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The Wick Square of the Free Field on the Torus as Diagonal Couplings: Summability in Dimension at Most Three, the Riccati Condition, and the Divergent Wick Constant

On negative Sobolev spaces of the torus, the Wick square of the free field corresponds to diagonal couplings that are summable Wick couplings in dimension at most three, satisfy the Riccati condition, and have a divergent Wick constant in dimension at least two.

Statement

In the setting of The Free Field on the Torus as the Gaussian Reference Measure, with Square-Integrable White Noise: Standing Notation, so that X=H−m(Tn)X=H^{-m}(\mathbb{T}^{n}) with n≤m+1n\le m+1, the weights are aj=(ρκ(j)m)2a_{j}=(\rho^{m}_{\kappa(j)})^{2} and the variances cj=(ρκ(j)m+1)2c_{j}=(\rho^{m+1}_{\kappa(j)})^{2}, where ρk2=μk−1\rho_{k}^{2}=\mu_{k}^{-1}; let (D,DΣ,E,Σ)(\mathcal{D},\mathcal{D}_{\Sigma},\mathcal{E},\Sigma) be the Gaussian entropy pair with temperature 11, whose hypothesis holds with the constant 11 by White Noise in the Square-Integrable Space and the Free Field on the Torus as Noise Weights and a Variance Sequence on a Negative Sobolev Space §ratio. For x∈Xx\in X, xjx_{j} is its jj-th coordinate as in A Diagonal Gaussian Reference Measure on the Noise Wasserstein Space, Rescaled Heads and Gaussian Tails: Standing Notation §background, and μkm\mu_{k}^{m} is the natural power; μk−1\mu_{k}^{-1} is the multiplicative inverse of μk\mu_{k}, which is positive since 1≤μk1\le\mu_{k}, and μk−2\mu_{k}^{-2} that of μk2\mu_{k}^{2}. Let w0∈Rw_{0}\in\mathbb{R} and let w=(wj)j∈Nw=(w_{j})_{j\in\mathbb{N}} with wj=w0 μκ(j)mw_{j}=w_{0}\,\mu_{\kappa(j)}^{m}. Convergent series are those of that definition, and min⁡{s,s′}\min\{s,s'\} is the minimum of s,s′∈Rs,s'\in\mathbb{R}.

1. (The couplings are the Wick square) For every x∈Xx\in X and j∈Nj\in\mathbb{N}, wj xj2=w0 x(κ(j))2w_{j}\,x_{j}^{2}=w_{0}\,x(\kappa(j))^{2}, where x(k)x(k) is the value at k∈Znk\in\mathbb{Z}^{n} of the coefficient family xx; moreover wjcj=w0 μκ(j)−1w_{j}c_{j}=w_{0}\,\mu_{\kappa(j)}^{-1} and ∣wj∣ cj≤∣w0∣|w_{j}|\,c_{j}\le|w_{0}|.

2. (Summability) Suppose n≤3n\le3. Then the series ∑j=1∞∣wj∣ cj2/aj=∑j=1∞∣w0∣ μκ(j)−2\sum_{j=1}^{\infty}|w_{j}|\,c_{j}^{2}/a_{j}=\sum_{j=1}^{\infty}|w_{0}|\,\mu_{\kappa(j)}^{-2} converges, so ww is a sequence of Wick couplings relative to this pair, with bound ∣w0∣|w_{0}|.

3. (The Riccati condition) Let λ0,θ∈R\lambda_{0},\theta\in\mathbb{R} be positive with ε0=1+λ0+2θmin⁡{w0,0}>0\varepsilon_{0}=1+\lambda_{0}+2\theta\min\{w_{0},0\}>0. Then

ajcj+λ0+2θ wjcj≥ε0for every j∈N.\frac{a_{j}}{c_{j}}+\lambda_{0}+2\theta\,w_{j}c_{j}\ge\varepsilon_{0}\qquad\text{for every }j\in\mathbb{N}.

4. (The Wick constant diverges) Suppose 2≤n2\le n and 0<w00<w_{0}. Then the series ∑j=1∞wjcj=∑j=1∞w0 μκ(j)−1\sum_{j=1}^{\infty}w_{j}c_{j}=\sum_{j=1}^{\infty}w_{0}\,\mu_{\kappa(j)}^{-1} does not converge.

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