TheoremBase

The weight identities are elementary properties of natural powers; the Hilbert structure, the isometry and the orthonormal basis are the transport lemma applied to the realisation map; the embedding of the square-integrable classes and the series form of membership and of the inner product come from Parseval and Riesz-Fischer along an enumeration; and the inclusion of the scale is the comparison test for the weighted series.

Proof

Each result cited is universally quantified over the data in its own statement, and so are the claims of the present lemma, which is stated for an arbitrary m∈Nm\in\mathbb{N}; claim 5 is applied below with m+1m+1 in place of mm. Write Λ=Λm\Lambda=\Lambda_{m}. Two coefficient families are equal exactly when their values agree at every point of Zn\mathbb{Z}^{n}. By The Negative-Order Sobolev Spaces of the Torus (i), a family cc lies in H−m(Tn)H^{-m}(\mathbb{T}^{n}) exactly when some class WW has W^(k)=ρkmc(k)\hat{W}(k)=\rho_{k}^{m}c(k) for every kk, and then Λc\Lambda c is that class; by Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (vi), Λ\Lambda is a linear bijection from the real vector space H−m(Tn)H^{-m}(\mathbb{T}^{n}) onto L2(Tn)L^{2}(\mathbb{T}^{n}), and by The Negative-Order Sobolev Spaces of the Torus (ii), ⟨c,d⟩H−m=⟨Λc,Λd⟩L2\langle c,d\rangle_{H^{-m}}=\langle\Lambda c,\Lambda d\rangle_{L^{2}}. Hence Transport of an Inner Product and of Hilbert Space Structure along a Linear Bijection applies with X=H−m(Tn)X=H^{-m}(\mathbb{T}^{n}), E=L2(Tn)E=L^{2}(\mathbb{T}^{n}) and T=ΛT=\Lambda, its transported inner product being ⟨ ⋅ ,⋅ ⟩H−m\langle\,\cdot\,,\cdot\,\rangle_{H^{-m}}, and its T−1T^{-1} the inverse Λ−1\Lambda^{-1}, which sends W∈L2(Tn)W\in L^{2}(\mathbb{T}^{n}) to the unique cc with Λc=W\Lambda c=W, by Bijection of Sets and claim 1 of that lemma. Squares of real numbers satisfy (ab)2=a2b2(ab)^{2}=a^{2}b^{2} by claim 3 of Properties of Natural Number Powers in a Field, and 0≤t20\le t^{2} for every real tt by claim 2 of Nonnegativity of Squares in an Ordered Field; the multiplicative inverse of a positive real number exists and is positive by claim 7 of Elementary Order Arithmetic in an Ordered Field.

Claim 1. Fix k∈Znk\in\mathbb{Z}^{n}. The number ρk\rho_{k} is positive, as recorded in Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families. Since 1≤μk1\le\mu_{k} by Summability of the Negative Powers of the Fourier Weights of the Torus (i) and 0≤μk−10\le\mu_{k}^{-1} by claim 7 of Elementary Order Arithmetic in an Ordered Field, claim 5 of Elementary Arithmetic in an Ordered Field gives ρk2=μk−1⋅1≤μk−1μk=1=12\rho_{k}^{2}=\mu_{k}^{-1}\cdot1\le\mu_{k}^{-1}\mu_{k}=1=1^{2}; as 0≤ρk0\le\rho_{k} and 0≤10\le1, claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field gives ρk≤1\rho_{k}\le1. By claim 5 of Properties of Natural Number Powers in a Field, 0≤ρkm0\le\rho_{k}^{m} and ρkm≤1m\rho_{k}^{m}\le1^{m}, and 1m=11^{m}=1 by claim 2 of that lemma; by claim 4 of that lemma ρkm≠0\rho_{k}^{m}\ne0, so 0<ρkm0<\rho_{k}^{m}. By claim 1 of that lemma, with S(m)=m+1S(m)=m+1 from Natural Numbers, ρkm+1=ρkmρk\rho_{k}^{m+1}=\rho_{k}^{m}\rho_{k}. Finally, by claim 3 of Properties of Natural Number Powers in a Field applied twice, (ρkm)2=ρkmρkm=(ρkρk)m=(μk−1)m(\rho_{k}^{m})^{2}=\rho_{k}^{m}\rho_{k}^{m}=(\rho_{k}\rho_{k})^{m}=(\mu_{k}^{-1})^{m} and (μk−1)mμkm=(μk−1μk)m=1m=1(\mu_{k}^{-1})^{m}\mu_{k}^{m}=(\mu_{k}^{-1}\mu_{k})^{m}=1^{m}=1; since μkm≠0\mu_{k}^{m}\ne0 by claim 4 of that lemma, (ρkm)2(\rho_{k}^{m})^{2} is the multiplicative inverse of μkm\mu_{k}^{m}, that is, (ρkm)2=1μkm(\rho_{k}^{m})^{2}=\tfrac{1}{\mu_{k}^{m}}.

