TheoremBase

The Gibbs Entropy Pair is Noise-Closed, and Its Penalty Bounds the Squared Noise Wasserstein Distance to the Reference Measure

Penalty sublevel sets of the Gibbs entropy pair are closed and bounded in the noise Wasserstein space, and the squared distance to the Gaussian reference measure is bounded by an affine function of the penalty.

Statement

In the setting of A Diagonal Gaussian Reference Measure on the Noise Wasserstein Space, Rescaled Heads and Gaussian Tails: Standing Notation, so that the reference measure is ρ=γc\rho=\gamma_{c}, let VV be an admissible cylindrical potential, let bb be a constant as in Admissible Cylindrical Potentials on a Hilbert Space in the Noise Geometry §below, let β\beta and κ\kappa be positive real numbers with ck≤κ akc_{k}\le\kappa\,a_{k} for every k∈Nk\in\mathbb{N}, and let (D,DΣ,E,Σ)(\mathcal{D},\mathcal{D}_{\Sigma},\mathcal{E},\Sigma) be the Gibbs entropy pair with potential VV and temperature β\beta, whose hypothesis holds with this κ\kappa; it is a noise penalty pair on Pρa\mathcal{P}^{a}_{\rho} by The Gibbs Entropy Pair is a Noise Penalty Pair, with Nonnegative Penalty and Dense Score Domain §pair. ZV,βZ_{V,\beta} is the normaliser of the Gibbs measure γβV\gamma^{V}_{\beta} of VV at temperature β\beta, log⁡\log is the natural logarithm, as in Relative Entropy of Probability Measures §relative-entropy, and WaW_{a} is the noise Wasserstein distance. Noise-closedness is read in the metric space (Pρa,Wa)(\mathcal{P}^{a}_{\rho},W_{a}) of 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 §metric; the real number quantified as cc in Noise-Closed Noise Penalty Pairs §noise-closed is a bound variable there, distinct from the variance sequence cc. For μ∈D\mu\in\mathcal{D} the number Wa(μ,ρ)W_{a}(\mu,\rho) is defined 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 §connected, since D⊆Pρa\mathcal{D}\subseteq\mathcal{P}^{a}_{\rho} by The Gibbs Entropy Pair on the Noise Wasserstein Space: Relative Entropy to the Gibbs Measure and the Gibbs Score Field §penalty-domain and ρ∈Pρa\rho\in\mathcal{P}^{a}_{\rho} 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.

1. (Noise-closed) The pair is noise-closed.

2. (Growth) For every μ∈D\mu\in\mathcal{D},

Wa(μ,ρ)2 ≤ 2κβ(E(μ)+b−βlog⁡ZV,β).W_{a}(\mu,\rho)^{2}\ \le\ \frac{2\kappa}{\beta}\Bigl(\mathcal{E}(\mu)+b-\beta\log Z_{V,\beta}\Bigr).

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