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Cyclotomic expansion of generalized Jones polynomials

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Abstract

In (Compos. Math. 152(7): 1333–1384, 2016), Berest and Samuelson proposed a conjecture that the Kauffman bracket skein module of any knot in \(S^3\) carries a natural action of a rank 1 double-affine Hecke algebra \(SH_{q,t_1, t_2}\) depending on 3 parameters \(q, t_1, t_2\). As a consequence, for a knot K satisfying this conjecture, we defined a three-variable polynomial invariant \(J^K_n(q,t_1,t_2)\) generalizing the classical coloured Jones polynomials \(J^K_n(q)\). In this paper, we give explicit formulas and provide a quantum group interpretation for the polynomials \(J^K_n(q,t_1,t_2)\). Our formulas generalize the so-called cyclotomic expansion of the classical Jones polynomials constructed by Habiro (Invent. Math. 171(1): 1–81, 2008) : as in the classical case, they imply the integrality of \(J^K_n(q,t_1,t_2)\) and, in fact, make sense for an arbitrary knot K independent of whether or not it satisfies the conjecture of Berest and Samuelson (Compos. Math. 152(7): 1333–1384, 2016). When one of the Hecke deformation parameters is set to be 1, we show that the coefficients of the (generalized) cyclotomic expansion of \(J^K_n(q,t_1)\) are expressed in terms of Macdonald orthogonal polynomials.

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Notes

  1. By contrast, the polynomials \(J^K_n(q,t_1,t_2)\) cannot be written, in general, as linear combinations of the classical coloured Jones polynomials \(J_n^K(q)\) with coefficients in \({\mathbb {C}}[q^{\pm 1}, t_1^{\pm 1}, t_2^{\pm 1}]\) (cf. Remark 3.4 in Sect. 3.2).

  2. For this reason and also to avoid confusion with terminology of [1] we will keep referring to \(J^K_n(q,t_1,t_2)\) as ‘generalized’ Jones polynomials, even though they are not generalizing the classical Jones polynomials in the same way as other multivariable polynomial knot invariants (arising, for example, from Khovanov homology).

  3. Abusing notation, we denote the extended pairing of nonsymmetric skein modules in the same way as the ‘symmetric’ (topological) one.

  4. The polynomials \(C_n(x;\beta | q)\) are sometimes called the q-ultraspherical (or Rogers) polynomials (cf. [11, Sect. 14.10.1]).

  5. Lawrence’s universal invariants can be defined for more general Lie algebras than \(\mathfrak {sl}_2\) and for more general link-type diagrams (bottom tangles), see [7].

  6. We warn the reader that our q differs from the q in [8]: in fact, the q in [8] equals \(v^2\), which is our \(q^4\).

  7. An (mn)-tangle is a properly embedded 1-manifold in \([0,1]\times [0,1]\) with m endpoints on \(\{0\}\times [0,1]\) and n endpoints on \(\{1\} \times [0,1]\).

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Acknowledgements

We would like to thank I. Cherednik, P. Di Francesco, N. Reshetikhin, and V. Turaev for interesting discussions, questions, and comments. We are especially grateful to G. Felder who clarified to us the structure of cyclotomic coefficients and their role in the Volume Conjecture. The work of the first author (Yu. B.) was partially supported by the NSF grant DMS 1702372 and the 2019 Simons Fellowship both of which are gratefully acknowledged. The work of the third author was partially supported by a Simons Travel Grant and a Simons Collaboration Grant which are also gratefully acknowledged.

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Berest, Y., Gallagher, J. & Samuelson, P. Cyclotomic expansion of generalized Jones polynomials. Lett Math Phys 111, 37 (2021). https://doi.org/10.1007/s11005-021-01373-6

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