Murakami's parametrization of the volume conjecture (J. Topology, 2013; restated as Conjecture 1.6 of arXiv:2312.00350) predicts that for every hyperbolic knot KK the colored Jones polynomial JN(K;e(2πi+u)/N)J_N(K;e^{(2\pi i+u)/N}) has, for uu in a punctured neighborhood of 00, a full leading asymptotic as N→∞N\to\infty whose exponential growth is governed by the potential function SK(u)S_K(u) — recovering the PSL(2;C)\mathrm{PSL}(2;\mathbb{C}) Chern–Simons invariant of the deformed representation ρu\rho_u — and whose prefactor is the homological adjoint Reidemeister torsion TK(ρu)T_K(\rho_u). All rigorous verifications to date concern the figure-eight knot only: most recently for real u>arccosh⁡(3/2)u>\operatorname{arccosh}(3/2) (arXiv:2312.00350, where ρu\rho_u is SL(2;R)\mathrm{SL}(2;\mathbb{R})-valued) and for complex evaluation exponents ξ\xi with 0<Im⁡ξ<π/20<\operatorname{Im}\xi<\pi/2 (arXiv:2602.01049, Feb 2026). The problem is to prove or refute the conjecture for hyperbolic knots other than the figure-eight knot, up to full generality, with the sign convention of the adjoint Reidemeister torsion fixed — a point the source itself leaves unresolved even for the figure-eight knot.

Background

The colored Jones polynomial JN(K;q)J_N(K;q) of a knot K⊂S3K\subset S^3 is the sequence of quantum invariants obtained by evaluating the knot with the NN-dimensional irreducible representation of the quantum group Uq(sl2)U_q(\mathfrak{sl}_2); J2J_2 is the classical Jones polynomial and qq is a complex parameter. Kashaev (1997) introduced an invariant built from the quantum dilogarithm and conjectured that it grows exponentially in NN at a rate given by the hyperbolic volume of the knot complement; Murakami and Murakami (2001) identified Kashaev's invariant with JN(K;e2πi/N)J_N(K;e^{2\pi i/N}) and formulated the Volume Conjecture: for any knot KK,

lim⁡N→∞2πNlog⁡∣JN(K;e2πi/N)∣=Vol⁡(S3∖K),\lim_{N\to\infty}\frac{2\pi}{N}\log\left|J_N\left(K;e^{2\pi i/N}\right)\right|=\operatorname{Vol}(S^3\setminus K),

where Vol⁡\operatorname{Vol} is the simplicial volume. A knot is hyperbolic when its complement carries a complete hyperbolic metric of finite volume; by Mostow rigidity this metric is unique, so the hyperbolic volume of the complement is a topological invariant, and for hyperbolic KK it coincides with the simplicial volume on the right-hand side. Dropping the absolute value gives a complex limit, conjectured by Murakami–Murakami–Okamoto–Takata–Yokota (2002) to equal the complex volume Vol⁡(K)+i CSSO(3)(K)\operatorname{Vol}(K)+i\,\mathrm{CS}^{\mathrm{SO}(3)}(K), where the Chern–Simons invariant is the secondary invariant of the Levi-Civita connection of the hyperbolic structure (the integral of the Chern–Simons 3-form over the complement, defined modulo 4π24\pi^2). A finer refinement, developed by Gukov, by Dimofte–Gukov–Lenells–Zagier, and by Gukov–Murakami, predicts the subleading prefactor of the asymptotics in terms of the adjoint Reidemeister torsion TK(ρ)T_K(\rho) — the Whitehead torsion of the cochain complex of S3∖KS^3\setminus K with coefficients twisted by Ad⁡∘ρ\operatorname{Ad}\circ\rho for a flat SL(2;C)\mathrm{SL}(2;\mathbb{C}) connection ρ\rho, a classical secondary invariant measuring the homological size of the flat connection.

Murakami (Journal of Topology, 2013) proposed the parametrized version: one perturbs the evaluation point 2πi2\pi i by a complex number uu and studies JN(K;eξ/N)J_N(K;e^{\xi/N}), where ξ:=u+2pπi\xi:=u+2p\pi i is the exponent of the evaluation point at winding pp, so that u=ξ−2pπiu=\xi-2p\pi i is the deformation parameter; the unperturbed point is p=1p=1, u=0u=0, i.e. ξ=2πi\xi=2\pi i, while the p=0p=0 case is ξ=u\xi=u. Let (μ,λ)(\mu,\lambda) be the standard meridian/longitude pair of KK, and let ρu:π1(S3∖K)→SL(2;C)\rho_u:\pi_1(S^3\setminus K)\to\mathrm{SL}(2;\mathbb{C}) be the irreducible representation — deforming the holonomy representation for small ∣u∣|u| — under which the meridian has eigenvalues e±u/2e^{\pm u/2} and the longitude has eigenvalues −e±v(u)/2-e^{\pm v(u)/2} for a companion function v(u)v(u). The conjecture predicts a complete leading asymptotic combining three classical ingredients: a potential function SK(u)S_K(u) (a Neumann–Zagier-type potential encoding the complex volume of the deformed structure), the homological adjoint Reidemeister torsion TK(ρu)T_K(\rho_u) in Porti's normalization with the meridian as homology basis, and the PSL(2;C)\mathrm{PSL}(2;\mathbb{C}) Chern–Simons invariant; the precise formula is stated in the problem statement. Physically this is the predicted semiclassical asymptotics of SL(2;C)\mathrm{SL}(2;\mathbb{C}) complex Chern–Simons theory, of which the colored Jones polynomial (the SU(2)\mathrm{SU}(2) theory) at the perturbed coupling is expected to be a sector.

