Exploring the spectrum of the hidden charm strange pentaquark in an SU(4) flavor-spin model

Abstract

We study the spectrum of the isoscalar pentaquark $udsc\overline{c}$, of either positive or negative parity, in a constituent quark model with linear confinement and a flavor-spin hyperfine interaction previously extended to SU(4) and used to describe the spectrum of the $uudc\overline{c}$ pentaquarks observed at LHCb in 2019. For positive parity we make a distinction between the case where one unit of angular momentum is located in the subsystem of four quarks and the case where the angular momentum is located in the relative motion between a ground state four-quark subsystem and the antiquark. The novelty is that we introduce the coupling between different flavor states, due to the breaking of exact SU(4)-flavor symmetry of the Hamiltonian model, both for positive and negative parity states. An important consequence is that the lowest state, located at 4404 MeV, has quantum numbers $J^P$ = $1/2^{-}$ while without coupling the lowest state has $J^P$ = $1/2^{+}$ or $3/2^{+}$.

arXiv comment26 pages, title slightly changed, other minor changes, it matches the published version. arXiv admin note: text overlap with arXiv:1902.07101

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• The $P_{cs}(4459)$ pentaquark from a combined effective field theory and phenomenological perspective
• Predicting the ${\bar{D}}_s^{(\ast )}{D}_s^{(\ast )}$ bound states as the partners of $X(3872)$
• Spin-parities of the $P_c(4440)$ and $P_c(4457)$ in the One-Boson-Exchange Model
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• Relations between strong decay widths of the $P_c$ pentaquarks in the SU(4) flavor-spin model
• Molecular $P_{\psi }$ pentaquarks from light-meson exchange saturation