Abstract

We study the chiral interactions of the hidden charm $D\bar{D}^*$ system within chiral effective field theory. Chiral Lagrangians are constructed by incorporating the chiral symmetry, heavy quark symmetry as well as proper charge conjugation properties of the heavy mesons. The interacting potentials of the $S$-wave $D\bar{D}^*$ are calculated up to second chiral order at 1-loop level, where complete two-pion exchange interactions are included. We further investigate the behaviors of the potentials in coordinate space, as well as their bound state properties. Our studies indicate that there exists a interacting strength ordering among considered four channels: $\text{str.}[0^+(1^{++})]>\text{str.}[0^-(1^{+-})] > \text{str.}[1^+(1^{+-})] > \text{str.}[1^-(1^{++})]$ where str. stands for the strength of the $D\bar{D}^*$ interaction. Moreover, we find that $X(3872)$ can be treated as a good candidate of $0^+(1^{++})$ molecular state. There also tends to form $0^-(1^{+-})$ and $1^+(1^{+-})$ molecular states and we expect the experiments to search for the predicted multi-structures around the $D\bar{D}^*$ mass region.

Highlights

  • In past two decades, abundant exotic hadrons have been discovered by upgraded τ-charm and b factories, such as BESIII, LHCb, Belle, BABAR, etc

  • II we describe the concerned DD Ã Lagrangians by considering the chiral symmetry and heavy quark symmetry, as well as by properly taking into account the charge conjugation properties of the heavy mesons

  • We substitute the calculated potentials into the Schrödinger equation and explore whether the DD Ã

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Summary

Introduction

Abundant exotic hadrons have been discovered by upgraded τ-charm and b factories, such as BESIII, LHCb, Belle, BABAR, etc. Various forms of exotic quark matters arise in hadron spectroscopy: pentaquarks (Pc and Pcs states), fully charmed tetraquark candidates [recently discovered Xð6900Þ], hidden charm tetraquark candidates (some XYZ states), etc. LHCb observed a doubly charmed structure Tcc [3] that is extremely close to the D0DÃþ threshold (the mass difference is −273 Æ 61 Æ 5þ−1141 keV). Tcc has a minimal ccud ̄ content. It may still be an ongoing progress that other forms of multiquark structures are prepared to be uncovered.

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