The LQG–SLE mating-map conjecture

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/κ16/\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.

Sources & referencesView supporting material

Primary source

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

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