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Proof of A Bound for the Lebesgue Measure of a Bounded Slab in Rn\mathbb{R}^n

lemmalem:lebesgue-slab-bound-rn-2026a
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Β· 7,155 chars Β· 13 deps Β· depth 15 Reason: Proof of the slab bound by counting the cells of a uniform grid that meet the slab against a Borel rectangle, then letting the mesh tend to zero.

After translating the centre to the origin and discarding a null boundary set, the slab is covered by the cells of a uniform grid of mesh mm on [βˆ’R,R)n[-R,R)^n; for each choice of the coordinates transverse to a distinguished direction the cells that meet the slab lie in a box whose thickness in that direction is 2ΟƒnΞ΄+O(1/m)2\sigma_n\delta+O(1/m), and mβ†’βˆžm\to\infty gives the bound.

Proof

Throughout, [m][m] denotes the initial segment determined by mm and [m]n[m]^{n} the set of nn-tuples in it, as in Uniform Grids on a Half-Open Box and Grid Hulls of a Compact Set in Rn\mathbb{R}^n. When n=1n=1 every sum or product over the indices lβ‰ il\ne i below is empty, and the factors mnβˆ’1m^{n-1}, hnβˆ’1h^{n-1} and (2R)nβˆ’1(2R)^{n-1} are to be read as 11; the argument is then valid verbatim.

Step 0: Ξ£\Sigma is Borel with finite measure. Put g(y)=βˆ₯yβˆ’zβˆ₯g(y)=\lVert y-z\rVert and β„“(y)=βˆ£Ξ½β‹…(yβˆ’z)∣\ell(y)=|\nu\cdot(y-z)|. Applying the triangle inequality of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n to yβˆ’z=(yβˆ’yβ€²)+(yβ€²βˆ’z)y-z=(y-y')+(y'-z) and to yβ€²βˆ’z=(yβ€²βˆ’y)+(yβˆ’z)y'-z=(y'-y)+(y-z), and using the absolute homogeneity recorded in the same lemma to get βˆ₯yβ€²βˆ’yβˆ₯=βˆ₯yβˆ’yβ€²βˆ₯\lVert y'-y\rVert=\lVert y-y'\rVert, gives g(y)βˆ’g(yβ€²)≀βˆ₯yβˆ’yβ€²βˆ₯g(y)-g(y')\le\lVert y-y'\rVert and g(yβ€²)βˆ’g(y)≀βˆ₯yβˆ’yβ€²βˆ₯g(y')-g(y)\le\lVert y-y'\rVert, hence ∣g(y)βˆ’g(yβ€²)βˆ£β‰€βˆ₯yβˆ’yβ€²βˆ₯|g(y)-g(y')|\le\lVert y-y'\rVert. Likewise, by Cauchy-Schwarz Inequality for the Euclidean Dot Product and the reverse triangle inequality for the absolute value (Properties of the Absolute Value in an Ordered Field), βˆ£β„“(y)βˆ’β„“(yβ€²)βˆ£β‰€βˆ£Ξ½β‹…(yβˆ’yβ€²)βˆ£β‰€βˆ₯Ξ½βˆ₯ βˆ₯yβˆ’yβ€²βˆ₯=βˆ₯yβˆ’yβ€²βˆ₯|\ell(y)-\ell(y')|\le|\nu\cdot(y-y')|\le\lVert\nu\rVert\,\lVert y-y'\rVert=\lVert y-y'\rVert.

The complement of Ξ£\Sigma is open. Indeed, let wβˆ‰Ξ£w\notin\Sigma. Then g(w)>Rg(w)>R or β„“(w)>Ξ΄\ell(w)>\delta; put Ξ·=g(w)βˆ’R\eta=g(w)-R in the first case and Ξ·=β„“(w)βˆ’Ξ΄\eta=\ell(w)-\delta in the second, so that 0<Ξ·0<\eta. Every wβ€²w' with βˆ₯wβ€²βˆ’wβˆ₯<Ξ·\lVert w'-w\rVert<\eta then satisfies g(wβ€²)>Rg(w')>R, respectively β„“(wβ€²)>Ξ΄\ell(w')>\delta, by the two Lipschitz estimates just proved, hence wβ€²βˆ‰Ξ£w'\notin\Sigma. So Ξ£\Sigma is closed, and therefore belongs to B(Rn)\mathcal{B}(\mathbb{R}^{n}) by The Borel Sigma-Algebra of a Euclidean Space as a Product, and Measurability of Projections, Sequentially Continuous Maps, and Open and Closed Sets. It is bounded, so Ξ»n(Ξ£)<∞\lambda_{n}(\Sigma)<\infty by Balls Have Positive Lebesgue Measure and Bounded Sets Have Finite Lebesgue Measure.

