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Infinite-dimensional nonlinear stationary Fokker-Planck-Kolmogorov equations

Vladimir I. Bogachev, Michael Röckner, Stanislav V. Shaposhnikov

TL;DR

The paper develops existence results for nonlinear stationary Fokker-Planck-Kolmogorov equations in infinite-dimensional settings driven by a Gaussian measure. It treats drift fields of the form $b(p,x)=-x+v(p,x)$ with $v$ bounded in the Cameron–Martin space and continuous in the density variable, constructing solutions as densities in $L^2(\gamma)$ via a Schauder fixed-point argument on the map $p\mapsto\varrho_p$, where $\varrho_p$ solves the corresponding linear equation. The authors extend the framework to Vlasov-type drifts, address parameter dependence with measurable selections, and discuss cases with unbounded components of $v$ under stronger continuity assumptions. The approach yields rigorous existence results and a robust method for handling nonlinear infinite-dimensional FPK equations relevant to statistical mechanics and stochastic analysis on function spaces.

Abstract

We prove existence of a probability solution to the nonlinear stationary Fokker-Planck-Kolmogorov equation on an infinite dimensional space with a centered Gaussian measure $γ$ with a unit diffusion operator and a drift of the form $-x+v(p,x)$, where $v$ is a bounded mapping with values in the Cameron-Martin space $H$ of $γ$ and $v$ is defined on the space $E\times X$, where is $E$ is the subset of $L^2(γ)$ consisting of probability densities. The equation has the form $L_{b(p,\bullet)} ^*(p\cdot γ)=0$ with $L_{b(p,\bullet)}\varphi =Δ_H \varphi + (b(p,\bullet) , D_{_H}\varphi)_{_H}$, so that the drift coefficient depends on the unknown solution, which makes the equation nonlinear. This dependence is assumed to satisfy a suitable continuity condition. This result is applied to drifts of Vlasov type defined by means of the convolution of a vector field with the solution. In addition, we consider a more general situation where only the components of $v$ are uniformly bounded and prove the existence of a probability solution under some stronger continuity condition on the drift.

Infinite-dimensional nonlinear stationary Fokker-Planck-Kolmogorov equations

TL;DR

The paper develops existence results for nonlinear stationary Fokker-Planck-Kolmogorov equations in infinite-dimensional settings driven by a Gaussian measure. It treats drift fields of the form with bounded in the Cameron–Martin space and continuous in the density variable, constructing solutions as densities in via a Schauder fixed-point argument on the map , where solves the corresponding linear equation. The authors extend the framework to Vlasov-type drifts, address parameter dependence with measurable selections, and discuss cases with unbounded components of under stronger continuity assumptions. The approach yields rigorous existence results and a robust method for handling nonlinear infinite-dimensional FPK equations relevant to statistical mechanics and stochastic analysis on function spaces.

Abstract

We prove existence of a probability solution to the nonlinear stationary Fokker-Planck-Kolmogorov equation on an infinite dimensional space with a centered Gaussian measure with a unit diffusion operator and a drift of the form , where is a bounded mapping with values in the Cameron-Martin space of and is defined on the space , where is is the subset of consisting of probability densities. The equation has the form with , so that the drift coefficient depends on the unknown solution, which makes the equation nonlinear. This dependence is assumed to satisfy a suitable continuity condition. This result is applied to drifts of Vlasov type defined by means of the convolution of a vector field with the solution. In addition, we consider a more general situation where only the components of are uniformly bounded and prove the existence of a probability solution under some stronger continuity condition on the drift.

Paper Structure

This paper contains 3 sections, 4 theorems, 57 equations.

Key Result

Theorem 2.1

Let $\mu$ be a Borel probability measure on $X$ such that $|v|_{_H}\in L^1(\mu)$ and $L_b^*\mu=0$ with respect to $\mathcal{F}\mathcal{C}_{0,\{e_n\}}$, where $b(x)=-x+v(x)$. Then $\mu$ is absolutely continuous with respect to $\gamma$ and for its Radon--Nikodym $f:=d\mu/d\gamma$ we have for every $\alpha<1/4$, where $C(\alpha)$ is a number depending only on $\alpha$.

Theorems & Definitions (8)

  • Theorem 2.1
  • Theorem 3.1
  • proof
  • Example 3.2
  • Proposition 3.3
  • proof
  • Theorem 3.4
  • proof