6533b7dbfe1ef96bd127099c
RESEARCH PRODUCT
Measurement of the Recoil Polarization in thep(e→,e′p→)π0Reaction at theΔ(1232)Resonance
I. EwaldJustin I. McintyreR. D. RansomeGlen A. WarrenU. MüllerH. SchmiedenTh. WalcherJ.m. FriedrichMichael SeimetzIngo SickD. BaumannHarald MerkelG. RosnerG. RosnerDaniela RoheF. KleinP. BartschA. WagnerJ. LacKlemen BohincKlemen BohincS. HedickeM. O. DistlerM. KahrauP. MerleR. BöhmS. S. KamalovS. S. KamalovS. ŠIrcaS. ŠIrcaM. DingM. WeisD. ElsnerA. SüleR. GeigesJ. BermuthM. PotokarL. TiatorS. DerberP. JenneweinK. W. KrygierTh. PospischilJ.m. FriedrichJ.m. FriedrichR. NeuhausenA. LiesenfeldDieter Drechselsubject
PhysicsParallel kinematicsRecoil protonRecoilGeneral Physics and AstronomyAtomic physicsPolarization (waves)description
The recoil proton polarization has been measured in the $p(\stackrel{\ensuremath{\rightarrow}}{e}{,e}^{\ensuremath{'}}\stackrel{\ensuremath{\rightarrow}}{p}){\ensuremath{\pi}}^{0}$ reaction in parallel kinematics around $W\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}1232\phantom{\rule{0ex}{0ex}}\mathrm{MeV}$, ${Q}^{2}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}0.121\phantom{\rule{0ex}{0ex}}(\mathrm{GeV}/c{)}^{2}$, and $\ensuremath{\epsilon}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}0.718$ using the polarized cw electron beam of the Mainz Microtron. All three proton polarization components, ${P}_{x}/{P}_{e}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}(\ensuremath{-}11.4\ifmmode\pm\else\textpm\fi{}1.3\ifmmode\pm\else\textpm\fi{}1.4)%$, ${P}_{y}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}(\ensuremath{-}43.1\ifmmode\pm\else\textpm\fi{}1.3\ifmmode\pm\else\textpm\fi{}2.2)%$, and ${P}_{z}/{P}_{e}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}(56.2\ifmmode\pm\else\textpm\fi{}1.5\ifmmode\pm\else\textpm\fi{}2.6)%$, could be measured simultaneously. The Coulomb quadrupole to magnetic dipole ratio, $\mathrm{CMR}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}(\ensuremath{-}6.4\ifmmode\pm\else\textpm\fi{}{0.7}_{\mathrm{stat}}\ifmmode\pm\else\textpm\fi{}{0.8}_{\mathrm{syst}})%$, was determined from ${P}_{x}$ in the framework of the Mainz Unitary Isobar Model. The consistency among the reduced polarizations and the extraction of the ratio of longitudinal-to-transverse response is discussed.
year | journal | country | edition | language |
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2001-04-02 | Physical Review Letters |