Are there narrow flavor-exotic tetraquarks in large-$N_c$ QCD?

TL;DR

This paper argues that large-$N_c$ QCD does not support narrow flavor-exotic tetraquarks due to the incompatibility of their decay channels with the diquark-antidiquark structure, though broad molecular states may still exist.

Contribution

It provides a theoretical argument against the existence of narrow flavor-exotic tetraquarks in large-$N_c$ QCD based on decay channel analysis.

Findings

Large-$N_c$ QCD predicts only one diquark-antidiquark structure.

Two narrow flavor-exotic tetraquarks with different decay channels cannot coexist.

The absence of narrow flavor-exotic tetraquarks aligns with experimental observations.

Abstract

A salient feature shared by all tetraquark candidates observed in experiment is the absence of flavor-exotic states of the type $\bar a b\bar c d$, with four different quark flavors. This phenomenon may be understood from the properties of large-$N_c$ QCD: On the one hand, consistency conditions for flavor-exotic Green functions, potentially containing these tetraquark poles, require the existence of two tetraquarks $T_A$ and $T_B$: each of them should decay dominantly via a single two-meson channel, $T_A\to M_{\bar a b}M_{\bar c d}$ and $T_B\to M_{\bar a d}M_{\bar c b}$, with suppressed rates $T_A\to M_{\bar a d}M_{\bar c b}$ and $T_B\to M_{\bar a b}M_{\bar c d}$. On the other hand, we have at hand only one diquark-antidiquark flavor structure $(\bar a \bar c)(b d)$ that might produce a compact tetraquark bound state. Taking into account that the diquark-antidiquark structure is the only viable candidate for a compact tetraquark state, one concludes that it is impossible to have two different narrow tetraquarks decaying dominantly into different two-meson channels. This contradiction suggests that large-$N_c$ QCD does not support the existence of narrow flavor-exotic tetraquarks. This argument does not rule out the possible existence of broad molecular-type flavor-exotic states, or of molecular-type bound states lying very close to the two-meson thresholds.