The channel conjugation symmetry for the six-parameter solution

Let {dϕ(α)}\{d_\phi(\alpha)\} be a solution of the six-parameter channel equation, and let ϕˉ\bar\phi denote the channel obtained by switching every upper assignment UU with the lower assignment LL and vice versa.

Channel conjugation symmetry. The transformed coefficients

dϕ(α)=α3dϕˉ(α1)d'_\phi(\alpha)=\alpha^3d_{\bar\phi}(\alpha^{-1})

form another solution. This is a symmetry of the explicitly studied six-parameter solution space, rather than a new global assertion about all Jack Littlewood–Richardson coefficients; the source presents it as a conjectural relation in its redundancy discussion.

Sources & referencesView supporting material

Primary source

Ryan Mickler, “The Stanley Conjecture Revisited”, arXiv:2401.01582 (2025).

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