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Our investigation accounts for all the $P$-wave intermediate diquark states, {\\it i.e.} $\\langle cc\\rangle[^1P_1]_{\\bar 3}$, $\\langle cc\\rangle[^3P_J]_{6}$, $\\langle bc\\rangle[^1P_1]_{\\bar 3/6}$, $\\langle bc\\rangle[^3P_J]_{\\bar 3/6}$, $\\langle bb\\rangle[^1P_1]_{\\bar 3}$, and $\\langle bb\\rangle[^3P_J]_{6}$ with $J = (0, 1, 2)$. 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