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Proof of The Sobolev Embedding of the First Sobolev Space of the Torus into the Sixth Lebesgue Space in Dimensions at Most Three

theoremthm:sobolev-embedding-h1-torus-2026a
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· 17,727 chars · 34 deps · depth 30 Reason: First publication: proof of the Sobolev embedding into the sixth Lebesgue space, by feeding powers of the function into the Gagliardo-Nirenberg inequality and cancelling a common factor, then extending from the continuously differentiable periodic class by mollification and Fatou's lemma.

Powers of the function are fed into the Gagliardo-Nirenberg inequality, with the resulting integrals estimated by Hoelder's inequality, and the common factor is cancelled; the constant five works in each of the three dimensions. The bound passes to the Sobolev space by mollification, an almost-everywhere convergent subsequence and Fatou's lemma.

Proof

Each result cited is universally quantified over the data in its own statement, and is applied here to the data named below. We use silently that the order of R\mathbb{R} is reflexive, transitive and antisymmetric, and that equal real numbers satisfy \le in both directions. Powers of nonnegative real numbers and their properties are those of Measure Spaces and the Lebesgue Integral: Standing Notation §powers; for a measurable ff on (Q,BQ,λQ)(Q,\mathcal{B}_{Q},\lambda_{Q}) and a real number rr with 0<r0<r, fr|f|^{r} denotes the map y(f(y))ry\mapsto(|f(y)|)^{r} of Power-Integrable Functions and the p-Seminorm §measurable-power.

Proof of claim 1. Let uCper1u\in C^{1}_{\mathrm{per}}. By Elementary Properties of the Weak Partial Derivative on the Torus §classical, uCperu\in C_{\mathrm{per}} and juCper\partial_{j}u\in C_{\mathrm{per}} for every j[n]j\in[n], the restrictions uQu|_{Q} and (ju)Q(\partial_{j}u)|_{Q} lie in Lt(Tn)\mathcal{L}^{t}(\mathbb{T}^{n}) for every real tt with 1t1\le t, and [(ju)Q][(\partial_{j}u)|_{Q}] is the jj-th weak partial derivative of [uQ][u|_{Q}]; so [uQ]H1(Tn)[u|_{Q}]\in H^{1}(\mathbb{T}^{n}) by The Sobolev Space of Once Weakly Differentiable Square-Integrable Classes on the Torus §space. Write

N=[uQ]H1,S=uQ6,N=\bigl\lVert[u|_{Q}]\bigr\rVert_{H^{1}},\qquad S=\lVert u|_{Q}\rVert_{6},

both nonnegative real numbers, the first by The Sobolev Space of Once Weakly Differentiable Square-Integrable Classes on the Torus §inner-product and the second by Power-Integrable Functions and the p-Seminorm §seminorm.

(R1) The two elementary bounds. By The Sobolev Space on the Torus is a Separable Hilbert Space Densely Embedded in the Square-Integrable Space §embedding, applied to U=[uQ]U=[u|_{Q}], and by The Lebesgue Space of Power-Integrable Functions §norm, which identifies the norm of a class with the seminorm of a representative,

uQ2N,(ju)Q2N(j[n]),\lVert u|_{Q}\rVert_{2}\le N,\qquad\bigl\lVert(\partial_{j}u)|_{Q}\bigr\rVert_{2}\le N\qquad(j\in[n]),

the norm L2\lVert\,\cdot\,\rVert_{L^{2}} of that theorem being the norm of L2(Tn)L^{2}(\mathbb{T}^{n}) fixed in The Flat Torus: Standing Notation §lebesgue and the jj-th weak partial derivative of [uQ][u|_{Q}] being [(ju)Q][(\partial_{j}u)|_{Q}].