Claim 2. By Transport of an Inner Product and of Hilbert Space Structure along a Linear Bijection (i), ∣c∣H−m=∥Λc∥L2|c|_{H^{-m}}=\lVert\Lambda c\rVert_{L^{2}} and dH−m(c,d)=dL2(Λc,Λd)d_{H^{-m}}(c,d)=d_{L^{2}}(\Lambda c,\Lambda d), the norm and distance of L2(Tn)L^{2}(\mathbb{T}^{n}) being those of its inner product by L²(μ) Is a Real Hilbert Space (i). Since L2(Tn)L^{2}(\mathbb{T}^{n}) is a real Hilbert space by L²(μ) Is a Real Hilbert Space (ii), Transport of an Inner Product and of Hilbert Space Structure along a Linear Bijection (iii) shows that H−m(Tn)H^{-m}(\mathbb{T}^{n}) with ⟨ ⋅ ,⋅ ⟩H−m\langle\,\cdot\,,\cdot\,\rangle_{H^{-m}} is a real Hilbert space. That Λ\Lambda is a linear bijection is Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (vi). Separability is proved after claim 4.

Claim 3. Let U∈L2(Tn)U\in L^{2}(\mathbb{T}^{n}) and let κ\kappa be an enumeration. Define the family c~∈Map(Zn,R)\tilde{c}\in\mathrm{Map}(\mathbb{Z}^{n},\mathbb{R}) by c~(k)=ρkmU^(k)\tilde{c}(k)=\rho_{k}^{m}\hat{U}(k). By Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (iv) the series ∑j=1∞U^(κ(j))2\sum_{j=1}^{\infty}\hat{U}(\kappa(j))^{2} converges with sum (∥U∥L2)2(\lVert U\rVert_{L^{2}})^{2}. For every jj, c~(κ(j))2=(ρκ(j)m)2U^(κ(j))2\tilde{c}(\kappa(j))^{2}=(\rho_{\kappa(j)}^{m})^{2}\hat{U}(\kappa(j))^{2}, where 0≤U^(κ(j))20\le\hat{U}(\kappa(j))^{2} and 0≤c~(κ(j))20\le\tilde{c}(\kappa(j))^{2} by claim 2 of Nonnegativity of Squares in an Ordered Field, and (ρκ(j)m)2≤1=12(\rho_{\kappa(j)}^{m})^{2}\le1=1^{2} by claim 1 and claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field; hence c~(κ(j))2≤U^(κ(j))2\tilde{c}(\kappa(j))^{2}\le\hat{U}(\kappa(j))^{2} by claim 5 of Elementary Arithmetic in an Ordered Field, the multiplier U^(κ(j))2\hat{U}(\kappa(j))^{2} being nonnegative. By Series of Nonnegative Real Numbers, Comparison, and the Geometric Series (iii), ∑j=1∞c~(κ(j))2\sum_{j=1}^{\infty}\tilde{c}(\kappa(j))^{2} converges with sum at most (∥U∥L2)2(\lVert U\rVert_{L^{2}})^{2}. By Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (v) there is exactly one W∈L2(Tn)W\in L^{2}(\mathbb{T}^{n}) with W^=c~\hat{W}=\tilde{c}, namely the sum of the convergent series ∑j=1∞c~(κ(j))Eκ(j)=∑j=1∞ρκ(j)mU^(κ(j))Eκ(j)\sum_{j=1}^{\infty}\tilde{c}(\kappa(j))E_{\kappa(j)}=\sum_{j=1}^{\infty}\rho_{\kappa(j)}^{m}\hat{U}(\kappa(j))E_{\kappa(j)}, and (∥W∥L2)2=∑j=1∞c~(κ(j))2≤(∥U∥L2)2(\lVert W\rVert_{L^{2}})^{2}=\sum_{j=1}^{\infty}\tilde{c}(\kappa(j))^{2}\le(\lVert U\rVert_{L^{2}})^{2}. Since W^(k)=ρkmU^(k)\hat{W}(k)=\rho_{k}^{m}\hat{U}(k) for every kk, the family U^\hat{U} lies in H−m(Tn)H^{-m}(\mathbb{T}^{n}) with ΛU^=W\Lambda\hat{U}=W; this gives the series representation of ΛU^\Lambda\hat{U}, and (∣U^∣H−m)2=(∥W∥L2)2≤(∥U∥L2)2(|\hat{U}|_{H^{-m}})^{2}=(\lVert W\rVert_{L^{2}})^{2}\le(\lVert U\rVert_{L^{2}})^{2} by claim 2, whence ∣U^∣H−m≤∥U∥L2|\hat{U}|_{H^{-m}}\le\lVert U\rVert_{L^{2}} by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field, both norms being nonnegative by Real Inner Product Spaces (ii). The map U↦U^U\mapsto\hat{U}, now regarded as a map into the vector space H−m(Tn)H^{-m}(\mathbb{T}^{n}), whose operations are those of Map(Zn,R)\mathrm{Map}(\mathbb{Z}^{n},\mathbb{R}) by The Negative-Order Sobolev Spaces of the Torus (i), is linear by Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (i) and satisfies U^=U^′\hat{U}=\hat{U}' only if U=U′U=U' by Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (ii).

