Recoil polarization measurements for neutral pion electroproduction at Q2=1(GeV/c)2 near the Δ resonance

dc.contributor.authorKelly, J.J.
dc.contributor.authorGayou, O.
dc.contributor.authorRoche, R.E.
dc.contributor.authorChai, Z.
dc.contributor.authorJones, M.K.
dc.contributor.authorSarty, A.J.
dc.contributor.authorFrullani, S.
dc.contributor.authorAniol, K.
dc.contributor.authorBeise, E.J.
dc.contributor.authorBenmokhtar, F.
dc.contributor.authorBertozzi, W.
dc.contributor.authorBoeglin, W.U.
dc.contributor.authorBotto, T.
dc.contributor.authorBrash, E.J.
dc.contributor.authorBreuer, H.
dc.contributor.authorBrown, E.
dc.contributor.authorBurtin, E.
dc.contributor.authorCalarco, J.R.
dc.contributor.authorCavata, C.
dc.contributor.authorChang, C.C.
dc.contributor.authorChant, N.S.
dc.contributor.authorChen, J.-P.
dc.contributor.authorComan, M.
dc.contributor.authorCrovelli, D.
dc.contributor.authorDe Leo, R.
dc.contributor.authorDieterich, S.
dc.contributor.authorEscoffier, S.
dc.contributor.authorFissum, K.G.
dc.contributor.authorGarde, V.
dc.contributor.authorGaribaldi, F.
dc.contributor.authorGeorgakopoulos, S.
dc.contributor.authorGilad, S.
dc.contributor.authorGilman, R.
dc.contributor.authorGlashausser, C.
dc.contributor.authorHansen, J.-O.
dc.contributor.authorHiginbotham, D.W.
dc.contributor.authorHotta, A.
dc.contributor.authorHuber, G.M.
dc.contributor.authorIbrahim, H.
dc.contributor.authorIodice, M.
dc.contributor.authorde Jager, C.W.
dc.contributor.authorJiang, X.
dc.contributor.authorKimenko, A.
dc.contributor.authorKozlov, A.
dc.contributor.authorKumbartzki, G.
dc.contributor.authorKuss, M.
dc.contributor.authorLagamba, L.
dc.contributor.authorLaveissiere, G.
dc.contributor.authorLeRose, J.J.
dc.contributor.authorLindgren, R.A.
dc.contributor.authorLiyange, N.
dc.contributor.authorLolos, G.J.
dc.contributor.authorLourie, R.W.
dc.contributor.authorMargaziotis, D.J.
dc.contributor.authorMarie, F.
dc.contributor.authorMarkowitz, P.
dc.contributor.authorMcAleer, S.
dc.contributor.authorMeekins, D.
dc.contributor.authorMichaels, R.
dc.contributor.authorMilbrath, B.D.
dc.contributor.authorMitchell, J.
dc.contributor.authorNappa, J.
dc.contributor.authorNeyret, D.
dc.contributor.authorPerdrisat, C.F.
dc.contributor.authorPotokar, M.
dc.contributor.authorPunjabi, V.A.
dc.contributor.authorPussieux, T.
dc.contributor.authorRansome, R.D.
dc.contributor.authorRoos, P.G.
dc.contributor.authorRvachev, M.
dc.contributor.authorSaha, A.
dc.contributor.authorSirca, S.
dc.contributor.authorSuleiman, R.
dc.contributor.authorStrauch, S.
dc.contributor.authorTemplon, J.A.
dc.contributor.authorTodor, L.
dc.contributor.authorUlmer, P.E.
dc.contributor.authorUrciuoli, G.M.
dc.contributor.authorWeinstein, L.B.
dc.contributor.authorWijsooriya, K.
dc.contributor.authorWojtsekhowski, B.
dc.contributor.authorZheng, X.
dc.contributor.authorZhu, L.
dc.contributor.authorJefferson Laboratory E91011 and Hall A Collaborations
dc.description.abstractWe measured angular distributions of differential cross section, beam analyzing power, and recoil polarization for neutral pion electroproduction at Q2=1.0 (GeV/c)2 in 10 bins of 1.17⩽W⩽1.35 GeV across the Δ resonance. A total of 16 independent response functions were extracted, of which 12 were observed for the first time. Comparisons with recent model calculations show that response functions governed by real parts of interference products are determined relatively well near the physical mass, W=MΔ≈1.232 GeV, but the variation among models is large for response functions governed by imaginary parts, and for both types of response functions, the variation increases rapidly with W>MΔ. We performed a multipole analysis that adjusts suitable subsets of ℓπ⩽2 amplitudes with higher partial waves constrained by baseline models. This analysis provides both real and imaginary parts. The fitted multipole amplitudes are nearly model independent—there is very little sensitivity to the choice of baseline model or truncation scheme. By contrast, truncation errors in the traditional Legendre analysis of N→Δ quadrupole ratios are not negligible. Parabolic fits to the W dependence around MΔ for the multiple analysis gives values for Re(S1+/M1+)=(-6.61±0.18)% and Re(E1+/M1+)=(-2.87±0.19)% for the pπ0 channel at W=1.232 GeV and Q2=1.0 (GeV/c)2 that are distinctly larger than those from the Legendre analysis of the same data. Similarly, the multipole analysis gives Re(S0+/M1+)=(+7.1±0.8)% at W=1.232 GeV, consistent with recent models, while the traditional Legendre analysis gives the opposite sign because its truncation errors are quite severe.en_US
dc.identifier.citationKelly, J.J. et al. "Recoil polarization measurements for neutral pion electroproduction at Q2=1(GeV/c)2 near the Δ resonance." Physical Review C 75, no. 2 (2007): 025201.en_US
dc.relation.isAvailableAtCollege of Computer, Mathematical & Physical Sciencesen_us
dc.relation.isAvailableAtDigital Repository at the University of Marylanden_us
dc.relation.isAvailableAtUniversity of Maryland (College Park, MD)en_us
dc.rights.license© 2007 The American Physical Society.
dc.subjectPion electroproductionen_US
dc.titleRecoil polarization measurements for neutral pion electroproduction at Q2=1(GeV/c)2 near the Δ resonanceen_US


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