(R2) Powers of uu. For k{2,3,4}k\in\{2,3,4\} let uku^{k} denote the pointwise product of kk copies of uu, formed as u2=uuu^{2}=uu, u3=u2uu^{3}=u^{2}u and u4=u3uu^{4}=u^{3}u. By claim 3 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set and Elementary Properties of Lattice-Periodic Functions §algebra, each uku^{k} lies in Cper1C^{1}_{\mathrm{per}}, and by the pointwise product rule of claim 1 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set,

j(u2)=2uju,j(u3)=3u2ju,j(u4)=4u3ju(j[n]),\partial_{j}(u^{2})=2u\,\partial_{j}u,\qquad\partial_{j}(u^{3})=3u^{2}\,\partial_{j}u,\qquad\partial_{j}(u^{4})=4u^{3}\,\partial_{j}u\qquad(j\in[n]),

each obtained from the previous one, since for instance j(u3u)=(3u2ju)u+u3ju=4u3ju\partial_{j}(u^{3}u)=\bigl(3u^{2}\partial_{j}u\bigr)u+u^{3}\partial_{j}u=4u^{3}\partial_{j}u. Moreover uk(y)=(u(y))k|u^{k}(y)|=(|u(y)|)^{k} for every yy, by claim 4 of Properties of the Absolute Value in an Ordered Field together with Properties of Real Powers of Nonnegative Real Numbers §exponents and Properties of Real Powers of Nonnegative Real Numbers §agreement, which give (u(y))k(|u(y)|)^{k} as the product of kk copies of u(y)|u(y)|.

Consequently, for k{2,3,4}k\in\{2,3,4\} and any real tt with 1t1\le t, the restriction (uk)Q(u^{k})|_{Q} and the map uQk|u|_{Q}|^{k} have the same absolute value at every point of QQ, so the seminorms (uk)Qt\lVert(u^{k})|_{Q}\rVert_{t} and uQkt\bigl\lVert|u|_{Q}|^{k}\bigr\rVert_{t} are equal, both being (Tn(u(y))ktdx)1/t\bigl(\int_{\mathbb{T}^{n}}(|u(y)|)^{kt}\,dx\bigr)^{1/t} by Power-Integrable Functions and the p-Seminorm §seminorm and Properties of Real Powers of Nonnegative Real Numbers §exponents. By Elementary Properties of the p-Seminorm §rescaling, applied to h=uQh=u|_{Q} with the exponents r=kr=k and s=ts=t,

uQkt=(uQkt)k.\bigl\lVert|u|_{Q}|^{k}\bigr\rVert_{t}=\bigl(\lVert u|_{Q}\rVert_{kt}\bigr)^{k}.

In particular (u3)Q2=S3\lVert(u^{3})|_{Q}\rVert_{2}=S^{3}, (u4)Q3/2=S4\lVert(u^{4})|_{Q}\rVert_{3/2}=S^{4}, uQ32=S3\bigl\lVert|u|_{Q}|^{3}\bigr\rVert_{2}=S^{3} and uQ22=(uQ4)2\bigl\lVert|u|_{Q}|^{2}\bigr\rVert_{2}=\bigl(\lVert u|_{Q}\rVert_{4}\bigr)^{2}.

(R3) Four integral estimates. The numbers 22 and 22 are conjugate exponents, since 1<21<2 and 12+12=1\tfrac12+\tfrac12=1. Hence Hoelder's Inequality, for Two and for Finitely Many Factors §holder, applied to the measure space (Q,BQ,λQ)(Q,\mathcal{B}_{Q},\lambda_{Q}) with p=q=2p=q=2, gives Tnfgdxf2g2\int_{\mathbb{T}^{n}}|fg|\,dx\le\lVert f\rVert_{2}\lVert g\rVert_{2} for all f,gL2(Tn)f,g\in\mathcal{L}^{2}(\mathbb{T}^{n}). The maps uQ2|u|_{Q}|^{2} and uQ3|u|_{Q}|^{3} belong to L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}): by Elementary Properties of the p-Seminorm §rescaling, applied to h=uQh=u|_{Q} with s=2s=2 and with r=2r=2 and r=3r=3 in turn, the map hr|h|^{r} lies in L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}) if and only if hh lies in L2r(Tn)\mathcal{L}^{2r}(\mathbb{T}^{n}), which it does, uQu|_{Q} belonging to Lt(Tn)\mathcal{L}^{t}(\mathbb{T}^{n}) for every real tt with 1t1\le t. Taking in turn f=uQ3f=|u|_{Q}|^{3} with g=(ju)Qg=(\partial_{j}u)|_{Q}, f=uQ3f=|u|_{Q}|^{3} with g=uQg=u|_{Q}, f=uQ2f=|u|_{Q}|^{2} with g=(ju)Qg=(\partial_{j}u)|_{Q} and f=uQ2f=|u|_{Q}|^{2} with g=uQg=u|_{Q}, and using (R1), (R2) and the fact that the values of uQk|u|_{Q}|^{k} are nonnegative by Properties of Real Powers of Nonnegative Real Numbers §values, we obtain for every j[n]j\in[n]

