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Proof of Uniform Convergence of the Fejer Means of a Continuous Periodic Function on the Torus

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· 17,598 chars · 35 deps · depth 31 Reason: Proof of uniform convergence of Fejer means (Block D).

The difference between the Fejer mean and the function is the cell integral of the translated kernel against the increment of the function; the part of the cell where the wrapped difference is far from the lattice is small by the far-field bound of the kernel, and on the rest the increment is small by uniform continuity and periodicity.

Proof

Each result cited is universally quantified over the data in its own statement. We use the notation of The Flat Torus: Standing Notation: the initial segments [n][n], points of Rn\mathbb{R}^{n} read as maps on [n][n], the sum and difference of points, formed coordinatewise, the Euclidean norm \lVert\,\cdot\,\rVert, the lattice Zn\mathbb{Z}^{n}, the cell Q={yRn:0yi<1 for every i[n]}Q=\{y\in\mathbb{R}^{n}:0\le y_{i}<1\text{ for every }i\in[n]\} of The Half-Open Unit Cell Tiles Euclidean Space §cell, which lies in B(Rn)\mathcal{B}(\mathbb{R}^{n}) by that clause, the wrapping map π\pi, the measure space (Q,BQ,λQ)(Q,\mathcal{B}_{Q},\lambda_{Q}) of The Flat Torus: Standing Notation §measure, which is the restriction of (Rn,B(Rn),λn)(\mathbb{R}^{n},\mathcal{B}(\mathbb{R}^{n}),\lambda_{n}) to QQ furnished by claim 1 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions, with the integral Tnvdx\int_{\mathbb{T}^{n}}v\,dx, and Lebesgue measure λn\lambda_{n} on B(Rn)\mathcal{B}(\mathbb{R}^{n}). Natural numbers are read in R\mathbb{R} through the canonical map ι\iota, and the quotient b/Nb/N of a real number bb by NNN\in\mathbb{N} is the one fixed in The Real Numbers: Standing Notation and Background §numbers, namely bι(N)1b\,\iota(N)^{-1}, the inverse existing by claim 3 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field. The symbol σNu\sigma_{N}u is the Fejer mean, not the constant σn\sigma_{n} of Euclidean Space and Lebesgue Measure: Standing Notation §sigma. Measurability and integrability of maps on Rn\mathbb{R}^{n}, and integrals Rn\int_{\mathbb{R}^{n}}, refer to (Rn,B(Rn),λn)(\mathbb{R}^{n},\mathcal{B}(\mathbb{R}^{n}),\lambda_{n}) as in The Fejer Means of a Continuous Periodic Function on the Torus; integrability includes measurability. 1A\mathbf{1}_{A} is the indicator of AA, and t|t| the absolute value of tRt\in\mathbb{R}. Since the sum and difference of points are formed coordinatewise and two points with the same coordinates are equal, by claim 1 of Euclidean Points as Tuples of Real Numbers, identities such as (ym)+m=y(y-m)+m=y and (ym)x=(yx)m(y-m)-x=(y-x)-m hold in Rn\mathbb{R}^{n} because they hold coordinatewise in the field R\mathbb{R}. Let ΦN\Phi_{N} be the Fejer kernel of the torus of order NN. Transitivity of \le on R\mathbb{R} is part of its being a total order, and the weak addition of inequalities aba\le b, cda+cb+dc\le d\Rightarrow a+c\le b+d follows from claims 2 and 3 of Elementary Arithmetic in an Ordered Field; both are used without further comment.

Fix uCperu\in C_{\mathrm{per}}. By Elementary Properties of Lattice-Periodic Functions §bounded there is a real number MM with 0M0\le M and u(z)M|u(z)|\le M for every zRnz\in\mathbb{R}^{n}.

The explicit statement. Let εR\varepsilon\in\mathbb{R} with 0<ε0<\varepsilon, and put θ=ε21\theta=\varepsilon\cdot2^{-1}, so that 0<θ0<\theta and θ+θ=ε\theta+\theta=\varepsilon by claim 8 of Elementary Order Arithmetic in an Ordered Field.

