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Proof of Elementary Properties of the Weak Partial Derivative on the Torus

lemmalem:weak-derivative-torus-basic-2026a
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· 14,360 chars · 33 deps · depth 27 Reason: First publication: integration by parts on the torus, linearity of the pairing, approximation of the test function and of the pair of classes with passage to the limit in the pairing bound, and testing against the periodised kernel for the mollification identity.

Agreement with the classical derivative is integration by parts on the torus; linearity and the class statements come from linearity of the pairing; the enlarged test class and the closure statement follow by approximating the test function, respectively the pair of classes, and passing to the limit in the pairing bound; mollification is handled by testing against the periodised kernel and differentiating it.

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 lemma. Throughout, every member of Lr(Tn)\mathcal{L}^{r}(\mathbb{T}^{n}) lies in L1(Tn)\mathcal{L}^{1}(\mathbb{T}^{n}) by The Periodic Extension of a Function on the Unit Cell §finite-measure, so Pairing an Integrable Function on the Torus with a Continuous Periodic Function §pairing applies to it; and a member of CperC^{\infty}_{\mathrm{per}} lies in Cper1C^{1}_{\mathrm{per}}, and a member of Cper1C^{1}_{\mathrm{per}} in CperC_{\mathrm{per}}, by claims 2 and 3 of Euclidean Space is Open in Itself, and CkC^k Maps are Continuous together with Lattice-Periodic Functions and the Periodic Function Classes §classes. For φCper1\varphi\in C^{1}_{\mathrm{per}} we have iφCper\partial_{i}\varphi\in C_{\mathrm{per}}, and for φCper\varphi\in C^{\infty}_{\mathrm{per}} we have iφCper\partial_{i}\varphi\in C^{\infty}_{\mathrm{per}}, by Elementary Properties of Lattice-Periodic Functions §derivative.

Step 1. Proof of claim 1.

Let uCper1u\in C^{1}_{\mathrm{per}} and let φCper\varphi\in C^{\infty}_{\mathrm{per}}, so that φCper1\varphi\in C^{1}_{\mathrm{per}}. By Vanishing Mean of a Derivative and Integration by Parts on the Torus §parts, applied with g=ug=u and h=φh=\varphi,

Tn(iu)φdx=Tnu(iφ)dx.\int_{\mathbb{T}^{n}}(\partial_{i}u)\,\varphi\,dx=-\int_{\mathbb{T}^{n}}u\,(\partial_{i}\varphi)\,dx .

In the abbreviation fixed in that lemma each side is the integral over Tn\mathbb{T}^{n} of the restriction to QQ of the displayed product, and the restriction of a pointwise product is the product of the restrictions, so the display says

TnuQ((iφ)Q)dx=Tn(iu)Q(φQ)dx.\int_{\mathbb{T}^{n}}u|_{Q}\,\bigl((\partial_{i}\varphi)|_{Q}\bigr)\,dx=-\int_{\mathbb{T}^{n}}(\partial_{i}u)|_{Q}\,(\varphi|_{Q})\,dx .

As φ\varphi was arbitrary, (iu)Q(\partial_{i}u)|_{Q} is an ii-th weak partial derivative of uQu|_{Q} in the sense of The Weak Partial Derivative on the Torus §weak-derivative; since uQu|_{Q} and (iu)Q(\partial_{i}u)|_{Q} lie in Lr(Tn)\mathcal{L}^{r}(\mathbb{T}^{n}) for every real rr with 1r1\le r, as recorded in the claim, The Weak Partial Derivative on the Torus §class-derivative gives that [(iu)Q][(\partial_{i}u)|_{Q}] is the ii-th weak partial derivative of [uQ][u|_{Q}] in Lr(Tn)L^{r}(\mathbb{T}^{n}).

Step 2. Proof of claim 2.

