The complexification of the volume conjecture

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Let H⊂S3\mathscr{H}\subset S^3 be a hyperbolic knot. Define its complex volume by

cv⁡(H)=−1Vol⁡(H)−2π2CS⁡SO(3)(H),\operatorname{cv}(\mathscr{H})=\sqrt{-1}\operatorname{Vol}(\mathscr{H})-2\pi^2\operatorname{CS}^{\rm{SO(3)}}(\mathscr{H}),

where CS⁡SO(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,

lim⁡N→∞log⁡JN(H;e2π−1/N)N=cv⁡(H)2π−1.\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.

References

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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