Now let k∈Znk\in\mathbb{Z}^{n} and put W=ρkmEkW=\rho_{k}^{m}E_{k}. For k′∈Znk'\in\mathbb{Z}^{n}, Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (i) and Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (iii) give W^(k′)=ρkmE^k(k′)\hat{W}(k')=\rho_{k}^{m}\hat{E}_{k}(k'), which equals ρkm\rho_{k}^{m} if k′=kk'=k and 00 otherwise; and ρk′mE^k(k′)\rho_{k'}^{m}\hat{E}_{k}(k') takes the same two values. So W^(k′)=ρk′mE^k(k′)\hat{W}(k')=\rho_{k'}^{m}\hat{E}_{k}(k') for every k′k', and by uniqueness ΛE^k=W=ρkmEk\Lambda\hat{E}_{k}=W=\rho_{k}^{m}E_{k}. Hence, by claim 2, Elementary Identities in a Real Inner Product Space (iv), Absolute Value in an Ordered Field with 0<ρkm0<\rho_{k}^{m}, and ∥Ek∥L2=1\lVert E_{k}\rVert_{L^{2}}=1 from The Trigonometric System on the Torus is Orthonormal (iii) and Real Inner Product Spaces (ii), ∣E^k∣H−m=∥ρkmEk∥L2=ρkm∥Ek∥L2=ρkm|\hat{E}_{k}|_{H^{-m}}=\lVert\rho_{k}^{m}E_{k}\rVert_{L^{2}}=\rho_{k}^{m}\lVert E_{k}\rVert_{L^{2}}=\rho_{k}^{m}.

