Superpolynomials for toric knots from evolution induced by cut-and-join operators
P. Dunin-Barkowski, A. Mironov, A. Morozov, A. Sleptsov, A. Smirnov
TL;DR
This work presents a streamlined, MacDonald-polynomial–based evolution for torus knot superpolynomials, derived by deforming the split W-representation of HOMFLY polynomials via a cut-and-join operator. By replacing Schur characters with MacDonald dimensions and refining expansion coefficients, the authors obtain explicit superpolynomials for arbitrary representations and many torus knots, including new results like P_{[1]}^{[m,km±1]}. The approach extends to non-torus knots and offers multiple reductions, such as Alexander and Heegaard–Floer polynomials, with Catalan-number connections in special limits. The framework emphasizes positivity of coefficients in the MacDonald-parameterization, though acknowledges subtleties around unknot choices and non-fundamental representations, suggesting a deep link to Khovanov–Rozhansky homologies and related algebraic structures. Overall, the paper provides a practical recursive scheme for computing torus-knot superpolynomials and highlights rich connections to matrix models, Hurwitz theory, and combinatorial path models.
Abstract
The colored HOMFLY polynomials, which describe Wilson loop averages in Chern-Simons theory, possess an especially simple representation for torus knots, which begins from quantum R-matrix and ends up with a trivially-looking split W representation familiar from character calculus applications to matrix models and Hurwitz theory. Substitution of MacDonald polynomials for characters in these formulas provides a very simple description of "superpolynomials", much simpler than the recently studied alternative which deforms relation to the WZNW theory and explicitly involves the Littlewood-Richardson coefficients. A lot of explicit expressions are presented for different representations (Young diagrams), many of them new. In particular, we provide the superpolynomial P_[1]^[m,km\pm 1] for arbitrary m and k. The procedure is not restricted to the fundamental (all antisymmetric) representations and the torus knots, still in these cases some subtleties persist.
