Gutz, E.E.GutzSokhoyan, V.V.SokhoyanPee, H. vanH. vanPeeAnisovich, A.V.A.V.AnisovichBacelar, J.C.S.J.C.S.BacelarBantes, B.B.BantesBartholomy, O.O.BartholomyBayadilov, D.D.BayadilovBeck, R.R.BeckBeloglazov, Y.A.Y.A.BeloglazovCastelijns, R.R.CastelijnsCrede, V.V.CredeDutz, H.H.DutzEhmanns, A.A.EhmannsElsner, D.D.ElsnerEssig, K.K.EssigEwald, R.R.EwaldFabry, I.I.FabryFornet-Ponse, K.K.Fornet-PonseFuchs, M.M.FuchsFunke, C.C.FunkeGothe, R.R.GotheGregor, R.R.GregorGridnev, A.B.A.B.GridnevHöffgen, StefanStefanHöffgenHoffmeister, P.P.HoffmeisterHorn, I.I.HornJaegle, I.I.JaegleJunkersfeld, J.J.JunkersfeldKalinowsky, H.H.KalinowskyKammer, S.S.KammerKleber, V.V.KleberKlein, FriedrichFriedrichKleinKlein, FrankFrankKleinKlempt, E.E.KlemptKonrad, M.M.KonradKotulla, M.M.KotullaKrusche, B.B.KruscheLang, M.M.LangLangheinrich, J.J.LangheinrichLöhner, H.H.LöhnerLopatin, I.V.I.V.LopatinLotz, J.J.LotzLugert, S.S.LugertMenze, D.D.MenzeMertens, T.T.MertensMesschendorp, J.G.J.G.MesschendorpMetag, V.V.MetagMorales, C.C.MoralesNanova, M.M.NanovaNikonov, V.A.V.A.NikonovNovinski, D.V.D.V.NovinskiNovotny, R.R.NovotnyOstrick, M.M.OstrickPant, L.M.L.M.PantPfeiffer, M.M.PfeifferRadkov, A.A.RadkovSarantsev, A.V.A.V.SarantsevSchadmand, S.S.SchadmandSchmidt, C.C.SchmidtSchmieden, H.H.SchmiedenSchoch, B.B.SchochShende, S.S.ShendeSüle, A.A.SüleSumachev, V.V.SumachevSzczepanek, T.T.SzczepanekThoma, U.U.ThomaTrnka, D.D.TrnkaWalther, D.D.WaltherWeinheimer, C.C.WeinheimerWendel, C.C.Wendel2022-03-042022-03-042008https://publica.fraunhofer.de/handle/publica/21790610.1140/epja/i2008-10566-9In photoproduction experiments, a large number of final states yielding various resonance contributions are accessible. To extract resonance parameters via partial-wave analysis not only the measurement of differential cross-sections is necessary, but also the determination of polarization observables. At the electron accelerator ELSA (Bonn) the coherent bremsstrahlung method was used to generate a linearly polarized photon beam. Using the CBELSA/TAPS detector setup, the beam asymmetry Sigma in the reaction gammaroh -> rohpi0eta was determined as a funkction of various masses and angles for photon energies between 970 MeV and 1650 MeV.en620539Measurement of the beam asymmetry Sigma in pi eta, production off the proton with the CBELSA/TAPS experimentjournal article