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The C-polynomial of a knot

2 Pith papers cite this work. Polarity classification is still indexing.

2 Pith papers citing it
abstract

In an earlier paper the first author defined a non-commutative A-polynomial for knots in 3-space, using the colored Jones function. The idea is that the colored Jones function of a knot satisfies a non-trivial linear q-difference equation. Said differently, the colored Jones function of a knot is annihilated by a non-zero ideal of the Weyl algebra which is generalted (after localization) by the non-commutative A-polynomial of a knot. In that paper, it was conjectured that this polynomial (which has to do with representations of the quantum group U_q(SL_2)) specializes at q=1 to the better known A-polynomial of a knot, which has to do with genuine SL_2(C) representations of the knot complement. Computing the non-commutative A-polynomial of a knot is a difficult task which so far has been achieved for the two simplest knots. In the present paper, we introduce the C-polynomial of a knot, along with its non-commutative version, and give an explicit computation for all twist knots. In a forthcoming paper, we will use this information to compute the non-commutative A-polynomial of twist knots. Finally, we formulate a number of conjectures relating the A, the C-polynomial and the Alexander polynomial, all confirmed for the class of twist knots.

fields

hep-th 2

years

2026 2

verdicts

UNVERDICTED 2

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representative citing papers

Two roles of Alexander in two Kashaev phases

hep-th · 2026-05-29 · unverdicted · novelty 5.0

Alexander polynomials appear in two opposite roles in two Kashaev phases of Chern-Simons theory due to co-existing branches in the quasiclassical limit with non-trivial versus vanishing classical actions.

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Showing 2 of 2 citing papers after filters.

  • Shading A-polynomials via huge representations of $U_q(\mathfrak{su}_N)$ hep-th · 2026-05-21 · unverdicted · none · ref 15 · internal anchor

    Authors propose shaded A-polynomials A_a(ℓ_b, m_c) for SU(N) via CG chords from huge representations of U_q(su_N) in the classical limit, with examples for knots 3_1, 4_1, 5_1 in su_3.

  • Two roles of Alexander in two Kashaev phases hep-th · 2026-05-29 · unverdicted · none · ref 78 · internal anchor

    Alexander polynomials appear in two opposite roles in two Kashaev phases of Chern-Simons theory due to co-existing branches in the quasiclassical limit with non-trivial versus vanishing classical actions.