Lower Convergence: The Solution with the Local Cost Is Asymptotically below the Mean-Field Solutions with the Mollified Costs
corollaryAnalysisProbabilityPDEcor:n-particle-mollified-lower-convergence-wasserstein-2026aIf tends to 0, the bounded solution of the equation with the local density cost is, uniformly on energy sublevel sets, asymptotically below the bounded solutions of the mean-field equations with the mollified mean-field costs.
In the setting of N-Particle Systems on the Wasserstein Space: Particles, Configurations and the Configuration Level. The letter , fixed in N-Particle Systems on the Wasserstein Space: Particles, Configurations and the Configuration Level §particles as the number of particles, is used here only as a running index of sequences; no object below depends on it otherwise. The letter , which denotes vector fields in Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation §fields, denotes here a mollifier kernel; the letter denotes the noise intensity, and the swap map written in Couplings on Euclidean Space: Product Coupling, Swap, Finiteness of the Cost, Push-Forward Couplings, Modifying One Marginal, Quantisation, Gluing over a Finitely Supported Measure, and the Lipschitz Bound §swap is not used; the letter denotes the control cost, and tolerances are written .
Let be a confining potential on , let be positive, let satisfy , let and let be a real matrix. Let be nonnegative, let be a convex Lipschitz integrand with constant , let be a mollifier kernel of radius on , and let be bounded and uniformly continuous for the Euclidean distance and the metric of The Absolute Value Metric on the Real Line. Let be real numbers with for every such that, for every positive , there is with for every with .
Let be the Langevin free-energy pair with potential and noise intensity , and let be the absolute value of . The function on is bounded and uniformly continuous for by Running Costs for N-Particle Systems: Integrals of Bounded Uniformly Continuous Functions and Costs of the Empirical Measure §integral, read with ; let be the unique bounded viscosity solution of the Langevin Hamilton-Jacobi equation with common noise and density cost with potential , noise intensity , discount , common-noise matrix , control cost , running cost and integrand , which exists and is unique by Well-Posedness of the Langevin Hamilton-Jacobi Equation with Common Noise and a Density Cost: Existence and Uniqueness of a Bounded Viscosity Solution §existence and Well-Posedness of the Langevin Hamilton-Jacobi Equation with Common Noise and a Density Cost: Existence and Uniqueness of a Bounded Viscosity Solution §uniqueness. For each , let be the mollified mean-field cost with data , , and , bounded and uniformly continuous for by The Mollified N-Particle Cost: Regularity, Its Tensor-Averaged Cost, and the Defect against the Local Cost §regularity, and let be the unique bounded viscosity solution of the Langevin Hamilton-Jacobi equation with common noise with potential , noise intensity , discount , common-noise matrix , control cost and running cost , which exists and is unique by Well-Posedness of the Hamilton-Jacobi Equation with Common Noise for Controlled Langevin Dynamics: Existence and Uniqueness of a Bounded Viscosity Solution §existence and Well-Posedness of the Hamilton-Jacobi Equation with Common Noise for Controlled Langevin Dynamics: Existence and Uniqueness of a Bounded Viscosity Solution §uniqueness.
(Lower convergence)¶ For all positive there is such that
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