TnuQ3(ju)QdxS3N,TnuQ4dxS3N,\int_{\mathbb{T}^{n}}|u|_{Q}|^{3}\,\bigl|(\partial_{j}u)|_{Q}\bigr|\,dx\le S^{3}N,\qquad\int_{\mathbb{T}^{n}}|u|_{Q}|^{4}\,dx\le S^{3}N, TnuQ2(ju)Qdx(uQ4)2N,TnuQ3dx(uQ4)2N,\int_{\mathbb{T}^{n}}|u|_{Q}|^{2}\,\bigl|(\partial_{j}u)|_{Q}\bigr|\,dx\le\bigl(\lVert u|_{Q}\rVert_{4}\bigr)^{2}N,\qquad\int_{\mathbb{T}^{n}}|u|_{Q}|^{3}\,dx\le\bigl(\lVert u|_{Q}\rVert_{4}\bigr)^{2}N ,

the second and fourth because the pointwise products uQ3uQ|u|_{Q}|^{3}\,u|_{Q} and uQ2uQ|u|_{Q}|^{2}\,u|_{Q} have absolute values uQ4|u|_{Q}|^{4} and uQ3|u|_{Q}|^{3}, by claim 4 of Properties of the Absolute Value in an Ordered Field and Properties of Real Powers of Nonnegative Real Numbers §exponents. By Comparison of the Lebesgue Seminorms on the Torus §comparison, applied with r=4r=4 and s=6s=6, we have uQ4S\lVert u|_{Q}\rVert_{4}\le S, so Properties of Real Powers of Nonnegative Real Numbers §monotone turns the last two bounds into S2NS^{2}N.

(R4) Cancelling a power. Let σ\sigma and τ\tau be nonnegative real numbers and let aa and bb be positive real numbers with σa+bτaσb\sigma^{a+b}\le\tau^{a}\,\sigma^{b}. Then στ\sigma\le\tau.

Indeed, if σ=0\sigma=0 then στ\sigma\le\tau since τ\tau is nonnegative. Otherwise 0<σ0<\sigma, so 0<σb0<\sigma^{b} by Properties of Real Powers of Nonnegative Real Numbers §values, and the multiplicative inverse cc of σb\sigma^{b} is positive by claim 7 of Elementary Order Arithmetic in an Ordered Field. Since σa+b=σaσb\sigma^{a+b}=\sigma^{a}\sigma^{b} by Properties of Real Powers of Nonnegative Real Numbers §exponents, multiplying the hypothesis by cc, which is legitimate by claim 5 of Elementary Arithmetic in an Ordered Field, gives σaτa\sigma^{a}\le\tau^{a}. Now Properties of Real Powers of Nonnegative Real Numbers §inverse, in the form sat    st1/as^{a}\le t\iff s\le t^{1/a} with t=τat=\tau^{a}, gives σ(τa)1/a=τ\sigma\le(\tau^{a})^{1/a}=\tau, the last equality by that same clause.

