Abstract

Decays of $B^0$ and $B_{s}^0$ mesons to the charmless baryonic final states $p \overline{p} h^+ h^{\prime-}$, where $h$ and $h^\prime$ each denote a kaon or a pion, are searched for using the LHCb detector. The analysis is based on a sample of proton-proton collision data collected at center-of-mass energies of $7$ and $8\,$TeV, corresponding to an integrated luminosity of $3\,$fb$^{-1}$. Four-body charmless baryonic $B_{s}^0$ decays are observed for the first time. The decays $B^0_{s}\to p \overline{p} K^+ K^-$, $B^0_{s}\to p \overline{p} K^\pm \pi^\mp$, $B^0\to p \overline{p} K^\pm \pi^\mp$ and $B^0\to p \overline{p} \pi^+\pi^-$ are observed with a significance greater than $5$ standard deviations; evidence at $4.1$ standard deviations is found for the $B^0\to p \overline{p} K^+ K^-$ decay and an upper limit is set on the branching fraction for $B^0_{s}\to p \overline{p} \pi^+ \pi^-$. Branching fractions in the kinematic region $m(p \overline{p})<2850\,$MeV$/c^2$ are measured relative to the $B^0 \to J/\psi (\to p \overline{p}) K^*(892)^0$ channel.

Highlights

  • Studies by the LHCb Collaboration have greatly increased the knowledge of the decays of B mesons to final states containing baryons

  • It is of great interest to search for further manifestations of CP violation in baryonic B decays, e.g. with so-called triple-product correlations (TPCs); see Ref. [6] and references therein

  • This paper presents a search for the decays of B0 and B0s mesons to the four-body charmless baryonic final states pphþh0−, where h and h0 each denote a kaon or a pion

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Summary

Introduction

Studies by the LHCb Collaboration have greatly increased the knowledge of the decays of B mesons to final states containing baryons. The final selection of B0ðsÞ candidates, formed by combining four charged hadron candidates—a proton, an antiproton and an oppositely charged pair of light mesons—is carried out with a filtering stage, followed by requirements on the response of a boosted decision tree (BDT) classifier [23,24] and on particle identification (PID).

Results
Conclusion

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