Abstract

We provide a holographic description of nonstrange multiquark exotics as compact topological molecules by binding heavy-light mesons to a tunneling configuration in $\mathrm{D}8\text{\ensuremath{-}}\mathrm{D}\overline{8}$ that is homotopic to the vacuum state with a fixed Chern-Simons number. In the tunneling process, the heavy-light mesons transmute to fermions. Their binding is generic and arises from a trade-off between the dipole attraction induced by the Chern-Simons term and the U(1) fermionic repulsion. In the heavy quark limit, the open-flavor tetraquark exotics $QQ\overline{q}\overline{q}$ and $\overline{Q}\overline{Q}qq$ emerge as bound Efimov states in a degenerate multiplet $I{J}^{\ensuremath{\pi}}=(0{0}^{+},0{1}^{+})$ with opposite intrinsic Chern-Simons numbers $\ifmmode\pm\else\textpm\fi{}\frac{1}{2}$. The hidden-flavor tetraquark exotics such as $Q\overline{Q}q\overline{q}$, $QQ\overline{Q}\overline{q}$, and $QQ\overline{Q}\overline{Q}$ as compact topological molecules are unbound. Other exotics are also discussed.

Highlights

  • Several experimental collaborations [1,2,3,4] have reported new multiquark exotic states such as the neutral Xð3872Þ and the charged Zcð3900ÞÆ and Zbð10610ÞÆ, a priori outside the canonical quark model classification

  • Some of the reported hidden-flavor tetraquark exotics appear to be loosely bound hadronic molecules of two heavy-light mesons [7,8,9,10,11,12,13,14,15], other explanations for their composition are suggested in Refs. [16,17,18,19]

  • The first estimates of the open-flavor and compact tetraquark exotics were made in the context of the bag model [20] and the random instanton model with full chiral and heavy

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Summary

INTRODUCTION

Several experimental collaborations [1,2,3,4] have reported new multiquark exotic states such as the neutral Xð3872Þ and the charged Zcð3900ÞÆ and Zbð10610ÞÆ, a priori outside the canonical quark model classification. Some of the reported hidden-flavor tetraquark exotics appear to be loosely bound hadronic molecules of two heavy-light mesons [7,8,9,10,11,12,13,14,15], other explanations for their composition are suggested in Refs. It is well established that the light quark sector of QCD exhibits spontaneous chiral symmetry breaking, while the heavy quark sector is characterized by heavy quark symmetry [34] Both symmetries are at the origin of the chiral doubling suggested in heavy-light mesons [35,36] and confirmed experimentally in Refs. It is important that a theoretical approach to the multiquark states should have manifest chiral and heavy quark symmetry, a clear organizational principle in the infrared, and should address concisely the multibody bound state problem.

D-brane setup
DBI action
Light fields
Heavy-light fields
TUNNELING FIELD AND ITS FERMIONIC ZERO MODE
MULTIQUARK EXOTICS AS TOPOLOGICAL MOLECULES
Heavy bound meson
Action for the topological molecule
Hamiltonian for the topological molecule
Classical binding energy
Quantum moduli
Multiquark exotics
Discussion
CONCLUSIONS
Full Text
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