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Study of the decay Bˉ0Λc+pˉπ+π\bar{B}^{0}\rightarrowΛ_{c}^{+}\bar{p}π^{+}π^{-} and its intermediate states

Published 1 Feb 2013 in hep-ex | (1302.0191v2)

Abstract: We study the decay Bˉ<sup>0Λc<sup>+pˉπ<sup>+π<sup>\bar{B}<sup>{0}\rightarrow\Lambda_{c}<sup>{+}\bar{p}\pi<sup>{+}\pi<sup>{-}, reconstructing the \Lambda_{c}{+} baryon in the pK<sup>π<sup>+p K<sup>{-}\pi<sup>{+} mode, using a data sample of 467×10<sup>6467\times 10<sup>{6} BBˉB\bar{B} pairs collected with the BaBar detector at the PEP-2 storage rings at SLAC. We measure branching fractions for decays with intermediate Σc\Sigma_{c} baryons to be B[Bˉ<sup>0Σc(2455)<sup>++pˉπ<sup>]=(21.3</sup></sup></sup>±1.0±1.0±5.5)×10<sup>5{\cal B}[\bar{B}<sup>{0}\rightarrow\Sigma_{c}(2455)<sup>{++}\bar{p}\pi<sup>{-}]=(21.3</sup></sup></sup> \pm 1.0 \pm 1.0 \pm 5.5) \times 10<sup>{-5}, B[Bˉ<sup>0Σc(2520)<sup>++pˉπ<sup>]=(11.5±</sup></sup></sup>1.0±0.5±3.0)×10<sup>5{\cal B}[\bar{B}<sup>{0}\rightarrow\Sigma_{c}(2520)<sup>{++}\bar{p}\pi<sup>{-}]=(11.5\pm</sup></sup></sup> 1.0 \pm 0.5 \pm 3.0)\times 10<sup>{-5}, B[Bˉ<sup>0Σc(2455)<sup>0pˉπ<sup>+]=(9.1</sup></sup></sup>±0.7±0.4±2.4)×10<sup>5{\cal B}[\bar{B}<sup>{0}\rightarrow\Sigma_{c}(2455)<sup>{0}\bar{p}\pi<sup>{+}]=(9.1</sup></sup></sup> \pm 0.7 \pm 0.4 \pm 2.4)\times10<sup>{-5}, and B[Bˉ<sup>0Σc(2520)<sup>0pˉπ<sup>+]=</sup></sup></sup>(2.2±0.7±0.1±0.6)×10<sup>5{\cal B}[\bar{B}<sup>{0}\rightarrow\Sigma_{c}(2520)<sup>{0}\bar{p}\pi<sup>{+}]=</sup></sup></sup> (2.2 \pm 0.7 \pm 0.1\pm 0.6) \times 10<sup>{-5}, where the uncertainties are statistical, systematic, and due to the uncertainty on the $\Lambda_{c}<sup>{+}\rightarrow\proton\Km\pi<sup>{+}$ branching fraction, respectively. For decays without Σc(2455)\Sigma_{c}(2455) or Σc(2520)\Sigma_{c}(2520) resonances, we measure B[Bˉ<sup>0Λc<sup>+pˉπ<sup>+π<sup>]<em>nonΣ</em>c=(79</sup></sup></sup></sup>±4±4±20)×10<sup>5{\cal B}[\bar{B}<sup>{0}\rightarrow\Lambda_{c}<sup>{+}\bar{p}\pi<sup>{+}\pi<sup>{-}]<em>{\mathrm{non-\Sigma</em>{c}}}=(79</sup></sup></sup></sup> \pm 4 \pm 4 \pm 20)\times10<sup>{-5}. The total branching fraction is determined to be B[Bˉ<sup>0Λc<sup>+pˉπ<sup>+π<sup>]total=(123</sup></sup></sup></sup>±5±7±32)×10<sup>5{\cal B}[\bar{B}<sup>{0}\rightarrow\Lambda_{c}<sup>{+}\bar{p}\pi<sup>{+}\pi<sup>{-}]_{\mathrm{total}}=(123</sup></sup></sup></sup> \pm 5 \pm 7 \pm 32)\times10<sup>{-5}. We examine multibody mass combinations in the resonant three-particle Σcpˉπ\Sigma_{c}\bar{p}\pi final states and in the four-particle Λc<sup>+pˉπ<sup>+π<sup>\Lambda_{c}<sup>{+}\bar{p}\pi<sup>{+}\pi<sup>{-} final state, and observe different characteristics for the pˉπ\bar{p}\pi combination in neutral versus doubly-charged Σc\Sigma_{c} decays.

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