The case n=1n=1. By The Gagliardo-Nirenberg Inequality on the Torus in Dimensions at Most Three §one, u(x)A1|u(x)|\le A_{1} for every xRnx\in\mathbb{R}^{n}, where A1=uQ1+(1u)Q1A_{1}=\lVert u|_{Q}\rVert_{1}+\lVert(\partial_{1}u)|_{Q}\rVert_{1}. By Comparison of the Lebesgue Seminorms on the Torus §comparison, applied with r=1r=1 and s=2s=2, and by (R1), each of the two seminorms is at most NN, so A1N+N=2NA_{1}\le N+N=2N. Hence u(x)2N|u(x)|\le2N for every xx, and Continuous Periodic Functions are Power-Integrable and Dense on the Torus §member, applied with p=6p=6 and M=2NM=2N, gives uQ62N\lVert u|_{Q}\rVert_{6}\le2N. Finally 2N5N2N\le5N by claim 5 of Elementary Arithmetic in an Ordered Field, since 252\le5 and 0N0\le N.

The case n=2n=2. Put v=u3v=u^{3}. By Elementary Properties of the p-Seminorm §power, applied with p=1p=1, and Properties of Real Powers of Nonnegative Real Numbers §agreement,

vQ1=TnuQ3dxS2N,(jv)Q1=3TnuQ2(ju)Qdx3S2N,\lVert v|_{Q}\rVert_{1}=\int_{\mathbb{T}^{n}}|u|_{Q}|^{3}\,dx\le S^{2}N,\qquad\bigl\lVert(\partial_{j}v)|_{Q}\bigr\rVert_{1}=3\int_{\mathbb{T}^{n}}|u|_{Q}|^{2}\,\bigl|(\partial_{j}u)|_{Q}\bigr|\,dx\le3S^{2}N,

by (R2), (R3) and claim 4 of Properties of the Absolute Value in an Ordered Field, which gives 3u2ju=3u2ju|3u^{2}\partial_{j}u|=3|u|^{2}|\partial_{j}u|, together with the linearity in claim 2 of Linearity and Monotonicity of the Lebesgue Integral. So the numbers Aj=vQ1+(jv)Q1A_{j}=\lVert v|_{Q}\rVert_{1}+\lVert(\partial_{j}v)|_{Q}\rVert_{1} of The Gagliardo-Nirenberg Inequality on the Torus in Dimensions at Most Three satisfy Aj4S2NA_{j}\le4S^{2}N for j[2]j\in[2]. By The Gagliardo-Nirenberg Inequality on the Torus in Dimensions at Most Three §two, applied to vCper1v\in C^{1}_{\mathrm{per}}, and by (R2),

S6=(S3)2=(vQ2)2A1A2(4S2N)2=16S4N2,S^{6}=\bigl(S^{3}\bigr)^{2}=\bigl(\lVert v|_{Q}\rVert_{2}\bigr)^{2}\le A_{1}A_{2}\le\bigl(4S^{2}N\bigr)^{2}=16\,S^{4}N^{2},

using Properties of Real Powers of Nonnegative Real Numbers §exponents for (S3)2=S6(S^{3})^{2}=S^{6}, claim 5 of Elementary Arithmetic in an Ordered Field twice for the product of the two bounds, and Properties of Real Powers of Nonnegative Real Numbers §product for the last equality. Since 16N2=(4N)216N^{2}=(4N)^{2} by Properties of Real Powers of Nonnegative Real Numbers §product, (R4) applied with σ=S\sigma=S, τ=4N\tau=4N, a=2a=2 and b=4b=4 gives S4NS\le4N, and 4N5N4N\le5N by claim 5 of Elementary Arithmetic in an Ordered Field.

