Abstract

We study the LHC discovery potential of the double-bottom tetraquarks bbu¯d¯, bbu¯s¯ and bbd¯s¯, the lightest of which having JP=1+, called T[u¯d¯]{bb}, T[u¯s¯]{bb} and T[d¯s¯]{bb}, are expected to be stable against strong decays. Employing the Monte Carlo generators MadGraph5_aMC@NLO and Pythia6, we simulate the process pp→b¯bb¯b+X and calculate the bb-diquark jet configurations, specified by the invariant mass interval Mbb<MT[q¯q¯′]{bb}+ΔM. Estimates of ΔM from the measured product σ(pp→Bc++X)B(Bc+→J/ψπ+) are presented and used to get the bb-diquark jet cross sections in double-bottom hadrons σ(pp→H{bb}+X), where H{bb} represent tetraquarks and baryons. This is combined with the LHCb data on the fragmentation b→Λb and b→B to obtain σ(pp→T[u¯d¯]{bb}+X)=(2.8−0.7+1.0)nb at s=13 TeV, and about a quarter of this for the T[u¯s¯]{bb} and T[d¯s¯]{bb}, each. We also present estimates of the production cross sections for the mixed bottom-charm tetraquarks, bcu¯d¯, bcu¯s¯ and bcd¯s¯, obtaining σ(pp→T[u¯d¯][bc]+X)=(103−25+39)nb at s=13 TeV, and the related ones having T[u¯s¯][bc] and T[d¯s¯][bc]. They have excellent discovery potential at the LHC, as their branching ratios in various charge combinations of BD(s)(γ) are anticipated to be large.

Highlights

  • The discovery of X(3872), followed by well over a dozen related mesonic states, X, Y, Z, and two baryonic states Pc(4380) and Pc(4450), has opened a second layer of “extraordinary” hadrons in QCD, containing four and five valence quarks and antiquarks [1]

  • The competing theoretical models put forward can be roughly classified into two categories: those reflecting the residual QCD long-distance effects, dominated by meson exchanges, and those reflecting genuine short-distance interactions, dominated by gluon exchanges

  • Heavy tetraquarks (DHTQ) Q i Q jqkqmust exist in the Heavy Quark Symmetry (HQS) limit

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Summary

Contents lists available at ScienceDirect

Discovery potential of stable and near-threshold doubly heavy tetraquarks at the LHC. Ahmed Ali a,∗, Qin Qin b, Wei Wang c a Deutsches Elektronen-Synchrotron DESY, D-22607 Hamburg, Germany b Theoretische Physik 1, Naturwissenschaftlich-Technische Fakultät, Universität Siegen, Walter-Flex-Strasse 3, D-57068 Siegen, Germany c INPAC, Shanghai Key Laboratory for Particle Physics and Cosmology, MOE Key Laboratory for Particle Physics, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China article info. Article history: Received 3 July 2018 Received in revised form 17 August 2018 Accepted 11 September 2018 Available online 14 September 2018 Editor: A. We study the LHC discovery potential of the double-bottom tetraquarks bbud, bbus ̄ and bbds ̄, the lightest of which having. Are presented and used to get the bb-diquark jet cross sections in double-bottom hadrons σ We present estimates of the production cross sections for the mixed bottom-charm tetraquarks, bcud ̄, bcus ̄. Excellent discovery (103+−3295 ) potential nb at the LHC, as their branching ratios in various charge combinations of B D(s)(γ ) are anticipated to be large

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