The complexification of the volume conjecture

From papers

Let HS3\mathscr{H}\subset S^3 be a hyperbolic knot. Define its complex volume by

cv(H)=1Vol(H)2π2CSSO(3)(H),\operatorname{cv}(\mathscr{H})=\sqrt{-1}\operatorname{Vol}(\mathscr{H})-2\pi^2\operatorname{CS}^{\rm{SO(3)}}(\mathscr{H}),

where CSSO(3)(H)\operatorname{CS}^{\rm{SO(3)}}(\mathscr{H}) is the Chern–Simons invariant modulo π2\pi^2. Complexification of the volume conjecture. For any hyperbolic knot H\mathscr{H} in S3S^3,

limNlogJN(H;e2π1/N)N=cv(H)2π1.\lim_{N\to\infty}\frac{\log J_N(\mathscr{H};e^{2\pi\sqrt{-1}/N})}{N}=\frac{\operatorname{cv}(\mathscr{H})}{2\pi\sqrt{-1}}.

This extends the volume conjecture from exponential growth rates involving real volume to a complex asymptotic incorporating the Chern–Simons invariant. Its status is not resolved in the source.

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Sources & referencesView supporting material

Primary source

Hitoshi Murakami, “The asymptotic behaviors of the colored Jones polynomials of the figure eight-knot, and an affine representation”, arXiv:2307.07100 (2023).

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