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Proof of The Fejer Means of a Continuous Periodic Function on the Torus

lemmalem:fejer-mean-torus-2026a
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Β· 7,392 chars Β· 27 deps Β· depth 30 Reason: Proof of the Fejer mean lemma (Block D).

An enumeration of the index set turns the Fejer mean into a finite linear combination of trigonometric system functions, to which the finite-combination lemma applies; the integral representation is the reproducing identity integrated term by term, and the mass is the representation applied to the constant function, where orthonormality kills every term but one.

Proof

Each result cited is universally quantified over the data in its own statement. The exponent of Continuous Periodic Functions are Power-Integrable and Dense on the Torus is taken to be p=2p=2 throughout, and ΞΉ\iota denotes the canonical map from N\mathbb{N} to R\mathbb{R}.

An enumeration of the index set. The set [2N+1]n[2N+1]^{n} is nonempty and finite by claim 3 of Finiteness of Cartesian Products, Tuple Sets, and Permutation Sets, as recorded in The Reproducing Identity for the Fejer Kernels of the Torus; being nonempty and finite, it has MM elements for some M∈NM\in\mathbb{N}, unique by Uniqueness of the Number of Elements, and there is a bijection Ο†:[M]β†’[2N+1]n\varphi:[M]\to[2N+1]^{n}. Fix one. By Sum over a Finite Index Set, for every map f:[2N+1]nβ†’Rf:[2N+1]^{n}\to\mathbb{R},

βˆ‘a∈[2N+1]nf(a)=βˆ‘j=1Mf(Ο†(j)).\sum_{a\in[2N+1]^{n}}f(a)=\sum_{j=1}^{M}f(\varphi(j)).

For j∈[M]j\in[M] write kj=k(Ο†(j))∈Znk_{j}=k(\varphi(j))\in\mathbb{Z}^{n}, Wj=WN,Ο†(j)W_{j}=W_{N,\varphi(j)} and u^j=⟨[ u∣Q ],Ekj⟩L2\hat{u}_{j}=\langle[\,u|_{Q}\,],E_{k_{j}}\rangle_{L^{2}}. Applying the display to the map a↦WN,a⟨[ u∣Q ],Ek(a)⟩L2ek(a)(x)a\mapsto W_{N,a}\langle[\,u|_{Q}\,],E_{k(a)}\rangle_{L^{2}}e_{k(a)}(x) for each fixed xx gives

ΟƒNu(x)=βˆ‘j=1M(Wju^j) ekj(x)(x∈Rn),\sigma_{N}u(x)=\sum_{j=1}^{M}\bigl(W_{j}\hat{u}_{j}\bigr)\,e_{k_{j}}(x)\qquad(x\in\mathbb{R}^{n}),

and each ekje_{k_{j}} lies in CperC_{\mathrm{per}} by The Trigonometric System on the Torus is Orthonormal Β§classes.

Claim 1. By the last display, ΟƒNu\sigma_{N}u is the map of Finite Linear Combinations of Continuous Periodic Functions and Their Classes on the Torus formed with the coefficients cj=Wju^jc_{j}=W_{j}\hat{u}_{j} and the maps gj=ekjg_{j}=e_{k_{j}}, so ΟƒNu∈Cper\sigma_{N}u\in C_{\mathrm{per}} by Finite Linear Combinations of Continuous Periodic Functions and Their Classes on the Torus Β§member.

Claim 2. Let U∈L2(Tn)U\in L^{2}(\mathbb{T}^{n}). With the same data, Finite Linear Combinations of Continuous Periodic Functions and Their Classes on the Torus §pairing gives

⟨U,[ (ΟƒNu)∣Q ]⟩L2=βˆ‘j=1MWju^jβ€‰βŸ¨U,Ekj⟩L2,\bigl\langle U,[\,(\sigma_{N}u)|_{Q}\,]\bigr\rangle_{L^{2}}=\sum_{j=1}^{M}W_{j}\hat{u}_{j}\,\langle U,E_{k_{j}}\rangle_{L^{2}},

since [ ekj∣Q ]=Ekj[\,e_{k_{j}}|_{Q}\,]=E_{k_{j}}. By the first display, applied to the map a↦WN,a⟨[ u∣Q ],Ek(a)⟩L2⟨U,Ek(a)⟩L2a\mapsto W_{N,a}\langle[\,u|_{Q}\,],E_{k(a)}\rangle_{L^{2}}\langle U,E_{k(a)}\rangle_{L^{2}}, the right-hand side is the sum over [2N+1]n[2N+1]^{n} asserted in claim 2.

