Abstract

The strong and radiative decays of the low-lying $\lambda$-mode $D$-wave $\Lambda_{c(b)}$, $\Sigma_{c(b)}$, $\Xi_{c(b)}$, $\Xi_{c(b)}'$, and $\Omega_{c(b)}$ baryons are studied in a constituent quark model. Our calculation shows the following: (i) The missing $\lambda$-mode $D$-wave $\Omega_{c(b)}$, $\Lambda_{b}$, and $\Xi_{b}$ baryons have a relatively narrow decay width of a few MeV or a few tens of MeV and their dominant strong and radiative decay channels can be ideal for searching for their signals in future experiments. (ii) The $\lambda$-mode $1D$-wave excitations in the $\Sigma_{c(b)}$ and $\Xi_{c(b)}'$ families appear to have a relatively broad width of $\sim 50-200$ MeV.Most of the $1D$-wave states have large decay rates into the $1P$-wave heavy baryons via the pionic or kaonic strong decay processes, which should be taken seriously in future observations. (iii) Both $\Lambda_c(2860)$ and $\Xi_c(3050)$ seem to favor the $J^P=3/2^+$ excitation $|^2D_{\lambda\lambda} \frac{3}{2}^+ \rangle$ of $\bar{\mathbf{3}}_F$, while both $\Lambda_c(2880)$ and $\Xi_c(3080)$ may be assigned as the $J^P=5/2^+$ excitation $|^2D_{\lambda\lambda} \frac{5}{2}^+ \rangle$ of $\bar{\mathbf{3}}_F$. The nature of $\Xi_c(3050)$ and $\Xi_c(3080)$ could be tested by the radiative transitions $\Xi_c(3055)^0\to \Xi_c(2790)^0 \gamma$ and $\Xi_c(3080)^0 \to \Xi_c(2815)^0 \gamma$, respectively.

Highlights

  • The LHC facility provides good opportunities for us to discover some of the missing heavy baryons

  • If the mass of jΛb2Dλλ52þi is less than 6200 masses of P-wave heavy baryons (MeV) as predicted in various quark models [21,27], the decays of jΛb2Dλλ52þi may be saturated by the Σbπ and ΣÃbπ channels

  • Strong decay partial widths of the main decay modes for the λ-mode D-wave Σc and Σb baryons, the masses (MeV) of which taken from the quark model predictions of Ref. [21]

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Summary

INTRODUCTION

The LHC facility provides good opportunities for us to discover some of the missing heavy baryons. We apply a nonrelativistic constituent quark model to study the strong decays with emission of one light pseudoscalar meson and the radiative decays with emission of one photon for the low-lying D-wave singly heavy baryons. Since the quark-meson coupling is invariant under the chiral transformation, some of the low-energy properties of QCD are retained [92,93,94] This method (i.e., ChQM) has been successfully applied to study the strong decays of heavy-light mesons and charmed and strange baryons [2,47,48,49,95,96,97,98,99,100].

Spectra
Decays
Λc states
Λb states
Ξc states
Ξb states
RESULTS
SUMMARY

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