The conjecture is proved only for the figure-eight knot 414_1, in the regimes examined so far: the logarithmic limit for small ∣u∣|u| (Murakami–Yokota 2007); the full formula for small ∣u∣|u| with nonzero winding pp, i.e. evaluation at ξ=u+2pπi\xi=u+2p\pi i (Murakami 2013); the boundary value u=κ=arccosh⁡(3/2)u=\kappa=\operatorname{arccosh}(3/2), where the representation degenerates to the parabolic one (Murakami, Algebraic & Geometric Topology 2025; polynomial growth at p=0p=0 was known from Hikami–Murakami 2008); real u>κu>\kappa with p=0p=0 (Murakami–Tran 2025) and with integer p≥1p\ge 1 (Murakami, arXiv:2312.00350, where ρu\rho_u is SL(2;R)\mathrm{SL}(2;\mathbb{R})-valued and the formula acquires an additional multiplicative factor Jp(E;e4Nπ2/ξ)J_p(\mathscr{E};e^{4N\pi^2/\xi})); the unperturbed point ξ=2πi\xi=2\pi i (Andersen–Hansen 2006); and complex ξ\xi with 0<Im⁡ξ<π/20<\operatorname{Im}\xi<\pi/2 on the p=0p=0 case of the parametrization, where ξ=u\xi=u (Murakami, arXiv:2602.01049). For hyperbolic knots other than 414_1 only the single-point refinement at the unperturbed evaluation ξ=2πi\xi=2\pi i (torsion and Chern–Simons at that one point) is known, for knots with at most seven crossings (Andersen–Hansen for 414_1; Ohtsuki for 525_2 and the seven-crossing knots; Ohtsuki–Yokota for 61,62,636_1,6_2,6_3), plus the ordinary volume conjecture (leading exponential rate only, no torsion or Chern–Simons prefactor) for some special families such as torus knots, twist knots, and double twist knots. Garoufalidis and Lê (2011) proved that for any knot JN(K;eu/N)→1/Δ(K;eu)J_N(K;e^{u/N})\to 1/\Delta(K;e^u) for uu near 00, where Δ\Delta is the Alexander polynomial, so the exponential growth concentrates on the 2πi2\pi i-sheets that the conjecture addresses. No verification of the parametrized conjecture — the full formula with torsion and Chern–Simons as functions of the deformation parameter uu — exists for any hyperbolic knot other than 414_1.

Problem Statement

Prove or refute the parametrization of the volume conjecture for hyperbolic knots other than the figure-eight knot. The conjecture (Murakami, J. Topology 6 (2013), 193–216; restated as Conjecture 1.6 of arXiv:2312.00350) asserts: for a hyperbolic knot KK, there exists a neighborhood UU of 00 in C\mathbb{C} such that for u∈U∖πiQu\in U\setminus\pi i\mathbb{Q},

JN(K;e(2πi+u)/N) ∼N→∞ −π2sinh⁡(u/2) TK(ρu)−1/2(N2πi+u)1/2exp⁡(SK(u)2πi+u N),J_N\left(K;e^{(2\pi i+u)/N}\right)\ \underset{N\to\infty}{\sim}\ \frac{\sqrt{-\pi}}{2\sinh(u/2)}\,T_K(\rho_u)^{-1/2}\left(\frac{N}{2\pi i+u}\right)^{1/2}\exp\left(\frac{S_K(u)}{2\pi i+u}\,N\right),

where ρu\rho_u is the irreducible SL(2;C)\mathrm{SL}(2;\mathbb{C}) representation of π1(S3∖K)\pi_1(S^3\setminus K) with meridian eigenvalues e±u/2e^{\pm u/2}, deforming the holonomy representation for small ∣u∣|u|; TK(ρu)T_K(\rho_u) is the homological adjoint Reidemeister torsion in Porti's normalization (meridian as homology generator); SK(u)S_K(u) is the potential function, from which the Chern–Simons invariant is recovered as CSu,v(u)(ρu)=SK(u)−uπi−u v(u)/4\mathrm{CS}_{u,v(u)}(\rho_u)=S_K(u)-u\pi i-u\,v(u)/4 with v(u)=2 dduSK(u)−2πiv(u)=2\,\frac{d}{du}S_K(u)-2\pi i.

Since the figure-eight knot case is settled in the regimes listed in the background, the open content is the conjecture for every hyperbolic knot other than the figure-eight knot, up to and including a proof for all hyperbolic knots; a proof for any single further knot or family would be partial progress rather than a full resolution. Any resolution must in particular fix the sign convention under which TK(ρu)T_K(\rho_u) enters the formula: the homological adjoint Reidemeister torsion is defined only up to an overall sign, and even the figure-eight identification in arXiv:2312.00350 is stated only 'up to a sign' (following Porti). A resolution by counterexample must exhibit a specific hyperbolic knot KK and admissible parameters un→0u_n\to0 (with each ρun\rho_{u_n} irreducible and μ\mu-regular in the sense of Porti, that is, regular with respect to the meridian so that the meridian-based torsion TK(ρun)T_K(\rho_{u_n}) is defined) along which the asymptotic formula provably fails; equivalently, it must show that no neighborhood UU of 00 satisfies the conjecture. Because the conjecture asserts the existence of UU, failure at admissible parameters that do not accumulate at 00 is not a refutation: a smaller neighborhood can exclude them.

References

  1. Hitoshi Murakami, The colored Jones polynomial of the figure-eight knot and an SL(2;R)-representation, arXiv:2312.00350 (2023). DOI: 10.48550/arXiv.2312.00350, https://arxiv.org/abs/2312.00350
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