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Proof of Continuous Periodic Functions are Power-Integrable and Dense on the Torus

lemmalem:continuous-periodic-dense-lp-torus-2026a
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· 12,013 chars · 28 deps · depth 24 Reason: Phase B: proof that continuous periodic functions are power-integrable and dense in every Lebesgue space of the torus.

Boundedness gives power-integrability. Density is obtained by approximating the indicators in a simple function using inner and outer regularity of Lebesgue measure, a cutoff function supported in the open cell, and periodisation.

Proof

Each result cited below is universally quantified over the data appearing in its own statement, and is applied to the data named here. The measure space is (Q,BQ,λQ)(Q,\mathcal{B}_{Q},\lambda_{Q}) of clause 3, with λQ(Q)=1\lambda_{Q}(Q)=1, unless (Rn,B(Rn),λn)(\mathbb{R}^{n},\mathcal{B}(\mathbb{R}^{n}),\lambda_{n}) is named instead. We use repeatedly that a map uCperu\in C_{\mathrm{per}}, being continuous on Rn\mathbb{R}^{n}, is measurable with respect to B(Rn)\mathcal{B}(\mathbb{R}^{n}) and B(R)\mathcal{B}(\mathbb{R}), by claim 3(a) of The Borel Sigma-Algebra of a Euclidean Space as a Product, and Measurability of Projections, Sequentially Continuous Maps, and Open and Closed Sets together with claim 5 there.

Claim 1. For a real cc we have

{xQ:c<u(x)}=Q{xRn:c<u(x)},\{x\in Q:c<u(x)\}=Q\cap\{x\in\mathbb{R}^{n}:c<u(x)\},

which belongs to B(Rn)\mathcal{B}(\mathbb{R}^{n}) and is contained in QQ, hence belongs to BQ\mathcal{B}_{Q}. By the criterion of clause 3, uQu|_{Q} is measurable. Next, u(x)M|u(x)|\le M for every xx, so by Properties of Real Powers of Nonnegative Real Numbers §monotone the power (u(x))p(|u(x)|)^{p} is at most MpM^{p} for every xQx\in Q. The constant function on QQ with value MpM^{p} is Mp1QM^{p}\,\mathbf{1}_{Q}, whose integral is MpλQ(Q)=MpM^{p}\lambda_{Q}(Q)=M^{p} by The Integral of an Indicator Function is the Measure of the Set and claim 1 of Linearity and Monotonicity of the Lebesgue Integral. Monotonicity of the integral of nonnegative measurable functions (claim 1 of Linearity and Monotonicity of the Lebesgue Integral) therefore gives

QuQpdλQMp<,\int_{Q}\bigl|u|_{Q}\bigr|^{p}\,d\lambda_{Q}\le M^{p}<\infty ,

so uQLp(Tn)u|_{Q}\in\mathcal{L}^{p}(\mathbb{T}^{n}) by Power-Integrable Functions and the p-Seminorm §space. Applying the monotone power tt1/pt\mapsto t^{1/p} (Properties of Real Powers of Nonnegative Real Numbers §monotone) and the identity (Mp)1/p=M(M^{p})^{1/p}=M (Properties of Real Powers of Nonnegative Real Numbers §inverse) gives uQpM\lVert u|_{Q}\rVert_{p}\le M for the pp-seminorm, and [uQ]Lp(Tn)=uQp\lVert[u|_{Q}]\rVert_{L^{p}(\mathbb{T}^{n})}=\lVert u|_{Q}\rVert_{p} by The Lebesgue Space of Power-Integrable Functions §norm.

