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Proof of The Lebesgue Bound for Periodic Convolution and Convergence of Mollifications

theoremthm:periodic-convolution-lp-torus-2026a
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· 12,427 chars · 27 deps · depth 27 Reason: First publication: Tonelli on the cell squared with Hoelder splitting the kernel, then convergence of mollifications by comparison with a continuous periodic function.

The periodised kernel turns the convolution into an integral over the cell, Tonelli's theorem on the cell squared exchanges the order of integration, and Hoelder's inequality splits the kernel between the two factors. Convergence of the mollifications follows by comparison with a nearby continuous periodic function, and density of the smooth periodic functions is then immediate.

Proof

Each result cited below is universally quantified over the data appearing in its own statement, and is applied here to the data named in the statement of this theorem. Let Ψ\Psi be the periodised kernel of ψ\psi, and for x,yRnx,y\in\mathbb{R}^{n} let Ψx\Psi_{x} and Ψy\Psi^{y} be the restrictions to QQ of Ψ(x,)\Psi(x,\cdot) and of Ψ(,y)\Psi(\cdot,y), each in L1(Tn)\mathcal{L}^{1}(\mathbb{T}^{n}) with integral of absolute value at most KK by that clause. We use repeatedly that for an integrable gg one has ggg-|g|\le g\le|g| pointwise by claim 3 of Properties of the Absolute Value in an Ordered Field, hence by claim 2 of Linearity and Monotonicity of the Lebesgue Integral and claim 6 of Properties of the Absolute Value in an Ordered Field,

gdμgdμ.()\Bigl|\int g\,d\mu\Bigr|\le\int|g|\,d\mu. \tag{$\ast$}

We also use that λQ(Q)=1\lambda_{Q}(Q)=1, from The Flat Torus: Standing Notation §measure.

Step 0. A measurable nonnegative integrand on the product.

Let uLp(Tn)u\in\mathcal{L}^{p}(\mathbb{T}^{n}). By The Periodic Extension of a Function on the Unit Cell §finite-measure the map uu lies in L1(Tn)\mathcal{L}^{1}(\mathbb{T}^{n}), so The Periodised Kernel of a Periodic Convolution §representation applies and gives

(ψu)(x)=TnΨxudy(xRn).(\psi\star u)(x)=\int_{\mathbb{T}^{n}}\Psi_{x}\,u\,dy\qquad(x\in\mathbb{R}^{n}).

The second projection (x,y)y(x,y)\mapsto y from Q×QQ\times Q to QQ is measurable with respect to BQBQ\mathcal{B}_{Q}\otimes\mathcal{B}_{Q} and BQ\mathcal{B}_{Q}, since the preimage of ABQA\in\mathcal{B}_{Q} is the measurable rectangle Q×AQ\times A, a member of the product σ\sigma-algebra by Product Sigma-Algebra. Hence (x,y)u(y)(x,y)\mapsto u(y) is measurable with respect to BQBQ\mathcal{B}_{Q}\otimes\mathcal{B}_{Q}. The restriction of Ψ\Psi to Q×QQ\times Q is measurable with respect to the same σ\sigma-algebra by The Periodised Kernel of a Periodic Convolution §joint. Consequently, by Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions and claim 4 of that lemma, the maps

(x,y)Ψ(x,y)u(y)and(x,y)Ψ(x,y)(u(y))p(x,y)\mapsto|\Psi(x,y)|\,|u(y)|\qquad\text{and}\qquad(x,y)\mapsto|\Psi(x,y)|\,\bigl(|u(y)|\bigr)^{p}

are measurable with respect to BQBQ\mathcal{B}_{Q}\otimes\mathcal{B}_{Q} and take values in [0,)[0,\infty), the second using Power-Integrable Functions and the p-Seminorm §measurable-power for measurability of up|u|^{p}. The measure λQ\lambda_{Q} is finite, hence σ\sigma-finite, so Tonelli and Fubini Theorems applies to (Q,BQ,λQ)(Q,\mathcal{B}_{Q},\lambda_{Q}) in both variables.

