TheoremBase

The Sobolev Triple of Order Two for the Wick-Square Problem: the Domain Is the Sobolev Space of Order -1, Unit Families Are Square-Summable, the Gradient Form and the Riccati Drift

For the Sobolev triple of orders -3 and -2 on the torus in dimension at most three: the domain of the form operator is the Sobolev space of order -1, pairings with unit families are explicit, the space is infinite-dimensional, the unit families are square-summable in the form space, the sum of squared mode pairings is a form between zero and the identity, and the Riccati drift is a monotone nonlinearity.

Statement

In the setting of The Wick-Square Problem on the Torus: Standing Notation, let (H,V,A)(H,V,A) be the Sobolev triple of order 22, so that H=H−3(Tn)H=H^{-3}(\mathbb{T}^{n}) and V=H−2(Tn)V=H^{-2}(\mathbb{T}^{n}), linear subspaces of Map(Zn,R)\mathrm{Map}(\mathbb{Z}^{n},\mathbb{R}) carrying the inner products, norms and distances of orders −3-3 and −2-2, written with the subscripts HH and VV; D(A)⊆VD(A)\subseteq V and A:D(A)→HA:D(A)\to H are the domain and the form operator of the triple. Since (V,dV)(V,d_{V}) is separable by The Negative-Order Sobolev Triple of the Torus: a Diagonal Hilbert Triple whose Form Operator Is One Minus the Laplacian §triple, we may and do work in the setting of Hilbert Triples: Standing Notation and Background for this triple. Sym(H)\mathrm{Sym}(H) and Sym(V)\mathrm{Sym}(V) are the sets of bounded symmetric bilinear forms on HH and on VV, with the orders ⪯\preceq, the zero form 0Sym0_{\mathrm{Sym}} and the identity forms IHI_{H} and IVI_{V} fixed there. The unit families eke_{k} of The Wick-Square Problem on the Torus: Standing Notation §units lie in H−1H^{-1}, hence in VV and in HH (The Negative-Order Sobolev Spaces of the Torus are Hilbert Spaces: the Embedding of the Square-Integrable Classes, the Rescaled Trigonometric Basis, the Series Form of the Inner Product and the Inclusion of the Scale §inclusion). Let κ\kappa be an enumeration of Zn\mathbb{Z}^{n} as in Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families, and let qkq_{k} be the Riccati coefficients. Then the following hold.

1. (The domain) D(A)=H−1D(A)=H^{-1}, and for every x∈H−1x\in H^{-1} the vector AxAx is the family k↦μkx(k)k\mapsto\mu_{k}x(k) and ∣Ax∣H=∣x∣H−1|Ax|_{H}=|x|_{H^{-1}}.

2. (Pairings) For z∈Hz\in H and k∈Znk\in\mathbb{Z}^{n}, ⟨z,ek⟩H=z(k)/μk3\langle z,e_{k}\rangle_{H}=z(k)/\mu_{k}^{3}; for z∈Vz\in V, ⟨z,ek⟩V=z(k)/μk2\langle z,e_{k}\rangle_{V}=z(k)/\mu_{k}^{2}. For x∈H−1x\in H^{-1} and z∈Hz\in H the families k↦∣x(k)z(k)∣/μk2k\mapsto|x(k)z(k)|/\mu_{k}^{2} and k↦x(k)z(k)/μk2k\mapsto x(k)z(k)/\mu_{k}^{2} are cube-summable and ⟨Ax,z⟩H=∑k∈Znx(k)z(k)/μk2\langle Ax,z\rangle_{H}=\sum_{k\in\mathbb{Z}^{n}}x(k)z(k)/\mu_{k}^{2}.

3. (Infinite dimension) HH, as a vector space over R\mathbb{R}, is not finite-dimensional.

4. (White noise) The sequence f=(eκ(j))j∈Nf=(e_{\kappa(j)})_{j\in\mathbb{N}} is square-summable in VV, with σ(f)=∑k∈Zn1/μk2\sigma(f)=\sum_{k\in\mathbb{Z}^{n}}1/\mu_{k}^{2}; and for every X∈Sym(V)X\in\mathrm{Sym}(V) the family k↦X(ek,ek)k\mapsto X(e_{k},e_{k}) is cube-summable, with lattice sum the trace TrfX\mathrm{Tr}_{f}X.

5. (The gradient form) For all p,p′∈Hp,p'\in H the families k↦∣⟨p,ek⟩H⟨p′,ek⟩H∣k\mapsto|\langle p,e_{k}\rangle_{H}\langle p',e_{k}\rangle_{H}| and k↦⟨p,ek⟩H⟨p′,ek⟩Hk\mapsto\langle p,e_{k}\rangle_{H}\langle p',e_{k}\rangle_{H} are cube-summable, and the map G:H×H→RG:H\times H\to\mathbb{R} sending (p,p′)(p,p') to the lattice sum of the latter belongs to Sym(H)\mathrm{Sym}(H) and satisfies 0Sym⪯G⪯IH0_{\mathrm{Sym}}\preceq G\preceq I_{H}.

6. (The Riccati drift) For every x∈Vx\in V the family Bqx:k↦2qkx(k)B_{q}x:k\mapsto2q_{k}x(k) lies in HH, and the map Bq:V→HB_{q}:V\to H so defined is a monotone nonlinearity for (H,V,A)(H,V,A).

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