Spectrum of the S-wave fully-heavy tetraquark states

Abstract

In present work, spectrum of the $S$-wave fully-heavy tetraquark states $QQ\bar{Q}\bar{Q}$ ($Q=c,b$), i.e., $cc\bar{c}\bar{c}$, $bb\bar{b}\bar{b}$, $cc\bar{b}\bar{b}$/$bb\bar{c}\bar{c}$, $bc\bar{c}\bar{c}$/ $cc\bar{b}\bar{c}$, $bb\bar{c}\bar{b}$/$cb\bar{b}\bar{b}$, and $bc\bar{b}\bar{c}$ are systematically investigated within an nonrelativistic constituent quark model, in which the Instanton-induced and one-gluon-exchange interactions are taken into account as the residual spin-dependent hyperfine interaction. Our results show that the states with $cc\bar{c}\bar{c}$ and $bb\bar{b}\bar{b}$ components could be located around $6500$ MeV and $19200$ MeV, respectively. Based on our calculations, the new $X(6900)$ state observed by LHCb may be not a ground $cc\bar{c}\bar{c}$ tetraquark state, while it could be an orbitally or radially excited state of $cc\bar{c}\bar{c}$ system. On the other hand, the recently reported $X(6600)$ state by CMS and ATLAS can be explained as a ground $cc\bar{c}\bar{c}$ tetraquark state with spin-parity $J^{PC}=0^{++}$.

arXiv commentVersion to appear in Eur. Phys. J. C

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• Benchmark calculations of fully heavy compact and molecular tetraquark states
• Going in quest of potential tetraquark interpretations for the newly observed $T_{\psi \psi }$ states in light of the diquark-antidiquark scenarios
• Study of $X(6900)$ with unitarized coupled channel scattering amplitudes
• Relativistic description of asymmetric fully heavy tetraquarks in the diquark-antidiquark model
• Fully heavy tetraquark resonant states with different flavors
• P-wave fully charm and fully bottom tetraquark states
• Charmoniumlike Channels $1^{+}$ with Isospin $1$ from Lattice and Effective Field Theory
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• Prediction of charmed-bottom pentaquarks in quark model
• The ground states of hidden-charm tetraquarks and their radial excitations
• Fully heavy tetraquark states with a diquark-antidiquark configuration
• Investigating the internal structure of $X(6900)$ in the $2J/\psi$ decay channel