2012/03/31 by H. Itoyama, А. Миронов, A. Mironov +3 · 2 citations
Mathematics · Physics and Astronomy · #Advanced Algebra and Geometry #Algebra over a field #Algebraic structures and combinatorial models #Antisymmetric relation #Combinatorics #Geometric and Algebraic Topology #HOMFLY polynomial #Knot (papermaking) #Mathematical analysis #Mathematical physics #Mathematics #Matrix polynomial #Polynomial #Pure mathematics #hep-th #math.GT #math.QA
paper · pdf · doi:10.1007/jhep07(2012)131
published as Journal of High Energy Physics Volume 2012, Number 7 (2012), 131 · 14 pages
arxiv created 2012/06/12 · openalex publication_date 2012/07/01 · arxiv updated 2012/08/01 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
Explicit answer is given for the HOMFLY polynomial of the figure eight knot 41 in arbitrary symmetric representation R=[p]. It generalizes the old answers for p=1 and 2 and the recently derived results for p=3,4, which are fully consistent with the Ooguri-Vafa conjecture. The answer can be considered as a quantization of the σR = σ[1]|R| identity for the "special" polynomials (they define the leading asymptotics of HOMFLY at q=1), and arises in a form, convenient for comparison with the representation of the Jones polynomials as sums of dilogarithm ratios. In particular, we construct a difference equation ("non-commutative A-polynomial") in the representation variable p. Simple symmetry transformation provides also a formula for arbitrary antisymmetric (fundamental) representation R=[1p], which also passes some obvious checks. Also straightforward is a deformation from HOMFLY to superpolynomials. Further generalizations seem possible to arbitrary Young diagrams R, but these expressions are harder to test because of the lack of alternative results, even partial.