TheoremBase

Computes the couplings from the basis clause and the ratio aja_j = mu cjc_j of the free-field data, converts cube-summability of the inverse Fourier weights into convergence or divergence of the series along the enumeration, and checks the Riccati bound by the factorisation (t-1)(1-2 theta w0/t)w_0/t) >= 0 when w0w_0 < 0.

Proof

Each result cited is universally quantified over the data in its own statement.

Fix j∈Nj\in\mathbb{N} and abbreviate r=ρκ(j)r=\rho_{\kappa(j)} and μ=μκ(j)\mu=\mu_{\kappa(j)}. By Summability of the Negative Powers of the Fourier Weights of the Torus §product (used with its ss taken to be nn), 1≤μ1\le\mu; hence μ\mu is positive and 0<μ−1≤10<\mu^{-1}\le1. The enumeration κ\kappa of The Free Field on the Torus as the Gaussian Reference Measure, with Square-Integrable White Noise: Standing Notation §data is a bijection N→Zn\mathbb{N}\to\mathbb{Z}^{n}, by the meaning of an enumeration in Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families. 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, aj=μ cja_{j}=\mu\,c_{j}, and cj>0c_{j}>0 by Variance Sequences and Their Truncations §variances, cc being a variance sequence 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 §variances; hence

cj=μ−1aj,ajcj=μ,cjaj=μ−1.(1)c_{j}=\mu^{-1}a_{j},\qquad\frac{a_{j}}{c_{j}}=\mu,\qquad\frac{c_{j}}{a_{j}}=\mu^{-1}.\tag{1}

Since r2=μ−1r^{2}=\mu^{-1}, the product rule for natural powers (Properties of Natural Number Powers in a Field §products) and its unit rule (Properties of Natural Number Powers in a Field §unit) give

aj=(rm)2=rmrm=(r r)m=(μ−1)m,μmaj=(μ μ−1)m=1m=1.(2)a_{j}=(r^{m})^{2}=r^{m}r^{m}=(r\,r)^{m}=(\mu^{-1})^{m},\qquad\mu^{m}a_{j}=(\mu\,\mu^{-1})^{m}=1^{m}=1.\tag{2}

Clause 1. Let x∈Xx\in X. The coordinate xjx_{j} is ⟨x,ej⟩H−m\langle x,e_{j}\rangle_{H^{-m}} (A Diagonal Gaussian Reference Measure on the Noise Wasserstein Space, Rescaled Heads and Gaussian Tails: Standing Notation §background with The Free Field on the Torus as the Gaussian Reference Measure, with Square-Integrable White Noise: Standing Notation §gaussian), which equals rm x(κ(j))r^{m}\,x(\kappa(j)) 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 §basis. Hence, using (2),

wj xj2=w0 μm (rm)2 x(κ(j))2=w0 μmaj x(κ(j))2=w0 x(κ(j))2.w_{j}\,x_{j}^{2}=w_{0}\,\mu^{m}\,(r^{m})^{2}\,x(\kappa(j))^{2}=w_{0}\,\mu^{m}a_{j}\,x(\kappa(j))^{2}=w_{0}\,x(\kappa(j))^{2}.

By (1) and (2), wjcj=w0 μmμ−1aj=w0 μ−1w_{j}c_{j}=w_{0}\,\mu^{m}\mu^{-1}a_{j}=w_{0}\,\mu^{-1}. Since cj>0c_{j}>0 and 0<μ−1≤10<\mu^{-1}\le1,

∣wj∣ cj=∣wjcj∣=∣w0∣ μ−1≤∣w0∣.|w_{j}|\,c_{j}=|w_{j}c_{j}|=|w_{0}|\,\mu^{-1}\le|w_{0}| .

Clause 2. Suppose n≤3n\le3. By clause 1 and (1),

∣wj∣ cj2aj=∣wj∣ cj⋅cjaj=∣w0∣ μ−1μ−1=∣w0∣ μ−2,\frac{|w_{j}|\,c_{j}^{2}}{a_{j}}=|w_{j}|\,c_{j}\cdot\frac{c_{j}}{a_{j}}=|w_{0}|\,\mu^{-1}\mu^{-1}=|w_{0}|\,\mu^{-2},