Claim 4. Let k∈Znk\in\mathbb{Z}^{n}. Since Λ\Lambda is a bijection, there is exactly one ζm,k∈H−m(Tn)\zeta_{m,k}\in H^{-m}(\mathbb{T}^{n}) with Λζm,k=Ek\Lambda\zeta_{m,k}=E_{k}, and it is the value at EkE_{k} of the map T−1T^{-1} of Transport of an Inner Product and of Hilbert Space Structure along a Linear Bijection. By The Negative-Order Sobolev Spaces of the Torus (i), E^k(k′)=ρk′mζm,k(k′)\hat{E}_{k}(k')=\rho_{k'}^{m}\zeta_{m,k}(k') for every k′k'; multiplying by (ρk′m)−1(\rho_{k'}^{m})^{-1}, which exists because 0<ρk′m0<\rho_{k'}^{m} by claim 1, and using Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (iii), ζm,k(k′)\zeta_{m,k}(k') equals (ρkm)−1=1ρkm(\rho_{k}^{m})^{-1}=\tfrac{1}{\rho_{k}^{m}} if k′=kk'=k and 00 otherwise. For c∈H−m(Tn)c\in H^{-m}(\mathbb{T}^{n}), by The Negative-Order Sobolev Spaces of the Torus (ii) and The Fourier Coefficients of a Square-Integrable Class on the Torus (i), ⟨c,ζm,k⟩H−m=⟨Λc,Ek⟩L2=Λc^(k)=ρkmc(k)\langle c,\zeta_{m,k}\rangle_{H^{-m}}=\langle\Lambda c,E_{k}\rangle_{L^{2}}=\widehat{\Lambda c}(k)=\rho_{k}^{m}c(k), the last by The Negative-Order Sobolev Spaces of the Torus (i). Finally let κ\kappa be an enumeration. By The Trigonometric System is an Orthonormal Basis of the Square-Integrable Space of the Torus (ii), (Eκ(j))j∈N(E_{\kappa(j)})_{j\in\mathbb{N}} is an orthonormal basis of L2(Tn)L^{2}(\mathbb{T}^{n}), so Transport of an Inner Product and of Hilbert Space Structure along a Linear Bijection (iv) shows that (T−1Eκ(j))j∈N=(ζm,κ(j))j∈N(T^{-1}E_{\kappa(j)})_{j\in\mathbb{N}}=(\zeta_{m,\kappa(j)})_{j\in\mathbb{N}} is an orthonormal basis of H−m(Tn)H^{-m}(\mathbb{T}^{n}).

Separability. An enumeration exists by The Integer Lattice Admits an Enumeration by the Natural Numbers (ii), so claim 4 furnishes an orthonormal basis of the real Hilbert space H−m(Tn)H^{-m}(\mathbb{T}^{n}), and A Real Hilbert Space with an Orthonormal Basis is Separable (ii) shows that (H−m(Tn),dH−m)(H^{-m}(\mathbb{T}^{n}),d_{H^{-m}}) is separable. This completes claim 2.

Claim 5. Let κ\kappa be an enumeration, let c∈Map(Zn,R)c\in\mathrm{Map}(\mathbb{Z}^{n},\mathbb{R}), and define c~∈Map(Zn,R)\tilde{c}\in\mathrm{Map}(\mathbb{Z}^{n},\mathbb{R}) by c~(k)=ρkmc(k)\tilde{c}(k)=\rho_{k}^{m}c(k), so that c~(κ(j))2=(ρκ(j)m)2c(κ(j))2\tilde{c}(\kappa(j))^{2}=(\rho_{\kappa(j)}^{m})^{2}c(\kappa(j))^{2} for every jj. If c∈H−m(Tn)c\in H^{-m}(\mathbb{T}^{n}), then Λc^=c~\widehat{\Lambda c}=\tilde{c}, and Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (iv) shows that ∑j=1∞c~(κ(j))2\sum_{j=1}^{\infty}\tilde{c}(\kappa(j))^{2} converges. Conversely, if that series converges, Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (v) furnishes W∈L2(Tn)W\in L^{2}(\mathbb{T}^{n}) with W^=c~\hat{W}=\tilde{c}, so c∈H−m(Tn)c\in H^{-m}(\mathbb{T}^{n}) by The Negative-Order Sobolev Spaces of the Torus (i). Now let c,d∈H−m(Tn)c,d\in H^{-m}(\mathbb{T}^{n}). By The Negative-Order Sobolev Spaces of the Torus (ii) and Properties of the Fourier Coefficients on the Torus, and the Realisation of Weighted Coefficient Families (iv), applied to Λc\Lambda c and Λd\Lambda d,