Claim 2. Let MM be as in claim 1. The product 1Qu\mathbf{1}_{Q}u is measurable with respect to B(Rn)\mathcal{B}(\mathbb{R}^{n}): for a real cc the set {x:c<1Q(x)u(x)}\{x:c<\mathbf{1}_{Q}(x)u(x)\} equals Q{x:c<u(x)}Q\cap\{x:c<u(x)\} when 0c0\le c, and equals the union of that set with the complement of QQ when c<0c<0; both lie in B(Rn)\mathcal{B}(\mathbb{R}^{n}). Moreover 1QuM1Q|\mathbf{1}_{Q}u|\le M\mathbf{1}_{Q} pointwise, and RnM1Qdλn=Mλn(Q)=M\int_{\mathbb{R}^{n}}M\mathbf{1}_{Q}\,d\lambda_{n}=M\lambda_{n}(Q)=M is finite by The Integral of an Indicator Function is the Measure of the Set, The Half-Open Unit Cell Tiles Euclidean Space §cell and claim 1 of Linearity and Monotonicity of the Lebesgue Integral; so 1Qu\mathbf{1}_{Q}u is integrable by the criterion recorded in Integrable Function and the Lebesgue Integral.

Let u+u^{+} and uu^{-} be the positive and negative parts of uu in the sense of Integrable Function and the Lebesgue Integral. The zero extension of (uQ)+(u|_{Q})^{+} off QQ is 1Qu+\mathbf{1}_{Q}u^{+}, and likewise for the negative parts. Claim 1 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions, applied to the measure space (Rn,B(Rn),λn)(\mathbb{R}^{n},\mathcal{B}(\mathbb{R}^{n}),\lambda_{n}) and to QB(Rn)Q\in\mathcal{B}(\mathbb{R}^{n}), therefore gives

Q(uQ)±dλQ=Rn1Qu±dλn,\int_{Q}(u|_{Q})^{\pm}\,d\lambda_{Q}=\int_{\mathbb{R}^{n}}\mathbf{1}_{Q}u^{\pm}\,d\lambda_{n},

both sides being finite. Subtracting the two identities and using Integrable Function and the Lebesgue Integral on each side yields TnuQdx=Rn1Qudλn\int_{\mathbb{T}^{n}}u|_{Q}\,dx=\int_{\mathbb{R}^{n}}\mathbf{1}_{Q}u\,d\lambda_{n}.

Claim 3. The maps u+vu+v and cucu lie in CperC_{\mathrm{per}} by Elementary Properties of Lattice-Periodic Functions §algebra, so their restrictions lie in Lp(Tn)\mathcal{L}^{p}(\mathbb{T}^{n}) by claim 1. Restriction commutes with the pointwise operations, that is (u+v)Q=uQ+vQ(u+v)|_{Q}=u|_{Q}+v|_{Q} and (cu)Q=c(uQ)(cu)|_{Q}=c\,(u|_{Q}) as maps on QQ, and the operations on classes are defined by representatives in The Lebesgue Space of Power-Integrable Functions §space. The two identities follow.

Claim 4. We first prove the approximation statement. Let fLp(Tn)f\in\mathcal{L}^{p}(\mathbb{T}^{n}) and let ε\varepsilon be a positive real.

Step 1: reduction to a simple function. By Simple Functions are Dense in the Lebesgue Space §approximation there is a simple function ss on (Q,BQ)(Q,\mathcal{B}_{Q}) lying in Lp(Tn)\mathcal{L}^{p}(\mathbb{T}^{n}) with fspε/2\lVert f-s\rVert_{p}\le\varepsilon/2.

Step 2: approximating one indicator. We show: for every ABQA\in\mathcal{B}_{Q} and every positive real η\eta there is vCperv\in C_{\mathrm{per}} with 1AvQpη\lVert\mathbf{1}_{A}-v|_{Q}\rVert_{p}\le\eta.

Let β\beta be a positive real with β14\beta\le\tfrac14, to be fixed at the end, and put

V={xRn:β<xi<1β for every i[n]}.V=\{x\in\mathbb{R}^{n}:\beta<x_{i}<1-\beta\ \text{for every}\ i\in[n]\}.

