Technical supplement to “Polarization transfer observables in elastic electron-proton scattering at Q2=2.5,5.2,6.8 and 8.5GeV2”

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creativework.keywordsElectromagnetic calorimeter, Magnetic spectrometer, Polarization transfer method, Proton form factors, Proton polarimeter, Spin transport
creativework.publisherElsevier B.V.en
dc.contributor.authorPuckett A.J.R.
dc.contributor.authorBrash E.J.
dc.contributor.authorJones M.K.
dc.contributor.authorLuo W.
dc.contributor.authorMeziane M.
dc.contributor.authorPentchev L.
dc.contributor.authorPerdrisat C.F.
dc.contributor.authorPunjabi V.
dc.contributor.authorWesselmann F.R.
dc.contributor.authorAfanasev A.
dc.contributor.authorAhmidouch A.
dc.contributor.authorAlbayrak I.
dc.contributor.authorAniol K.A.
dc.contributor.authorArrington J.
dc.contributor.authorAsaturyan A.
dc.contributor.authorBaghdasaryan H.
dc.contributor.authorBenmokhtar F.
dc.contributor.authorBertozzi W.
dc.contributor.authorBimbot L.
dc.contributor.authorBosted P.
dc.contributor.authorBoeglin W.
dc.contributor.authorButuceanu C.
dc.contributor.authorCarter P.
dc.contributor.authorChernenko S.
dc.contributor.authorChristy M.E.
dc.contributor.authorCornejo J.C.
dc.contributor.authorCovrig S.
dc.contributor.authorDanagoulian S.
dc.contributor.authorDaniel A.
dc.contributor.authorDavidenko A.
dc.contributor.authorDay D.
dc.contributor.authorDhamija S.
dc.contributor.authorDutta D.
dc.contributor.authorEnt R.
dc.contributor.authorFrullani S.
dc.contributor.authorFenker H.
dc.contributor.authorFrlez E.
dc.contributor.authorGaribaldi F.
dc.contributor.authorGaskell D.
dc.contributor.authorGilad S.
dc.contributor.authorGilman R.
dc.contributor.authorGoncharenko Y.
dc.contributor.authorHafidi K.
dc.contributor.authorHamilton D.
dc.contributor.authorHiginbotham D.W.
dc.contributor.authorHinton W.
dc.contributor.authorHorn T.
dc.contributor.authorHu B.
dc.contributor.authorHuang J.
dc.contributor.authorHuber G.M.
dc.contributor.authorJensen E.
dc.contributor.authorKeppel C.
dc.contributor.authorKhandaker M.
dc.contributor.authorKing P.
dc.contributor.authorKirillov D.
dc.contributor.authorKohl M.
dc.contributor.authorKravtsov V.
dc.contributor.authorKumbartzki G.
dc.contributor.authorLi Y.
dc.contributor.authorMamyan V.
dc.contributor.authorMargaziotis D.J.
dc.contributor.authorMarsh A.
dc.contributor.authorMatulenko Y.
dc.contributor.authorMaxwell J.
dc.contributor.authorMbianda G.
dc.contributor.authorMeekins D.
dc.contributor.authorMelnik Y.
dc.contributor.authorMiller J.
dc.contributor.authorMkrtchyan A.
dc.contributor.authorMkrtchyan H.
dc.contributor.authorMoffit B.
dc.contributor.authorMoreno O.
dc.contributor.authorMulholland J.
dc.contributor.authorNarayan A.
dc.contributor.authorNedev S.
dc.contributor.authorNuruzzaman
dc.contributor.authorPiasetzky E.
dc.contributor.authorPierce W.
dc.contributor.authorPiskunov N.M.
dc.contributor.authorProk Y.
dc.contributor.authorRansome R.D.
dc.contributor.authorRazin D.S.
dc.contributor.authorReimer P.
dc.contributor.authorReinhold J.
dc.contributor.authorRondon O.
dc.contributor.authorShabestari M.
dc.contributor.authorShahinyan A.
dc.contributor.authorShestermanov K.
dc.contributor.authorŠirca S.
dc.contributor.authorSitnik I.
dc.contributor.authorSmykov L.
dc.contributor.authorSmith G.
dc.contributor.authorSolovyev L.
dc.contributor.authorSolvignon P.
dc.contributor.authorSubedi R.
dc.contributor.authorTomasi-Gustafsson E.
dc.contributor.authorVasiliev A.
dc.contributor.authorVeilleux M.
dc.contributor.authorWojtsekhowski B.B.
dc.contributor.authorWood S.
dc.contributor.authorYe Z.
dc.contributor.authorZanevsky Y.
dc.contributor.authorZhang X.
dc.contributor.authorZhang Y.
dc.contributor.authorZheng X.
dc.contributor.authorZhu L.
dc.date.accessioned2024-07-10T14:27:04Z
dc.date.accessioned2024-07-10T14:49:00Z
dc.date.available2024-07-10T14:27:04Z
dc.date.available2024-07-10T14:49:00Z
dc.date.issued2018-12-01
dc.description.abstractThe GEp-III and GEp-2γ experiments, carried out in Jefferson Lab's Hall C from 2007–2008, consisted of measurements of polarization transfer in elastic electron–proton scattering at momentum transfers of Q2=2.5,5.2,6.8, and 8.54 GeV 2. These measurements were carried out to improve knowledge of the proton electromagnetic form factor ratio R=μpGE p∕GM p at large values of Q2 and to search for effects beyond the Born approximation in polarization transfer observables at Q2=2.5GeV2. The final results of both experiments were reported in a recent archival publication. A full reanalysis of the data from both experiments was carried out in order to reduce the systematic and, for the GEp-2γ experiment, statistical uncertainties. This technical note provides additional details of the final analysis omitted from the main publication, including the final evaluation of the systematic uncertainties.
dc.identifier.doi10.1016/j.nima.2018.09.022
dc.identifier.issn0168-9002
dc.identifier.scopusSCOPUS_ID:85053438223en
dc.identifier.urihttps://rlib.uctm.edu/handle/123456789/490
dc.language.isoen
dc.source.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=85053438223&origin=inward
dc.titleTechnical supplement to “Polarization transfer observables in elastic electron-proton scattering at Q2=2.5,5.2,6.8 and 8.5GeV2”
dc.typeArticle
oaire.citation.volume910
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