Dynamical generation of charmonium-like tetraquarks in an off-shell coupled-channel formalism

TL;DR

This paper models the dynamical generation of charmonium-like tetraquark states using an off-shell coupled-channel approach, successfully reproducing known states and predicting new resonances in the 3.6 to 4.3 GeV range.

Contribution

It introduces a novel off-shell coupled-channel formalism that respects heavy-quark symmetries and excludes s-channel poles to study exotic tetraquark states.

Findings

Reproduces the $ ext{X}(3872)$ as a bound state near the $Dar{D}^*$ threshold.

Predicts new resonances at 3861 MeV, 3961 MeV, 4005 MeV, and 4030 MeV.

Highlights the importance of $D^*ar{D}^*$ channels in state formation.

Abstract

We investigate the dynamical generation of charmonium-like ($I=0$) with spin-parity $J^{PC}=0^{++}, 1^{++}, 2^{++}$, and $3^{--}$ in the mass range of $3.6$ to $4.3$ GeV. We employ the off-shell coupled-channel formalism, constructing kernel amplitudes from effective Lagrangians that respect heavy-quark spin-flavor and chiral symmetries. To focus solely on dynamically generated states, we explicitly exclude $s$-channel pole diagrams and include only $t$- and $u$-channel meson exchanges. Solving the integral equations, we identify six poles in the complex energy plane. In the scalar ($0^{++}$) sector, we find a bound state below the $D\bar{D}$ threshold and a resonance at $\sqrt{s_R}=(3861-i\,23)\,\mathrm{MeV}$. For the axial-vector ($1^{++}$) sector, the experimentally observed $\chi_{c1}(3872)$ is reproduced as a bound state near the $D\bar{D}^*$ threshold, alongside a broader resonance at $(3961-i\,32)\,\mathrm{MeV}$, which is a plausible candidate for the $X(3940)$. Furthermore, we find a narrow tensor ($2^{++}$) state at $4005\,\mathrm{MeV}$ and a vector ($3^{--}$) state at $4030\,\mathrm{MeV}$. The present results demonstrate that coupled-channel dynamics, particularly involving the $D^*\bar{D}^*$ channel, play a crucial role in the formation of these charmonium-like exotic states.