Study of X(3872) in BB meson decays

preprint2008arXivOpen access

Abstract

We present results on the X(3872), produced in B+→X(3872)K+B^+ \to X(3872) K^+ and B0→X(3872)KS0B^0 \to X(3872) K^0_S decays where X(3872)→J/ψπ+π−X(3872) \to J/ψπ^+ π^-. We report the first statistically significant observation of B0→X(3872)KS0B^0 \to X(3872) K^0_S and measure the ratio of branching fractions to be B(B0→X(3872)K0)B(B+→X(3872)K+)=0.82±0.22±0.05\frac{{\cal B}(B^0 \to X(3872)K^0)} {{\cal B}(B^+ \to X(3872)K^+)} = 0.82 \pm 0.22 \pm 0.05, consistent with unity. The mass difference between the X(3872) states produced in B+B^+ and B0B^0 decay is found to be δM≡MXK+−MXK0=(+0.18±0.89±0.26)δM \equiv M_{XK^+} - M_{XK^0} = (+0.18 \pm 0.89 \pm 0.26) MeV/c2c^2, consistent with zero. In addition, we search for the X(3872) in the decay B0→X(3872)K+π−B^0 \to X(3872)K^+π^-, X(3872)→J/ψπ+π−X(3872) \to J/ψπ^+ π^-. We measure B(B0→X(3872)(K+π−)NR)×B(X(3872)→J/ψπ+π−)=(8.1±2.0−1.4+1.1)×10−6{\cal B}(B^0 \to X(3872) (K^+ π^-)_{NR}) \times {\cal B}(X(3872) \to J/ψπ^+ π^-) = (8.1 \pm 2.0 ^{+1.1}_{-1.4})\times 10^{-6} and we set the 90% C.L. limit, B(B0→X(3872)K∗(892)0)×B(X(3872)→J/ψπ+π−)<3.4×10−6{\cal B}(B^0 \to X(3872)K^{*}(892)^0) \times {\cal B}(X(3872) \to J/ψπ^+ π^-) < 3.4 \times 10^{-6}. The analysis is based on a 605 fb−1^{-1} data sample collected at the Υ(4S)Υ(4S) with the Belle detector at the KEKB collider.

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