Let u,uu,u' represent U,UU,U' and let g,gg,g' represent iU,iU\partial_{i}U,\partial_{i}U'. Then u+cuLp(Tn)u+c\,u'\in\mathcal{L}^{p}(\mathbb{T}^{n}) and g+cgLq(Tn)g+c\,g'\in\mathcal{L}^{q}(\mathbb{T}^{n}) by Minkowski's Inequality and the Seminormed Space of Power-Integrable Functions §vector-space, and they represent U+cUU+c\,U' and iU+ciU\partial_{i}U+c\,\partial_{i}U' by The Lebesgue Space of Power-Integrable Functions §space, under which the vector operations on classes are induced by the pointwise ones. Let φCper\varphi\in C^{\infty}_{\mathrm{per}}. Using Pairing an Integrable Function on the Torus with a Continuous Periodic Function §linear twice and the defining identities for UU and for UU',

Tn(u+cu)((iφ)Q)dx=Tnu((iφ)Q)dx+cTnu((iφ)Q)dx=Tn(g+cg)(φQ)dx.\int_{\mathbb{T}^{n}}(u+c\,u')\,\bigl((\partial_{i}\varphi)|_{Q}\bigr)\,dx =\int_{\mathbb{T}^{n}}u\,\bigl((\partial_{i}\varphi)|_{Q}\bigr)dx+c\int_{\mathbb{T}^{n}}u'\,\bigl((\partial_{i}\varphi)|_{Q}\bigr)dx =-\int_{\mathbb{T}^{n}}(g+c\,g')\,(\varphi|_{Q})\,dx .

As φ\varphi was arbitrary, claim 2 follows by The Weak Partial Derivative on the Torus §class-derivative, which also supplies the uniqueness that makes the displayed identification legitimate.

Step 3. Proof of claim 3.

Let φCper1\varphi\in C^{1}_{\mathrm{per}} and put

D=Tnu((iφ)Q)dx+Tng(φQ)dx,K=Tnudx+Tngdx,D=\int_{\mathbb{T}^{n}}u\,\bigl((\partial_{i}\varphi)|_{Q}\bigr)\,dx+\int_{\mathbb{T}^{n}}g\,(\varphi|_{Q})\,dx , \qquad K=\int_{\mathbb{T}^{n}}|u|\,dx+\int_{\mathbb{T}^{n}}|g|\,dx ,

both real numbers, KK being nonnegative by claim 1 of Linearity and Monotonicity of the Lebesgue Integral. We show that Dθ|D|\le\theta for every real θ\theta with 0<θ0<\theta; then D=0D=0 by Comparison of Real Numbers with Arbitrary Positive Slack §vanishing, which is claim 3.

Let θ\theta be a real number with 0<θ0<\theta and put η=θ(1+K)1\eta=\theta\,(1+K)^{-1}, a positive real number by claims 7 and 5 of Elementary Order Arithmetic in an Ordered Field, since 0<1+K0<1+K by claims 6 and 3 of that lemma, applied with 0<10<1 and 0K0\le K. By Existence of Mollifier Kernels of Every Radius there is a mollifier kernel ρ\rho of radius 11 on Rn\mathbb{R}^{n}. By Transfer of a Partial Derivative in Periodic Convolution §uniform-c1, applied with that kernel, the function φ\varphi and the tolerance η\eta, there is a positive real ε0\varepsilon_{0} such that for every real ε\varepsilon with 0<ε<ε00<\varepsilon<\varepsilon_{0} the map φε=ρε(φQ)\varphi_{\varepsilon}=\rho_{\varepsilon}\star(\varphi|_{Q}) satisfies

φε(x)φ(x)ηandiφε(x)iφ(x)η(xRn).|\varphi_{\varepsilon}(x)-\varphi(x)|\le\eta\qquad\text{and}\qquad|\partial_{i}\varphi_{\varepsilon}(x)-\partial_{i}\varphi(x)|\le\eta\qquad(x\in\mathbb{R}^{n}).

Fix such an ε\varepsilon, for instance ε0/2\varepsilon_{0}/2, positive and smaller than ε0\varepsilon_{0} by claim 8 of Elementary Order Arithmetic in an Ordered Field. Here φQL1(Tn)\varphi|_{Q}\in\mathcal{L}^{1}(\mathbb{T}^{n}) by Continuous Periodic Functions are Power-Integrable and Dense on the Torus §member and ρε\rho_{\varepsilon} is smooth by Mollifier Kernel of Radius δ\delta on Rn\mathbb{R}^n, so φεCper\varphi_{\varepsilon}\in C^{\infty}_{\mathrm{per}} by Properties of Periodic Convolution on the Torus §smooth. The defining identity for UU, applied with the test function φε\varphi_{\varepsilon}, gives

Tnu((iφε)Q)dx+Tng(φεQ)dx=0.\int_{\mathbb{T}^{n}}u\,\bigl((\partial_{i}\varphi_{\varepsilon})|_{Q}\bigr)\,dx+\int_{\mathbb{T}^{n}}g\,(\varphi_{\varepsilon}|_{Q})\,dx=0 .