The case n=3n=3. Put v=u4v=u^{4}. Exactly as in the previous case, with the first and second estimates of (R3) in place of the third and fourth,

vQ1=TnuQ4dxS3N,(jv)Q1=4TnuQ3(ju)Qdx4S3N,\lVert v|_{Q}\rVert_{1}=\int_{\mathbb{T}^{n}}|u|_{Q}|^{4}\,dx\le S^{3}N,\qquad\bigl\lVert(\partial_{j}v)|_{Q}\bigr\rVert_{1}=4\int_{\mathbb{T}^{n}}|u|_{Q}|^{3}\,\bigl|(\partial_{j}u)|_{Q}\bigr|\,dx\le4S^{3}N,

so Aj5S3NA_{j}\le5S^{3}N for j[3]j\in[3]. By The Gagliardo-Nirenberg Inequality on the Torus in Dimensions at Most Three §three, applied to vv, together with (R2), Properties of Real Powers of Nonnegative Real Numbers §monotone, Properties of Real Powers of Nonnegative Real Numbers §exponents and Properties of Real Powers of Nonnegative Real Numbers §product,

S6=(S4)3/2=(vQ3/2)3/2(A1A2A3)1/2((5S3N)3)1/2=(5N)3/2S9/2,S^{6}=\bigl(S^{4}\bigr)^{3/2}=\bigl(\lVert v|_{Q}\rVert_{3/2}\bigr)^{3/2}\le\bigl(A_{1}A_{2}A_{3}\bigr)^{1/2}\le\Bigl(\bigl(5S^{3}N\bigr)^{3}\Bigr)^{1/2}=\bigl(5N\bigr)^{3/2}\,S^{9/2},

the second inequality because A1A2A3(5S3N)3A_{1}A_{2}A_{3}\le(5S^{3}N)^{3} by claim 5 of Elementary Arithmetic in an Ordered Field applied twice, all factors being nonnegative. Now (R4), applied with σ=S\sigma=S, τ=5N\tau=5N, a=3/2a=3/2 and b=9/2b=9/2, gives S5NS\le5N.

In each of the three cases uQ6=S5N\lVert u|_{Q}\rVert_{6}=S\le5N, which is claim 1.

Proof of claim 2. Let UH1(Tn)U\in H^{1}(\mathbb{T}^{n}), let vv be a representative of UU and put N=UH1N=\lVert U\rVert_{H^{1}}, a nonnegative real number.

Step 1: mollification. Let ρ\rho be a mollifier kernel of radius 11 on Rn\mathbb{R}^{n}, which exists by Existence of Mollifier Kernels of Every Radius, and for a natural number kk let ρ1/k\rho_{1/k} be its rescaling with parameter 1/k1/k. By The Sobolev Space on the Torus is a Separable Hilbert Space Densely Embedded in the Square-Integrable Space §mollify, applied with δ=1\delta=1, with UU and with the representative vv, the maps uk=ρ1/kvu_{k}=\rho_{1/k}\star v lie in CperC^{\infty}_{\mathrm{per}} and the classes Uk=[ukQ]U_{k}=[u_{k}|_{Q}] lie in H1(Tn)H^{1}(\mathbb{T}^{n}); moreover UkH1N\lVert U_{k}\rVert_{H^{1}}\le N by The Sobolev Space on the Torus is a Separable Hilbert Space Densely Embedded in the Square-Integrable Space §mollify-bound, and the sequence (Uk)kN(U_{k})_{k\in\mathbb{N}} converges to UU in H1(Tn)H^{1}(\mathbb{T}^{n}) by The Sobolev Space on the Torus is a Separable Hilbert Space Densely Embedded in the Square-Integrable Space §mollify-converge.

A smooth map on Rn\mathbb{R}^{n} is of class C1C^{1} by Smooth Map on a Euclidean Open Set, so each uku_{k}, being Zn\mathbb{Z}^{n}-periodic and smooth, lies in Cper1C^{1}_{\mathrm{per}} by Lattice-Periodic Functions and the Periodic Function Classes §classes. Claim 1, applied to uku_{k}, therefore gives

ukQ65UkH15N,\lVert u_{k}|_{Q}\rVert_{6}\le5\lVert U_{k}\rVert_{H^{1}}\le5N ,

the second inequality by claim 5 of Elementary Arithmetic in an Ordered Field.

