First observation of Λb0Σc()++D()K\Lambda_{b}^{0} \rightarrow \Sigma_c^{(*)++} D^{(*)-} K^{-} decays

Abstract

International audienceThe four decays, Λb0Σc()++D()K\Lambda_{b}^{0} \rightarrow \Sigma_c^{(*)++} D^{(*)-} K^{-}, are observed for the first time using proton-proton collision data collected with the LHCb detector at a centre-of-mass energy of 13TeV13\,\rm{TeV}, corresponding to an integrated luminosity of 6fb16\,\rm{fb}^{-1}. By considering the Λb0Λc+D0K\Lambda_b^0 \rightarrow \Lambda_c^{+} \overline{D}^0 K^{-} decay as reference channel, the following branching fraction ratios are measured to be, B(Λb0Σc++DK)B(Λb0Λc+D0K)=0.282±0.016±0.016±0.005,B(Λb0Σc++DK)B(Λb0Σc++DK)=0.460±0.052±0.028,B(Λb0Σc++DK)B(Λb0Σc++DK)=2.261±0.202±0.129±0.046,B(Λb0Σc++DK)B(Λb0Σc++DK)=0.896±0.137±0.066±0.018,\frac{\cal{B} (\Lambda_{b}^{0} \rightarrow \Sigma_{c}^{++} \rm{D}^{-} {K}^{-})}{\cal{B}(\Lambda_{b}^{0} \rightarrow \Lambda_c^{+} \rm \overline{D}^0 {K}^{-})} = {0.282}\pm{0.016}\pm{0.016}\pm{0.005}, \frac{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_{c}^{*++} \rm {D}^{-} {K}^{-})}{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_c^{++} \rm {D}^{-} {K}^{-})} = {0.460}\pm{0.052}\pm{0.028}, \frac{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_{c}^{++} \rm {D}^{*-} {K}^{-})}{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_c^{++} \rm {D}^{-} {K}^{-})} = {2.261}\pm{0.202}\pm{0.129}\pm{0.046}, \frac{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_{c}^{*++} \rm D^{*-} K^{-})}{\cal{B}(\Lambda_{b}^{0} \rightarrow \Sigma_c^{++} \rm D^{-} K^{-})} = {0.896}\pm{0.137}\pm{0.066}\pm{0.018}, where the first uncertainties are statistical, the second are systematic, and the third are due to uncertainties in the branching fractions of intermediate particle decays. These initial observations mark the beginning of pentaquark searches in these modes, with more data set to become available following the LHCb upgrade

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