The maps iφεiφ\partial_{i}\varphi_{\varepsilon}-\partial_{i}\varphi and φεφ\varphi_{\varepsilon}-\varphi lie in CperC_{\mathrm{per}} by Elementary Properties of Lattice-Periodic Functions §algebra, used with the scalar 1-1, and are bounded in absolute value by η\eta; so Pairing an Integrable Function on the Torus with a Continuous Periodic Function §linear and Pairing an Integrable Function on the Torus with a Continuous Periodic Function §pairing give

Tnu((iφε)Q)dxTnu((iφ)Q)dxηTnudx,\Bigl|\int_{\mathbb{T}^{n}}u\,\bigl((\partial_{i}\varphi_{\varepsilon})|_{Q}\bigr)dx-\int_{\mathbb{T}^{n}}u\,\bigl((\partial_{i}\varphi)|_{Q}\bigr)dx\Bigr|\le\eta\int_{\mathbb{T}^{n}}|u|\,dx ,

and likewise with gg, φε\varphi_{\varepsilon}, φ\varphi in place of uu, iφε\partial_{i}\varphi_{\varepsilon}, iφ\partial_{i}\varphi. Subtracting the vanishing identity from DD and applying the triangle inequality, claim 5 of Properties of the Absolute Value in an Ordered Field,

DηTnudx+ηTngdx=ηKη(1+K)=θ,|D|\le\eta\int_{\mathbb{T}^{n}}|u|\,dx+\eta\int_{\mathbb{T}^{n}}|g|\,dx=\eta\,K\le\eta\,(1+K)=\theta ,

the last inequality by claim 5 of Elementary Arithmetic in an Ordered Field with the nonnegative factor η\eta, since K1+KK\le1+K.

Step 4. Proof of claim 4.

By Mollifier Kernel of Radius δ\delta on Rn\mathbb{R}^n the map ρε\rho_{\varepsilon} is smooth and vanishes at every yy with εδ<y\varepsilon\delta<\lVert y\rVert, so it satisfies the hypotheses placed on a kernel in The Periodised Kernel of a Periodic Convolution, with the radius εδ\varepsilon\delta; and iρε\partial_{i}\rho_{\varepsilon} is continuous and vanishes at every such yy by Convolution of a Locally Integrable Function with a Compactly Supported Kernel §derivative, so it does too. Let Ψ\Psi be the periodised kernel of ρε\rho_{\varepsilon} and Ψ(i)\Psi^{(i)} that of iρε\partial_{i}\rho_{\varepsilon}, and for xRnx\in\mathbb{R}^{n} let Ψx\Psi_{x} and Ψx(i)\Psi^{(i)}_{x} be the restrictions to QQ of Ψ(x,)\Psi(x,\cdot) and Ψ(i)(x,)\Psi^{(i)}(x,\cdot). Both ρεu\rho_{\varepsilon}\star u and ρεg\rho_{\varepsilon}\star g lie in CperC^{\infty}_{\mathrm{per}} by Properties of Periodic Convolution on the Torus §smooth.

Fix xRnx\in\mathbb{R}^{n}. By that same clause and The Periodised Kernel of a Periodic Convolution §representation, applied to the kernel iρε\partial_{i}\rho_{\varepsilon} and the function uu,

i(ρεu)(x)=((iρε)u)(x)=TnΨx(i)udy.\partial_{i}(\rho_{\varepsilon}\star u)(x)=\bigl((\partial_{i}\rho_{\varepsilon})\star u\bigr)(x)=\int_{\mathbb{T}^{n}}\Psi^{(i)}_{x}\,u\,dy .

By The Periodised Kernel of a Periodic Convolution §derivative we have iΨ(x,)=Ψ(i)(x,)\partial_{i}\Psi(x,\cdot)=-\Psi^{(i)}(x,\cdot) as maps on Rn\mathbb{R}^{n}, so Ψx(i)\Psi^{(i)}_{x} is the restriction to QQ of iΨ(x,)-\partial_{i}\Psi(x,\cdot), and claim 2 of Linearity and Monotonicity of the Lebesgue Integral, with the scalar 1-1, gives

TnΨx(i)udy=Tnu((iΨ(x,))Q)dy.\int_{\mathbb{T}^{n}}\Psi^{(i)}_{x}\,u\,dy=-\int_{\mathbb{T}^{n}}u\,\bigl((\partial_{i}\Psi(x,\cdot))|_{Q}\bigr)\,dy .