Claim 3. Fix x∈Rnx\in\mathbb{R}^{n} and let y∈Rny\in\mathbb{R}^{n}. By The Reproducing Identity for the Fejer Kernels of the Torus §product, applied to the pair of points y,xy,x, and the first display,

Ξ¦N(yβˆ’x)=βˆ‘a∈[2N+1]nWN,a ek(a)(y) ek(a)(x)=βˆ‘j=1MWj ekj(y) ekj(x).\Phi_{N}(y-x)=\sum_{a\in[2N+1]^{n}}W_{N,a}\,e_{k(a)}(y)\,e_{k(a)}(x)=\sum_{j=1}^{M}W_{j}\,e_{k_{j}}(y)\,e_{k_{j}}(x).

Multiplying by the real number 1Q(y)u(y)\mathbf{1}_{Q}(y)u(y) and moving it inside the sum by the homogeneity of finite sums, claim 3 of Properties of Finite Sums, then rearranging each summand by the commutativity and associativity of multiplication, gives

1Q(y) ΦN(yβˆ’x) u(y)=βˆ‘j=1MΞ²j hj(y),Ξ²j=Wj ekj(x),hj=1Q ekj u,\mathbf{1}_{Q}(y)\,\Phi_{N}(y-x)\,u(y)=\sum_{j=1}^{M}\beta_{j}\,h_{j}(y),\qquad \beta_{j}=W_{j}\,e_{k_{j}}(x),\quad h_{j}=\mathbf{1}_{Q}\,e_{k_{j}}\,u,

where hj:Rnβ†’Rh_{j}:\mathbb{R}^{n}\to\mathbb{R} is the pointwise product. For each j∈[M]j\in[M] the map ekjue_{k_{j}}u lies in CperC_{\mathrm{per}} by Elementary Properties of Lattice-Periodic Functions Β§algebra, so by Continuous Periodic Functions are Power-Integrable and Dense on the Torus Β§integral the map hj=1Q(ekju)h_{j}=\mathbf{1}_{Q}(e_{k_{j}}u) is measurable and integrable, and

∫Rnhj dΞ»n=∫Tn(ekju)∣Q dx.\int_{\mathbb{R}^{n}}h_{j}\,d\lambda_{n}=\int_{\mathbb{T}^{n}}(e_{k_{j}}u)|_{Q}\,dx .

The restriction (ekju)∣Q(e_{k_{j}}u)|_{Q} is the pointwise product of ekj∣Qe_{k_{j}}|_{Q} and u∣Qu|_{Q}, both of which lie in L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}) by Continuous Periodic Functions are Power-Integrable and Dense on the Torus Β§member; so by The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space Β§inner-product the right-hand side equals ⟨Ekj,[ u∣Q ]⟩L2\langle E_{k_{j}},[\,u|_{Q}\,]\rangle_{L^{2}}, which is u^j\hat{u}_{j} by the symmetry of the inner product, condition (a) of Real Inner Product Space Β§inner-product. Now Linearity of the Lebesgue Integral over a Finite Sum of Integrable Functions, applied to the integrable maps hjh_{j} and the coefficients Ξ²j\beta_{j}, shows by its clause Linearity of the Lebesgue Integral over a Finite Sum of Integrable Functions Β§integrable that y↦1Q(y)Ξ¦N(yβˆ’x)u(y)y\mapsto\mathbf{1}_{Q}(y)\Phi_{N}(y-x)u(y) is measurable and integrable, and by Linearity of the Lebesgue Integral over a Finite Sum of Integrable Functions Β§linear that

∫Rn1Q(y) ΦN(yβˆ’x) u(y) dΞ»n(y)=βˆ‘j=1MΞ²ju^j=βˆ‘j=1M(Wju^j)ekj(x)=ΟƒNu(x),\int_{\mathbb{R}^{n}}\mathbf{1}_{Q}(y)\,\Phi_{N}(y-x)\,u(y)\,d\lambda_{n}(y)=\sum_{j=1}^{M}\beta_{j}\hat{u}_{j}=\sum_{j=1}^{M}\bigl(W_{j}\hat{u}_{j}\bigr)e_{k_{j}}(x)=\sigma_{N}u(x),

the middle equality by commutativity of multiplication and the last by the second display.

