\begin{document}$ J^P=\frac{1}{2}^\pm, \frac{3}{2}^\pm, \frac{5}{2}^\pm$\end{document} and \begin{document}$ \frac{7}{2}^+$\end{document} are reported. We compare the results with those obtained by the other theoretical formalisms. There is a general agreement for the mass of the ground state in each sector of triply heavy baryons. However, the situation is more puzzling for the excited states, and appropriate comments about the most relevant features of our comparison are given."> Triply heavy baryons in the constituent quark model -
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