Abstract
We construct an effective hadronic model including single heavy baryons (SHBs) belonging to the $(\mathbf{3},\mathbf{3})$ representation under $\mbox{SU}(3)_L \times \mbox{SU}(3)_R$ symmetry, respecting the chiral symmetry and heavy-qaurk spin-flavor symmetry. When the chiral symmetry is spontaneously broken, the SHBs are divided into the baryons with negative parity of $\bar{\mathbf 3}$ representation under $\mbox{SU}(3)$ flavor symmetry which is the chiral partners to the ones with positive parity of ${\mathbf 6}$ representation. We determine the model parameters from the available experimental data for the masses and strong decay widths of $\Sigma_c^{(\ast)}$, $\Lambda_c (2595)$, $\Xi_c (2790)$, and $\Xi_c (2815)$. Then, we predict the masses and strong decay widths of other baryons including $\Xi_b$ with negative parity. We also study radiative decays of SHBs including $\Omega_c^\ast$ and $\Omega_b^\ast$ with positive parity.
Highlights
The spontaneous chiral symmetry breaking, which is one of the most essential properties of QCD, is expected to generate a part of hadron masses and causes the mass difference between chiral partners
There, we considered the chiral partners of ΣQ (Q 1⁄4 c, b) baryons with positive parity as ΛQ baryons with negative parity: a heavy-quark doublet of (Λcð2595; JP 1⁄4 1=2−Þ, Λcð2625; 3=2−Þ) is regarded as the chiral partners to the doublet of (Σcð2455; 1=2þÞ, Σcð2520; 3=2þÞ), and (Λbð5912; 1=2−Þ, Λbð5920; 3=2−Þ) to (Σbð1=2þÞ, ΣÃbð3=2þÞ)
We study the radiative decays of singly heavy baryons (SHBs) in Sec
Summary
The spontaneous chiral symmetry breaking, which is one of the most essential properties of QCD, is expected to generate a part of hadron masses and causes the mass difference between chiral partners. There are several studies of hadrons including heavy quarks based on the chiral partner structure. The chiral partner structure of heavy-light mesons is studied in, e.g., Refs. [12], we proposed a new chiral partner structure for SHBs including a heavy quark and two light quarks. There, we considered the chiral partners of ΣQ (Q 1⁄4 c, b) baryons with positive parity as ΛQ baryons with negative parity: a heavy-quark doublet of (Λcð2595; JP 1⁄4 1=2−Þ, Λcð2625; 3=2−Þ) is regarded as the chiral partners to the doublet of (Σcð2455; 1=2þÞ, Σcð2520; 3=2þÞ), and (Λbð5912; 1=2−Þ, Λbð5920; 3=2−Þ) to (Σbð1=2þÞ, ΣÃbð3=2þÞ) Based on this structure, we predicted the pionic.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.