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Proof of Finite Linear Combinations of Continuous Periodic Functions and Their Classes on the Torus

lemmalem:finite-sum-continuous-periodic-torus-2026a
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Β· 3,775 chars Β· 9 deps Β· depth 25 Reason: Proof of the finite-combination lemma (Block D).

Induction on the number of summands, using the pairwise closure of the periodic class and the linearity of the restriction map; the pairing is then the linearity of the inner product in a finite sum.

Proof

Each result cited is universally quantified over the data in its own statement. Throughout, SS is the successor map of Natural Numbers, so that M+1=S(M)M+1=S(M); the exponent of Continuous Periodic Functions are Power-Integrable and Dense on the Torus is taken to be p=2p=2 throughout.

We prove claims 1 and 2 together by induction. Let TT be the set of those M∈NM\in\mathbb{N} for which the following holds: for every map c:[M]β†’Rc:[M]\to\mathbb{R} and every choice of gj∈Cperg_{j}\in C_{\mathrm{per}} for j∈[M]j\in[M], the map u(x)=βˆ‘j=1Mcjgj(x)u(x)=\sum_{j=1}^{M}c_{j}g_{j}(x) lies in CperC_{\mathrm{per}} and satisfies [ u∣Q ]=βˆ‘j=1Mcj[ gj∣Q ][\,u|_{Q}\,]=\sum_{j=1}^{M}c_{j}[\,g_{j}|_{Q}\,] in L2(Tn)L^{2}(\mathbb{T}^{n}). In the latter identity every class [ gj∣Q ][\,g_{j}|_{Q}\,] is defined, since gj∣Q∈L2(Tn)g_{j}|_{Q}\in\mathcal{L}^{2}(\mathbb{T}^{n}) by Continuous Periodic Functions are Power-Integrable and Dense on the Torus Β§member.

Base case. Let M=1M=1 and let cc and g1g_{1} be given. By claim 1 of Properties of Finite Sums, u(x)=c1g1(x)u(x)=c_{1}g_{1}(x) for every xx, so u=c1g1u=c_{1}g_{1} is the scalar multiple, which lies in CperC_{\mathrm{per}} by Elementary Properties of Lattice-Periodic Functions Β§algebra. By Continuous Periodic Functions are Power-Integrable and Dense on the Torus Β§linear, [ (c1g1)∣Q ]=c1[ g1∣Q ][\,(c_{1}g_{1})|_{Q}\,]=c_{1}[\,g_{1}|_{Q}\,], and this equals βˆ‘j=11cj[ gj∣Q ]\sum_{j=1}^{1}c_{j}[\,g_{j}|_{Q}\,] by claim 1 of Properties of Finite Sums of Vectors. So 1∈T1\in T.

Inductive step. Let M∈TM\in T, and let c:[M+1]β†’Rc:[M+1]\to\mathbb{R} and gj∈Cperg_{j}\in C_{\mathrm{per}} for j∈[M+1]j\in[M+1] be given. Let cβ€²c' be the restriction of cc to [M][M] and let v:Rnβ†’Rv:\mathbb{R}^{n}\to\mathbb{R} be the map v(x)=βˆ‘j=1Mcjβ€²gj(x)v(x)=\sum_{j=1}^{M}c'_{j}g_{j}(x). By the restriction and recursion clause, claim 1 of Properties of Finite Sums, for every x∈Rnx\in\mathbb{R}^{n}

u(x)=βˆ‘j=1M+1cjgj(x)=(βˆ‘j=1Mcjgj(x))+cM+1gM+1(x)=v(x)+cM+1gM+1(x),u(x)=\sum_{j=1}^{M+1}c_{j}g_{j}(x)=\Bigl(\sum_{j=1}^{M}c_{j}g_{j}(x)\Bigr)+c_{M+1}g_{M+1}(x)=v(x)+c_{M+1}g_{M+1}(x),

