One Force -- One Solution principle for the open KPZ equation

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Fix u,v∈Ru,v\in\R. Let h0,h~0∈C⁡([0,1])h_0,\tilde h_0\in\operatorname{C}([0,1]) be arbitrary random functions on the same probability space, and let ξ\xi be white noise on R×[0,1]\mathbb{R}\times[0,1]. Let h(t,x)=h(t,x;t0)h(t,x)=h(t,x;t_0) and h~(t,x)=h~(t,x;t0)\tilde h(t,x)=\tilde h(t,x;t_0) solve the open KPZ equation driven by ξ\xi, started at time t0≤0t_0\leq 0 from h0h_0 and h~0\tilde h_0, respectively. One Force -- One Solution principle. For every real s<s′s<s', the random functions (t,x)↦h(t,x)−h(t,0)(t,x)\mapsto h(t,x)-h(t,0) and (t,x)↦h~(t,x)−h~(t,0)(t,x)\mapsto\tilde h(t,x)-\tilde h(t,0) converge almost surely in C⁡([s,s′];C⁡~([0,1]))\operatorname{C}([s,s'];\widetilde{\operatorname{C}}([0,1])) to the same limit as t0→−∞t_0\to-\infty. This principle is stated as a conjecture for the open KPZ equation; the supplied context gives no resolution status.

References

Primary source

Alisa Knizel and Konstantin Matetski, “The strong Feller property of the open KPZ equation”, arXiv:2211.04466 (2022).

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