6533b833fe1ef96bd129b8c2
RESEARCH PRODUCT
Measurement of the parity violating asymmetry in the quasielastic electron-deuteron scattering and improved determination of the magnetic strange form factor and the isovector anapole radiative correction
R. KunneJ. ArvieuxC. WeinrichR. FrascariaJongmin LeeStanley B. KowalskiS. OngY. ImaiKurt AulenbacherD. Balaguer RíosD. Von HarrachHarald MerkelM. C. Mora EspíB. GläserE. SchillingR. KotheL. CapozzaJ. Van De WieleU. MüllerJ. DiefenbachF. E. MaasS. BaunackE. M. KabußYelena ProkM. A. El-yakoubisubject
Particle physicsacceleratorparity: violation: asymmetrymedia_common.quotation_subjectLattice field theoryisovectorelectron deuteron: inelastic scatteringpolarized beamElectron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]form factor: axial-vector01 natural sciencesAsymmetryMainz Linac0103 physical sciencesdeuterium: targetradiative correctionelectron: beam010306 general physicsmedia_commonPhysicsQuasielastic scatteringIsovector010308 nuclear & particles physicsScatteringbackgroundlattice field theoryParity (physics)helicityanapoleHelicityelectron deuteron: scatteringexperimental resultsdescription
A new measurement of the parity-violating asymmetry in the electron-deuteron quasielastic scattering for backward angles at $⟨{Q}^{2}⟩=0.224\text{ }\text{ }{(\mathrm{GeV}/c)}^{2}$, obtained in the A4 experiment at the Mainz Microtron accelerator (MAMI) facility, is presented. The measured asymmetry is ${A}_{PV}^{d}=(\ensuremath{-}20.11\ifmmode\pm\else\textpm\fi{}0.8{7}_{\mathrm{stat}}\ifmmode\pm\else\textpm\fi{}\phantom{\rule{0ex}{0ex}}1.0{3}_{\mathrm{sys}})\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}6}$. A combination of these data with the proton measurements of the parity-violating asymmetry in the A4 experiment yields a value for the effective isovector axial-vector form factor of ${G}_{A}^{e,(T=1)}=\ensuremath{-}0.19\ifmmode\pm\else\textpm\fi{}0.43$ and ${R}_{A}^{(T=1),\mathrm{anap}}=\ensuremath{-}0.41\ifmmode\pm\else\textpm\fi{}0.35$ for the anapole radiative correction. When combined with a reanalysis of measurements obtained in the G0 experiment at the Thomas Jefferson National Accelerator Facility, the uncertainties are further reduced to ${G}_{M}^{s}=0.17\ifmmode\pm\else\textpm\fi{}0.11$ for the magnetic strange form factors, and ${R}_{A}^{(T=1),\mathrm{anap}}=\ensuremath{-}0.54\ifmmode\pm\else\textpm\fi{}0.26$.
year | journal | country | edition | language |
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2016-09-12 |