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Study of the BX(3872)(D0Dˉ0)KB\to X(3872)(\to D^{*0}\bar D^0)K decay

Abstract

We present a study of BX(3872)KB\to X(3872)K with X(3872) decaying to D0Dˉ0D^{*0}\bar D^0 using a sample of 657 million BBˉB\bar B pairs recorded at the Υ(4S)\Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric-energy e+ee^+e^- collider. Both D0D0γD^{*0}\to D^0\gamma and D0D0π0D^{*0}\to D^0\pi^0 decay modes are used. We find a peak of 50.111.1+14.850.1^{+14.8}_{-11.1} events with a mass of (3872.90.40.5+0.6+0.4)MeV/c2(3872.9^{+0.6 +0.4}_{-0.4 -0.5}){\rm MeV}/c^2, a width of (3.91.41.1+2.8+0.2)MeV/c2(3.9^{+2.8 +0.2}_{-1.4 -1.1}){\rm MeV}/c^2 and a product branching fraction B(BX(3872)K)×B(X(3872)D0Dˉ0)=(0.80±0.20±0.10)×104{\cal B}(B\to X(3872)K)\times{\cal B}(X(3872)\to D^{*0}\bar D^0)=(0.80\pm0.20\pm0.10)\times10^{-4}, where the first errors are statistical and the second ones are systematic. The significance of the signal is 6.4σ6.4\sigma. The difference between the fitted mass and the D0Dˉ0D^{*0}\bar D^0 threshold is calculated to be (1.10.40.3+0.6+0.1)MeV/c2(1.1^{+0.6 +0.1}_{-0.4 -0.3}){\rm MeV}/c^2. We also obtain an upper limit on the product of branching fractions B(BY(3940)K)×B(Y(3940)D0Dˉ0){\cal B}(B\to Y(3940)K)\times{\cal B}(Y(3940)\to D^{*0}\bar D^0) of 0.67×1040.67\times10^{-4} at 90% CL.Comment: 7 pages, 3 figures, BELLE-CONF-0832 contributed to ICHEP 2008, revised and submitted to Phys. Rev. D R

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