Abstract

We use lattice QCD to investigate the spectrum of the $\bar{b} \bar{b} u d$ four-quark system with quantum numbers $I(J^P) = 0(1^+)$. We use five different gauge-link ensembles with $2+1$ flavors of domain-wall fermions, including one at the physical pion mass, and treat the heavy $\bar{b}$ quark within the framework of lattice nonrelativistic QCD. Our work improves upon previous similar computations by considering in addition to local four-quark interpolators also nonlocal two-meson interpolators and by performing a L\"uscher analysis to extrapolate our results to infinite volume. We obtain a binding energy of $(-128 \pm 24 \pm 10) \, \textrm{MeV}$, corresponding to the mass $(10476 \pm 24 \pm 10) \, \textrm{MeV}$, which confirms the existence of a $\bar{b} \bar{b} u d$ tetraquark that is stable with respect to the strong and electromagnetic interactions.

Highlights

  • Mesons, i.e., hadrons with integer spin, were first envisioned by Gell-Mann and Zweig [1,2] to be built from one, two or more quark-antiquark pairs

  • Exotic mesons can be characterized as having JPC quantum numbers that cannot be constructed in the simple quark-antiquark model, or as having a manifestly exotic quark flavor content

  • We used the conjugate gradient (CG) solver combined with low-mode deflation, where in the case of the approximate propagators the CG iteration count is fixed to a smaller value, NCG;sl, than needed for the exact propagators

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Summary

INTRODUCTION

I.e., hadrons with integer spin, were first envisioned by Gell-Mann and Zweig [1,2] to be built from one, two or more quark-antiquark pairs. In this paper we perform a lattice QCD study of the bb ̄ ud four-quark system with quantum numbers IðJPÞ 1⁄4 0ð1þÞ, using NRQCD bquarks and domain-wall light quarks We make use of both local interpolating fields (in which the four quarks are jointly projected to zero momentum) and nonlocal interpolating fields (in which each of the two quark-antiquark pairs forming a color-singlet is projected to zero momentum individually) It has been shown in previous studies of other systems [44,45] that including both types of interpolating fields is required to reliably determine ground-state energies in exotic channels.

Gauge-link configurations and light-quark propagators
Bottom-quark propagators
INTERPOLATING OPERATORS AND CORRELATION FUNCTIONS
B and BÃ meson
ENERGIES AND KINETIC MASSES OF THE B AND BÃ MESONS
THE LOWEST ENERGY LEVELS OF THE bbud SYSTEM
Nsloppy
Dependence of the fit results on the choices of interpolating fields
Overlap factors
Final results for the lowest two energy levels on each ensemble
SCATTERING ANALYSIS
Relation between finite-volume energy levels and infinite-volume phase shifts
Effective-range expansion and determination of the bound-state pole
Numerical results
FIT OF THE PION-MASS DEPENDENCE AND ESTIMATES OF SYSTEMATIC UNCERTAINTIES
Findings
VIII. CONCLUSIONS
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