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000890808 0247_ $$2doi$$a10.1103/PhysRevD.103.034016
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000890808 0247_ $$2ISSN$$a1538-4500
000890808 0247_ $$2ISSN$$a1550-2368
000890808 0247_ $$2ISSN$$a1550-7998
000890808 0247_ $$2ISSN$$a2470-0010
000890808 0247_ $$2ISSN$$a2470-0029
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000890808 1001_ $$0P:(DE-HGF)0$$aBaru, V.$$b0$$eCorresponding author
000890808 245__ $$aInsights into Z b ( 10610 ) and Z b ( 10650 ) from dipion transitions from ϒ ( 10860 )
000890808 260__ $$aMelville, NY$$bInst.812068$$c2021
000890808 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2021-02-22
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000890808 520__ $$aThe dipion transitions Υ(10860)→π+π−Υ(nS) (n=1, 2, 3) are studied in the framework of a unitary and analytic coupled-channel formalism previously developed for analyzing experimental data on the bottomoniumlike states Zb(10610) and Zb(10650) [Phys. Rev. D 98, 074023 (2018)] and predicting the properties of their spin partners [Phys. Rev. D 99, 094013 (2019)]. In this work we use a relatively simple but realistic version of this approach, where the scattering and production amplitudes are constructed employing only short-ranged interactions between the open- and hidden-flavor channels consistent with the constraints from heavy quark spin symmetry, for an extended analysis of the experimental line shapes. In particular, the transitions from the Υ(10860) to the final states ππhb(mP) (m=1, 2) and πB(*)¯B∗ already studied before, are now augmented by the Υ(10860)→π+π−Υ(nS) final states (n=1, 2, 3). This is achieved by employing dispersion theory to account for the final state interaction of the ππ subsystem including its coupling to the K¯K channel. Fits to the two-dimensional Dalitz plots for the π+π−Υ final states were performed. Two real subtraction constants are adjusted to achieve the best description of the Dalitz plot for each Υ(nS) (n=1, 2, 3) while all the parameters related to the properties of the Zbs are kept fixed from the previous study. A good overall description of the data for all Υ(10860)→π+π−Υ(nS) channels achieved in this work provides additional strong support for the molecular interpretation of the Zb states.
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000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.108.122001
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.110.252001
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.110.252002
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.111.019901
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.111.242001
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.100.142001
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.80.031104
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.88.074026
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.112.222002
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.ppnp.2016.11.003
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.physrep.2016.11.002
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.ppnp.2017.08.003
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/RevModPhys.90.015004
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/RevModPhys.90.015003
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.ppnp.2019.04.003
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.physrep.2020.05.001
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.116.212001
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.85.054011
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1142/S0217751X15300021
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.physletb.2018.01.039
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.84.054010
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1140/epja/i2011-11120-6
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.84.056015
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.physletb.2011.09.039
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1088/0954-3899/39/10/105001
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.84.054002
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.86.014004
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000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1088/1361-6471/ab2678
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000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.99.094013
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevLett.115.202001
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.93.074031
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.92.036002
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1007/JHEP02(2016)009
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1140/epjc/s10052-018-6416-6
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000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1016/j.physletb.2019.134851
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.89.053015
000890808 999C5 $$2Crossref$$9-- missing cx lookup --$$a10.1103/PhysRevD.83.074004
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