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Improved measurement of Born cross sections for χbJωχ_{bJ}\,ω and χbJ(π+ππ0)nonωχ_{bJ}\,(π^+π^-π^0)_{\rm non-ω} (JJ = 0, 1, 2) at Belle and Belle II

Published 29 Oct 2025 in hep-ex | (2510.25461v1)

Abstract: We study the processes χbJω\chi_{bJ}\,\omega and χbJ(π<sup>+π<sup>π<sup>0)</sup></sup></sup>nonω\chi_{bJ}\,(\pi<sup>+\pi<sup>-\pi<sup>0)_{\rm</sup></sup></sup> non-\omega} (JJ = 0, 1, 2) at center-of-mass energies s\sqrt{s} from 10.73--11.02 GeV using a 142.5fb<sup>1142.5\,\mathrm{fb}<sup>{-1} data sample collected with the Belle detector at the KEKB asymmetric-energy e<sup>+</sup>e<sup>e<sup>+</sup> e<sup>- collider; and at s10.75\sqrt{s}\sim10.75 GeV using a 19.8fb<sup>119.8\,\mathrm{fb}<sup>{-1} sample collected with Belle II at SuperKEKB. We find that the Υ(10753)\Upsilon(10753) state decays into χbJω\chi_{bJ}\,\omega but not into χbJ(π<sup>+π<sup>π<sup>0)</sup></sup></sup>nonω\chi_{bJ}\,(\pi<sup>+\pi<sup>-\pi<sup>0)_{\rm</sup></sup></sup> non-\omega}, while the Υ(10860)\Upsilon(10860) state, in contrast, decays into χbJ(π<sup>+π<sup>π<sup>0)</sup></sup></sup>nonω\chi_{bJ}\,(\pi<sup>+\pi<sup>-\pi<sup>0)_{\rm</sup></sup></sup> non-\omega} but not into χbJω\chi_{bJ}\,\omega. The mass and width of the Υ(10753)\Upsilon(10753) state are measured to be (10756.1±3.4(stat.)±2.7(syst.))(10756.1\pm3.4({\rm stat.})\pm2.7({\rm syst.})) MeV/c<sup>2c<sup>2 and (32.2±11.3(stat.)±14.9(syst.))(32.2\pm11.3({\rm stat.})\pm14.9({\rm syst.})) MeV. The products of the partial width to e<sup>+e<sup>e<sup>+e<sup>- and branching fractions for Υ(10753)χb1ω\Upsilon(10753)\to\chi_{b1}\,\omega and Υ(10753)χb2ω\Upsilon(10753)\to\chi_{b2}\,\omega are (1.46±0.25(stat.)±0.20(syst.)1.46\pm0.25({\rm stat.})\pm 0.20({\rm syst.})) eV and (1.29±0.38(stat.)±0.31(syst.)1.29\pm0.38({\rm stat.})\pm 0.31({\rm syst.})) eV.

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