TheoremBase

The Entropy Inequality for Nonnegative Functions, and Quadratic Moments Bounded by the Relative Entropy with Respect to a Diagonal Gaussian Measure

The integral of a nonnegative function is at most the relative entropy plus the logarithm of its exponential moment under the reference measure; relative to a diagonal Gaussian this bounds diagonal quadratic moments, and the second moment, linearly by the relative entropy with explicit constants.

Statement

In the settings of The Real Numbers: Standing Notation and Background and The Intrinsic Calculus on the Wasserstein Space: Standing Notation, finite relative entropy and H(⋅ ∣ ⋅)H(\cdot\,|\,\cdot) are those of that definition on (Rd,B(Rd))(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d})); Borel and integrable are as in Probability Measures on Euclidean Space and Random Vectors: Standing Notation §measures, a nonnegative Borel function being integrated as a [0,∞][0,\infty]-valued map; exp⁡\exp is the exponential function and log⁡\log the natural logarithm.

1. (Entropy inequality) Let γ,ν∈P(Rd)\gamma,\nu\in\mathcal{P}(\mathbb{R}^{d}) with ν\nu of finite relative entropy with respect to γ\gamma, and let h:Rd→[0,∞)h:\mathbb{R}^{d}\to[0,\infty) be Borel with exp⁡∘h\exp\circ h integrable with respect to γ\gamma. Then hh is integrable with respect to ν\nu, ∫Rdexp⁡∘h dγ\int_{\mathbb{R}^{d}}\exp\circ h\,d\gamma is a positive real number, and

∫Rdh dν≤H(ν ∣ γ)+log⁡∫Rdexp⁡∘h dγ.\int_{\mathbb{R}^{d}}h\,d\nu\le H(\nu\,|\,\gamma)+\log\int_{\mathbb{R}^{d}}\exp\circ h\,d\gamma .

2. (Diagonal quadratic moments) Let cc be a variance vector, with greatest variance cmax⁡c_{\max}, let γc\gamma_{c} be the diagonal Gaussian measure with variances cc, let w=(w1,…,wd)∈Rdw=(w_{1},\dots,w_{d})\in\mathbb{R}^{d} with wi≥0w_{i}\ge0 for every i∈[d]i\in[d], and let t∈Rt\in\mathbb{R} be positive with 4twici≤14tw_{i}c_{i}\le1 for every i∈[d]i\in[d]. Then for every μ∈P(Rd)\mu\in\mathcal{P}(\mathbb{R}^{d}) of finite relative entropy with respect to γc\gamma_{c} the function x↦∑i=1dwixi2x\mapsto\sum_{i=1}^{d}w_{i}x_{i}^{2} is integrable with respect to μ\mu and

∫Rd∑i=1dwixi2 μ(dx)≤1t H(μ ∣ γc)+2∑i=1dwici.\int_{\mathbb{R}^{d}}\sum_{i=1}^{d}w_{i}x_{i}^{2}\,\mu(dx)\le\frac{1}{t}\,H(\mu\,|\,\gamma_{c})+2\sum_{i=1}^{d}w_{i}c_{i}.

3. (Second moment) Let cc and γc\gamma_{c} be as in clause 2. Every μ∈P(Rd)\mu\in\mathcal{P}(\mathbb{R}^{d}) of finite relative entropy with respect to γc\gamma_{c} belongs to P2(Rd)\mathcal{P}_{2}(\mathbb{R}^{d}), and its second moment satisfies

M2(μ)≤4cmax⁡ H(μ ∣ γc)+2∑i=1dci.M_{2}(\mu)\le4c_{\max}\,H(\mu\,|\,\gamma_{c})+2\sum_{i=1}^{d}c_{i}.

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