Step 1: uniform continuity. By A Continuous Lattice-Periodic Function is Uniformly Continuous §uniform, applied to uu and θ\theta, there is a real number rr with 0<r0<r such that u(z)u(z)θ|u(z)-u(z')|\le\theta for all z,zRnz,z'\in\mathbb{R}^{n} with zzr\lVert z-z'\rVert\le r.

Step 2: the choice of δ\delta. Put sn=i=1n1s_{n}=\sum_{i=1}^{n}1, a finite sum of real numbers. Since 010\le1 by claim 1 of Elementary Arithmetic in an Ordered Field, claim 6 of Properties of Finite Sums gives 1sn1\le s_{n}, hence 0<sn0<s_{n} by claim 6 and claim 2 of Elementary Order Arithmetic in an Ordered Field; so sn1s_{n}^{-1} exists and is positive by claim 7 of that lemma, and 0<rsn10<r\,s_{n}^{-1} by claim 5. Put δ1=2121\delta_{1}=2^{-1}\cdot2^{-1}, which is positive by claims 8 and 5 of Elementary Order Arithmetic in an Ordered Field and satisfies 2δ1=21<12\delta_{1}=2^{-1}<1, the inequality being claim 8 applied with ε=1\varepsilon=1 there. By claim 9 of Elementary Order Arithmetic in an Ordered Field let δ\delta be a least element of δ1\delta_{1} and rsn1r\,s_{n}^{-1}: δδ1\delta\le\delta_{1}, δrsn1\delta\le r\,s_{n}^{-1}, and δ\delta equals one of the two, so 0<δ0<\delta. Then 2δ2δ12\delta\le2\delta_{1} by claim 5 of Elementary Arithmetic in an Ordered Field, so 2δ<12\delta<1 by claim 2 of Elementary Order Arithmetic in an Ordered Field; and δsnrsn1sn=r\delta\,s_{n}\le r\,s_{n}^{-1}s_{n}=r by claim 5 of Elementary Arithmetic in an Ordered Field. Consequently also δ1δ\delta\le1-\delta, since δ+δ=2δ<1\delta+\delta=2\delta<1 gives δ<1δ\delta<1-\delta by claim 1 of Elementary Order Arithmetic in an Ordered Field.

Step 3: a norm bound. Let zRnz\in\mathbb{R}^{n} satisfy ziδ|z_{i}|\le\delta for every i[n]i\in[n]. Then zr\lVert z\rVert\le r. Indeed, for every ii, zi2=zi2z_{i}^{2}=|z_{i}|^{2} by claim 1 of Nonnegativity of Squares in an Ordered Field, and zi2δ2|z_{i}|^{2}\le\delta^{2} by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field, since 0zi0\le|z_{i}| by claim 1 of Properties of the Absolute Value in an Ordered Field. Hence each difference δ2zi2\delta^{2}-z_{i}^{2} is nonnegative by claim 3 of Elementary Arithmetic in an Ordered Field, their sum is nonnegative by claim 5 of Properties of Finite Sums, and by claims 2 and 3 of that lemma and claim 3 of Elementary Arithmetic in an Ordered Field,

z2=i=1nzi2i=1nδ2=δ2sn,\lVert z\rVert^{2}=\sum_{i=1}^{n}z_{i}^{2}\le\sum_{i=1}^{n}\delta^{2}=\delta^{2}s_{n},

the first equality by claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n. Since 1sn1\le s_{n} and 0δ2sn0\le\delta^{2}s_{n} by claim 2 of Nonnegativity of Squares in an Ordered Field and claim 5 of Elementary Arithmetic in an Ordered Field, the latter claim gives δ2snδ2snsn=(δsn)2\delta^{2}s_{n}\le\delta^{2}s_{n}s_{n}=(\delta s_{n})^{2}, and (δsn)2r2(\delta s_{n})^{2}\le r^{2} by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field, since 0δsnr0\le\delta s_{n}\le r. Thus z2r2\lVert z\rVert^{2}\le r^{2}, and since 0z0\le\lVert z\rVert by claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n and 0r0\le r, claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field gives zr\lVert z\rVert\le r.

