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Observation of h1 (1380) in the J/ψ →η′K K ̄ π decay Observation of h1 (1380) in Jψ

dc.contributor.authorAblikim M.
dc.contributor.authorAchasov M.N.
dc.contributor.authorAhmed S.
dc.contributor.authorAlbrecht M.
dc.contributor.authorAmoroso A.
dc.contributor.authorAn F.F.
dc.contributor.authorAn Q.
dc.contributor.authorBai J.Z.
dc.contributor.authorBai Y.
dc.contributor.authorBakina O.
dc.contributor.authorBaldini Ferroli R.
dc.contributor.authorBan Y.
dc.contributor.authorBennett D.W.
dc.contributor.authorBennett J.V.
dc.contributor.authorBerger N.
dc.contributor.authorBertani M.
dc.contributor.authorBettoni D.
dc.contributor.authorBian J.M.
dc.contributor.authorBianchi F.
dc.contributor.authorBoger E.
dc.contributor.authorBoyko I.
dc.contributor.authorBriere R.A.
dc.contributor.authorCai H.
dc.contributor.authorCai X.
dc.contributor.authorCakir O.
dc.contributor.authorCalcaterra A.
dc.contributor.authorCao G.F.
dc.contributor.authorCetin S.A.
dc.contributor.authorChai J.
dc.contributor.authorChang J.F.
dc.contributor.authorChelkov G.
dc.contributor.authorChen G.
dc.contributor.authorChen H.S.
dc.contributor.authorChen J.C.
dc.contributor.authorChen M.L.
dc.contributor.authorChen P.L.
dc.contributor.authorChen S.J.
dc.contributor.authorChen X.R.
dc.contributor.authorChen Y.B.
dc.contributor.authorChu X.K.
dc.contributor.authorCibinetto G.
dc.contributor.authorDai H.L.
dc.contributor.authorDai J.P.
dc.contributor.authorDbeyssi A.
dc.contributor.authorDedovich D.
dc.contributor.authorDeng Z.Y.
dc.contributor.authorDenig A.
dc.contributor.authorDenysenko I.
dc.contributor.authorDestefanis M.
dc.contributor.authorDe Mori F.
dc.contributor.authorDing Y.
dc.contributor.authorDong C.
dc.contributor.authorDong J.
dc.contributor.authorDong L.Y.
dc.contributor.authorDong M.Y.
dc.contributor.authorDou Z.L.
dc.contributor.authorDu S.X.
dc.contributor.authorDuan P.F.
dc.contributor.authorFang J.
dc.contributor.authorFang S.S.
dc.contributor.authorFang Y.
dc.contributor.authorFarinelli R.
dc.contributor.authorFava L.
dc.contributor.authorFegan S.
dc.contributor.authorFeldbauer F.
dc.contributor.authorFelici G.
dc.contributor.authorFeng C.Q.
dc.contributor.authorFioravanti E.
dc.contributor.authorFritsch M.
dc.contributor.authorFu C.D.
dc.contributor.authorGao Q.
dc.contributor.authorGao X.L.
dc.contributor.authorGao Y.
dc.contributor.authorGao Y.G.
dc.contributor.authorGao Z.
dc.contributor.authorGarzia I.
dc.contributor.authorGoetzen K.
dc.contributor.authorGong L.
dc.contributor.authorGong W.X.
dc.contributor.authorGradl W.
dc.contributor.authorGreco M.
dc.contributor.authorGu M.H.
dc.contributor.authorGu Y.T.
dc.contributor.authorGuo A.Q.
dc.contributor.authorGuo R.P.
dc.contributor.authorGuo Y.P.
dc.contributor.authorHaddadi Z.
dc.contributor.authorHan S.
dc.contributor.authorHao X.Q.
dc.contributor.authorHarris F.A.
dc.contributor.authorHe K.L.
dc.contributor.authorHe X.Q.
dc.contributor.authorHeinsius F.H.
dc.contributor.authorHeld T.
dc.contributor.authorHeng Y.K.
dc.contributor.authorHoltmann T.
dc.contributor.authorHou Z.L.
dc.contributor.authorHu H.M.
dc.contributor.authorHu T.
dc.contributor.authorHu Y.
dc.contributor.buuauthorTAPAN, İLHAN
dc.contributor.departmentFizik Bölümü
dc.contributor.orcid0009-0002-8119-1445
dc.contributor.scopusid 8905787000
dc.date.accessioned2025-05-13T09:42:47Z
dc.date.issued2018-10-01
dc.description.abstractUsing 1.31×109 J/ψ events collected by the BESIII detector at the BEPCII e+e- collider, we report the first observation of the h1(1380) in J/ψ→η′h1(1380) with a significance of more than ten standard deviations. The mass and width of the possible axial-vector strangeonium candidate h1(1380) are measured to be M=(1423.2±2.1±7.3) MeV/c2 and Γ=(90.3±9.8±17.5) MeV. The product branching fractions, assuming no interference, are determined to be B(J/ψ→η′h1(1380))×B(h1(1380)→K∗(892)+K-+c.c.)=(1.51±0.09±0.21)×10-4 in η′K+K-π0 mode and B(J/ψ→η′h1(1380))×B(h1(1380)→K∗(892)K̄+c.c.)=(2.16±0.12±0.29)×10-4 in η′KS0K±π mode. The first uncertainties are statistical and the second are systematic. Isospin symmetry violation is observed in the decays h1(1380)→K∗(892)+K-+c.c. and h1(1380)→K∗(892)0K̄0+c.c.. Based on the measured h1(1380) mass, the mixing angle between the states h1(1170) and h1(1380) is determined to be (35.9±2.6)°, consistent with theoretical expectations.
dc.identifier.doi10.1103/PhysRevD.98.072005
dc.identifier.issn2470-0010
dc.identifier.issue7
dc.identifier.scopus2-s2.0-85056173867
dc.identifier.urihttps://hdl.handle.net/11452/52215
dc.identifier.volume98
dc.indexed.scopusScopus
dc.language.isoen
dc.publisherAmerican Physical Society
dc.relation.journalPhysical Review D
dc.rightsinfo:eu-repo/semantics/openAccess
dc.subjectHadronic decays
dc.subjectParticle decays
dc.subjectParticle phenomena
dc.titleObservation of h1 (1380) in the J/ψ →η′K K ̄ π decay Observation of h1 (1380) in Jψ
dc.typeArticle
dspace.entity.typePublication
local.contributor.departmentFizik Bölümü
local.indexed.atScopus
relation.isAuthorOfPublication197aec07-a4ed-42b7-a3d3-d7476357d6ef
relation.isAuthorOfPublication.latestForDiscovery197aec07-a4ed-42b7-a3d3-d7476357d6ef

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