Step 1. Proof of claim 1.

That (ψu)Q(\psi\star u)|_{Q} lies in Lp(Tn)\mathcal{L}^{p}(\mathbb{T}^{n}) is Properties of Periodic Convolution on the Torus §bound. It remains to prove the inequality. By the representation of step 0, by ()(\ast), and by claim 4 of Properties of the Absolute Value in an Ordered Field,

(ψu)(x)TnΨ(x,y)u(y)dy(xQ).(1)|(\psi\star u)(x)|\le\int_{\mathbb{T}^{n}}|\Psi(x,y)|\,|u(y)|\,dy\qquad(x\in Q). \tag{1}

The case p=1p=1. Integrating (1) over QQ, using claim 1 of Linearity and Monotonicity of the Lebesgue Integral for monotonicity and then the Tonelli identity of Tonelli and Fubini Theorems to exchange the order,

Tn(ψu)QdxQ(QΨ(x,y)u(y)dλQ(y))dλQ(x)=Qu(y)(QΨydλQ)dλQ(y).\int_{\mathbb{T}^{n}}\bigl|(\psi\star u)|_{Q}\bigr|\,dx\le\int_{Q}\Bigl(\int_{Q}|\Psi(x,y)|\,|u(y)|\,d\lambda_{Q}(y)\Bigr)d\lambda_{Q}(x)=\int_{Q}|u(y)|\Bigl(\int_{Q}|\Psi^{y}|\,d\lambda_{Q}\Bigr)d\lambda_{Q}(y).

By The Periodised Kernel of a Periodic Convolution §mass-bound the inner integral is at most KK, so by monotonicity again the right-hand side is at most Ku1K\lVert u\rVert_{1}. Since u1=QudλQ\lVert u\rVert_{1}=\int_{Q}|u|\,d\lambda_{Q} by Power-Integrable Functions and the p-Seminorm §seminorm and Properties of Real Powers of Nonnegative Real Numbers §agreement, this is the asserted inequality for p=1p=1.

The case 1<p1<p. Let qq be the conjugate exponent of pp, so 1/p+1/q=11/p+1/q=1. Fix xQx\in Q and put, on QQ,

a=Ψx1/q,b=Ψx1/pu.a=|\Psi_{x}|^{1/q},\qquad b=|\Psi_{x}|^{1/p}\,|u| .

By Properties of Real Powers of Nonnegative Real Numbers §inverse we have aq=Ψxa^{q}=|\Psi_{x}| and bp=Ψxupb^{p}=|\Psi_{x}|\,|u|^{p}, the latter also using Properties of Real Powers of Nonnegative Real Numbers §product. Both aa and bb are measurable by Power-Integrable Functions and the p-Seminorm §measurable-power and Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions. Now QaqdλQ=QΨxdλQK<\int_{Q}a^{q}\,d\lambda_{Q}=\int_{Q}|\Psi_{x}|\,d\lambda_{Q}\le K<\infty, so aLq(Tn)a\in\mathcal{L}^{q}(\mathbb{T}^{n}) with aqK1/q\lVert a\rVert_{q}\le K^{1/q} by Power-Integrable Functions and the p-Seminorm §seminorm and Properties of Real Powers of Nonnegative Real Numbers §monotone; and Ψ(x,)\Psi(x,\cdot) is bounded, say by MM', being a member of CperC_{\mathrm{per}} by The Periodised Kernel of a Periodic Convolution §regularity and bounded by Elementary Properties of Lattice-Periodic Functions §bounded, so QbpdλQMQupdλQ<\int_{Q}b^{p}\,d\lambda_{Q}\le M'\int_{Q}|u|^{p}\,d\lambda_{Q}<\infty and bLp(Tn)b\in\mathcal{L}^{p}(\mathbb{T}^{n}).

