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Study of B ± K ± ( K S K π ) 0 decay and determination of η c and η c ( 2 S ) parameters

机译: B ± K ± K S K π 0 衰减和 η c 和< mml:math xmlns:mml =“ http://www.w3.org/1998/Math/MathML” altimg =“ si3.gif” display =“ inline” overflow =“ scroll”> η c 2 S 参数

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We report the results of a study of B ± → K ± η c and B ± → K ± η c ( 2 S ) decays followed by η c and η c ( 2 S ) decays to ( K S K π ) 0 . The results are obtained from a data sample containing 535 million B B ˉ -meson pairs collected by the Belle experiment at the KEKB e + e ? collider. We measure the products of the branching fractions B ( B ± → K ± η c ) B ( η c → K S K ± π ? ) = ( 26.7 ± 1.4 ( stat ) ? 2.6 + 2.9 ( syst ) ± 4.9 ( model ) ) × 10 ? 6 and B ( B ± → K ± η c ( 2 S ) ) B ( η c ( 2 S ) → K S K ± π ? ) = ( 3.4 ? 1.5 + 2.2 ( stat + model ) ? 0.4 + 0.5 ( syst ) ) × 10 ? 6 . Interference with the non-resonant component leads to significant model uncertainty in the measurement of these product branching fractions. Our analysis accounts for this interference and allows the model uncertainty to be reduced. We also obtain the following charmonia masses and widths: M ( η c ) = ( 2985.4 ± 1.5 ( stat ) ? 2.0 + 0.5 ( syst ) ) MeV / c 2 , Γ ( η c ) = ( 35.1 ± 3.1 ( stat ) ? 1.6 + 1.0 ( syst ) ) MeV / c 2 , M ( η c ( 2 S ) ) = ( 3636.1 ? 4.2 + 3.9 ( stat + model ) ? 2.0 + 0.7 ( syst ) ) MeV / c 2 , Γ ( η c ( 2 S ) ) = ( 6.6 ? 5.1 + 8.4 ( stat + model ) ? 0.9 + 2.6 ( syst ) ) MeV / c 2 .
机译:我们报告了B±→K±ηc和B±→K±ηc(2 S)衰减,接着是ηc和ηc(2 S)衰减至(K S Kπ)0的研究结果。结果是从一个包含5.35亿个B B me-介子对的数据样本获得的,该对样本是通过Belle实验在KEKB e + e处收集的。对撞机。我们测量分支分数B(B±→K±ηc)B(ηc→KSK±π?)=(26.7±1.4(stat)?2.6 + 2.9(syst)±4.9(模型))×的乘积10? 6和B(B±→K±ηc(2 S))B(ηc(2 S)→KSK±π?)=(3.4?1.5 + 2.2(stat +模型)?0.4 + 0.5(syst)) ×10 6。干扰非谐振成分会导致这些产品分支分数的测量中出现明显的模型不确定性。我们的分析解决了这种干扰,并减少了模型的不确定性。我们还获得了以下吸附剂的质量和宽度:M(ηc)=(2985.4±1.5(stat)≤2.0 + 0.5(syst))MeV / c 2,Γ(ηc)=(35.1±3.1(stat)? 1.6 + 1.0(syst))MeV / c 2,M(ηc(2 S))=(3636.1?4.2 + 3.9(stat +模型)?2.0 + 0.7(syst))MeV / c 2,Γ(ηc (2 S))=(6.6?5.1 + 8.4(统计+模型)?0.9 + 2.6(系统))MeV / c 2。

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