Abstract

In the paper, we present a detailed discussion on the semi-inclusive production of doubly heavy baryons ($\Xi_{bc}$ and $\Xi_{bb}$) through top-quark decay channel, $t\rightarrow \Xi_{bQ^{\prime}}+ \bar {Q^{\prime}} + W^+ $, within the framework of non-relativistic QCD (NRQCD). In our calculations, the contributions from the intermediate diquark states, $\langle bc\rangle[^{3}S_{1}]_{\mathbf{\bar 3}/ \mathbf{6}}$, $\langle bc\rangle[^{1}S_{0}]_{\mathbf{\bar 3}/ \mathbf{6}}$, $\langle bb\rangle[^{1}S_{0}]_{\mathbf{6}}$ and $\langle bb\rangle[^{3}S_{1}]_{\mathbf{\bar 3}}$, have been taken into consideration. Main uncertainties from the heavy quark mass $(m_c,~m_b~\mbox{or}~m_t)$, the renormalization scale $\mu_r$, and the nonperturbative transition probability have been estimated. For a comparison, we also analyze the production of doubly heavy baryons under the approximate fragmentation function approach. Estimated at the LHC or a High Luminosity LHC with $\mathcal{L}$ =$10^{34-36}~\rm{cm}^{-2}~\rm{s}^{-1}$, there will be about $2.25\times10^{4-6}$ events of $\Xi_{bc}$ and $9.49\times10^{2-4}$ events of $\Xi_{bb}$ produced in one operation year through top-quark decays.

Highlights

  • The LHCb Collaboration of the CERN LHC announced its first observation of the doubly heavy baryon Ξþccþ [1] for the proton-proton center-of-mass collision energy of 13 TeV and an integrated luminosity of 1.7 fb−1, confirming the success of the quark model [2,3,4,5]

  • We present a detailed discussion on the semi-inclusive production of doubly heavy baryons (Ξbc and Ξbb) through top-quark decay channel, t → ΞbQ0 þ Q 0 þ Wþ, within the framework of nonrelativistic QCD

  • We analyze the production of doubly heavy baryons under the approximate fragmentation function approach

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Summary

INTRODUCTION

The LHCb Collaboration of the CERN LHC announced its first observation of the doubly heavy baryon Ξþccþ [1] for the proton-proton center-of-mass collision energy of 13 TeV and an integrated luminosity of 1.7 fb−1, confirming the success of the quark model [2,3,4,5]. We shall discuss the production of doubly heavy baryons ΞbQ0 via the top-quark decays at the LHC or its successor [the High Luminosity LHC (HL-LHC)]. In addition to the conventional fixed-order calculations, the production of doubly heavy baryon ΞbQ0 from topquark decays can be described by using the fragmentation function approach. The fragmentation function approach resums the large logarithms such as lnðMΞbQ0 =EÞ and could provide a more reliable prediction in specific kinematic regions, where E is the energy of the corresponding baryon Such kinds of large logarithms always come from the collinear emissions for high-order calculations or small pt regions. We shall concentrate on the fixed-order calculation with the NRQCD and shall give a simple discussion on how the fragmentation function approach may change the behaviors of the energy fraction of the produced doubly heavy baryons.

Fixed-order calculation within the NRQCD framework
Fragmentation function approach
NUMERICAL RESULTS
Basic results
Differential decay widths
Theoretical uncertainties
SUMMARY
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