Claim 4. Let 00 denote the origin of Rn\mathbb{R}^{n}, all of whose coordinates are 00; it lies in Zn\mathbb{Z}^{n} by Lattice-Periodic Functions and the Periodic Function Classes Β§lattice, since 0∈Z0\in\mathbb{Z} by claim 2 of Arithmetic, Order and Discreteness of the Integers. By The Trigonometric System on the Torus Β§one-dimensional and The Trigonometric System on the Torus Β§system, e0(y)=∏i=1nΟ•0(yi)=∏i=1n1=1e_{0}(y)=\prod_{i=1}^{n}\phi_{0}(y_{i})=\prod_{i=1}^{n}1=1 for every y∈Rny\in\mathbb{R}^{n}, the last step by claim 3 of Properties of Finite Products applied with i=1i=1 there, every factor other than the first being 11. Also e0∈Cpere_{0}\in C_{\mathrm{per}} by The Trigonometric System on the Torus is Orthonormal Β§classes.

Fix x∈Rnx\in\mathbb{R}^{n} and apply claim 3 to u=e0u=e_{0}: the map y↦1Q(y)Ξ¦N(yβˆ’x)e0(y)y\mapsto\mathbf{1}_{Q}(y)\Phi_{N}(y-x)e_{0}(y), which is y↦1Q(y)Ξ¦N(yβˆ’x)y\mapsto\mathbf{1}_{Q}(y)\Phi_{N}(y-x) because e0(y)=1e_{0}(y)=1, is measurable and integrable, and its integral equals ΟƒNe0(x)\sigma_{N}e_{0}(x). It remains to show ΟƒNe0(x)=1\sigma_{N}e_{0}(x)=1.

Let a0∈[2N+1]na^{0}\in[2N+1]^{n} be the tuple with ai0=N+1a^{0}_{i}=N+1 for every i∈[n]i\in[n]; here N+1∈[2N+1]N+1\in[2N+1] because N+1<(N+1)+N=N+(N+1)=2N+1N+1<(N+1)+N=N+(N+1)=2N+1 by claim 6 of Properties of the Order on the Natural Numbers and claim 4 of Arithmetic of Addition on the Natural Numbers, hence N+1≀2N+1N+1\le2N+1 by claim 1 of the former. The summands of ΟƒNe0(x)\sigma_{N}e_{0}(x) involve ⟨[ e0∣Q ],Ek(a)⟩L2=⟨E0,Ek(a)⟩L2\langle[\,e_{0}|_{Q}\,],E_{k(a)}\rangle_{L^{2}}=\langle E_{0},E_{k(a)}\rangle_{L^{2}}, since E0=[ e0∣Q ]E_{0}=[\,e_{0}|_{Q}\,] by The Trigonometric System on the Torus is Orthonormal Β§classes. For a∈[2N+1]na\in[2N+1]^{n}, by The Trigonometric System on the Torus is Orthonormal Β§orthonormal the number ⟨E0,Ek(a)⟩L2\langle E_{0},E_{k(a)}\rangle_{L^{2}} equals 11 if k(a)=0k(a)=0 and 00 otherwise. Now k(a)=0k(a)=0 holds exactly when k(a)i=0k(a)_{i}=0, that is ΞΉ(ai)=ΞΉ(N)+1=ΞΉ(N+1)\iota(a_{i})=\iota(N)+1=\iota(N+1), for every i∈[n]i\in[n], by claim 1 of Euclidean Points as Tuples of Real Numbers and claim 1 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field; by the injectivity of ΞΉ\iota, claim 7 of that lemma, this holds exactly when ai=N+1a_{i}=N+1 for every i∈[n]i\in[n], that is, exactly when a=a0a=a^{0}, two maps on [n][n] being equal when their values agree everywhere. Hence the summand WN,a⟨E0,Ek(a)⟩L2ek(a)(x)W_{N,a}\langle E_{0},E_{k(a)}\rangle_{L^{2}}e_{k(a)}(x) of ΟƒNe0(x)\sigma_{N}e_{0}(x) vanishes for every aβ‰ a0a\ne a^{0}, and claims 4 and 1 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set, applied with E={a0}E=\{a^{0}\}, give

ΟƒNe0(x)=WN,a0β€‰βŸ¨E0,E0⟩L2 e0(x)=WN,a0.\sigma_{N}e_{0}(x)=W_{N,a^{0}}\,\langle E_{0},E_{0}\rangle_{L^{2}}\,e_{0}(x)=W_{N,a^{0}} .

Finally, the integer attached to ai0=N+1a^{0}_{i}=N+1 in The Reproducing Identity for the Fejer Kernels of the Torus is ΞΉ(N+1)βˆ’ΞΉ(N)βˆ’1=0\iota(N+1)-\iota(N)-1=0, so wN,N+1=1βˆ’βˆ£0∣N=1w_{N,N+1}=1-\tfrac{|0|}{N}=1 by Absolute Value in an Ordered Field, and WN,a0=∏i=1n1=1W_{N,a^{0}}=\prod_{i=1}^{n}1=1 by claim 3 of Properties of Finite Products as above. This proves claim 4.

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