Step 4: the far-field data. Apply The Fejer Kernel of the Torus: Nonnegativity, Periodicity, Mass and the Far-Field Integral Bound §tail with this δ\delta: with KδK_{\delta} the closed interval determined by δ\delta and 1δ1-\delta, that is, the set of tRt\in\mathbb{R} with δt1δ\delta\le t\le1-\delta, and Eδ={yQ:yiKδ for some i[n]}E_{\delta}=\{y\in Q:y_{i}\in K_{\delta}\text{ for some }i\in[n]\}, one has EδBQE_{\delta}\in\mathcal{B}_{Q}, for every NNN\in\mathbb{N} the map gN=1EδΦNQg_{N}=\mathbf{1}_{E_{\delta}}\Phi_{N}|_{Q} on QQ is integrable with respect to λQ\lambda_{Q}, and there is a real number bδb_{\delta} with 0bδ0\le b_{\delta} and TngNdxbδ/N\int_{\mathbb{T}^{n}}g_{N}\,dx\le b_{\delta}/N for every NNN\in\mathbb{N}. Each gNg_{N} is nonnegative, as the product of the indicator and the kernel, which is nonnegative by The Fejer Kernel of the Torus: Nonnegativity, Periodicity, Mass and the Far-Field Integral Bound §nonnegative, by claim 5 of Elementary Arithmetic in an Ordered Field.

Step 5: the choice of N0N_{0}. By claim 1 of The Archimedean Property of the Real Numbers there is N0NN_{0}\in\mathbb{N} with 2Mbδθ1<ι(N0)2Mb_{\delta}\theta^{-1}<\iota(N_{0}), where θ1\theta^{-1} exists by claim 7 of Elementary Order Arithmetic in an Ordered Field. Let NNN\in\mathbb{N} with N0NN_{0}\le N. Then ι(N0)ι(N)\iota(N_{0})\le\iota(N), by claim 6 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field if N0<NN_{0}<N and trivially if N0=NN_{0}=N; so 2Mbδθ1<ι(N)2Mb_{\delta}\theta^{-1}<\iota(N) by claim 2 of Elementary Order Arithmetic in an Ordered Field. Multiplying by θ\theta and then by ι(N)1\iota(N)^{-1}, both positive by claims 3 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field and 7 of Elementary Order Arithmetic in an Ordered Field, claim 10 of the latter gives

2MbδN<θ.\frac{2Mb_{\delta}}{N}<\theta .

Step 6: the basic identity. Fix NNN\in\mathbb{N} with N0NN_{0}\le N and xRnx\in\mathbb{R}^{n}. Let ρ:RnR\rho:\mathbb{R}^{n}\to\mathbb{R} be ρ(y)=1Q(y)ΦN(yx)\rho(y)=\mathbf{1}_{Q}(y)\Phi_{N}(y-x). By The Fejer Means of a Continuous Periodic Function on the Torus §mass, ρ\rho is integrable with Rnρdλn=1\int_{\mathbb{R}^{n}}\rho\,d\lambda_{n}=1, and by The Fejer Means of a Continuous Periodic Function on the Torus §integral the pointwise product ρu\rho u is integrable with Rnρudλn=σNu(x)\int_{\mathbb{R}^{n}}\rho u\,d\lambda_{n}=\sigma_{N}u(x). Moreover 0ρ(y)0\le\rho(y) for every yy, by The Fejer Kernel of the Torus: Nonnegativity, Periodicity, Mass and the Far-Field Integral Bound §nonnegative, 01Q(y)0\le\mathbf{1}_{Q}(y) and claim 5 of Elementary Arithmetic in an Ordered Field. By claim 2 of Linearity and Monotonicity of the Lebesgue Integral, applied with a=1a=1 and b=u(x)b=-u(x),