⟨c,d⟩H−m=⟨Λc,Λd⟩L2=∑j=1∞Λc^(κ(j)) Λd^(κ(j))=∑j=1∞(ρκ(j)m)2 c(κ(j)) d(κ(j)),\langle c,d\rangle_{H^{-m}}=\langle\Lambda c,\Lambda d\rangle_{L^{2}}=\sum_{j=1}^{\infty}\widehat{\Lambda c}(\kappa(j))\,\widehat{\Lambda d}(\kappa(j))=\sum_{j=1}^{\infty}(\rho_{\kappa(j)}^{m})^{2}\,c(\kappa(j))\,d(\kappa(j)),

the series converging, since Λc^(k)Λd^(k)=ρkmc(k)ρkmd(k)=(ρkm)2c(k)d(k)\widehat{\Lambda c}(k)\widehat{\Lambda d}(k)=\rho_{k}^{m}c(k)\rho_{k}^{m}d(k)=(\rho_{k}^{m})^{2}c(k)d(k). Taking d=cd=c and using (∣c∣H−m)2=⟨c,c⟩H−m(|c|_{H^{-m}})^{2}=\langle c,c\rangle_{H^{-m}} from Real Inner Product Spaces (ii) gives the last assertion.

Claim 6. Let c∈H−m(Tn)c\in H^{-m}(\mathbb{T}^{n}) and let κ\kappa be an enumeration, which exists by The Integer Lattice Admits an Enumeration by the Natural Numbers (ii). By claim 5, ∑j=1∞(ρκ(j)m)2c(κ(j))2\sum_{j=1}^{\infty}(\rho_{\kappa(j)}^{m})^{2}c(\kappa(j))^{2} converges with sum (∣c∣H−m)2(|c|_{H^{-m}})^{2}. For every kk, claim 1 gives (ρkm+1)2=(ρkmρk)2=(ρkm)2ρk2(\rho_{k}^{m+1})^{2}=(\rho_{k}^{m}\rho_{k})^{2}=(\rho_{k}^{m})^{2}\rho_{k}^{2} with ρk2≤1=12\rho_{k}^{2}\le1=1^{2} by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field applied to 0≤ρk≤10\le\rho_{k}\le1; hence, since 0≤(ρkm+1)2c(k)20\le(\rho_{k}^{m+1})^{2}c(k)^{2} and 0≤(ρkm)2c(k)20\le(\rho_{k}^{m})^{2}c(k)^{2} by claim 2 of Nonnegativity of Squares in an Ordered Field and claim 3 of Properties of Natural Number Powers in a Field, claim 5 of Elementary Arithmetic in an Ordered Field with the nonnegative multiplier (ρkm)2c(k)2(\rho_{k}^{m})^{2}c(k)^{2} gives

0≤(ρkm+1)2c(k)2=ρk2 (ρkm)2c(k)2≤(ρkm)2c(k)2.0\le(\rho_{k}^{m+1})^{2}c(k)^{2}=\rho_{k}^{2}\,(\rho_{k}^{m})^{2}c(k)^{2}\le(\rho_{k}^{m})^{2}c(k)^{2}.

By Series of Nonnegative Real Numbers, Comparison, and the Geometric Series (iii), ∑j=1∞(ρκ(j)m+1)2c(κ(j))2\sum_{j=1}^{\infty}(\rho_{\kappa(j)}^{m+1})^{2}c(\kappa(j))^{2} converges with sum at most (∣c∣H−m)2(|c|_{H^{-m}})^{2}. By claim 5 applied with m+1m+1 in place of mm, c∈H−(m+1)(Tn)c\in H^{-(m+1)}(\mathbb{T}^{n}) and (∣c∣H−(m+1))2(|c|_{H^{-(m+1)}})^{2} is that sum, so (∣c∣H−(m+1))2≤(∣c∣H−m)2(|c|_{H^{-(m+1)}})^{2}\le(|c|_{H^{-m}})^{2}, and ∣c∣H−(m+1)≤∣c∣H−m|c|_{H^{-(m+1)}}\le|c|_{H^{-m}} by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field, both norms being nonnegative.

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