The map Ψ(x,)\Psi(x,\cdot) lies in CperC^{\infty}_{\mathrm{per}} by The Periodised Kernel of a Periodic Convolution §regularity, so the defining identity for UU, applied with the test function Ψ(x,)\Psi(x,\cdot), and then The Periodised Kernel of a Periodic Convolution §representation applied to the kernel ρε\rho_{\varepsilon} and the function gg, give

Tnu((iΨ(x,))Q)dy=TngΨxdy=(ρεg)(x).\int_{\mathbb{T}^{n}}u\,\bigl((\partial_{i}\Psi(x,\cdot))|_{Q}\bigr)\,dy=-\int_{\mathbb{T}^{n}}g\,\Psi_{x}\,dy=-(\rho_{\varepsilon}\star g)(x).

Combining the three displays, i(ρεu)(x)=(ρεg)(x)\partial_{i}(\rho_{\varepsilon}\star u)(x)=(\rho_{\varepsilon}\star g)(x). As xx was arbitrary, claim 4 follows.

Step 5. Proof of claim 5.

Let φCper\varphi\in C^{\infty}_{\mathrm{per}}. By Elementary Properties of Lattice-Periodic Functions §bounded there are nonnegative reals MM and MM' with φ(x)M|\varphi(x)|\le M and iφ(x)M|\partial_{i}\varphi(x)|\le M' for every xx; put N=M+MN=M+M', so that NN is nonnegative and bounds both, by claim 2 of Elementary Arithmetic in an Ordered Field and claim 3 of that lemma. Let u,g,uk,gku,g,u_{k},g_{k} be representatives of U,G,Uk,GkU,G,U_{k},G_{k} and put

D=Tnu((iφ)Q)dx+Tng(φQ)dx.D=\int_{\mathbb{T}^{n}}u\,\bigl((\partial_{i}\varphi)|_{Q}\bigr)\,dx+\int_{\mathbb{T}^{n}}g\,(\varphi|_{Q})\,dx .

For every kk the defining identity for UkU_{k} gives Tnuk((iφ)Q)dx+Tngk(φQ)dx=0\int_{\mathbb{T}^{n}}u_{k}((\partial_{i}\varphi)|_{Q})dx+\int_{\mathbb{T}^{n}}g_{k}(\varphi|_{Q})dx=0, so by Pairing an Integrable Function on the Torus with a Continuous Periodic Function §linear, Pairing an Integrable Function on the Torus with a Continuous Periodic Function §pairing and the triangle inequality, claim 5 of Properties of the Absolute Value in an Ordered Field,

DNTnuukdx+NTnggkdx.|D|\le N\int_{\mathbb{T}^{n}}|u-u_{k}|\,dx+N\int_{\mathbb{T}^{n}}|g-g_{k}|\,dx .

The differences uuku-u_{k} and ggkg-g_{k} lie in L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}) by Minkowski's Inequality and the Seminormed Space of Power-Integrable Functions §vector-space, used with the scalar 1-1. Now Tnuukdx=uuk1\int_{\mathbb{T}^{n}}|u-u_{k}|\,dx=\lVert u-u_{k}\rVert_{1} by Power-Integrable Functions and the p-Seminorm §seminorm and Properties of Real Powers of Nonnegative Real Numbers §agreement, and uuk1uuk2\lVert u-u_{k}\rVert_{1}\le\lVert u-u_{k}\rVert_{2} by The Periodic Extension of a Function on the Unit Cell §finite-measure; and uuk2\lVert u-u_{k}\rVert_{2} is the distance from UkU_{k} to UU in the metric of L2(Tn)L^{2}(\mathbb{T}^{n}), by The Lebesgue Space of Power-Integrable Functions §norm and Real Normed Space and Real Banach Space §distance. The same holds for gg and gkg_{k}.