σNu(x)u(x)=Rnρudλnu(x)Rnρdλn=Rn(ρuu(x)ρ)dλn,\sigma_{N}u(x)-u(x)=\int_{\mathbb{R}^{n}}\rho u\,d\lambda_{n}-u(x)\int_{\mathbb{R}^{n}}\rho\,d\lambda_{n}=\int_{\mathbb{R}^{n}}\bigl(\rho u-u(x)\rho\bigr)\,d\lambda_{n},

and by the same claim σNu(x)u(x)Rnρuu(x)ρdλn|\sigma_{N}u(x)-u(x)|\le\int_{\mathbb{R}^{n}}|\rho u-u(x)\rho|\,d\lambda_{n}.

Let ψ:RnR\psi:\mathbb{R}^{n}\to\mathbb{R} be the map ψ=1Quu(x)1Q\psi=|\mathbf{1}_{Q}u-u(x)\mathbf{1}_{Q}|, formed pointwise. It is measurable: 1Qu\mathbf{1}_{Q}u is measurable by Continuous Periodic Functions are Power-Integrable and Dense on the Torus §integral, 1Q\mathbf{1}_{Q} is measurable by claim 1 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions since QB(Rn)Q\in\mathcal{B}(\mathbb{R}^{n}), and claims 2 and 4 of that lemma apply. For yQy\in Q one has ψ(y)=u(y)u(x)\psi(y)=|u(y)-u(x)|, and for yQy\notin Q one has ψ(y)=0\psi(y)=0. Consequently, for every yRny\in\mathbb{R}^{n},

ρ(y)u(y)u(x)ρ(y)=ρ(y)u(y)u(x)=ρ(y)ψ(y),|\rho(y)u(y)-u(x)\rho(y)|=|\rho(y)|\,|u(y)-u(x)|=\rho(y)\,\psi(y),

by distributivity, claim 4 of Properties of the Absolute Value in an Ordered Field, ρ(y)=ρ(y)|\rho(y)|=\rho(y) from Absolute Value in an Ordered Field, and the fact that both sides vanish for yQy\notin Q. So ρψ=ρuu(x)ρ\rho\psi=|\rho u-u(x)\rho| is integrable: it is measurable by claim 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and its absolute value is itself, whose integral is finite because ρuu(x)ρ\rho u-u(x)\rho is integrable, so the criterion of Integrable Function and the Lebesgue Integral applies. Hence σNu(x)u(x)Rnρψdλn|\sigma_{N}u(x)-u(x)|\le\int_{\mathbb{R}^{n}}\rho\psi\,d\lambda_{n}. Finally 0ψ(y)2M0\le\psi(y)\le2M for every yy: nonnegativity is claim 1 of Properties of the Absolute Value in an Ordered Field, the bound is trivial off QQ, and for yQy\in Q claims 5 and 2 of that lemma give u(y)u(x)u(y)+u(x)M+M=2M|u(y)-u(x)|\le|u(y)|+|u(x)|\le M+M=2M.

