2025/07/22 by Zhao-Sai Jia, Gang Li, Jia, Zhao-Sai +3
Physics and Astronomy · Medicine · #Particle physics theoretical and experimental studies #Quantum Chromodynamics and Particle Interactions #Medical Imaging Techniques and Applications
paper · pdf · doi:10.48550/arxiv.2507.16618
The hidden-charm decays serve as irreplaceable platforms for probing the structures of charmonium-like states, such as X(3872), Y(4260), Zc(3900), and their heavy-quark-symmetry partners. In the hadronic molecular scenario, these hidden-charm decays are denominated by intermediate meson loops (IMLs), and the couplings of χcJ→ D(∗)D(∗) are building blocks of the amplitudes for the pionic and radiative transitions of the charmonium-like states to the χcJ and hc states, e.g., X(3872)→ π0χcJ, ππχcJ, γχcJ and Y(4260)→ π0 hc, ηhc. These couplings can not be extracted from the partial decay widths of the χcJ directly and only have estimated values from the vector meson dominance (VMD) model. Utilizing the recent precise determination of the pole position and the isospin breaking properties of the X(3872), we give an estimation on the upper bounds of the absolute values of the χcJ→ D(∗)D(∗) couplings. Our results show that the VMD model may over estimate the χcJ→ D(∗)D(∗) couplings considering the X(3872) as a DD* hadronic molecule with a binding energy about tens of keV. These upper limits can be used and tested in other hidden-charm transitions of the charmonium-like states to the χcJ and hc.