The pointwise product satisfies ab=Ψx1/qΨx1/pu=Ψxua\,b=|\Psi_{x}|^{1/q}|\Psi_{x}|^{1/p}|u|=|\Psi_{x}|\,|u|, by Properties of Real Powers of Nonnegative Real Numbers §exponents with 1/q+1/p=11/q+1/p=1, followed by Properties of Real Powers of Nonnegative Real Numbers §agreement, which gives t1=tt^{1}=t for nonnegative tt. Applying Hoelder's Inequality, for Two and for Finitely Many Factors §holder to the conjugate pair q,pq,p and the functions aLqa\in\mathcal{L}^{q}, bLpb\in\mathcal{L}^{p},

QΨxudλQ=ab1aqbpK1/q(QΨxupdλQ)1/p.\int_{Q}|\Psi_{x}|\,|u|\,d\lambda_{Q}=\lVert a\,b\rVert_{1}\le\lVert a\rVert_{q}\,\lVert b\rVert_{p}\le K^{1/q}\Bigl(\int_{Q}|\Psi_{x}|\,|u|^{p}\,d\lambda_{Q}\Bigr)^{1/p}.

Combining with (1) and raising to the power pp, which preserves the inequality by Properties of Real Powers of Nonnegative Real Numbers §monotone, and using Properties of Real Powers of Nonnegative Real Numbers §product and Properties of Real Powers of Nonnegative Real Numbers §inverse,

((ψu)(x))pKp/qQΨ(x,y)u(y)pdλQ(y)(xQ).\bigl(|(\psi\star u)(x)|\bigr)^{p}\le K^{p/q}\int_{Q}|\Psi(x,y)|\,|u(y)|^{p}\,d\lambda_{Q}(y)\qquad(x\in Q).

Integrating over xQx\in Q, using monotonicity and then the Tonelli identity of Tonelli and Fubini Theorems and The Periodised Kernel of a Periodic Convolution §mass-bound as in the case p=1p=1,

Q(ψu)QpdλQKp/qQu(y)p(QΨydλQ)dλQ(y)Kp/qK(up)p.\int_{Q}\bigl|(\psi\star u)|_{Q}\bigr|^{p}\,d\lambda_{Q}\le K^{p/q}\int_{Q}|u(y)|^{p}\Bigl(\int_{Q}|\Psi^{y}|\,d\lambda_{Q}\Bigr)d\lambda_{Q}(y)\le K^{p/q}\cdot K\cdot\bigl(\lVert u\rVert_{p}\bigr)^{p}.

Since p/q+1=p(11/p)+1=pp/q+1=p(1-1/p)+1=p, Properties of Real Powers of Nonnegative Real Numbers §agreement, which identifies KK with K1K^{1}, together with Properties of Real Powers of Nonnegative Real Numbers §exponents gives Kp/qK=KpK^{p/q}\cdot K=K^{p}, so the right-hand side is (Kup)p\bigl(K\lVert u\rVert_{p}\bigr)^{p} by Properties of Real Powers of Nonnegative Real Numbers §product. Taking the power 1/p1/p of both sides, which preserves the inequality by Properties of Real Powers of Nonnegative Real Numbers §monotone, and using Power-Integrable Functions and the p-Seminorm §seminorm together with Properties of Real Powers of Nonnegative Real Numbers §inverse, we obtain (ψu)QpKup\lVert(\psi\star u)|_{Q}\rVert_{p}\le K\lVert u\rVert_{p}.

Step 2. Proof of claim 2.

By Rescaling a Mollifier Kernel the map ρε\rho_{\varepsilon} is a mollifier kernel of radius εδ\varepsilon\delta on Rn\mathbb{R}^{n}. By the nonnegativity and unit-mass conditions of Mollifier Kernel of Radius δ\delta on Rn\mathbb{R}^n, together with claim 1 of Properties of the Absolute Value in an Ordered Field, the constant KK attached to the kernel ρε\rho_{\varepsilon} by The Periodised Kernel of a Periodic Convolution §mass equals Rnρεdλn=1\int_{\mathbb{R}^{n}}\rho_{\varepsilon}\,d\lambda_{n}=1.

