For a displacement convex noise penalty pair with lower semicontinuous penalty whose squared noise Wasserstein distance to the reference measure is controlled by the penalty, control cost at most one and a bounded uniformly continuous running cost, the penalty-drift Hamilton-Jacobi operator is locally strictly proper, shift-coercive, shift-semicontinuous, satisfies the first-order structure condition and has momentum-continuous shifts.
In the setting of First-Order Equations on the Noise Wasserstein Space Relative to a Noise Penalty Pair: Standing Notation, let be a noise penalty pair on , let satisfy and , let , and let be the Hamilton-Jacobi operator with penalty drift of the pair with discount , control cost and running cost , a first-order equation operator over by that clause, with -shifts and relative to the pair. Displacement convexity of the pair, being locally strictly proper with properness constants, the shift-coercivity condition, the shift-semicontinuity condition, the first-order structure condition at uniquely noise-mapped pairs and momentum-continuous shifts are those of the definitions cited. Lower semicontinuity of and uniform continuity of are taken relative to in the metric space of First-Order Equations on the Noise Wasserstein Space Relative to a Noise Penalty Pair: Standing Notation §space, with carrying the metric of The Absolute Value Metric on the Real Line, and boundedness of is that of that definition; is the absolute value of . For the number is a nonnegative real number, because by Noise Penalty Pairs on the Noise Wasserstein Space: the Penalty, Its Score, and Their Domains §pair and by 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 §reference. Assume the following.
(Convexity) The pair is displacement convex.
(Lower semicontinuity of the penalty) is lower semicontinuous on .
(Growth) There is with
(Running cost) is bounded and uniformly continuous on ; that is, there is with and for every , and for every positive there is a positive such that for all with .
Then the following hold.
1. (Local strict properness) For every positive , is a properness constant for at ; hence is locally strictly proper.
2. (Shift-coercivity) satisfies the shift-coercivity condition.
3. (Shift-semicontinuity) satisfies the shift-semicontinuity condition.
4. (Structure) satisfies the first-order structure condition at uniquely noise-mapped pairs.
5. (Momentum) has momentum-continuous shifts relative to the pair.
6. (Conclusion) Consequently is locally strictly proper, satisfies the shift-coercivity condition, the shift-semicontinuity condition and the first-order structure condition at uniquely noise-mapped pairs, and has momentum-continuous shifts relative to the pair.
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