Step 7: the splitting. Let g~N:RnR\tilde{g}_{N}:\mathbb{R}^{n}\to\mathbb{R} be the periodic extension of gNg_{N}, so that g~N(z)=gN(π(z))\tilde{g}_{N}(z)=g_{N}(\pi(z)). By The Periodic Extension of a Function on the Unit Cell §extension it is measurable and Zn\mathbb{Z}^{n}-periodic, and g~N(y)=gN(y)\tilde{g}_{N}(y)=g_{N}(y) for yQy\in Q. Hence 1Qg~N\mathbf{1}_{Q}\tilde{g}_{N} is the map equal to gNg_{N} on QQ and to 00 outside QQ, that is, the zero extension of gNg_{N} in the sense of Zero Extension of a Real-Valued Function, and the Unit-Cell Integral of a Continuous Function §extension; so by that clause, applied to the measure space (Rn,B(Rn),λn)(\mathbb{R}^{n},\mathcal{B}(\mathbb{R}^{n}),\lambda_{n}), its restriction (Q,BQ,λQ)(Q,\mathcal{B}_{Q},\lambda_{Q}) and the map gNg_{N}, which is integrable with respect to λQ\lambda_{Q} by Step 4 and hence measurable with respect to BQ\mathcal{B}_{Q}, the map 1Qg~N\mathbf{1}_{Q}\tilde{g}_{N} is integrable with Rn1Qg~Ndλn=TngNdx\int_{\mathbb{R}^{n}}\mathbf{1}_{Q}\tilde{g}_{N}\,d\lambda_{n}=\int_{\mathbb{T}^{n}}g_{N}\,dx. For zRnz\in\mathbb{R}^{n}, by The Half-Open Unit Cell Tiles Euclidean Space §wrap one has π(z)=zm\pi(z)=z-m for some mZnm\in\mathbb{Z}^{n} and π(z)Q\pi(z)\in Q, so that ΦN(z)=ΦN((zm)+m)=ΦN(zm)=ΦN(π(z))\Phi_{N}(z)=\Phi_{N}((z-m)+m)=\Phi_{N}(z-m)=\Phi_{N}(\pi(z)) by The Fejer Kernel of the Torus: Nonnegativity, Periodicity, Mass and the Far-Field Integral Bound §periodic, and hence

g~N(z)=1Eδ(π(z))ΦN(z)(zRn),\tilde{g}_{N}(z)=\mathbf{1}_{E_{\delta}}(\pi(z))\,\Phi_{N}(z)\qquad(z\in\mathbb{R}^{n}),

where 1Eδ(π(z))\mathbf{1}_{E_{\delta}}(\pi(z)) is 11 if π(z)Eδ\pi(z)\in E_{\delta} and 00 otherwise. By The Cell Integral of a Translated Periodic Function §shift, applied to w=g~Nw=\tilde{g}_{N} and xx, the map τ:RnR\tau:\mathbb{R}^{n}\to\mathbb{R}, τ(y)=1Q(y)g~N(yx)\tau(y)=\mathbf{1}_{Q}(y)\tilde{g}_{N}(y-x), is integrable and

Rnτdλn=Rn1Qg~Ndλn=TngNdxbδN.\int_{\mathbb{R}^{n}}\tau\,d\lambda_{n}=\int_{\mathbb{R}^{n}}\mathbf{1}_{Q}\tilde{g}_{N}\,d\lambda_{n}=\int_{\mathbb{T}^{n}}g_{N}\,dx\le\frac{b_{\delta}}{N}.

Also 0τ(y)0\le\tau(y) for every yy, since gNg_{N} is nonnegative. For yRny\in\mathbb{R}^{n} write χ(y)=1Eδ(π(yx)){0,1}\chi(y)=\mathbf{1}_{E_{\delta}}(\pi(y-x))\in\{0,1\}, so that τ(y)=χ(y)ρ(y)\tau(y)=\chi(y)\rho(y).

Let A=τψA=\tau\psi and B=ρψAB=\rho\psi-A, formed pointwise; both are measurable by claims 2 and 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions. For every yy, A(y)=χ(y)ρ(y)ψ(y)A(y)=\chi(y)\rho(y)\psi(y) with 0χ(y)10\le\chi(y)\le1, so 0A(y)ρ(y)ψ(y)0\le A(y)\le\rho(y)\psi(y) by claim 5 of Elementary Arithmetic in an Ordered Field, and hence 0B(y)0\le B(y) by claim 3 of that lemma; also B(y)ρ(y)ψ(y)B(y)\le\rho(y)\psi(y) since 0A(y)0\le A(y). As ρψ\rho\psi is integrable, claim 1 of Linearity and Monotonicity of the Lebesgue Integral, applied to the nonnegative maps AA, BB and ρψ\rho\psi with their values read in [0,][0,\infty], the two readings of measurability agreeing by Measure Spaces and the Lebesgue Integral: Standing Notation §measurable, bounds the integrals of A=AA=|A| and B=BB=|B| by that of ρψ\rho\psi, which is finite; so AA and BB are integrable by Integrable Function and the Lebesgue Integral, and ρψ=A+B\rho\psi=A+B gives, by claim 2 of Linearity and Monotonicity of the Lebesgue Integral,

