Study of the Hadronic Transitions ΥΥ(2S)→(η,π0)Υ\rightarrow (η,π^0)Υ(1S) at Belle

preprint2012arXivOpen access

Abstract

We study the rare hadronic transitions Υ(2S)→Υ(1S)ηΥ(2S)\rightarrow Υ(1S)η and Υ(2S)→Υ(1S)π0Υ(2S)\rightarrow Υ(1S)π^0 using a sample of 158 ×106\times 10^6 Υ(2S)Υ(2S) decays collected with the Belle detector at the KEKB asymmetric-energy e+e−e^+ e^- collider. We observe the ηη meson decay to γγγγ and π+π−π0π^+π^-π^0 final states; the Υ(1S)Υ(1S) is reconstructed in the μ+μ−μ^+μ^- and e+e−e^+e^- decay modes. We measure the ratios of branching fractions (B{\mathcal B}) B(Υ(2S)→Υ(1S)η)B(Υ(2S)→Υ(1S)π+π−)\frac{{\mathcal B}(Υ(2S)\rightarrowΥ(1S)η)}{{\mathcal B}(Υ(2S)\rightarrowΥ(1S)π^+π^-)} = (1.99±\pm0.14 (stat) ±\pm0.11 (syst)) ×10−3\times 10^{-3} and B(Υ(2S)→Υ(1S)π0)B(Υ(2S)→Υ(1S)π+π−)<2.3×10−4\frac{{\mathcal B}(Υ(2S)\rightarrowΥ(1S)π^0)}{{\mathcal B}(Υ(2S)\rightarrowΥ(1S)π^+π^-)} < 2.3 \times 10^{-4} at the 90% confidence level (CL). Assuming the value B(Υ(2S)→Υ(1S)π−π+){\mathcal B}(Υ(2S) \rightarrow Υ(1S)π^-π^+) = (17.92±\pm0.26)%, we obtain B(Υ(2S)→Υ(1S)η)=(3.57±0.25(stat) ±0.21(syst))×10−4 {\mathcal B}(Υ(2S)\rightarrowΥ(1S)η) = (3.57 \pm 0.25 ({\rm stat})\ \pm 0.21 ({\rm syst}))\times 10^{-4} and $ {\mathcal B}(Υ(2S)\rightarrowΥ(1S)π^0) < 4.1\times 10^{-5}\ ({\rm 90%\ CL}). $

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