Observation of tree-level B decays with ssˉs\bar{s} Production from Gluon Radiation

preprint2008arXivOpen access

Abstract

We report on our search for B−→Ds(∗)+K−π−B^- \to D^{(*)+}_s K^- π^-, B0ˉ→Ds(∗)+KS0π−\bar{B^0} \to D_s^{(*)+} K_S^0 π^-, and B−→Ds(∗)+K−K−B^- \to D^{(*)+}_s K^- K^- decays in 383 million $\FourS \to B \Bbar$ events collected by the Babar detector at the PEP2 asymmetric-energy BB-factory. The decays proceed via a tree-level b→cb\to c quark transition in which a gluon radiates into an ssˉs\bar{s} pair. Their branching fractions are measured to be B(B−→Ds+K−π−)=(2.02±0.13stat±0.38syst)×10−4,{\cal B}(B^- \to D^+_s K^- π^-) = (2.02 \pm 0.13_{stat} \pm 0.38_{syst}) \times 10^{-4}, B(B−→Ds∗+K−π−)=(1.67±0.16stat±0.35syst)×10−4,{\cal B}(B^- \to D^{*+}_s K^- π^-)= (1.67 \pm 0.16_{stat} \pm 0.35_{syst}) \times 10^{-4}, B(B0ˉ→Ds+KS0π−)=(0.55±0.13stat±0.10syst)×10−4,{\cal B}(\bar{B^0} \to D_s^{+} K_S^0 π^-)= (0.55 \pm 0.13_{stat} \pm 0.10_{syst}) \times 10^{-4}, and B(B−→Ds+K−K−)=(0.11±0.04stat±0.02syst)×10−4{\cal B}(B^- \to D_s^{+} K^- K^-) = (0.11 \pm 0.04_{stat} \pm 0.02_{syst}) \times 10^{-4}. Upper limits at the 90% C.L. are set on B(B0ˉ→Ds∗+KS0π−)<0.55×10−4{\cal B}(\bar{B^0} \to D_s^{*+} K_S^0 π^-)< 0.55 \times 10^{-4} and B(B−→Ds∗+K−K−)<0.15×10−4{\cal B}(B^- \to D_s^{*+} K^- K^-) < 0.15 \times 10^{-4}. We present evidence that the invariant mass distributions of Ds(∗)+K−D^{(*)+}_s K^- pairs from B−→Ds(∗)+K−π−B^- \to D^{(*)+}_s K^- π^- decays are inconsistent with the phase-space model, suggesting the presence of charm resonances lying below the Ds(∗)+K−D^{(*)+}_s K^- threshold.

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