Heavy baryon spectroscopy in the QCD string model

dc.creatorGrach, I. L.
dc.creatorNarodetskii, I. M.
dc.creatorTrusov, M. A.
dc.creatorVeselov, A. I.
dc.date2008-11-13
dc.date.accessioned2026-07-07T10:18:04Z
dc.date.available2026-07-07T10:18:04Z
dc.descriptionQCD string model formulated in the framework of the Field Correlator Method (FCM) in QCD is employed to calculate the masses of $Σ_c$, $Ξ_c$ and recently observed at Tevatron $Σ_b$, $Ξ_b$ baryons and their orbital excitations. The auxiliary field formalism allows one to write a simple local form of the effective Hamiltonian for the three quark system, which comprises both confinement and relativistic effects, and contains only universal parameters: the string tension $σ$, the strong coupling constant $α_s$, and the bare (current) quark masses $m_i$. We calculate the hyperfine splitting with account of the both perturbative and non--perturbative spin-spin forces between quarks in a baryon. For the orbital excitations we estimate the string correction for the confinement potential - the leading correction to the contribution of the proper inertia of the rotating string. This correction lowers the masses of the P-states by 50 MeV. We find our numerical results to be in good agreement with experimental data.
dc.descriptionContribution at PANIC08, Eilat, Israel, November 2008
dc.identifierhttps://arxiv.org/abs/0811.2184
dc.identifierhttp://arxiv.org/abs/0811.2184
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/174070
dc.subjectHigh Energy Physics - Phenomenology
dc.titleHeavy baryon spectroscopy in the QCD string model
dc.typetext

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