inclusive cross s...
The E12-14-012 experiment, performed in Jefferson Lab Hall A, has measured the (e,e′p) cross section...
The electron (anti-)neutrino component of the T2K neutrino beam constitutes the largest background i...
The first direct measurement of electron neutrino quasielastic and quasielasticlike scattering on hy...
The E12-14-012 experiment, performed in Jefferson Lab Hall A, has collected exclusive electron-scatt...