μ−1μ−1\mu^{-1}\mu^{-1} being the inverse of μ2=μμ\mu^{2}=\mu\mu. Since n≤3<4=2⋅2n\le3<4=2\cdot2, Lattice Sums of the Fourier Weights of the Torus, and the Negative Sobolev Norms as Lattice Sums §convergent with s=2s=2 shows that the family k↦1/μk2k\mapsto1/\mu_{k}^{2} on Zn\mathbb{Z}^{n} is cube-summable. Its values are positive, so by Lattice Sums along Cubes: Linearity, Nonnegative Families, Absolute Summability, Comparison and Finitely Supported Families §enumeration, applied with the bijection κ\kappa, the series ∑j=1∞μκ(j)−2\sum_{j=1}^{\infty}\mu_{\kappa(j)}^{-2} converges; by Elementary Properties of Series of Real Numbers §linearity so does ∑j=1∞∣w0∣ μκ(j)−2\sum_{j=1}^{\infty}|w_{0}|\,\mu_{\kappa(j)}^{-2}, which is, term by term, the series ∑j=1∞∣wj∣ cj2/aj\sum_{j=1}^{\infty}|w_{j}|\,c_{j}^{2}/a_{j}. Together with ∣wj∣ cj≤∣w0∣|w_{j}|\,c_{j}\le|w_{0}| for every jj (clause 1), this is the condition of The Wick-Square Corrector and the Score-Paired Wick-Square Cost Relative to a Diagonal Gaussian Measure on a Hilbert Space §couplings, so ww is a sequence of Wick couplings with bound ∣w0∣|w_{0}|. That definition applies to the pair of the statement: β=1\beta=1 and the constant 11 are positive, and cj≤1⋅ajc_{j}\le1\cdot a_{j} for every jj 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.

Clause 3. Let λ0,θ\lambda_{0},\theta be positive with ε0=1+λ0+2θmin⁡{w0,0}>0\varepsilon_{0}=1+\lambda_{0}+2\theta\min\{w_{0},0\}>0. By (1) and clause 1, with t=μ≥1t=\mu\ge1,

ajcj+λ0+2θ wjcj=t+λ0+2θw0t.\frac{a_{j}}{c_{j}}+\lambda_{0}+2\theta\,w_{j}c_{j}=t+\lambda_{0}+\frac{2\theta w_{0}}{t}.

Suppose first 0≤w00\le w_{0}. Then min⁡{w0,0}=0\min\{w_{0},0\}=0 by Minimum of Two Elements of a Totally Ordered Set: it is w0w_{0} if w0≤0w_{0}\le0, in which case w0=0w_{0}=0, and 00 otherwise, so ε0=1+λ0\varepsilon_{0}=1+\lambda_{0}; since t≥1t\ge1 and 2θw0/t≥02\theta w_{0}/t\ge0, the displayed quantity is at least 1+λ0=ε01+\lambda_{0}=\varepsilon_{0}. Suppose next w0<0w_{0}<0. Then min⁡{w0,0}=w0\min\{w_{0},0\}=w_{0} by Minimum of Two Elements of a Totally Ordered Set, so ε0=1+λ0+2θw0\varepsilon_{0}=1+\lambda_{0}+2\theta w_{0}, and

t+λ0+2θw0t−ε0=(t−1)+2θw0(1t−1)=(t−1)−2θw0(t−1)t=(t−1)(1−2θw0t).t+\lambda_{0}+\frac{2\theta w_{0}}{t}-\varepsilon_{0}=(t-1)+2\theta w_{0}\Bigl(\frac{1}{t}-1\Bigr)=(t-1)-\frac{2\theta w_{0}(t-1)}{t}=(t-1)\Bigl(1-\frac{2\theta w_{0}}{t}\Bigr).

Here t−1≥0t-1\ge0, and −2θw0/t>0-2\theta w_{0}/t>0 because θ,t>0\theta,t>0 and w0<0w_{0}<0, so the second factor exceeds 11; the product is nonnegative. In both cases ajcj+λ0+2θwjcj≥ε0\frac{a_{j}}{c_{j}}+\lambda_{0}+2\theta w_{j}c_{j}\ge\varepsilon_{0}, and jj was arbitrary.

Clause 4. Suppose 2≤n2\le n and 0<w00<w_{0}. By clause 1, wjcj=w0 μκ(j)−1w_{j}c_{j}=w_{0}\,\mu_{\kappa(j)}^{-1} for every jj, so the two series of the claim agree term by term. The family k↦1/μkk\mapsto1/\mu_{k} on Zn\mathbb{Z}^{n} has positive values, and by Lattice Sums of the Fourier Weights of the Torus, and the Negative Sobolev Norms as Lattice Sums §divergent the set of its cube sums is not bounded above, so it is not cube-summable by Lattice Sums along Cubes: Linearity, Nonnegative Families, Absolute Summability, Comparison and Finitely Supported Families §nonnegative. By Lattice Sums along Cubes: Linearity, Nonnegative Families, Absolute Summability, Comparison and Finitely Supported Families §enumeration, applied with the bijection κ\kappa, the series ∑j=1∞μκ(j)−1\sum_{j=1}^{\infty}\mu_{\kappa(j)}^{-1} does not converge. If ∑j=1∞w0 μκ(j)−1\sum_{j=1}^{\infty}w_{0}\,\mu_{\kappa(j)}^{-1} converged, then multiplying by w0−1w_{0}^{-1}, which exists as w0>0w_{0}>0, Elementary Properties of Series of Real Numbers §linearity would make ∑j=1∞μκ(j)−1\sum_{j=1}^{\infty}\mu_{\kappa(j)}^{-1} converge, a contradiction. Hence ∑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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