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Changing the Variances of a Diagonal Gaussian Reference by a Diagonal Quadratic: the Same Measures and Domains, with Penalty and Score Shifted by a Diagonal Quadratic Profile

Changing the inverse variances of a diagonal Gaussian reference by a summable diagonal perturbation leaves the noise-connected measures, the finite-entropy measures and the score domain unchanged, and shifts the relative entropy by a diagonal quadratic profile plus a constant and the score by its gradient field.

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 β,κ∈R\beta,\kappa\in\mathbb{R} be positive 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 Gaussian entropy pair with temperature β\beta, whose hypothesis holds with this κ\kappa. Let d=(dk)k∈Nd=(d_{k})_{k\in\mathbb{N}} be an admissible sequence with ck−1+dk>0c_{k}^{-1}+d_{k}>0 for every k∈Nk\in\mathbb{N}, let Φd\Phi_{d} be the diagonal quadratic profile with coefficients dd and VdV_{d} its gradient field, and let c′=(ck′)k∈Nc'=(c'_{k})_{k\in\mathbb{N}} with ck′=(ck−1+dk)−1c'_{k}=(c_{k}^{-1}+d_{k})^{-1}. log⁡\log is the natural logarithm, absolute convergence of series is that of Series of Real Numbers §absolute, and H(⋅ ∣ ⋅)H(\cdot\,|\,\cdot) the relative entropy of Relative Entropy of Probability Measures §relative-entropy.

1. (The new variances) c′c' is a variance sequence; there is a positive κ′∈R\kappa'\in\mathbb{R} with ck′≤κ′ akc'_{k}\le\kappa'\,a_{k} for every k∈Nk\in\mathbb{N}; and the series ∑k=1∞log⁡(ck′/ck)\sum_{k=1}^{\infty}\log(c'_{k}/c_{k}) converges absolutely.

Fix such a κ′\kappa'; the sets D′\mathcal{D}' and DΣ′\mathcal{D}'_{\Sigma} below do not depend on this choice, being defined through relative entropy, the relative score and Fisher information with respect to γc′\gamma_{c'} only. Read A Diagonal Gaussian Reference Measure on the Noise Wasserstein Space, Rescaled Heads and Gaussian Tails: Standing Notation with c′c' in place of cc, so that its reference measure is ρ′=γc′\rho'=\gamma_{c'}, the diagonal Gaussian measure on XX with variances c′c', and its set of noise-connected measures is Pρ′a\mathcal{P}^{a}_{\rho'}; and let (D′,DΣ′,E′,Σ′)(\mathcal{D}',\mathcal{D}'_{\Sigma},\mathcal{E}',\Sigma') be the Gaussian entropy pair relative to γc′\gamma_{c'} with temperature β\beta, whose hypothesis holds with κ′\kappa'.

2. (The same measures) γc′∈Pρa\gamma_{c'}\in\mathcal{P}^{a}_{\rho}, and Pρ′a=Pρa\mathcal{P}^{a}_{\rho'}=\mathcal{P}^{a}_{\rho}.

3. (The same domains) D′=D\mathcal{D}'=\mathcal{D} and DΣ′=DΣ\mathcal{D}'_{\Sigma}=\mathcal{D}_{\Sigma}.

4. (The penalty) For every μ∈D\mu\in\mathcal{D},

H(μ ∣ γc′)=H(μ ∣ γc)+Φd(μ)+12∑k=1∞log⁡ck′ck,soE′(μ)=E(μ)+β Φd(μ)+β2∑k=1∞log⁡ck′ck.H(\mu\,|\,\gamma_{c'})=H(\mu\,|\,\gamma_{c})+\Phi_{d}(\mu)+\frac{1}{2}\sum_{k=1}^{\infty}\log\frac{c'_{k}}{c_{k}},\qquad\text{so}\qquad\mathcal{E}'(\mu)=\mathcal{E}(\mu)+\beta\,\Phi_{d}(\mu)+\frac{\beta}{2}\sum_{k=1}^{\infty}\log\frac{c'_{k}}{c_{k}} .

5. (The score) Let ν∈DΣ\nu\in\mathcal{D}_{\Sigma}, with relative score (ζk)k∈N(\zeta_{k})_{k\in\mathbb{N}} with respect to γc\gamma_{c}. Its relative score with respect to γc′\gamma_{c'} is the sequence of the classes ζk+dkxk\zeta_{k}+d_{k}x_{k} in L2(ν)L^{2}(\nu), and its noise score fields ZνaZ^{a}_{\nu} relative to γc\gamma_{c} and Zν′aZ'^{a}_{\nu} relative to γc′\gamma_{c'} (The Noise Score Field of a Measure of Finite Weighted Fisher Information: Existence, Norm, Pairing with Noise Gradients, Head Approximation and Tangency §field) satisfy Zν′a=Zνa+Vd(ν)Z'^{a}_{\nu}=Z^{a}_{\nu}+V_{d}(\nu); hence Σ′(ν)=Σ(ν)+β Vd(ν)\Sigma'(\nu)=\Sigma(\nu)+\beta\,V_{d}(\nu).

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