TheoremBase

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

Each negative-order Sobolev space of the torus is a real Hilbert space isometric to the square-integrable classes through the realisation map; the Fourier coefficient families of square-integrable classes embed contractively; the realisation preimages of the trigonometric classes form an orthonormal basis along any enumeration; the inner product is a weighted series of coefficient products, which also characterises membership; and each space is contained in the next one of lower order with a smaller norm.

Statement

We work in the setting of The Flat Torus: Standing Notation, used here with a natural number nn satisfying 1≤n1\le n, and in the setting of Real Hilbert Spaces: Standing Notation and Background, whose standing space HH is not used here; the integer lattice Zn\mathbb{Z}^{n} and the real Hilbert space L2(Tn)L^{2}(\mathbb{T}^{n}), with inner product ⟨ ⋅ ,⋅ ⟩L2\langle\,\cdot\,,\cdot\,\rangle_{L^{2}}, norm ∥ ⋅ ∥L2\lVert\,\cdot\,\rVert_{L^{2}} and distance dL2d_{L^{2}}, are the ones fixed there. The real vector space Map(Zn,R)\mathrm{Map}(\mathbb{Z}^{n},\mathbb{R}) of coefficient families, the Fourier coefficient family U^\hat{U} of a class UU, the classes EkE_{k}, the enumerations κ\kappa of the lattice, the Fourier weights μk\mu_{k}, the positive numbers ρk\rho_{k} with ρk2=1μk\rho_{k}^{2}=\tfrac{1}{\mu_{k}}, and the natural powers tlt^{l} of real numbers, in particular ρkl\rho_{k}^{l} and μkl\mu_{k}^{l} for l∈Nl\in\mathbb{N}, with t2=ttt^{2}=tt, are as in Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families. For l∈Nl\in\mathbb{N}, H−l(Tn)H^{-l}(\mathbb{T}^{n}) is the Sobolev space of order −l-l with its realisation map Λl\Lambda_{l} and its inner product ⟨ ⋅ ,⋅ ⟩H−l\langle\,\cdot\,,\cdot\,\rangle_{H^{-l}}, norm ∣⋅∣H−l|\cdot|_{H^{-l}} and distance dH−ld_{H^{-l}}; in claim 6, H−(m+1)(Tn)H^{-(m+1)}(\mathbb{T}^{n}) and ∣⋅∣H−(m+1)|\cdot|_{H^{-(m+1)}} are these for l=m+1l=m+1. Series of real numbers and series in a real inner product space are as defined there. Let m∈Nm\in\mathbb{N}. Then the following hold.

1. (The weights) For every k∈Znk\in\mathbb{Z}^{n}: ρk≤1\rho_{k}\le1, 0<ρkm≤10<\rho_{k}^{m}\le1, ρkm+1=ρkmρk\rho_{k}^{m+1}=\rho_{k}^{m}\rho_{k}, and (ρkm)2 μkm=1(\rho_{k}^{m})^{2}\,\mu_{k}^{m}=1, so that (ρkm)2=1μkm(\rho_{k}^{m})^{2}=\tfrac{1}{\mu_{k}^{m}}.

2. (Hilbert space) H−m(Tn)H^{-m}(\mathbb{T}^{n}) with ⟨ ⋅ ,⋅ ⟩H−m\langle\,\cdot\,,\cdot\,\rangle_{H^{-m}} is a real Hilbert space, and the metric space (H−m(Tn),dH−m)(H^{-m}(\mathbb{T}^{n}),d_{H^{-m}}) is separable. The realisation map Λm\Lambda_{m} is a linear bijection from H−m(Tn)H^{-m}(\mathbb{T}^{n}) onto L2(Tn)L^{2}(\mathbb{T}^{n}), and

∣c∣H−m=∥Λmc∥L2,dH−m(c,d)=dL2(Λmc,Λmd)for all c,d∈H−m(Tn).|c|_{H^{-m}}=\lVert\Lambda_{m}c\rVert_{L^{2}},\qquad d_{H^{-m}}(c,d)=d_{L^{2}}(\Lambda_{m}c,\Lambda_{m}d)\qquad\text{for all }c,d\in H^{-m}(\mathbb{T}^{n}).