Let ηR\eta\in\mathbb{R} with 0<η0<\eta. The numbers η/3\eta/3 and η/2\eta/2 are positive by claim 8 of Elementary Order Arithmetic in an Ordered Field and claim 7 of the same lemma. By Continuous Periodic Functions are Power-Integrable and Dense on the Torus §dense the set of classes [wQ][w|_{Q}] with wCperw\in C_{\mathrm{per}} is dense in Lp(Tn)L^{p}(\mathbb{T}^{n}), so by Characterization of the Closure in a Metric Space by Open Balls the open ball of centre [u][u] and radius η/3\eta/3 in Lp(Tn)L^{p}(\mathbb{T}^{n}) meets it: there is wCperw\in C_{\mathrm{per}} with [wQ][u]Lp(Tn)<η/3\lVert[w|_{Q}]-[u]\rVert_{L^{p}(\mathbb{T}^{n})}<\eta/3, that is, wQup<η/3\lVert w|_{Q}-u\rVert_{p}<\eta/3 by The Lebesgue Space of Power-Integrable Functions §norm.

By A Continuous Lattice-Periodic Function is Uniformly Continuous §uniform, applied to ww with the tolerance η/3\eta/3, there is a real rr with 0<r0<r such that w(x)w(z)η/3|w(x)-w(z)|\le\eta/3 whenever xzr\lVert x-z\rVert\le r. Put ε0=r/δ\varepsilon_{0}=r/\delta, a positive real by claim 7 of Elementary Order Arithmetic in an Ordered Field, and let ε\varepsilon be real with 0<ε<ε00<\varepsilon<\varepsilon_{0}, so that εδ<r\varepsilon\delta<r.

By Minkowski's Inequality and the Seminormed Space of Power-Integrable Functions §minkowski, applied twice,

(ρεu)Qup(ρεu)Q(ρε(wQ))Qp+(ρε(wQ))QwQp+wQup.\bigl\lVert(\rho_{\varepsilon}\star u)|_{Q}-u\bigr\rVert_{p}\le \bigl\lVert(\rho_{\varepsilon}\star u)|_{Q}-\bigl(\rho_{\varepsilon}\star(w|_{Q})\bigr)|_{Q}\bigr\rVert_{p} +\bigl\lVert\bigl(\rho_{\varepsilon}\star(w|_{Q})\bigr)|_{Q}-w|_{Q}\bigr\rVert_{p} +\bigl\lVert w|_{Q}-u\bigr\rVert_{p}.

For the first summand, wQLp(Tn)w|_{Q}\in\mathcal{L}^{p}(\mathbb{T}^{n}) by Continuous Periodic Functions are Power-Integrable and Dense on the Torus §member, and Properties of Periodic Convolution on the Torus §linear with the scalar 1-1 gives ρεuρε(wQ)=ρε(uwQ)\rho_{\varepsilon}\star u-\rho_{\varepsilon}\star(w|_{Q})=\rho_{\varepsilon}\star(u-w|_{Q}); by claim 1 of this theorem, applied to the kernel ρε\rho_{\varepsilon} whose constant is 11, that summand is at most uwQp<η/3\lVert u-w|_{Q}\rVert_{p}<\eta/3.

For the second summand, Properties of Periodic Convolution on the Torus §uniform, applied to the mollifier kernel ρε\rho_{\varepsilon} of radius εδ\varepsilon\delta and to ww with the bound η/3\eta/3 — legitimate because xzεδ\lVert x-z\rVert\le\varepsilon\delta implies xzr\lVert x-z\rVert\le r and hence w(x)w(z)η/3|w(x)-w(z)|\le\eta/3 — gives

(ρε(wQ))(x)w(x)η/3(xRn).\bigl|\bigl(\rho_{\varepsilon}\star(w|_{Q})\bigr)(x)-w(x)\bigr|\le\eta/3\qquad(x\in\mathbb{R}^{n}).

