By analyzing ð448.1 ` 2.9Þ × 106 ψ ð3686Þ events collected with the BESIII detector operating at the BEPCII collider, the decays of χcJ → 4K0S (J 1⁄4 0, 1, 2) are observed for the first time with statistical significances of 26.5σ, 5.9σ and 11.4σ, respectively. The product branching fractions of ψð3686Þ → γχcJ, χcJ → 4K0S are presented, and the branching fractions of χcJ → 4K0S decays are determined to be Bχc0→4K0S 1⁄4 ð5.76 ` 0.34 ` 0.38Þ × 10−4, Bχc1→4K0S 1⁄4 ð0.35 ` 0.09 ` 0.03Þ × 10−4 and Bχc2→4K0S 1⁄4 ð1.14 ` 0.15 ` 0.08Þ × 10−4, where the first uncertainties are statistical and the second are systematic, respectively.
Observation of χcJ→4KS0
Cibinetto, G.;Farinelli, R.;Garzia, I.;Mezzadri, G.;Savrié, M.;
2019
Abstract
By analyzing ð448.1 ` 2.9Þ × 106 ψ ð3686Þ events collected with the BESIII detector operating at the BEPCII collider, the decays of χcJ → 4K0S (J 1⁄4 0, 1, 2) are observed for the first time with statistical significances of 26.5σ, 5.9σ and 11.4σ, respectively. The product branching fractions of ψð3686Þ → γχcJ, χcJ → 4K0S are presented, and the branching fractions of χcJ → 4K0S decays are determined to be Bχc0→4K0S 1⁄4 ð5.76 ` 0.34 ` 0.38Þ × 10−4, Bχc1→4K0S 1⁄4 ð0.35 ` 0.09 ` 0.03Þ × 10−4 and Bχc2→4K0S 1⁄4 ð1.14 ` 0.15 ` 0.08Þ × 10−4, where the first uncertainties are statistical and the second are systematic, respectively.File | Dimensione | Formato | |
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PhysRevD.99.052008.pdf
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