Step 2: an almost everywhere convergent subsequence. By The Sobolev Space on the Torus is a Separable Hilbert Space Densely Embedded in the Square-Integrable Space §embedding the distance in L2(Tn)L^{2}(\mathbb{T}^{n}) between two members of H1(Tn)H^{1}(\mathbb{T}^{n}) is at most their distance in H1(Tn)H^{1}(\mathbb{T}^{n}), so any positive real witnessing the convergence of (Uk)(U_{k}) to UU in H1(Tn)H^{1}(\mathbb{T}^{n}) witnesses it in L2(Tn)L^{2}(\mathbb{T}^{n}) as well; thus (Uk)(U_{k}) converges to UU in L2(Tn)L^{2}(\mathbb{T}^{n}) by Convergent Sequence in a Metric Space. By The Riesz-Fischer Theorem: the Lebesgue Space is a Real Banach Space §subsequence, applied with p=2p=2 to this sequence, to the representatives ukQu_{k}|_{Q} of UkU_{k} and to the representative vv of UU, there are natural numbers m1<m2<m_{1}<m_{2}<\dots and a null set E0E_{0} such that for every yQE0y\in Q\setminus E_{0} the sequence (umj(y))jN(u_{m_{j}}(y))_{j\in\mathbb{N}} converges to v(y)v(y). That clause also provides a dominating function, which is not needed here. A null set is not required to lie in BQ\mathcal{B}_{Q}, so we enlarge it: by Null Set of a Measure there is EBQE\in\mathcal{B}_{Q} with E0EE_{0}\subseteq E and λQ(E)=0\lambda_{Q}(E)=0, and this EE is itself a null set. Since QEQE0Q\setminus E\subseteq Q\setminus E_{0}, the sequence (umj(y))jN(u_{m_{j}}(y))_{j\in\mathbb{N}} converges to v(y)v(y) for every yQEy\in Q\setminus E.

Step 3: two maps into the extended half-line. For jNj\in\mathbb{N} let gj:Q[0,]g_{j}:Q\to[0,\infty] be the map taking the value (umj(y))6(|u_{m_{j}}(y)|)^{6} at yQEy\in Q\setminus E and the value 00 at yEy\in E, and let g:Q[0,]g:Q\to[0,\infty] take the value (v(y))6(|v(y)|)^{6} at yQEy\in Q\setminus E and the value 00 at yEy\in E. The maps umjQ6|u_{m_{j}}|_{Q}|^{6} and v6|v|^{6} are measurable with respect to BQ\mathcal{B}_{Q} by Power-Integrable Functions and the p-Seminorm §measurable-power, the set QEQ\setminus E lies in BQ\mathcal{B}_{Q}, that being a σ\sigma-algebra on QQ of which EE is a member, and its indicator is measurable by claim 1 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and gjg_{j} and gg are the pointwise products of these, hence measurable by claim 3 of that lemma; their values are nonnegative by Properties of Real Powers of Nonnegative Real Numbers §values, so they are measurable as maps into [0,][0,\infty] by Measure Spaces and the Lebesgue Integral: Standing Notation §measurable.

