We study compact hidden charm pentaquarks in the Born–Oppenheimer approximation, previously introduced for tetraquarks, assuming the heavy pair to be in a color octet. We show that Fermi statistics applied to the complex of the three light quarks, also in color octet, requires S-wave pentaquark ground states to consist of three octets of flavour-SU(3)f\documentclass[12pt]{minimal}
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\begin{document}$$_f$$\end{document}, two with spin 1/2 and one with spin 3/2, in line with the observed, strangeness S=0,-1\documentclass[12pt]{minimal}
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\begin{document}$$S=0,-1$$\end{document}, spectrum. Additional lines corresponding to decays into J/ψ+Σ\documentclass[12pt]{minimal}
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\begin{document}$$J/\psi +\Xi $$\end{document} are predicted. In the language of non-relativistic SU(6), ground state pentaquarks form either a 56\documentclass[12pt]{minimal}
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\begin{document}$${\varvec{56}}$$\end{document} or a 20\documentclass[12pt]{minimal}
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\begin{document}$${\varvec{20}}$$\end{document} representation, distinguished by presence or absence of pentaquarks decaying in the spin 3/2 decuplet, e.g. in J/ψ+Δ++\documentclass[12pt]{minimal}
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\begin{document}$$J/\psi +\Delta ^{++}$$\end{document}. Observation of a strangeness S=-2\documentclass[12pt]{minimal}
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\begin{document}$$S=-2$$\end{document} or isospin I=3/2\documentclass[12pt]{minimal}
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\begin{document}$$I=3/2$$\end{document} pentaquarks would be a clear signature of compact, QCD bound pentaquarks.
