Probing double hadron resonances by the complex scaling method

Abstract

Many newly discovered excited states are interpreted as bound states of hadrons. Can these hadrons also form resonant states? In this paper, we extend the complex scaling method (CSM) to calculate the bound state and resonant state consistently for the ${\Lambda }_{c}D(\bar{D})$ and ${\Lambda }_c{\Lambda }_c({\bar{\Lambda }}_c)$ systems. For these systems, the $\pi ,\eta ,\rho$ meson exchange contributions are suppressed, the contributions of intermediate- and short-range forces from $\sigma /\omega$ exchange are dominant. Our results indicate that ${\Lambda }_{c}D$ system can not form bound state and resonant state. There exist resonant states in a wide range of parameters for ${\Lambda }_c\bar{D}$ and ${\Lambda }_c{\Lambda }_c({\bar{\Lambda }}_c)$ systems. For these systems, the larger bound state energy, the easier to form resonant states. Among all the resonant states, the energies and widths of the P wave resonant states are smaller and more stable, which is possible to be observed in the experiments. The energies of D and F wave resonant states can reach dozens of MeV and the widths can reach hundreds of MeV.

7 pages, 6 figures, accepted by Physical Review C

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Cited by in corpus (3)

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• Explanation of Y(4630) as hadronic resonant state
• Complex-scaled no-core shell model calculations of bound and unbound nuclear states in light nuclei