For laws of distributions on the torus with finite entropy relative to the free field, and a bounded running cost uniformly continuous for the Wasserstein distance with cost, the Hamilton-Jacobi equation with the free-field score drift has comparison and exactly one bounded viscosity solution.
In the setting of The Free Field on the Torus as the Gaussian Reference Measure, with Square-Integrable White Noise: Standing Notation, let be the Gaussian entropy pair with temperature , whose hypothesis holds with the constant by White Noise in the Square-Integrable Space and the Free Field on the Torus as Noise Weights and a Variance Sequence on a Negative Sobolev Space §ratio; thus is the set of Borel probability measures on of finite relative entropy with respect to the free field , by The Gaussian Entropy Pair on the Noise Wasserstein Space: Relative Entropy and the Noise Score Field §penalty-domain. is the noise Wasserstein distance, whose cost equals when with , by White Noise in the Square-Integrable Space and the Free Field on the Torus as Noise Weights and a Variance Sequence on a Negative Sobolev Space §noise-space, and is the metric space of The Noise Wasserstein Distance is a Metric on the Measures Noise-Connected to the Reference Measure: Existence of Noise-Optimal Couplings, Comparison with the Quadratic Wasserstein Distance and Lower Semicontinuity §metric, which contains . Let denote the absolute value of . Let satisfy and , and let be bounded and uniformly continuous on , relative to in and with carrying the metric of The Absolute Value Metric on the Real Line. Fix with and for every ; such a exists, since if bounds on as in Bounded Real-Valued Function on a Set, the larger of and serves. Viscosity subsolutions, supersolutions and solutions are those of the Hamilton-Jacobi equation with Gaussian score drift relative to the free field with temperature (so that its score term is ), discount , control cost and running cost ,
an equation in read as in that clause, with the noise score field of .
1. (Comparison) Let and satisfy and for every , let be a viscosity subsolution and a viscosity supersolution. Then for every .
2. (Existence) There is a viscosity solution with, denoting the multiplicative inverse of ,
3. (Uniqueness) Let be viscosity solutions, each bounded. Then for every . Consequently, together with claim 2, the equation has exactly one bounded viscosity solution .
Loading…
No relations recorded yet.