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Hidden-bottom hadronic transitions of Υ(10753)Υ(10753)

Published 5 Dec 2023 in hep-ph and hep-ex | (2312.02761v1)

Abstract: Assuming that the Υ(10753)\Upsilon(10753) is a $4S$-$3D$ mixed state, we investigated the hidden-bottom hadronic decays of the Υ(10753)ηb(1S)ω(η<sup>())\Upsilon(10753) \to \eta_b(1S)\omega(\eta<sup>{(\prime)}) via the intermediate meson loops. In a commonly accepted range of the model parameter α\alpha in the form factor, the predicted branching ratios may reach to the order of 10<sup>310<sup>{-3}--10<sup>210<sup>{-2}. The relative ratio of the partial decay widths of the Υ(10753)ηbη<sup>()\Upsilon(10753)\to\eta_b\eta<sup>{(\prime)} to Υ(10753)ηbω\Upsilon(10753)\to \eta_b\omega is found to be dependent on the η\eta-$\eta&#39;$ mixing angle. In addition, we also calculated the ratios of the partial decays widths of the Υ(10753)ηbω\Upsilon(10753) \to \eta_b \omega to Υ(10753)Υ(nS)π<sup>+π<sup>\Upsilon(10753)\to \Upsilon(nS)\pi<sup>+\pi<sup>- (n=1,2n=1\,,2), which are found to be around 0.4 and 0.2 for n=1n=1 and n=2n=2, respectively. These values are in accordance with the preliminary experimental results. The calculations presented here tend to favor the Υ(10753)\Upsilon(10753) as the $4S$-$3D$ mixture. We hope these predictions could be verified by the future BelleII experiments.

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