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The ergodic theory of SPDEs in a weak-noise regime

Mathew Joseph, Davar Khoshnevisan, Kunwoo Kim, Carl Mueller

Abstract

Consider a parabolic SPDE \[ \partial_t u = Δu + σ(u)η, \] on $(0\,,\infty)\times\mathbb{R}^d$, where $η$ is a centered, generalized Gaussian noise with $\text{Cov}[η(t\,,x)\,,η(s\,,y)]=δ_0(t-s)Λ(x-y)$ for a tempered Borel measure $Λ$ that is positive definite and satisfies a mild weak-noise. The existence of invariant measures of versions of these types of SPDEs has been studied at great length, particularly in the ``weak-noise regime''; see for example Assing and Manthey \cite{AssingManthey2003}, Chen and Eisenberg \cite{ChenEisenberg2024}, Chen, Ouyang, Tindel, and Xia \cite{ChenOuyangTindelXia2024}, Eckmann and Hairer \cite{EckmannHairer2001}, Misiats and Stanzhytskyi \cite{MSY2020}, Yu Gu and Jiawei Li \cite{GuLi2020}, and Tessitore and Zabczyk \cite{TessitoreZabczyk1998}. Here, we characterize all annealed, ergodic, invariant measures for the above SPDE in the weak-noise regime.

The ergodic theory of SPDEs in a weak-noise regime

Abstract

Consider a parabolic SPDE on , where is a centered, generalized Gaussian noise with for a tempered Borel measure that is positive definite and satisfies a mild weak-noise. The existence of invariant measures of versions of these types of SPDEs has been studied at great length, particularly in the ``weak-noise regime''; see for example Assing and Manthey \cite{AssingManthey2003}, Chen and Eisenberg \cite{ChenEisenberg2024}, Chen, Ouyang, Tindel, and Xia \cite{ChenOuyangTindelXia2024}, Eckmann and Hairer \cite{EckmannHairer2001}, Misiats and Stanzhytskyi \cite{MSY2020}, Yu Gu and Jiawei Li \cite{GuLi2020}, and Tessitore and Zabczyk \cite{TessitoreZabczyk1998}. Here, we characterize all annealed, ergodic, invariant measures for the above SPDE in the weak-noise regime.
Paper Structure (15 sections, 25 theorems, 228 equations)

This paper contains 15 sections, 25 theorems, 228 equations.

Key Result

Corollary 1.2

Choose and fix an arbitrary $\theta\in\mathbb{R}$. Then, $\nu_\theta$ is the only mean-$\theta$ time-ergodic invariant measure among all laws of spatially stationary, spatially ergodic random fields should there be any.

Theorems & Definitions (56)

  • Corollary 1.2
  • Conjecture 1
  • Conjecture 2
  • Definition 2.1
  • Proposition 2.2
  • Lemma 2.3
  • Remark 2.4
  • proof
  • Lemma 2.5
  • proof
  • ...and 46 more