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000220578 0247_ $$2doi$$a10.1103/PhysRevD.91.112007
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000220578 0247_ $$2ISSN$$a1089-4918
000220578 0247_ $$2ISSN$$a1550-2368
000220578 0247_ $$2ISSN$$a1550-7998
000220578 0247_ $$2arXiv$$aarXiv:1410.7641
000220578 0247_ $$2WOS$$aWOS:000356135800001
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000220578 0881_ $$aBelle preprint 2014-17; arXiv:1410.7641
000220578 088__ $$2Belle$$aBelle preprint 2014-17
000220578 088__ $$2arXiv$$aarXiv:1410.7641
000220578 1001_ $$0P:(DE-HGF)0$$aWang, X. L.$$b0
000220578 245__ $$aMeasurement of $e^{+}  e^{-} \to π^{+}  π^{-}  ψ ( 2 S )$ via initial state radiation at Belle
000220578 260__ $$a[S.l.]$$bAmerican Physical Society$$c2015
000220578 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2015-06-12
000220578 264_1 $$2Crossref$$3print$$bAmerican Physical Society (APS)$$c2015-06-01
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000220578 500__ $$aOA
000220578 520__ $$aWe report measurement of the cross section of e+e-→π+π-ψ(2S) between 4.0 and 5.5 GeV, based on an analysis of initial state radiation events in a 980 fb−1 data sample recorded with the Belle detector. The properties of the Y(4360) and Y(4660) states are determined. Fitting the mass spectrum of π+π-ψ(2S) with two coherent Breit-Wigner functions, we find two solutions with identical mass and width but different couplings to electron-positron pairs: MY(4360)=(4347±6±3) MeV/c2, ΓY(4360)=(103±9±5) MeV, MY(4660)=(4652±10±8) MeV/c2, ΓY(4660)=(68±11±1) MeV; and B[Y(4360)→π+π-ψ(2S)]·ΓY(4360)e+e-=(10.9±0.6±0.7) eV and B[Y(4660)→π+π-ψ(2S)]·ΓY(4660)e+e-=(8.1±1.1±0.5) eV for one solution; or B[Y(4360)→π+π-ψ(2S)]·ΓY(4360)e+e-=(9.2±0.6±0.6) eV and B[Y(4660)→π+π-ψ(2S)]·ΓY(4660)e+e-=(2.0±0.3±0.2) eV for the other. Here, the first errors are statistical and the second systematic. Evidence for a charged charmoniumlike structure at 4.05 GeV/c2 is observed in the π±ψ(2S) intermediate state in the Y(4360) decays.
000220578 536__ $$0G:(DE-H253)POF2-BELLE-I-II-Exp.-20130405$$aExperiments at KEK (BELLE I/II) (POF2-515)$$cPOF2-515$$fPOF II$$x0
000220578 542__ $$2Crossref$$i2015-06-12$$uhttp://link.aps.org/licenses/aps-default-license
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000220578 650_7 $$2INSPIRE$$aelectron positron: annihilation
000220578 650_7 $$2INSPIRE$$aelectron positron: colliding beams
000220578 650_7 $$2INSPIRE$$aradiation: initial-state interaction
000220578 650_7 $$2INSPIRE$$apsi(3685): electroproduction
000220578 650_7 $$2INSPIRE$$apsi(3685): hadronic decay
000220578 650_7 $$2INSPIRE$$api: pair production
000220578 650_7 $$2INSPIRE$$across section: energy dependence
000220578 650_7 $$2INSPIRE$$amass spectrum: (psi(3685) pi+ pi-)
000220578 650_7 $$2INSPIRE$$amass enhancement: (4360)
000220578 650_7 $$2INSPIRE$$amass enhancement: (4660)
000220578 650_7 $$2INSPIRE$$amodel: Breit-Wigner
000220578 650_7 $$2INSPIRE$$aresonance: mass
000220578 650_7 $$2INSPIRE$$aresonance: width
000220578 650_7 $$2INSPIRE$$aexperimental results
000220578 650_7 $$2INSPIRE$$aBELLE
000220578 650_7 $$2INSPIRE$$aKEK TRISTAN Stor
000220578 650_7 $$2INSPIRE$$aelectron positron --> psi(3685) pi+ pi-
000220578 650_7 $$2INSPIRE$$apsi(3685) --> J/psi(3100) pi+ pi-
000220578 650_7 $$2INSPIRE$$a10.6 GeV-cms
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000220578 7001_ $$0P:(DE-HGF)0$$aYuan, C. Z.$$b1
000220578 7001_ $$0P:(DE-HGF)0$$aShen, C. P.$$b2
000220578 7001_ $$0P:(DE-HGF)0$$aWang, P.$$b3
000220578 7001_ $$0P:(DE-HGF)0$$aAbdesselam, A.$$b4
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000220578 7001_ $$0P:(DE-HGF)0$$aWatanabe, Y.$$b147
000220578 7001_ $$0P:(DE-HGF)0$$aWon, E.$$b148
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000220578 7001_ $$0P:(DE-HGF)0$$aZhang, Z. P.$$b151
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000220578 7001_ $$0P:(DE-HGF)0$$aBelle Collaboration$$b154$$eCollaboration author
000220578 77318 $$2Crossref$$3journal-article$$a10.1103/physrevd.91.112007$$b : American Physical Society (APS), 2015-06-12$$n11$$p112007$$tPhysical Review D$$v91$$x1550-7998$$y2015
000220578 773__ $$0PERI:(DE-600)2844732-3$$a10.1103/PhysRevD.91.112007$$gVol. 91, no. 11, p. 112007$$n11$$p112007$$tPhysical review / D$$v91$$x1550-7998$$y2015
000220578 7870_ $$0PUBDB-2014-03907$$aWang, X. L. et.al.$$d2014$$iIsParent$$rBelle preprint 2014-17; arXiv:1410.7641$$tMeasurement of $e^+e^- \to \pi^+\pi^-\psi(2S)$ via Initial State Radiation at Belle
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