The Dyson Hamilton-Jacobi Equation with Common Noise and a Confining Potential on the Wasserstein Space of the Real Line
equationAnalysisProbabilityPDEeq:dyson-confined-hamilton-jacobi-wasserstein-2026bThe discounted Dyson Hamilton-Jacobi equation with common noise and a confining potential V on the Wasserstein space of the real line, the penalty-drift equation of the confined logarithmic-energy pair with unit control cost.
In the setting of The Intrinsic Calculus on the Wasserstein Space: Standing Notation, in dimension , with the identifications of One-Dimensional Test Functions: Scalars, Derivatives, and the Difference Quotient of the Derivative. Let be a confining potential, with derivative , let be positive, let be nonnegative, let , and let be the confined logarithmic-energy pair with potential and inverse temperature , a penalty pair by The Confined Logarithmic-Energy Pair is a Displacement Convex, Wasserstein-Coercive Penalty Pair with Closed Score and Regular Penalised Maxima §pair, so that for , with the free score. For , and are the inner product and norm of , and is the trace of .
1. (The operator)¶ The Dyson Hamilton-Jacobi operator with common noise and confining potential is the Hamilton-Jacobi operator with common noise and penalty drift of that pair with discount , common-noise intensity , control cost and running cost , a second-order equation operator over ; by the formula for , its value at is
2. (The equation)¶ The Dyson Hamilton-Jacobi equation with common noise and confining potential is
that is, , with in the bundle , and . Its classical and viscosity solutions, subsolutions and supersolutions are those of The Discounted Hamilton-Jacobi Equation with Common Noise and a Penalty Drift on the Wasserstein Space §equation for this pair and these coefficients.
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