The LQG–SLE mating-map conjecture

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Let κ′∈(4,∞)\kappa'\in(4,\infty) and θ∈[0,2π)\theta\in[0,2\pi). Consider a 16/κ′\sqrt{16/\kappa'}-LQG on a bounded domain decorated by curves η\bm\eta and η′\bm\eta' with parameters κ′\kappa' and 16/κ′16/\kappa', respectively, and angle θ\theta. Define ψκ′,θ\bm\psi_{\kappa',\theta} by

η(t)=η′(ψκ′,θ(t)),t∈[0,1].\bm\eta(t)=\bm\eta'(\bm\psi_{\kappa',\theta}(t)),\qquad t\in[0,1].

Let φZκ′,θ\varphi_{{\bm{\mathscr Z}}_{\kappa',\theta}} be the function constructed from the solution flow of the generalized LQG SDE for different starting times.

LQG–SLE mating-map conjecture. Almost surely,

ψκ′,θ(t)=φZκ′,θ(t),t∈[0,1].\bm\psi_{\kappa',\theta}(t)=\varphi_{{\bm{\mathscr Z}}_{\kappa',\theta}}(t),\qquad t\in[0,1].

This would identify the curve-interaction time change in the LQG–SLE construction with the flow generated by the conjectural SDE, extending the explicitly known special case κ′=12\kappa'=12 and θ=π/2\theta=\pi/2.

References

Primary source

Jacopo Borga, “Random Permutations – A geometric point of view”, arXiv:2107.09699 (2021).

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