CLAS Physics Database

Electron Scattering from a High-Momentum Neutron in Deuterium

Spokesperson
Sebastian Kuhn
Year
2002
Abstract
We report results from an experiment measuring the semiinclusive reaction D(e,e`ps) where the proton ps is moving at a large angle relative to the momentum transfer. If we assume that the proton was a spectator to the reaction taking place on the neutron in deuterium, the initial state of that neutron can be inferred. This method, known as spectator tagging, can be used to study electron scattering from high-momentum (off-shell) neutrons in deuterium. The data were taken with a 5.765 GeV electron beam on a deuterium target in Jefferson Laboratory's Hall B, using the CLAS detector. A reduced cross section was extracted for different values of final-state missing mass $W^{*}$, backward proton momentum $\vec{p}_{s}$ and momentum transfer $Q^{2}$. The data are compared to a simple PWIA spectator model. A strong enhancement in the data observed at transverse kinematics is not reproduced by the PWIA model and can be associated with the contribution of final state interactions (FSI) that were not incorporated into the model. A ``bound neutron structure function'' \f2neff was extracted as a function of $W^{*}$ and the scaling variable $x^{*}$ at extreme backward kinematics, where effects of FSI appear to be small. For $p_{s}>400\,\,\mathrm{MeV/c}$, where the neutron is far off-shell, the model overestimates the value of $F_{2n}$ in the region of $x^{*}$ between 0.25 and 0.6. A modification of the bound neutron structure function is one of possible effects that can cause the observed deviation.
Publication
  1. A. V. Klimenko, S. E. Kuhn, and CLAS Collaboration Electron Scattering From High-Momentum Neutrons in Deuterium // Phys. Rev. C 73, 035212 (2006) arXiv:nucl-ex/0510032
Quantities
F2 * P(Pt) F2 * P(Ps) F2(x*,Q2)

Measurements

ID Quantity Beam Target Final state Q2min,
GeV2
Q2max,
GeV2
Wmin,
GeV
Wmax,
GeV
E90M201 F2 * P(Pt) e d p+X 0.45 0.45 2.4 2.4
E90M202 F2 * P(Pt) e d p+X 0.55 0.55 2.4 2.4
E90M203 F2 * P(Pt) e d p+X 0.65 0.65 2.4 2.4
E90M204 F2 * P(Pt) e d p+X 0.35 0.35 2.4 2.4
E90M205 F2 * P(Pt) e d p+X 0.45 0.45 2.4 2.4
E90M206 F2 * P(Pt) e d p+X 0.55 0.55 2.4 2.4
E90M207 F2 * P(Pt) e d p+X 0.65 0.65 2.4 2.4
E90M208 F2 * P(Pt) e d p+X 0.18 0.18 2.4 2.4
E90M209 F2 * P(Pt) e d p+X 0.25 0.25 2.4 2.4
E90M210 F2 * P(Pt) e d p+X 0.35 0.35 2.4 2.4
E90M211 F2 * P(Pt) e d p+X 0.45 0.45 2.4 2.4
E90M212 F2 * P(Pt) e d p+X 0.55 0.55 2.4 2.4
E90M213 F2 * P(Pt) e d p+X 0.65 0.65 2.4 2.4
E90M214 F2 * P(Pt) e d p+X 0.25 0.25 2.4 2.4
E90M215 F2 * P(Pt) e d p+X 0.35 0.35 2.4 2.4
E90M216 F2 * P(Pt) e d p+X 0.45 0.45 2.4 2.4
E90M217 F2 * P(Pt) e d p+X 0.55 0.55 2.4 2.4
E90M218 F2 * P(Pt) e d p+X 0.65 0.65 2.4 2.4
E90M219 F2 * P(Pt) e d p+X 0.18 0.18 2.4 2.4
E90M220 F2 * P(Pt) e d p+X 0.25 0.25 2.4 2.4
E90M221 F2 * P(Pt) e d p+X 0.35 0.35 2.4 2.4
E90M222 F2 * P(Pt) e d p+X 0.45 0.45 2.4 2.4
E90M223 F2 * P(Pt) e d p+X 0.55 0.55 2.4 2.4
E90M224 F2 * P(Pt) e d p+X 0.65 0.65 2.4 2.4
E90M225 F2 * P(Pt) e d p+X 0.25 0.25 2.4 2.4
E90M226 F2 * P(Pt) e d p+X 0.35 0.35 2.4 2.4
E90M227 F2 * P(Pt) e d p+X 0.45 0.45 2.4 2.4
E90M228 F2 * P(Pt) e d p+X 0.55 0.55 2.4 2.4
E90M229 F2 * P(Pt) e d p+X 0.65 0.65 2.4 2.4
E90M230 F2 * P(Pt) e d p+X 0.18 0.18 2.4 2.4
E90M231 F2 * P(Pt) e d p+X 0.25 0.25 2.4 2.4
E90M232 F2 * P(Pt) e d p+X 0.35 0.35 2.4 2.4
E90M233 F2 * P(Pt) e d p+X 0.45 0.45 2.4 2.4
E90M234 F2 * P(Pt) e d p+X 0.55 0.55 2.4 2.4
E90M235 F2 * P(Pt) e d p+X 0.65 0.65 2.4 2.4
E90M236 F2 * P(Pt) e d p+X 0.25 0.25 2.4 2.4
E90M237 F2 * P(Pt) e d p+X 0.35 0.35 2.4 2.4
E90M238 F2 * P(Pt) e d p+X 0.45 0.45 2.4 2.4
E90M239 F2 * P(Pt) e d p+X 0.55 0.55 2.4 2.4
E90M240 F2 * P(Pt) e d p+X 0.65 0.65 2.4 2.4
E90M241 F2 * P(Pt) e d p+X 0.18 0.18 2.4 2.4
E90M242 F2 * P(Pt) e d p+X 0.25 0.25 2.4 2.4
E90M243 F2 * P(Pt) e d p+X 0.35 0.35 2.4 2.4
E90M244 F2 * P(Pt) e d p+X 0.45 0.45 2.4 2.4
E90M245 F2 * P(Pt) e d p+X 0.55 0.55 2.4 2.4
E90M246 F2 * P(Pt) e d p+X 0.65 0.65 2.4 2.4
E90M247 F2 * P(Pt) e d p+X 0.25 0.25 2.4 2.4
E90M248 F2 * P(Pt) e d p+X 0.35 0.35 2.4 2.4
E90M249 F2 * P(Pt) e d p+X 0.45 0.45 2.4 2.4
E90M250 F2 * P(Pt) e d p+X 0.55 0.55 2.4 2.4
E90M251 F2 * P(Pt) e d p+X 0.65 0.65 2.4 2.4