VV is open: for xVx\in V let rr be the least element of the finite set {xiβ:i[n]}{1βxi:i[n]}\{x_{i}-\beta:i\in[n]\}\cup\{1-\beta-x_{i}:i\in[n]\} of positive reals, positive by repeated use of claim 9 of Elementary Order Arithmetic in an Ordered Field; if yx<r\lVert y-x\rVert<r then yixi<r|y_{i}-x_{i}|<r for every ii by claim 4 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, whence β<yi<1β\beta<y_{i}<1-\beta. Also VQ˚V\subseteq\mathring{Q}, since 0<β0<\beta and 1β<11-\beta<1.

Put Aβ=AVA_{\beta}=A\cap V, a member of BQ\mathcal{B}_{Q}. Every xAAβx\in A\setminus A_{\beta} lies in QQ and has some coordinate with xiβx_{i}\le\beta or 1βxi1-\beta\le x_{i}, so

AAβi[n](SiTi),Si={xQ:xiβ},Ti={xQ:1βxi}.A\setminus A_{\beta}\subseteq\bigcup_{i\in[n]}\bigl(S_{i}\cup T_{i}\bigr),\qquad S_{i}=\{x\in Q:x_{i}\le\beta\},\quad T_{i}=\{x\in Q:1-\beta\le x_{i}\}.

Each SiS_{i} is the Borel rectangle whose iith factor is the interval {t:0tβ}\{t:0\le t\le\beta\} and whose other factors are {t:0t<1}\{t:0\le t<1\}, and each TiT_{i} is the Borel rectangle whose iith factor is {t:1βt<1}\{t:1-\beta\le t<1\} and whose other factors are the same; by claim 4 of Existence of Lebesgue Measure on the Real Line and the rectangle identity of Lebesgue Measure on Rn\mathbb{R}^n each has measure β\beta. By the monotonicity and finite subadditivity of a measure recorded in Basic Properties of a Measure, λn(AAβ)2nβ\lambda_{n}(A\setminus A_{\beta})\le2n\beta.

Since λn(Aβ)λn(Q)=1<\lambda_{n}(A_{\beta})\le\lambda_{n}(Q)=1<\infty, Outer and Inner Regularity of Lebesgue Measure on Rn\mathbb{R}^n §inner-compact provides a compact KAβK\subseteq A_{\beta} with λn(AβK)β\lambda_{n}(A_{\beta}\setminus K)\le\beta, and Outer and Inner Regularity of Lebesgue Measure on Rn\mathbb{R}^n §outer provides an open U0KU_{0}\supseteq K with λn(U0K)β\lambda_{n}(U_{0}\setminus K)\le\beta. Put U=U0VU=U_{0}\cap V, an open set with KUK\subseteq U (because KAβVK\subseteq A_{\beta}\subseteq V), with UVQ˚U\subseteq V\subseteq\mathring{Q}, and with λn(UK)λn(U0K)β\lambda_{n}(U\setminus K)\le\lambda_{n}(U_{0}\setminus K)\le\beta.

Apply Continuous Partition of Unity Subordinate to a Finite Open Cover of a Compact Set in a Metric Space in the metric space (Rn,dE)(\mathbb{R}^{n},d_{E}) to the compact set KK and the one-member family consisting of the open set UU, which covers KK. It yields a continuous g:RnRg:\mathbb{R}^{n}\to\mathbb{R} with 0g10\le g\le1 and a closed DUD\subseteq U such that gg vanishes off DD and g(x)=1g(x)=1 for every xKx\in K. In particular gg vanishes off UU, and UQ˚U\subseteq\mathring{Q}, so Elementary Properties of Lattice-Periodic Functions §periodisation applies with W=UW=U: the map v=gπv=g\circ\pi lies in CperC_{\mathrm{per}}, agrees with gg on QQ, and satisfies 0v10\le v\le1.

