Abstract

A search is performed for the as yet unobserved baryonic $\Lambda_b \rightarrow \Lambda \eta^\prime$ and $\Lambda_b \rightarrow \Lambda \eta$ decays with 3$fb^{-1}$ of proton-proton collision data recorded by the LHCb experiment. The $B^0 \rightarrow K_S^0 \eta^\prime$ decay is used as a normalisation channel. No significant signal is observed for the $\Lambda_b \rightarrow \Lambda \eta^\prime$ decay. An upper limit is found on the branching fraction of $\mathcal{B}(\Lambda_b \rightarrow \Lambda \eta^\prime)<3.1\times10^{-6}$} at 90\% confidence level. Evidence is seen for the presence of the $\Lambda_b \rightarrow \Lambda \eta$ decay at the level of $3\sigma$ significance, with a branching fraction $\mathcal{B}(\Lambda_b \rightarrow \Lambda \eta)=(9.3^{+7.3}_{-5.3})\times10^{-6}$}.

Highlights

  • One consequence of the mixing is the difference in branching fractions for b-hadron decays to final states containing η and η mesons

  • This paper describes the search for the Λ0b → Λη and Λ0b → Λη decays and measurement of the relative branching fractions with respect to the B0 → K0η decay, using the 3 fb−1 of data in pp collisions collected in 2011 and 2012 by the LHCb experiment

  • A search is performed for the Λ0b → Λη and Λ0b → Λη decays in the full dataset recorded by the LHCb experiment during 2011 and 2012, corresponding to an integrated luminosity of 3 fb−1

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Summary

Fit results and signal yields

An unbinned extended maximum likelihood fit to the candidate b-hadron mass spectrum is performed on the data which pass the selection. The most likely backgrounds are: b-hadron decay modes to mesons with open charm and an η( ) meson, with a π0 meson which is not reconstructed; the nonresonant decays to K0S or Λ particles with two charged pions which are combined with a combinatorial photon, π0 or η meson to form an η( ) meson candidate; or, in the case of the η → π+π−γ decays, the nonresonant B0 → K0Sπ+π−γ or Λ0b → Λπ+π−γ decays. An unbinned extended maximum likelihood fit is performed using the same model as for the B0 decay, with an exponential function to describe the combinatorial background and a sum of two Gaussian functions to model the signal; all parameters are fixed to the values found from fits to the simulation, and only the numbers of signal and background events are allowed

LHCb Long Λ0
Branching fraction measurement
Conclusions
Full Text
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