Entropy-Penalised Viscosity Subsolutions, Supersolutions and Solutions of the Discounted Hamilton-Jacobi-Bellman Equation on the Torus Wasserstein Space
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Sub- and supersolutions tested at strict extrema of the function minus an intrinsic test function and a small multiple of the entropy. The extremal measure must have finite Fisher information, and the score form of the equation must hold there up to a tolerance proportional to the multiple.
1. (Subsolution)u is an entropy-penalised viscosity subsolution of (E) if there are a real number δ0>0 and a nondecreasing function c:[0,∞)→[0,∞) with the following property. For every intrinsic test function φ on Pac(Td), every real δ with 0<δ≤δ0, and every μ∈PEnt(Td) such that
u(ν)−φ(ν)−δEnt(ν)<u(μ)−φ(μ)−δEnt(μ)for every ν∈PEnt(Td) with ν=μ,
one has μ∈PI(Td) and
ρu(μ)+H(μ,∇φ(μ))+2σ2⟨∇φ(μ),ξμ⟩μ≤δc(∥∇φ(μ)∥μ).
2. (Supersolution)u is an entropy-penalised viscosity supersolution of (E) if there are a real number δ0>0 and a nondecreasing function c:[0,∞)→[0,∞) with the following property. For every intrinsic test function φ on Pac(Td), every real δ with 0<δ≤δ0, and every μ∈PEnt(Td) such that
u(ν)−φ(ν)+δEnt(ν)>u(μ)−φ(μ)+δEnt(μ)for every ν∈PEnt(Td) with ν=μ,
3. (Solution)u is an entropy-penalised viscosity solution of (E) if it is both an entropy-penalised viscosity subsolution and an entropy-penalised viscosity supersolution of (E).
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