Put E=((AK)(UK))QE=\bigl((A\setminus K)\cup(U\setminus K)\bigr)\cap Q, a member of BQ\mathcal{B}_{Q}. Note first that (1E)p=1E(\mathbf{1}_{E})^{p}=\mathbf{1}_{E}: indeed 0p=00^{p}=0 by Real Power of a Nonnegative Real Number §power, while 1p=1p1p1^{p}=1^{p}\cdot1^{p} by Properties of Real Powers of Nonnegative Real Numbers §product and 1p01^{p}\ne0 by Properties of Real Powers of Nonnegative Real Numbers §values, so cancelling the nonzero factor gives 1p=11^{p}=1. Hence 1ELp(Tn)\mathbf{1}_{E}\in\mathcal{L}^{p}(\mathbb{T}^{n}), its ppth power having integral λQ(E)λQ(Q)=1<\lambda_{Q}(E)\le\lambda_{Q}(Q)=1<\infty by The Integral of an Indicator Function is the Measure of the Set and Basic Properties of a Measure. For xQx\in Q with xEx\notin E we have 1A(x)=v(x)\mathbf{1}_{A}(x)=v(x): if xKx\in K then xAx\in A and g(x)=1g(x)=1, so both values are 11; if xKx\notin K then xAx\notin A and xUx\notin U, so 1A(x)=0\mathbf{1}_{A}(x)=0 and g(x)=0g(x)=0. For xEx\in E both 1A(x)\mathbf{1}_{A}(x) and v(x)v(x) lie between 00 and 11, so 1A(x)v(x)1|\mathbf{1}_{A}(x)-v(x)|\le1. Hence 1AvQ1E|\mathbf{1}_{A}-v|_{Q}|\le\mathbf{1}_{E} pointwise on QQ, and Elementary Properties of the p-Seminorm §comparison gives

1AvQp1Ep=(λQ(E))1/p,\lVert\mathbf{1}_{A}-v|_{Q}\rVert_{p}\le\lVert\mathbf{1}_{E}\rVert_{p}=\bigl(\lambda_{Q}(E)\bigr)^{1/p},

using (1E)p=1E(\mathbf{1}_{E})^{p}=\mathbf{1}_{E} as just noted, together with The Integral of an Indicator Function is the Measure of the Set. Finally

λQ(E)λn(AK)+λn(UK)(λn(AAβ)+λn(AβK))+β2nβ+β+β=(2n+2)β,\lambda_{Q}(E)\le\lambda_{n}(A\setminus K)+\lambda_{n}(U\setminus K)\le\bigl(\lambda_{n}(A\setminus A_{\beta})+\lambda_{n}(A_{\beta}\setminus K)\bigr)+\beta\le2n\beta+\beta+\beta=(2n+2)\beta,

again by Basic Properties of a Measure. Choosing β\beta to be the least of 14\tfrac14 and ηp/(2n+2)\eta^{p}/(2n+2) makes λQ(E)ηp\lambda_{Q}(E)\le\eta^{p} and hence 1AvQp(ηp)1/p=η\lVert\mathbf{1}_{A}-v|_{Q}\rVert_{p}\le(\eta^{p})^{1/p}=\eta, by Properties of Real Powers of Nonnegative Real Numbers §monotone and Properties of Real Powers of Nonnegative Real Numbers §inverse.

