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

Fix u,vRu,v\in\R. Let h0,h~0C([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 t00t_0\leq 0 from h0h_0 and h~0\tilde h_0, respectively. One Force -- One Solution principle. For every real s<ss<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 t0t_0\to-\infty. This principle is stated as a conjecture for the open KPZ equation; the supplied context gives no resolution status.

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Primary source

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

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