3. (The square-integrable classes embed) Let U∈L2(Tn)U\in L^{2}(\mathbb{T}^{n}). Then U^∈H−m(Tn)\hat{U}\in H^{-m}(\mathbb{T}^{n}) and ∣U^∣H−m≤∥U∥L2|\hat{U}|_{H^{-m}}\le\lVert U\rVert_{L^{2}}; for every enumeration κ\kappa the series ∑j=1∞ρκ(j)m U^(κ(j)) Eκ(j)\sum_{j=1}^{\infty}\rho_{\kappa(j)}^{m}\,\hat{U}(\kappa(j))\,E_{\kappa(j)} converges in L2(Tn)L^{2}(\mathbb{T}^{n}) with sum ΛmU^\Lambda_{m}\hat{U}. The map U↦U^U\mapsto\hat{U} from L2(Tn)L^{2}(\mathbb{T}^{n}) to H−m(Tn)H^{-m}(\mathbb{T}^{n}) is linear and injective: if U,U′∈L2(Tn)U,U'\in L^{2}(\mathbb{T}^{n}) satisfy U^=U^′\hat{U}=\hat{U}', then U=U′U=U'. Moreover, for every k∈Znk\in\mathbb{Z}^{n},

ΛmE^k=ρkm Ek,∣E^k∣H−m=ρkm.\Lambda_{m}\hat{E}_{k}=\rho_{k}^{m}\,E_{k},\qquad |\hat{E}_{k}|_{H^{-m}}=\rho_{k}^{m}.

4. (The rescaled trigonometric basis) For k∈Znk\in\mathbb{Z}^{n} let ζm,k\zeta_{m,k} be the unique element of H−m(Tn)H^{-m}(\mathbb{T}^{n}) with Λmζm,k=Ek\Lambda_{m}\zeta_{m,k}=E_{k}. Then ζm,k(k′)\zeta_{m,k}(k') equals 1ρkm\tfrac{1}{\rho_{k}^{m}} if k′=kk'=k and equals 00 if k′≠kk'\ne k; for every c∈H−m(Tn)c\in H^{-m}(\mathbb{T}^{n}),

⟨c,ζm,k⟩H−m=ρkm c(k);\langle c,\zeta_{m,k}\rangle_{H^{-m}}=\rho_{k}^{m}\,c(k);

and for every enumeration κ\kappa the sequence (ζm,κ(j))j∈N(\zeta_{m,\kappa(j)})_{j\in\mathbb{N}} is an orthonormal basis of H−m(Tn)H^{-m}(\mathbb{T}^{n}).

5. (Membership and the inner product as series) Let κ\kappa be an enumeration. A coefficient family c∈Map(Zn,R)c\in\mathrm{Map}(\mathbb{Z}^{n},\mathbb{R}) belongs to H−m(Tn)H^{-m}(\mathbb{T}^{n}) if and only if the series ∑j=1∞(ρκ(j)m)2 c(κ(j))2\sum_{j=1}^{\infty}(\rho_{\kappa(j)}^{m})^{2}\,c(\kappa(j))^{2} converges. For c,d∈H−m(Tn)c,d\in H^{-m}(\mathbb{T}^{n}) the series ∑j=1∞(ρκ(j)m)2 c(κ(j)) d(κ(j))\sum_{j=1}^{\infty}(\rho_{\kappa(j)}^{m})^{2}\,c(\kappa(j))\,d(\kappa(j)) converges with sum ⟨c,d⟩H−m\langle c,d\rangle_{H^{-m}}; in particular (∣c∣H−m)2=∑j=1∞(ρκ(j)m)2 c(κ(j))2(|c|_{H^{-m}})^{2}=\sum_{j=1}^{\infty}(\rho_{\kappa(j)}^{m})^{2}\,c(\kappa(j))^{2}.

6. (The scale) H−m(Tn)⊆H−(m+1)(Tn)H^{-m}(\mathbb{T}^{n})\subseteq H^{-(m+1)}(\mathbb{T}^{n}), and ∣c∣H−(m+1)≤∣c∣H−m|c|_{H^{-(m+1)}}\le|c|_{H^{-m}} for every c∈H−m(Tn)c\in H^{-m}(\mathbb{T}^{n}).

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