Step 3: from indicators to ss. Let s=l=1rcl1Als=\sum_{l=1}^{r}c_{l}\mathbf{1}_{A_{l}} be the standard representation of ss, with distinct values clc_{l} and Al=s1({cl})BQA_{l}=s^{-1}(\{c_{l}\})\in\mathcal{B}_{Q}. Let L={l[r]:cl0}L=\{l\in[r]:c_{l}\ne0\}; since the terms with cl=0c_{l}=0 contribute nothing, s=lLcl1Als=\sum_{l\in L}c_{l}\mathbf{1}_{A_{l}} pointwise on QQ. If LL is empty then ss is the zero map, and the map uu with constant value 00 lies in CperC_{\mathrm{per}} with suQp=0ε/2\lVert s-u|_{Q}\rVert_{p}=0\le\varepsilon/2. Otherwise put C=lLclC=\sum_{l\in L}|c_{l}|, a positive real. Apply Step 2 to each AlA_{l}, lLl\in L, with η=ε/(2C)\eta=\varepsilon/(2C), obtaining vlCperv_{l}\in C_{\mathrm{per}} with 1AlvlQpε/(2C)\lVert\mathbf{1}_{A_{l}}-v_{l}|_{Q}\rVert_{p}\le\varepsilon/(2C), and put u=lLclvlu=\sum_{l\in L}c_{l}v_{l}, which lies in CperC_{\mathrm{per}} by Elementary Properties of Lattice-Periodic Functions §algebra. Then suQ=lLcl(1AlvlQ)s-u|_{Q}=\sum_{l\in L}c_{l}\bigl(\mathbf{1}_{A_{l}}-v_{l}|_{Q}\bigr) pointwise on QQ, so by Minkowski's Inequality and the Seminormed Space of Power-Integrable Functions §finite-sums and Elementary Properties of the p-Seminorm §homogeneous,

suQplLcl1AlvlQpCε2C=ε2.\lVert s-u|_{Q}\rVert_{p}\le\sum_{l\in L}|c_{l}|\,\bigl\lVert\mathbf{1}_{A_{l}}-v_{l}|_{Q}\bigr\rVert_{p}\le C\cdot\frac{\varepsilon}{2C}=\frac{\varepsilon}{2}.

Step 4: conclusion. By Minkowski's Inequality and the Seminormed Space of Power-Integrable Functions §minkowski,

fuQpfsp+suQpε2+ε2=ε,\bigl\lVert f-u|_{Q}\bigr\rVert_{p}\le\lVert f-s\rVert_{p}+\bigl\lVert s-u|_{Q}\bigr\rVert_{p}\le\frac{\varepsilon}{2}+\frac{\varepsilon}{2}=\varepsilon ,

and [f][uQ]Lp(Tn)=fuQp\lVert[f]-[u|_{Q}]\rVert_{L^{p}(\mathbb{T}^{n})}=\lVert f-u|_{Q}\rVert_{p} by The Lebesgue Space of Power-Integrable Functions §space and The Lebesgue Space of Power-Integrable Functions §norm. This is the approximation statement.

Density. Let FLp(Tn)F\in L^{p}(\mathbb{T}^{n}) and choose a representative fLp(Tn)f\in\mathcal{L}^{p}(\mathbb{T}^{n}) with F=[f]F=[f]. For each kNk\in\mathbb{N} the approximation statement, applied with ε=1/k\varepsilon=1/k, provides ukCperu_{k}\in C_{\mathrm{per}} with F[ukQ]Lp(Tn)1/k\lVert F-[u_{k}|_{Q}]\rVert_{L^{p}(\mathbb{T}^{n})}\le1/k; the choice of one such uku_{k} for each kk uses countable choice. Given a positive real ε\varepsilon, The Archimedean Property of the Real Numbers provides k0Nk_{0}\in\mathbb{N} with 1<k0ε1<k_{0}\varepsilon, and then F[ukQ]Lp(Tn)1/k<ε\lVert F-[u_{k}|_{Q}]\rVert_{L^{p}(\mathbb{T}^{n})}\le1/k<\varepsilon for every kk0k\ge k_{0}. So the sequence ([ukQ])kN([u_{k}|_{Q}])_{k\in\mathbb{N}} in C\mathcal{C} converges to FF in the metric of Lp(Tn)L^{p}(\mathbb{T}^{n}), and FF lies in the closure of C\mathcal{C} by Sequential Characterization of the Closure in a Metric Space. As FF was arbitrary, the closure of C\mathcal{C} is all of Lp(Tn)L^{p}(\mathbb{T}^{n}), that is, C\mathcal{C} is dense.

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