{ "id": "2405.19039", "version": "v1", "published": "2024-05-29T12:26:54.000Z", "updated": "2024-05-29T12:26:54.000Z", "title": "Heavy baryons in the relativized quark model with chromodynamics", "authors": [ "Xin-Zhen Weng", "Wei-Zhen Deng", "Shi-Lin Zhu" ], "comment": "20 pages, 10 figures", "categories": [ "hep-ph", "hep-ex", "hep-lat" ], "abstract": "Following the work of Capstick and Isgur [\\href{https://doi.org/10.1103/PhysRevD.34.2809}{Phys.~Rev.~D~34,~2809~(1986)}], we systematically study the mass spectrum of the heavy baryons in the relativized quark potential model with chromodynamics. Besides the original Godfrey-Isgur (GI) model, we also adopt a modified GI model which replaces the linear confinement by a screened one. The two models give similar results in our work. All heavy baryons observed so far can be explained as three-quark states. In particular, we identify the $\\Omega_{c}(3000)$/$\\Omega_{b}(6316)$, $\\Omega_{c}(3050)$/$\\Omega_{b}(6330)$, $\\Omega_{c}(3065)$/$\\Omega_{b}(6340)$ and $\\Omega_{c}(3090)$/$\\Omega_{b}(6350)$ states as the $p_{\\lambda}$ excitations with quantum numbers $1/2^{-}$, $3/2^{-}$, $3/2^{-}$ and $5/2^{-}$. The $\\Omega_{c}(3120)$ is a $3/2^{-}$ state with the $p_{\\rho}$ excitation, whose bottom partner is predicted to be $\\Omega_{b}(6446/6457,3/2^{-})$. The higher state $\\Omega_{c}(3188)$ is the $2s_{\\lambda}$ excitation with quantum numbers $1/2^{+}$, and $\\Omega_{c}(3327)$ is a $d_{\\lambda}$ excitation with quantum numbers $3/2^{+}$ or $5/2^{+}$. In addition, the $\\Lambda_{c}(2940)$ with quantum numbers $J^{P}=3/2^{-}$ could be explained as the $p_{\\rho}$ excitation.", "revisions": [ { "version": "v1", "updated": "2024-05-29T12:26:54.000Z" } ], "analyses": { "keywords": [ "heavy baryons", "relativized quark model", "quantum numbers", "chromodynamics", "excitation" ], "note": { "typesetting": "TeX", "pages": 20, "language": "en", "license": "arXiv", "status": "editable" } } }