so u=v+cM+1gM+1u=v+c_{M+1}g_{M+1} is the pointwise sum of vv and the scalar multiple cM+1gM+1c_{M+1}g_{M+1}. Since M∈TM\in T, the map vv lies in CperC_{\mathrm{per}} and [ v∣Q ]=βˆ‘j=1Mcjβ€²[ gj∣Q ][\,v|_{Q}\,]=\sum_{j=1}^{M}c'_{j}[\,g_{j}|_{Q}\,]. The map cM+1gM+1c_{M+1}g_{M+1} lies in CperC_{\mathrm{per}} by Elementary Properties of Lattice-Periodic Functions Β§algebra, and so does the sum uu, by the same clause. By Continuous Periodic Functions are Power-Integrable and Dense on the Torus Β§linear, applied to the sum v+cM+1gM+1v+c_{M+1}g_{M+1} and to the scalar multiple cM+1gM+1c_{M+1}g_{M+1},

[ u∣Q ]=[ v∣Q ]+[ (cM+1gM+1)∣Q ]=(βˆ‘j=1Mcjβ€²[ gj∣Q ])+cM+1[ gM+1∣Q ]=βˆ‘j=1M+1cj[ gj∣Q ],[\,u|_{Q}\,]=[\,v|_{Q}\,]+[\,(c_{M+1}g_{M+1})|_{Q}\,]=\Bigl(\sum_{j=1}^{M}c'_{j}[\,g_{j}|_{Q}\,]\Bigr)+c_{M+1}[\,g_{M+1}|_{Q}\,]=\sum_{j=1}^{M+1}c_{j}[\,g_{j}|_{Q}\,],

the last equality by the restriction and recursion clause, claim 1 of Properties of Finite Sums of Vectors, applied in the vector space L2(Tn)L^{2}(\mathbb{T}^{n}) to the (M+1)(M+1)-tuple with components cj[ gj∣Q ]c_{j}[\,g_{j}|_{Q}\,]. Hence M+1∈TM+1\in T.

By Principle of Induction for the Natural Numbers, T=NT=\mathbb{N}. This proves claim 1, the membership u∣Q∈L2(Tn)u|_{Q}\in\mathcal{L}^{2}(\mathbb{T}^{n}) following from Continuous Periodic Functions are Power-Integrable and Dense on the Torus §member, and claim 2.

Claim 3. Let U∈L2(Tn)U\in L^{2}(\mathbb{T}^{n}). The space L2(Tn)L^{2}(\mathbb{T}^{n}) with βŸ¨β€‰β‹…β€‰,β‹…β€‰βŸ©L2\langle\,\cdot\,,\cdot\,\rangle_{L^{2}} is a real inner product space by The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space Β§inner-product. Let G∈L2(Tn)MG\in L^{2}(\mathbb{T}^{n})^{M} be the MM-tuple with components Gj=[ gj∣Q ]G_{j}=[\,g_{j}|_{Q}\,]. By claim 2, [ u∣Q ]=βˆ‘j=1McjGj[\,u|_{Q}\,]=\sum_{j=1}^{M}c_{j}G_{j}, so the second identity of Inner Products Against Finite Sums, and Orthonormal Families, in a Real Inner Product Space Β§combinations, applied with w=Uw=U, gives

⟨U,[ u∣Q ]⟩L2=⟨U,βˆ‘j=1McjGj⟩L2=βˆ‘j=1Mcj⟨U,Gj⟩L2=βˆ‘j=1Mcj⟨U,[ gj∣Q ]⟩L2.\bigl\langle U,[\,u|_{Q}\,]\bigr\rangle_{L^{2}}=\Bigl\langle U,\sum_{j=1}^{M}c_{j}G_{j}\Bigr\rangle_{L^{2}}=\sum_{j=1}^{M}c_{j}\langle U,G_{j}\rangle_{L^{2}}=\sum_{j=1}^{M}c_{j}\bigl\langle U,[\,g_{j}|_{Q}\,]\bigr\rangle_{L^{2}} .
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