The strong force which binds hadrons is described by the theory of quantum
chromodynamics (QCD). Determining the character and manifestations of QCD is one of the …

We highlight the progress, current status, and open challenges of QCD-driven physics, in
theory and in experiment. We discuss how the strong interaction is intimately connected to a …

Models of weakly interacting massive particles (WIMPs) specified at the electroweak scale
are systematically matched to effective theories at hadronic scales where WIMP-nucleus …

We present high statistics results for the structure of the nucleon from a mixed-action
calculation using 2+ 1 flavors of asqtad sea and domain-wall valence fermions. We perform …

We present results for the isovector electromagnetic form factors of the nucleon computed on
the coordinated lattice simulations ensembles with N f= 2+ 1 flavors of O (a)-improved …

The Q weak experiment has measured the parity-violating asymmetry in e→ p elastic
scattering at Q 2= 0.025 (GeV/c) 2, employing 145 μ A of 89% longitudinally polarized …

We extract the individual contributions from u and d quarks to the Dirac and Pauli form
factors of the proton, after a critical examination of the available measurements of …

The u-and d-quark contributions to the elastic nucleon electromagnetic form factors have
been determined by using experimental data on GE n, GM n, GE p, and GM p. Such a flavor …

We have measured parity-violating asymmetries in elastic electron-proton and quasielastic
electron-deuteron scattering at Q 2= 0.22 and 0.63 GeV 2. They are sensitive to strange …

We present lattice-QCD results for the electromagnetic form factors of the proton and neutron
including both quark-connected and-disconnected contributions. The parametrization of the …