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R. J. Feuerbach

Researcher at Thomas Jefferson National Accelerator Facility

Publications -  48
Citations -  1505

R. J. Feuerbach is an academic researcher from Thomas Jefferson National Accelerator Facility. The author has contributed to research in topics: Nucleon & Scattering. The author has an hindex of 21, co-authored 48 publications receiving 1404 citations.

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Scaling tests of the cross section for deeply virtual Compton scattering.

TL;DR: The first measurements of the e[over -->]p-->epgamma cross section in the deeply virtual Compton scattering (DVCS) regime and the valence quark region are presented, proving that generalized parton distributions (GPDs) are accessible to experiment at moderate Q(2), and the first model-independent measurement of linear combinations of GPDs and GPD integrals up to the twist-3 approximation.
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Precision Measurements of the Nucleon Strange Form Factors at Q 2 ∼ 0.1 GeV 2

A. Acha, +102 more
TL;DR: In this article, the parity-violating asymmetry A_PV in elastic scattering of 3 GeV electrons off hydrogen and 4He targets with ~6.0 degrees was measured.
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Parity-violating electron scattering from 4He and the strange electric form factor of the nucleon.

K. A. Aniol, +79 more
TL;DR: For the first time, the strange electric form factor of the nucleon G(E)s can be isolated and the parity-violating electroweak asymmetry in the elastic scattering of polarized electrons from 4He is measured.
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Investigation of proton-proton short-range correlations via the 12C(e,e'pp) reaction.

R. Shneor, +80 more
TL;DR: At these kinematics, with a missing momentum greater than the Fermi momentum of nucleons in a nucleus and far from the delta excitation, short-range nucleon-nucleon correlations are predicted to dominate the reaction.
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Constraints on the nucleon strange form factors at Q2 ∼ 0.1 GeV2

K. A. Aniol, +80 more
- 20 Apr 2006 - 
TL;DR: In this paper, the most precise measurement to date of parity-violating asymmetry in elastic electron-proton scattering was reported, with the result A PV = ( − 1.14 ± 0.6 × 10 −6 ) where the first two errors are experimental and the last error is due to the uncertainty in the neutron electromagnetic form factor.