$P$-wave coupled channel effects in electron-positron annihilation

TL;DR

This study systematically analyzes P-wave coupled channel effects in electron-positron annihilation near charm meson thresholds, revealing pole structures related to known states and potential exotic molecules, using a coupled-channel approach and experimental data fitting.

Contribution

It introduces a coupled-channel framework to study P-wave effects in $e^+e^-$ annihilation, extracting pole positions and analyzing HQSS breaking effects, with implications for exotic hadronic states.

Findings

Identified poles corresponding to $ ext{ψ}(3770)$ and $ ext{ψ}(4040)$ states.

Found an additional pole near the $Dar{D}^*+c.c.$ threshold related to $G(3900)$.

Quantified HQSS breaking effects through deviations in coupling ratios.

Abstract

$P$-wave coupled channel effects arising from the $D\bar{D}$, $D\bar{D}^*+c.c.$, and $D^*\bar{D}^*$ thresholds in $e^+e^-$ annihilations are systematically studied. We provide an exploratory study by solving the Lippmann-Schwinger equation with short-ranged contact potentials obtained in the heavy quark limit. These contact potentials can be extracted from the $P$-wave interactions in the $e^+e^-$ annihilations, and then be employed to investigate possible isosinglet $P$-wave hadronic molecules. In particular, such an investigation may provide information about exotic candidates with quantum numbers $J^{PC}=1^{-+}$. In the mass region of the $D\bar{D}$, $D\bar{D}^*+c.c.$, and $D^*\bar{D}^*$ thresholds, there are two quark model bare states, i.e. the $\psi(3770)$ and $\psi(4040)$, which are assigned as $(1^3D_1)$ and $(3^1S_1)$ states, respectively. By an overall fit of the cross sections of $e^+e^-\to D\bar{D}$, $D\bar{D}^*+c.c.$, $D^*\bar{D}^*$, we determine the physical coupling constants to each channel and extract the pole positions of the $\psi(3770)$ and $\psi(4040)$. The deviation of the ratios from that in the heavy quark spin symmetry (HQSS) limit reflects the HQSS breaking effect due to the mass splitting between the $D$ and the $D^*$. Besides the two poles, we also find a pole a few MeV above the $D\bar{D}^*+c.c.$ threshold which can be related to the so-called $G(3900)$ observed earlier by BABAR and Belle. This scenario can be further scrutinized by measuring the angular distribution in the $D^*\bar{D}^*$ channel with high luminosity experiments.