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Amplitude analysis of the χc1ηπ+πχ_{c1} \to ηπ^+π^- decays

Published 8 Oct 2016 in hep-ex | (1610.02479v3)

Abstract: Using 448.0×10<sup>6448.0 \times 10<sup>6~ψ(3686)\psi(3686) events collected with the BESIII detector, an amplitude analysis is performed for ψ(3686)γχc1\psi(3686)\to\gamma\chi_{c1}, χc1ηπ<sup>+π<sup>\chi_{c1}\to\eta\pi<sup>+\pi<sup>- decays. The most dominant two-body structure observed is a0(980)<sup>±π<sup>a_0(980)<sup>{\pm}\pi<sup>{\mp}; a0(980)<sup>±ηπ<sup>±a_0(980)<sup>{\pm}\to\eta\pi<sup>{\pm}. The a0(980)a_0(980) line shape is modeled using a dispersion relation, and a significant non-zero a0(980)a_0(980) coupling to the η<sup>π\eta<sup>{\prime}\pi channel is measured. We observe χc1a2(1700)π\chi_{c1}\to a_2(1700)\pi production for the first time, with a significance larger than 17σ\sigma. The production of mesons with exotic quantum numbers, J<sup>PC=1<sup>+J<sup>{PC}=1<sup>{-+}, is investigated, and upper limits for the branching fractions χc1π1(1400)<sup>±π<sup>\chi_{c1}\to \pi_1(1400)<sup>{\pm}\pi<sup>{\mp}, χc1π1(1600)<sup>±π<sup>\chi_{c1}\to \pi_1(1600)<sup>{\pm}\pi<sup>{\mp}, and χc1π1(2015)<sup>±π<sup>\chi_{c1}\to\pi_1(2015)<sup>{\pm}\pi<sup>{\mp}, with subsequent π1(X)<sup>±</sup>ηπ<sup>±\pi_1(X)<sup>{\pm}</sup> \to \eta\pi<sup>{\pm} decay, are determined.

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