Observation of \(e^+e^-\to\omega\chi_{bJ}(1P)\) and search for \(X_b \to \omega\Upsilon(1S)\) at \(\sqrt{s}\) near 10.75 GeV
We study the processes \(e^+e^-\to\omega\chi_{bJ}(1P)\) (\(J\) = 0, 1, or 2) using samples at center-of-mass energies \(\sqrt{s}\) = 10.701, 10.745, and 10.805 GeV, corresponding to 1.6, 9.8, and 4.7 fb\(^{-1}\) of integrated luminosity, respectively. These data were collected with the Belle II dete...
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Veröffentlicht in: | arXiv.org 2023-01 |
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Sprache: | eng |
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Zusammenfassung: | We study the processes \(e^+e^-\to\omega\chi_{bJ}(1P)\) (\(J\) = 0, 1, or 2) using samples at center-of-mass energies \(\sqrt{s}\) = 10.701, 10.745, and 10.805 GeV, corresponding to 1.6, 9.8, and 4.7 fb\(^{-1}\) of integrated luminosity, respectively. These data were collected with the Belle II detector during special operations of the SuperKEKB collider above the \(\Upsilon(4S)\) resonance. We report the first observation of \(\omega\chi_{bJ}(1P)\) signals at \(\sqrt{s}\) = 10.745 GeV. By combining Belle II data with Belle results at \(\sqrt{s}\) = 10.867 GeV, we find energy dependencies of the Born cross sections for \(e^+e^-\to \omega\chi_{b1,b2}(1P)\) to be consistent with the shape of the \(\Upsilon(10753)\) state. These data indicate that the internal structures of the \(\Upsilon(10753)\) and \(\Upsilon(10860)\) states may differ. Including data at \(\sqrt{s}\) = 10.653 GeV, we also search for the bottomonium equivalent of the \(X(3872)\) state decaying into \(\omega\Upsilon(1S)\). No significant signal is observed for masses between 10.45 and 10.65 GeV/\(c^2\). |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.2208.13189 |