Let ϑ\vartheta be a real number with 0<ϑ0<\vartheta and put θ=ϑ(1+2N)1\theta=\vartheta\,(1+2N)^{-1}, positive by claims 7 and 5 of Elementary Order Arithmetic in an Ordered Field, since 02N0\le2N by claim 2 of Elementary Arithmetic in an Ordered Field and hence 0<1+2N0<1+2N by claims 6 and 3 of the former lemma. Since (Uk)(U_{k}) converges to UU and (Gk)(G_{k}) to GG in that metric, Convergent Sequence in a Metric Space provides indices beyond which each distance is at most θ\theta; choosing a kk beyond both and combining with the two displays,

DNθ+Nθ=2Nθ(1+2N)θ=ϑ,|D|\le N\theta+N\theta=2N\theta\le(1+2N)\,\theta=\vartheta ,

by claim 5 of Elementary Arithmetic in an Ordered Field with the nonnegative factor θ\theta. As ϑ\vartheta was arbitrary and D|D| is nonnegative, Comparison of Real Numbers with Arbitrary Positive Slack §vanishing gives D=0D=0. As φ\varphi was arbitrary, GG is the ii-th weak partial derivative of UU by The Weak Partial Derivative on the Torus §class-derivative.

Step 6. Proof of claim 6.

The constant map with value 00 on Rn\mathbb{R}^{n} is smooth by claim 2 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set, and it is Zn\mathbb{Z}^{n}-periodic because its values at xx and at x+mx+m are both 00, for every xRnx\in\mathbb{R}^{n} and every mZnm\in\mathbb{Z}^{n}; hence it lies in Cper1C^{1}_{\mathrm{per}}. Claim 1, used with r=2r=2 and applied at every index j[n]j\in[n] in place of ii, that claim being stated for an arbitrary index, gives [uQ]W[u|_{Q}]\in W for every uCper1u\in C^{1}_{\mathrm{per}}; in particular the class of the constant map just described lies in WW, so WW is nonempty. If U,VWU,V\in W and cRc\in\mathbb{R} then U+cVL2(Tn)U+c\,V\in L^{2}(\mathbb{T}^{n}) by The Riesz-Fischer Theorem: the Lebesgue Space is a Real Banach Space §normed, and for each j[n]j\in[n] its jj-th weak partial derivative exists in L2(Tn)L^{2}(\mathbb{T}^{n}) by claim 2, used with p=q=2p=q=2 and the index jj; so U+cVWU+c\,V\in W and WW is a linear subspace of L2(Tn)L^{2}(\mathbb{T}^{n}).

For U,VWU,V\in W every term of U,VW\langle U,V\rangle_{W} is a real number, so the map is defined; the index set [n][n] is nonempty because 1n1\le n. By claim 1 of Properties of a Sum over a Finite Index Set the sum j=1n\sum_{j=1}^{n} agrees with the sum over the finite set [n][n] of Sum over a Finite Index Set, for which claims 3 and 4 of that lemma give additivity and homogeneity. By The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space §inner-product the map ,L2\langle\,\cdot\,,\cdot\,\rangle_{L^{2}} is an inner product, hence symmetric, linear in its first argument and positive definite by Real Inner Product Space §inner-product; and by claim 2 the map UjUU\mapsto\partial_{j}U is linear on WW for each jj. Symmetry of ,W\langle\,\cdot\,,\cdot\,\rangle_{W} follows termwise, and linearity in the first argument follows from linearity of ,L2\langle\,\cdot\,,\cdot\,\rangle_{L^{2}}, linearity of UjUU\mapsto\partial_{j}U, and the additivity and homogeneity of the sum just cited.

For positivity, let UWU\in W. Each term jU,jUL2\langle\partial_{j}U,\partial_{j}U\rangle_{L^{2}} is nonnegative, so by induction over the members of [n][n], using claim 2 of Elementary Arithmetic in an Ordered Field and the peeling identity of Peeling, Splitting, and Interchange for Sums over a Finite Index Set, the sum is nonnegative; hence 0U,UL2U,UW0\le\langle U,U\rangle_{L^{2}}\le\langle U,U\rangle_{W} by claim 3 of Elementary Arithmetic in an Ordered Field. If U,UW=0\langle U,U\rangle_{W}=0 then U,UL2=0\langle U,U\rangle_{L^{2}}=0, so UU is the zero element of L2(Tn)L^{2}(\mathbb{T}^{n}) by the positive definiteness of that inner product; and conversely U,UW=0\langle U,U\rangle_{W}=0 when UU is the zero element, by the linearity just established. So ,W\langle\,\cdot\,,\cdot\,\rangle_{W} meets the conditions of Real Inner Product Space §inner-product and WW with it is a real inner product space. \blacksquare

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