TheoremBase

Well-Posedness and Lipschitz Regularity for the Quadratic Control Problem on Unitary Laws under Strong Free Noise

Under strong free noise, LfL_f at most rho beta2/(4K)beta^2/(4K), the quadratic control equation on unitary laws has exactly one viscosity solution; it is Lf/rho−LipschitzL_f/rho-Lipschitz in the gauge distance and bounded by sup|f|/rho.

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}.

Then there is a map V:Ld→RV:\mathcal{L}_{d}\to\mathbb{R} with the following properties.

1. (Existence) VV is a viscosity solution of The Discounted Hamilton-Jacobi-Bellman Equation on Unitary Laws with Free Unitary Noise §equation with Hamiltonian HQH_{Q}.

2. (Uniqueness) Every viscosity solution of The Discounted Hamilton-Jacobi-Bellman Equation on Unitary Laws with Free Unitary Noise §equation with Hamiltonian HQH_{Q} equals VV.

3. (Lipschitz bound) ∣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}.

4. (Bound) For every real MM with ∣f(λ)∣≤M|f(\lambda)|\le M for all λ∈Ld\lambda\in\mathcal{L}_{d}, ∣V(λ)∣≤M/ρ|V(\lambda)|\le M/\rho for every λ∈Ld\lambda\in\mathcal{L}_{d}.

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