In this paper, a multiorbital generalization of standard spin fluctuation theory is considered within an on-site approximation. For f electrons, this theory leads to an instability for a superconducting pair state which obeys Hund's rules, with L=5, S=1, and J=4. The degeneracy of this state is broken by crystalline effects, and realistic calculations for UPt₃ find a pair state with Γ₆^- (E₂ᵤ) symmetry, consistent with current experimental constraints.
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M. R. Norman (1994) studied this question.
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