Variational structures for the Fokker–Planck equation with general Dirichlet boundary conditions

We prove the convergence of a modified Jordan-Kinderlehrer-Otto scheme to a solution to the Fokker-Planck equation in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>Ω</mml:mi> <mml:mo>⋐</mml:mo> <mml:msup><mml:mrow><mml:mi>R</mml:mi></mml:mrow> <mml:mi>d</mml:mi></mml:msup> </mml:mrow> </mml:math> with general-strictly positive and temporally constant-Dirichlet boundary conditions. We work under mild assumptions on the domain, the drift, and the initial datum. In the special case where <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>Ω</mml:mi></mml:math> is an interval in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>R</mml:mi></mml:mrow> <mml:mn>1</mml:mn></mml:msup> </mml:math> , we prove that such a solution is a gradient flow-curve of maximal slope-within a suitable space of measures, endowed with a modified Wasserstein distance. Our discrete scheme and modified distance draw inspiration from contributions by A. Figalli and N. Gigli [J. Math. Pures Appl. 94, (2010), pp. 107-130], and J. Morales [J. Math. Pures Appl. 112, (2018), pp. 41-88] on an optimal-transport approach to evolution equations with Dirichlet boundary conditions. Similarly to these works, we allow the mass to flow from/to the boundary <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>∂</mml:mi> <mml:mi>Ω</mml:mi></mml:mrow> </mml:math> throughout the evolution. However, our leading idea is to also keep track of the mass at the boundary by working with measures defined on the whole closure <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mover><mml:mi>Ω</mml:mi> <mml:mo>¯</mml:mo></mml:mover> </mml:math> . The driving functional is a modification of the classical relative entropy that also makes use of the information at the boundary. As an intermediate result, when <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>Ω</mml:mi></mml:math> is an interval in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>R</mml:mi></mml:mrow> <mml:mn>1</mml:mn></mml:msup> </mml:math> , we find a formula for the descending slope of this geodesically nonconvex functional.

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Journal
Calculus of Variations and Partial Differential Equations
Published
2025-12-06
DOI
https://doi.org/10.1007/s00526-025-03193-1
Primary Topic
Gas Dynamics and Kinetic Theory
Type
article
Field-Weighted Citation Impact
0.00

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article

Variational structures for the Fokker–Planck equation with general Dirichlet boundary conditions

Filippo Quattrocchi
Calculus of Variations and Partial Differential Equations
Gas Dynamics and Kinetic Theory
article

Variational structures for the Fokker–Planck equation with general Dirichlet boundary conditions

Filippo Quattrocchi
article en

Abstract

We prove the convergence of a modified Jordan-Kinderlehrer-Otto scheme to a solution to the Fokker-Planck equation in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>Ω</mml:mi> <mml:mo>⋐</mml:mo> <mml:msup><mml:mrow><mml:mi>R</mml:mi></mml:mrow> <mml:mi>d</mml:mi></mml:msup> </mml:mrow> </mml:math> with general-strictly positive and temporally constant-Dirichlet boundary conditions. We work under mild assumptions on the domain, the drift, and the initial datum. In the special case where <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>Ω</mml:mi></mml:math> is an interval in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>R</mml:mi></mml:mrow> <mml:mn>1</mml:mn></mml:msup> </mml:math> , we prove that such a solution is a gradient flow-curve of maximal slope-within a suitable space of measures, endowed with a modified Wasserstein distance. Our discrete scheme and modified distance draw inspiration from contributions by A. Figalli and N. Gigli [J. Math. Pures Appl. 94, (2010), pp. 107-130], and J. Morales [J. Math. Pures Appl. 112, (2018), pp. 41-88] on an optimal-transport approach to evolution equations with Dirichlet boundary conditions. Similarly to these works, we allow the mass to flow from/to the boundary <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>∂</mml:mi> <mml:mi>Ω</mml:mi></mml:mrow> </mml:math> throughout the evolution. However, our leading idea is to also keep track of the mass at the boundary by working with measures defined on the whole closure <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mover><mml:mi>Ω</mml:mi> <mml:mo>¯</mml:mo></mml:mover> </mml:math> . The driving functional is a modification of the classical relative entropy that also makes use of the information at the boundary. As an intermediate result, when <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>Ω</mml:mi></mml:math> is an interval in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>R</mml:mi></mml:mrow> <mml:mn>1</mml:mn></mml:msup> </mml:math> , we find a formula for the descending slope of this geodesically nonconvex functional.

Calculus of Variations and Partial Differential EquationsVol. 65(1)
Institute of Science and Technology Austria (AT)
Institute of Science and Technology Austria, Austrian Science Fund
Openalex Percentile: Top 48%
Gas Dynamics and Kinetic Theory
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