<p>We establish interior regularity results for first-order, stationary, local mean-field game (MFG) systems. Specifically, we study solutions of the coupled system consisting of a Hamilton–Jacobi–Bellman equation <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1099_Article_IEq1.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="123" /> </InlineMediaObject> <EquationSource Format="TEX">\(H(x, Du, m) = 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>H</mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>D</mi> <mi>u</mi> <mo>,</mo> <mi>m</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> and a transport equation <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1099_Article_IEq2.gif" Format="GIF" Height="20" Rendition="HTML" Resolution="72" Type="Linedraw" Width="209" /> </InlineMediaObject> <EquationSource Format="TEX">\(-\operatorname {div}(m D_pH(x, Du, m)) = 0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo>-</mo> <mo>div</mo> <mo stretchy="false">(</mo> <mi>m</mi> <msub> <mi>D</mi> <mi>p</mi> </msub> <mi>H</mi> <mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo>,</mo> <mi>D</mi> <mi>u</mi> <mo>,</mo> <mi>m</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation> in a domain <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1099_Article_IEq3.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="55" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega \subset {\mathbb {R}}^d\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="normal">Ω</mi> <mo>⊂</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mi>d</mi> </msup> </mrow> </math></EquationSource> </InlineEquation>. Under suitable structural assumptions on the Hamiltonian <i>H</i>, without requiring monotonicity of the system, convexity of the Hamiltonian, separability in variables, or smoothness beyond basic continuity in (<i>p</i>,&#xa0;<i>m</i>), we introduce a notion of weak solutions that allows the application of techniques from elliptic regularity theory. Our main contribution is to prove that the value function <i>u</i> is locally Hölder continuous in <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="30_2025_1099_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(\Omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="normal">Ω</mi> </math></EquationSource> </InlineEquation>. The proof leverages the connection between first-order MFG systems and quasilinear equations in divergence form, adapting classical techniques to handle the specific structure of MFG systems.</p>

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Regularity for weak solutions to first-order local mean field games

  • AbdulRahman M. Alharbi,
  • Giuseppe Di Fazio,
  • Diogo A. Gomes,
  • Melih Ucer

摘要

We establish interior regularity results for first-order, stationary, local mean-field game (MFG) systems. Specifically, we study solutions of the coupled system consisting of a Hamilton–Jacobi–Bellman equation \(H(x, Du, m) = 0\) H ( x , D u , m ) = 0 and a transport equation \(-\operatorname {div}(m D_pH(x, Du, m)) = 0\) - div ( m D p H ( x , D u , m ) ) = 0 in a domain \(\Omega \subset {\mathbb {R}}^d\) Ω R d . Under suitable structural assumptions on the Hamiltonian H, without requiring monotonicity of the system, convexity of the Hamiltonian, separability in variables, or smoothness beyond basic continuity in (pm), we introduce a notion of weak solutions that allows the application of techniques from elliptic regularity theory. Our main contribution is to prove that the value function u is locally Hölder continuous in \(\Omega \) Ω . The proof leverages the connection between first-order MFG systems and quasilinear equations in divergence form, adapting classical techniques to handle the specific structure of MFG systems.