We claim that g(y)lim infjgj(y)g(y)\le\liminf_{j}g_{j}(y) for every yQy\in Q, the limit inferior being the one defined in Fatou's Lemma. For yEy\in E this holds because g(y)=0g(y)=0 and every value gj(y)g_{j}(y) is nonnegative, so every greatest lower bound occurring in the definition is nonnegative and hence so is their least upper bound. Let then yQEy\in Q\setminus E and write αj=gj(y)\alpha_{j}=g_{j}(y) and α=g(y)\alpha=g(y). By claim 7 of Properties of the Absolute Value in an Ordered Field the sequence (umj(y))j(|u_{m_{j}}(y)|)_{j} converges to v(y)|v(y)|, and then Properties of Real Powers of Nonnegative Real Numbers §continuity, applied with the exponent 66, shows that (αj)j(\alpha_{j})_{j} converges to α\alpha. Let ε\varepsilon be a real number with 0<ε0<\varepsilon. There is kNk\in\mathbb{N} with αjα<ε|\alpha_{j}-\alpha|<\varepsilon for every jNj\in\mathbb{N} with kjk\le j, so αεαj\alpha-\varepsilon\le\alpha_{j} for all such jj by claim 3 of Properties of the Absolute Value in an Ordered Field; hence αε\alpha-\varepsilon is a lower bound of the values αj\alpha_{j} with kjk\le j, so αεinfjkαjlim infjαj\alpha-\varepsilon\le\inf_{j\ge k}\alpha_{j}\le\liminf_{j}\alpha_{j}, the last step because that greatest lower bound is one of the numbers whose least upper bound is the limit inferior. Write L=lim infjαjL=\liminf_{j}\alpha_{j}. If L=L=\infty then αL\alpha\le L; otherwise LL is a nonnegative real number, and if L<αL<\alpha we may take ε=(αL)/2\varepsilon=(\alpha-L)/2, which is positive by claim 3 of Elementary Arithmetic in an Ordered Field and claim 8 of Elementary Order Arithmetic in an Ordered Field, and then αεL\alpha-\varepsilon\le L together with ε<αL\varepsilon<\alpha-L, again by claim 8, gives L<αεLL<\alpha-\varepsilon\le L, a contradiction. So αL\alpha\le L in every case.

Step 4: Fatou's lemma. For every jj and every yQy\in Q we have gj(y)umjQ6(y)g_{j}(y)\le|u_{m_{j}}|_{Q}|^{6}(y), the two being equal off EE and the right-hand side being nonnegative on EE. So The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §comparison, Elementary Properties of the p-Seminorm §power applied with p=6p=6, Step 1 and Properties of Real Powers of Nonnegative Real Numbers §monotone give

TngjdxTnumjQ6dx=(umjQ6)6(5N)6(jN).\int_{\mathbb{T}^{n}}g_{j}\,dx\le\int_{\mathbb{T}^{n}}|u_{m_{j}}|_{Q}|^{6}\,dx=\bigl(\lVert u_{m_{j}}|_{Q}\rVert_{6}\bigr)^{6}\le(5N)^{6}\qquad(j\in\mathbb{N}).

Consequently (5N)6(5N)^{6} is an upper bound of every greatest lower bound occurring in the definition of lim infjTngjdx\liminf_{j}\int_{\mathbb{T}^{n}}g_{j}\,dx, so that limit inferior is at most (5N)6(5N)^{6}. By Fatou's Lemma, applied to the measure space (Q,BQ,λQ)(Q,\mathcal{B}_{Q},\lambda_{Q}) and the sequence (gj)(g_{j}), and by Step 3 with The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §comparison,

TngdxTn(lim infjgj)dxlim infjTngjdx(5N)6.\int_{\mathbb{T}^{n}}g\,dx\le\int_{\mathbb{T}^{n}}\Bigl(\liminf_{j}g_{j}\Bigr)dx\le\liminf_{j}\int_{\mathbb{T}^{n}}g_{j}\,dx\le(5N)^{6}.

Step 5: conclusion. The maps gg and v6|v|^{6} agree at every point of QEQ\setminus E, and EE is null, so they agree almost everywhere and The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §comparison gives

Tnv6dx=Tngdx(5N)6,\int_{\mathbb{T}^{n}}|v|^{6}\,dx=\int_{\mathbb{T}^{n}}g\,dx\le(5N)^{6},

which is finite. The map vv is measurable with respect to BQ\mathcal{B}_{Q}, being a member of L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}), so vL6(Tn)v\in\mathcal{L}^{6}(\mathbb{T}^{n}) by Power-Integrable Functions and the p-Seminorm §space. Finally, 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,

v6=(Tnv6dx)1/6((5N)6)1/6=5N,\lVert v\rVert_{6}=\Bigl(\int_{\mathbb{T}^{n}}|v|^{6}\,dx\Bigr)^{1/6}\le\bigl((5N)^{6}\bigr)^{1/6}=5N ,

which is claim 2.

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