Rnρψdλn=RnAdλn+RnBdλn.\int_{\mathbb{R}^{n}}\rho\psi\,d\lambda_{n}=\int_{\mathbb{R}^{n}}A\,d\lambda_{n}+\int_{\mathbb{R}^{n}}B\,d\lambda_{n}.

Step 8: the far part. For every yy, A(y)=τ(y)ψ(y)τ(y)2M=2Mτ(y)A(y)=\tau(y)\psi(y)\le\tau(y)\,2M=2M\tau(y) by claim 5 of Elementary Arithmetic in an Ordered Field, since 0τ(y)0\le\tau(y) and ψ(y)2M\psi(y)\le2M. The map 2Mτ2M\tau is integrable by claim 2 of Linearity and Monotonicity of the Lebesgue Integral, and the same claim gives

RnAdλnRn2Mτdλn=2MRnτdλn2MbδN<θ,\int_{\mathbb{R}^{n}}A\,d\lambda_{n}\le\int_{\mathbb{R}^{n}}2M\tau\,d\lambda_{n}=2M\int_{\mathbb{R}^{n}}\tau\,d\lambda_{n}\le2M\,\frac{b_{\delta}}{N}<\theta,

using 02M0\le2M with claim 5 of Elementary Arithmetic in an Ordered Field for the second inequality and Step 5 for the last.

Step 9: the near part. We claim B(y)θρ(y)B(y)\le\theta\rho(y) for every yRny\in\mathbb{R}^{n}. If yQy\notin Q then ρ(y)=0\rho(y)=0 and ψ(y)=0\psi(y)=0, so B(y)=0=θρ(y)B(y)=0=\theta\rho(y). If yQy\in Q and χ(y)=1\chi(y)=1, then A(y)=ρ(y)ψ(y)A(y)=\rho(y)\psi(y), so B(y)=0θρ(y)B(y)=0\le\theta\rho(y) by claim 5 of Elementary Arithmetic in an Ordered Field. Suppose finally yQy\in Q and χ(y)=0\chi(y)=0, so that A(y)=0A(y)=0 and B(y)=ρ(y)u(y)u(x)B(y)=\rho(y)|u(y)-u(x)|. We show u(y)u(x)θ|u(y)-u(x)|\le\theta, which gives B(y)ρ(y)θ=θρ(y)B(y)\le\rho(y)\theta=\theta\rho(y) by claim 5 of Elementary Arithmetic in an Ordered Field.

Put w=yxw=y-x and q=π(w)q=\pi(w); by The Half-Open Unit Cell Tiles Euclidean Space §wrap, qQq\in Q and q=wmq=w-m for some mZnm\in\mathbb{Z}^{n}. Since χ(y)=0\chi(y)=0, qEδq\notin E_{\delta}, so for every i[n]i\in[n] the coordinate qiq_{i} does not lie in KδK_{\delta}: it is not the case that both δqi\delta\le q_{i} and qi1δq_{i}\le1-\delta. Also 0qi<10\le q_{i}<1 since qQq\in Q. The order of R\mathbb{R} being total, either qi<δq_{i}<\delta, or δqi\delta\le q_{i} and then 1δ<qi1-\delta<q_{i}. Let mm' be the point of Rn\mathbb{R}^{n} with mi=mim'_{i}=m_{i} if qi<δq_{i}<\delta and mi=mi+1m'_{i}=m_{i}+1 otherwise, which exists by claim 2 of Euclidean Points as Tuples of Real Numbers; every mim'_{i} is an integer by claim 2 of Arithmetic, Order and Discreteness of the Integers, so mZnm'\in\mathbb{Z}^{n} by Lattice-Periodic Functions and the Periodic Function Classes §lattice. Put w=wmw'=w-m', so that wi=wimiw'_{i}=w_{i}-m'_{i} for every ii. If qi<δq_{i}<\delta, then wi=wimi=qiw'_{i}=w_{i}-m_{i}=q_{i}, and 0qi0\le q_{i} gives wi=qi<δ|w'_{i}|=q_{i}<\delta by Absolute Value in an Ordered Field. Otherwise wi=wimi1=qi1w'_{i}=w_{i}-m_{i}-1=q_{i}-1, which is negative because qi<1q_{i}<1 (claim 1 of Elementary Order Arithmetic in an Ordered Field), so wi=(qi1)=1qi|w'_{i}|=-(q_{i}-1)=1-q_{i} by Absolute Value in an Ordered Field, and 1δ<qi1-\delta<q_{i} gives 1qi<δ1-q_{i}<\delta by claim 1 of Elementary Order Arithmetic in an Ordered Field. In either case wiδ|w'_{i}|\le\delta, so wr\lVert w'\rVert\le r by Step 3.

