Abstract

The kinematic dependences of the relative production rates, $f_{\Lambda_b^0}/f_d$, of $\Lambda_b^0$ baryons and $\bar{B}^0$ mesons are measured using $\Lambda_b^0 \rightarrow \Lambda_c^+ \pi^-$ and $\bar{B}^0 \rightarrow D^+ \pi^-$ decays. The measurements use proton-proton collision data, corresponding to an integrated luminosity of 1 fb$^{-1}$ at a centre-of-mass energy of 7 TeV, recorded in the forward region with the LHCb experiment. The relative production rates are observed to depend on the transverse momentum, $p_T$, and pseudorapidity, $\eta$, of the beauty hadron, in the studied kinematic region $1.5 < p_T < 40$ GeV/$c$ and $2 < \eta < 5$. Using a previous LHCb measurement of $f_{\Lambda_b^0}/f_d$ in semileptonic decays, the branching fraction $\mathcal{B}(\Lambda_b^0 \rightarrow \Lambda_c^+ \pi^-) = \Big( 4.30 \pm 0.03 \,\, ^{+0.12}_{-0.11} \pm 0.26 \pm 0.21 \Big) \times 10^{-3}$ is obtained, where the first uncertainty is statistical, the second is systematic, the third is from the previous LHCb measurement of $f_{\Lambda_b^0}/f_d$ and the fourth is due to the $\bar{B}^0 \rightarrow D^+ \pi^-$ branching fraction. This is the most precise measurement of a $\Lambda_b^0$ branching fraction to date.

Highlights

  • Efficiencies particle identification (PID) boosted decision tree (BDT) Sample size Trigger Other Bin centre Total pT binsR = a + exp(b + c × pT) a b c+−00..74% +−51..57%+−00..52% +−22..81%+−00..23% +−21..61%0.0% +−57..86% ±12.1%0.5% −+1145..12% ±9.0%2.5% +−190..62% ±10.8%±0.3% ±0.3% +−1144..65% +−1177..17%±0.1% +−1144..99%

  • The relative production rates are observed to depend on the transverse momentum, pT, and pseudorapidity, η, of the beauty hadron, in the studied kinematic region 1.5 < pT < 40 GeV/c and 2 < η < 5

  • The study of the dependences of fΛ0b /fd on the pT and η of the b hadron and the measurement of the branching fraction of Λ0b → Λ+c π− decays are performed using candidates restricted to the fiducial region 1.5 < pT < 40 GeV/c and 2 < η < 5

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Summary

Detector and simulation

The LHCb detector [12] is a single-arm forward spectrometer covering the pseudorapidity range 2 < η < 5, designed for the study of particles containing b or c quarks. The trigger consists of a hardware stage, based on information from the calorimeter and muon systems, followed by a software stage, which applies a full event reconstruction. The software trigger requires a two-, three- or four-track secondary vertex (SV) with a large sum of the pT of the particles and a significant displacement from the primary pp interaction vertices (PVs). At least one charged particle should have pT > 1.7 GeV/c and χ2IP with respect to any PV greater than 16, where χ2IP is defined as the difference in fit χ2 of a given PV reconstructed with and without the considered track. Simulated collision events are used to estimate the efficiency of the reconstruction and selection steps for signal as well as background b-hadron decay modes. The interaction of the generated particles with the detector and its response are implemented using the Geant toolkit [17, 18] as described in ref. [19]

Event selection
Event yields
Results
Systematic uncertainties
Background
Conclusions
Full Text
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