Writing t=η/3t=\eta/3, the difference h=(ρε(wQ))QwQh=\bigl(\rho_{\varepsilon}\star(w|_{Q})\bigr)|_{Q}-w|_{Q} therefore satisfies ht|h|\le t on QQ, so hptp|h|^{p}\le t^{p} by Properties of Real Powers of Nonnegative Real Numbers §monotone and

QhpdλQtpλQ(Q)=tp\int_{Q}|h|^{p}\,d\lambda_{Q}\le t^{p}\lambda_{Q}(Q)=t^{p}

by claim 1 of Linearity and Monotonicity of the Lebesgue Integral and The Integral of an Indicator Function is the Measure of the Set; hence hp(tp)1/p=t=η/3\lVert h\rVert_{p}\le(t^{p})^{1/p}=t=\eta/3 by Power-Integrable Functions and the p-Seminorm §seminorm, Properties of Real Powers of Nonnegative Real Numbers §monotone and Properties of Real Powers of Nonnegative Real Numbers §inverse.

The third summand is less than η/3\eta/3. Adding the three bounds gives (ρεu)Qupη\lVert(\rho_{\varepsilon}\star u)|_{Q}-u\rVert_{p}\le\eta, as asserted.

For the final sentence, let η\eta be a positive real and let ε0\varepsilon_{0} be as above. By The Archimedean Property of the Real Numbers there is a natural number k0k_{0} with 1/ε0<k01/\varepsilon_{0}<k_{0}, hence 1/k0<ε01/k_{0}<\varepsilon_{0} by claim 7 of Elementary Order Arithmetic in an Ordered Field. For every natural kk with k0kk_{0}\le k we have 0<1/k1/k0<ε00<1/k\le1/k_{0}<\varepsilon_{0}, so

[(ρ1/ku)Q][u]Lp(Tn)=(ρ1/ku)Qupη,\bigl\lVert[(\rho_{1/k}\star u)|_{Q}]-[u]\bigr\rVert_{L^{p}(\mathbb{T}^{n})}=\bigl\lVert(\rho_{1/k}\star u)|_{Q}-u\bigr\rVert_{p}\le\eta ,

using The Lebesgue Space of Power-Integrable Functions §norm. As η\eta was an arbitrary positive real, the sequence of these classes converges to [u][u] in Lp(Tn)L^{p}(\mathbb{T}^{n}).

Step 3. Proof of claim 3.

By Existence of Mollifier Kernels of Every Radius there is a mollifier kernel ρ\rho of radius 11 on Rn\mathbb{R}^{n}. Let cLp(Tn)c\in L^{p}(\mathbb{T}^{n}) and let θ\theta be a positive real; choose a representative uLp(Tn)u\in\mathcal{L}^{p}(\mathbb{T}^{n}) with [u]=c[u]=c, which exists by The Lebesgue Space of Power-Integrable Functions §equivalence. By claim 2, applied with η=θ/2\eta=\theta/2, there is a positive real ε\varepsilon with (ρεu)Qupθ/2<θ\lVert(\rho_{\varepsilon}\star u)|_{Q}-u\rVert_{p}\le\theta/2<\theta. The kernel ρε\rho_{\varepsilon} is smooth by Mollifier Kernel of Radius δ\delta on Rn\mathbb{R}^n and Rescaling a Mollifier Kernel, so ρεuCper\rho_{\varepsilon}\star u\in C^{\infty}_{\mathrm{per}} by Properties of Periodic Convolution on the Torus §smooth. Hence the open ball of centre cc and radius θ\theta in Lp(Tn)L^{p}(\mathbb{T}^{n}) contains the class [(ρεu)Q][(\rho_{\varepsilon}\star u)|_{Q}], a member of {[wQ]:wCper}\{[w|_{Q}]:w\in C^{\infty}_{\mathrm{per}}\}. As cc and θ\theta were arbitrary, Characterization of the Closure in a Metric Space by Open Balls gives that the closure of that set is all of Lp(Tn)L^{p}(\mathbb{T}^{n}), that is, the set is dense. \blacksquare

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