TheoremBase

Lipschitz-Cone Comparison for the Quadratic Control Problem on Unitary Laws under Strong Free Noise

If the source is Lf−LipschitzL_f-Lipschitz in the gauge distance with LfL_f at most rho beta2/(4K)beta^2/(4K), every subsolution minus every supersolution of the quadratic control equation is bounded by L times the gauge distance for L between Lf/rhoL_f/rho and beta2/(4K)beta^2/(4K); hence comparison, uniqueness, and the Lipschitz bound Lf/rhoL_f/rho for solutions.

Statement

In the setting of Unitary Laws with Free Unitary Noise: Standing Data, with the conventions of Unitary Laws with Free Unitary Noise: Standing Data §spaces, let HQH_{Q} be the quadratic control Hamiltonian, ρ,β\rho,\beta the constants, ff the source, and KK a trilinear constant. Suppose that there is a real Lf≥0L_{f}\ge0 with

∣f(μ)−f(ν)∣≤Lf dL(μ,ν)for all μ,ν∈Ld,andLf≤ρ β24K.|f(\mu)-f(\nu)|\le L_{f}\,d_{\mathcal{L}}(\mu,\nu)\quad\text{for all }\mu,\nu\in\mathcal{L}_{d},\qquad\text{and}\qquad L_{f}\le\frac{\rho\,\beta^{2}}{4K}.

1. (Lipschitz cone) Let LL be a real number with Lf/ρ≤L≤β2/(4K)L_{f}/\rho\le L\le\beta^{2}/(4K). If uu is a viscosity subsolution and vv a viscosity supersolution of The Discounted Hamilton-Jacobi-Bellman Equation on Unitary Laws with Free Unitary Noise §equation with Hamiltonian HQH_{Q}, then u(μ)−v(ν)≤L dL(μ,ν)u(\mu)-v(\nu)\le L\,d_{\mathcal{L}}(\mu,\nu) for all μ,ν∈Ld\mu,\nu\in\mathcal{L}_{d}.

2. (Comparison) If uu and vv are as in clause 1, then u(λ)≤v(λ)u(\lambda)\le v(\lambda) for every λ∈Ld\lambda\in\mathcal{L}_{d}.

3. (Uniqueness) The Discounted Hamilton-Jacobi-Bellman Equation on Unitary Laws with Free Unitary Noise §equation with Hamiltonian HQH_{Q} has at most one viscosity solution.

4. (Lipschitz bound) Every viscosity solution VV of The Discounted Hamilton-Jacobi-Bellman Equation on Unitary Laws with Free Unitary Noise §equation with Hamiltonian HQH_{Q} satisfies ∣V(μ)−V(ν)∣≤(Lf/ρ) dL(μ,ν)|V(\mu)-V(\nu)|\le(L_{f}/\rho)\,d_{\mathcal{L}}(\mu,\nu) for all μ,ν∈Ld\mu,\nu\in\mathcal{L}_{d}.

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