6533b85cfe1ef96bd12bd2ef

RESEARCH PRODUCT

Measurement of the Neutron Electric to Magnetic Form Factor Ratio atQ2=1.58  GeV2Using the ReactionHe→3(e→,e′n)pp

J. PochodzallaM. M. SargsianS. ŠIrcaT. HehlC. J. YoonS. Sánchez MajosHarald MerkelJ. KrimmerC. Ayerbe GayosoM. WendelB. S. SchlimmeL. NungesserM. O. DistlerM. WeinrieferU. MüllerP. GrabmayrMihael MakekD. KiselevM. PotokarP. AchenbachM. Gómez RodríguezIngo SickF. FellenbergerB. A. OttH. FonvieilleLuca DoriaD. G. MiddletonJan C. BernauerTh. ChallandWerner HeilR. BöhmDamir Bosnar

subject

PhysicsSystematic error010308 nuclear & particles physicsGeneral Physics and AstronomyElectron01 natural sciencesHelicityPolarized target0103 physical sciencesMagnetic form factorHigh Energy Physics::ExperimentNeutronAtomic physicsNuclear Experiment010306 general physics

description

A measurement of beam helicity asymmetries in the reaction $^{3}\stackrel{\ensuremath{\rightarrow}}{\mathrm{He}}(\stackrel{\ensuremath{\rightarrow}}{e},{e}^{\ensuremath{'}}n)pp$ is performed at the Mainz Microtron in quasielastic kinematics to determine the electric to magnetic form factor ratio of the neutron ${G}_{E}^{n}/{G}_{M}^{n}$ at a four-momentum transfer ${Q}^{2}=1.58\text{ }\text{ }{\mathrm{GeV}}^{2}$. Longitudinally polarized electrons are scattered on a highly polarized $^{3}\mathrm{He}$ gas target. The scattered electrons are detected with a high-resolution magnetic spectrometer, and the ejected neutrons are detected with a dedicated neutron detector composed of scintillator bars. To reduce systematic errors, data are taken for four different target polarization orientations allowing the determination of ${G}_{E}^{n}/{G}_{M}^{n}$ from a double ratio. We find ${\ensuremath{\mu}}_{n}{G}_{E}^{n}/{G}_{M}^{n}=0.250\ifmmode\pm\else\textpm\fi{}0.058(\mathrm{stat})\ifmmode\pm\else\textpm\fi{}0.017(\mathrm{syst})$.

https://doi.org/10.1103/physrevlett.111.132504