Abstract

If a knot is represented by an m-strand braid, then HOMFLY polynomial in representation R is a sum over characters in all representations Q\in R^{\otimes m}. Coefficients in this sum are traces of products of quantum R-matrices along the braid, but these matrices act in the space of intertwiners, and their size is equal to the multiplicity M_{RQ} of Q in R^{\otimes m}. If R is the fundamental representation R=[1], then M_{[1] Q} is equal to the number of paths in representation graph, which lead from the fundamental vertex [1] to the vertex Q. In the basis of paths the entries of the m-1 relevant R-matrices are associated with the pairs of paths and are non-vanishing only when the two paths either coincide or differ by at most one vertex; as a corollary R-matrices consist of just 1x1 and 2x2 blocks, given by very simple explicit expressions. If cabling method is used to color the knot with the representation R, then the braid has m|R| strands, Q have a bigger size m|R|, but only paths passing through the vertex R are included into the sums over paths which define the products and traces of the m|R|-1 relevant R-matrices. In the case of SU(N) this path sum formula can also be interpreted as a multiple sum over the standard Young tableaux. By now it provides the most effective way for evaluation of the colored HOMFLY polynomials, conventional or extended, for arbitrary braids.

Highlights

  • Knot polynomials are currently among the central objects of interest in quantum field theory; they are exactly at the border between the known and unknown

  • They depend on a closed contour K in a three dimensional manifold M, on the representation R of the gauge group G = SU(N) and on the coupling constant q = e2πi/(k+N)

  • In formula (7) the knot and group dependencies are separated and one can consider HR as a function of A = qN rather than N; the parameter N enters only the quantum dimensions χQ and can be substituted by A. This formula introduces the extended HOMFLY polynomial HR{p}, if χQ are interpreted as characters, which are functions of infinitely many timevariables {pk} instead of N or A [70, 85]

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Summary

Introduction

Knot polynomials are currently among the central objects of interest in quantum field theory; they are exactly at the border between the known and unknown. Advances in High Energy Physics [22,23,24,25,26,27,28,29,30,31,32] are connected to the S-duality between the N = 2 supersymmetric Yang-Mills theories [33,34,35,36,37,38,39,40,41,42,43,44] This makes the study of knot polynomials the task after the structure of conformal blocks themselves more or less understood in terms of the Dotsenko-Fateev matrix models [45,46,47,48,49,50,51,52,53,54,55] and other similar representations [56, 57]. The goal of this letter is to summarize the results of our method [70, 85,86,87], which provides a complete, nice, and practically efficient solution to this problem

HOMFLY Polynomials via Quantum R-Matrices
R-Matrices via Paths in the Representation Graph
Examples
Cabling Method
Open Questions
Full Text
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