Now (ym)x=wm=w(y-m')-x=w-m'=w', so (ym)xr\lVert(y-m')-x\rVert\le r and Step 1 gives u(ym)u(x)θ|u(y-m')-u(x)|\le\theta. Since mZnm'\in\mathbb{Z}^{n} and uu is Zn\mathbb{Z}^{n}-periodic by Lattice-Periodic Functions and the Periodic Function Classes §classes and Lattice-Periodic Functions and the Periodic Function Classes §periodic, u(y)=u((ym)+m)=u(ym)u(y)=u((y-m')+m')=u(y-m'). Hence u(y)u(x)θ|u(y)-u(x)|\le\theta, proving the claim.

The map θρ\theta\rho is integrable with integral θ\theta by claim 2 of Linearity and Monotonicity of the Lebesgue Integral and Step 6, and the same claim gives RnBdλnRnθρdλn=θ\int_{\mathbb{R}^{n}}B\,d\lambda_{n}\le\int_{\mathbb{R}^{n}}\theta\rho\,d\lambda_{n}=\theta.

Step 10: conclusion. By Steps 6 to 9 and claim 3 of Elementary Order Arithmetic in an Ordered Field,

σNu(x)u(x)RnAdλn+RnBdλn<θ+θ=ε.|\sigma_{N}u(x)-u(x)|\le\int_{\mathbb{R}^{n}}A\,d\lambda_{n}+\int_{\mathbb{R}^{n}}B\,d\lambda_{n}<\theta+\theta=\varepsilon .

As NNN\in\mathbb{N} with N0NN_{0}\le N and xRnx\in\mathbb{R}^{n} were arbitrary, this proves the explicit statement, with the inequality even strict.

Uniform convergence. Let εR\varepsilon'\in\mathbb{R} with 0<ε0<\varepsilon'. By claim 8 of Elementary Order Arithmetic in an Ordered Field the number ε=ε21\varepsilon=\varepsilon'\cdot2^{-1} is positive and satisfies ε<ε\varepsilon<\varepsilon'. The explicit statement furnishes N0NN_{0}\in\mathbb{N} with σNu(x)u(x)ε<ε|\sigma_{N}u(x)-u(x)|\le\varepsilon<\varepsilon', hence σNu(x)u(x)<ε|\sigma_{N}u(x)-u(x)|<\varepsilon' by claim 2 of Elementary Order Arithmetic in an Ordered Field, for every NNN\in\mathbb{N} with N0NN_{0}\le N and every xRnx\in\mathbb{R}^{n}. This is the condition of Pointwise and Uniform Convergence of a Sequence of Real-Valued Functions §uniform for the sequence (σNu)NN(\sigma_{N}u)_{N\in\mathbb{N}} of maps from D=RnD=\mathbb{R}^{n} to R\mathbb{R}, the limit f=uf=u, the subset S=RnS=\mathbb{R}^{n} and K=N0K=N_{0}.

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