Abstract

Inspired by the discovery of two pentaquarks $P_{c}(4380)$ and $P_{c}(4450)$ at the LHCb detector, we study possible hidden-charm molecular pentaquarks in the framework of quark delocalization color screening model. Our results suggest that both $N\eta_{c}$ with $IJ^{P}=\frac{1}{2}\frac{1}{2}^{-}$ and $NJ/\psi$ with $IJ^{P}=\frac{1}{2}\frac{3}{2}^{-}$ are bounded by channels coupling. However, $NJ/\psi$ with $IJ^{P}=\frac{1}{2}\frac{3}{2}^{-}$ may be a resonance state in the $D-$wave $N\eta_{c}$ scattering process. Moreover, $P_{c}(4380)$ can be explained as the molecular pentaquark of $\Sigma^{*}_{c}D$ with quantum numbers $IJ^{P}=\frac{1}{2}\frac{3}{2}^{-}$. The state $\Sigma^{*}_{c}D^{*}$ with $IJ^{P}=\frac{1}{2}\frac{5}{2}^{-}$ is a resonance, it may not be a good candidate of the observed $P_{c}(4450)$ because of the opposite parity of the state to $P_{c}(4380)$, although the mass of the state is not far from the experimental value. In addition, the calculation is extended to the hidden-bottom pentaquarks, the similar properties as that of hidden-charm pentaquarks system are obtained.

Highlights

  • In the past decade, many near-threshold charmoniumlike states have been observed at Belle, BaBar, BESIII, and LHCb, triggering lots of studies on the molecule-like hadrons containing heavy quarks

  • In the heavy quark sector, the large masses of the heavy quarks reduce the kinetic of the system, which makes it easier to form bound states or resonances

  • There is a stable state, the mass of which is lower than the threshold of N J/ψ, and the main channel of this state is N J/ψ, with the ratio of 80.8

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Summary

Introduction

Many near-threshold charmoniumlike states have been observed at Belle, BaBar, BESIII, and LHCb, triggering lots of studies on the molecule-like hadrons containing heavy quarks. Quarks confined in one nucleon are allowed to delocalize to a nearby nucleon and the confinement interaction between quarks in different baryon orbits is modified to include a color screening factor The latter is a model description of the hidden color channel-coupling effect [23]. The resonating-group method (RGM) is employed to study the possible hidden-charm molecular pentaquarks in QDCSM, and the channel-coupling effect are considered. All other parameters are taken from our previous work [31], except for the charm and bottom quark masses mc and mb, which are fixed by a fitting to the masses of the charmed and bottom baryons and mesons. It has been used to explain the cross-over transition between hadron phase and quark–gluon plasma phase [35]

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