Step 1: reduction to z=0z=0. By the translation invariance of Ξ»n\lambda_{n} (Translation and Reflection Invariance of Lebesgue Measure on Rn\mathbb{R}^n), Ξ»n(Ξ£)=Ξ»n(Ξ£βˆ’z)\lambda_{n}(\Sigma)=\lambda_{n}(\Sigma-z), and Ξ£βˆ’z={w∈Rn:βˆ₯wβˆ₯≀R,Β βˆ£Ξ½β‹…wβˆ£β‰€Ξ΄}\Sigma-z=\{w\in\mathbb{R}^{n}:\lVert w\rVert\le R,\ |\nu\cdot w|\le\delta\}. We may therefore assume z=0z=0 and write Ξ£={w:βˆ₯wβˆ₯≀R,Β βˆ£Ξ½β‹…wβˆ£β‰€Ξ΄}\Sigma=\{w:\lVert w\rVert\le R,\ |\nu\cdot w|\le\delta\}.

Step 2: a distinguished coordinate. By Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, βˆ‘l=1nΞ½l2=βˆ₯Ξ½βˆ₯2=1\sum_{l=1}^{n}\nu_{l}^{2}=\lVert\nu\rVert^{2}=1. If Ξ½l2<1/n\nu_{l}^{2}<1/n held for every ll we would get 1=βˆ‘lΞ½l2<nβ‹…(1/n)=11=\sum_{l}\nu_{l}^{2}<n\cdot(1/n)=1, which is false; so there is i∈{1,…,n}i\in\{1,\dots,n\} with Ξ½i2β‰₯1/n\nu_{i}^{2}\ge 1/n, that is ∣νi∣β‰₯1/Οƒn|\nu_{i}|\ge 1/\sigma_{n}, since Οƒn2=n\sigma_{n}^{2}=n and Οƒn>0\sigma_{n}>0. Applying Cauchy-Schwarz Inequality for the Euclidean Dot Product to the vectors (∣ν1∣,…,∣νn∣)(|\nu_{1}|,\dots,|\nu_{n}|) and (1,…,1)(1,\dots,1), whose norms are βˆ₯Ξ½βˆ₯=1\lVert\nu\rVert=1 and Οƒn\sigma_{n}, gives

βˆ‘l=1n∣νlβˆ£β‰€Οƒn.\sum_{l=1}^{n}|\nu_{l}|\le\sigma_{n}.

Step 3: discarding a null set. Put B={x∈Rn:βˆ’R≀xl<RΒ forΒ everyΒ l}B=\{x\in\mathbb{R}^{n}:-R\le x_{l}<R\ \text{for every }l\}. If w∈Σw\in\Sigma then wl2β‰€βˆ‘lβ€²wlβ€²2=βˆ₯wβˆ₯2≀R2w_{l}^{2}\le\sum_{l'}w_{l'}^{2}=\lVert w\rVert^{2}\le R^{2}, so βˆ’R≀wl≀R-R\le w_{l}\le R for every ll; hence wβˆˆΞ£βˆ–Bw\in\Sigma\setminus B only if wl=Rw_{l}=R for some ll. Therefore Ξ£βˆ–BβŠ†β‹ƒl=1nZl\Sigma\setminus B\subseteq\bigcup_{l=1}^{n}Z_{l}, where Zl=A1Γ—β‹―Γ—AnZ_{l}=A_{1}\times\dots\times A_{n} with Al={R}A_{l}=\{R\} and Alβ€²=[βˆ’R,R]A_{l'}=[-R,R] for lβ€²β‰ ll'\ne l. Each ZlZ_{l} is a Borel rectangle, and by claim 1 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl\mathbb{R}^l together with claim 4 of Existence of Lebesgue Measure on the Real Line (which gives Ξ»([βˆ’R,R])=2R\lambda([-R,R])=2R and Ξ»({R})=0\lambda(\{R\})=0) its measure is (2R)nβˆ’1β‹…0=0(2R)^{n-1}\cdot 0=0. By the countable subadditivity and monotonicity of Ξ»n\lambda_{n} (claims 4 and 2 of Basic Properties of a Measure) we conclude Ξ»n(Ξ£βˆ–B)=0\lambda_{n}(\Sigma\setminus B)=0 and hence

Ξ»n(Ξ£)≀λn(Σ∩B).\lambda_{n}(\Sigma)\le\lambda_{n}(\Sigma\cap B).

Step 4: the grid estimate. Let m∈Nm\in\mathbb{N} and put h=2R/mh=2R/m. Apply the grid claim with c=(βˆ’R,…,βˆ’R)c=(-R,\dots,-R) and s=2Rs=2R: its half-open box is exactly BB, and the cells Qm,jQ_{m,j} with j∈[m]nj\in[m]^{n} are pairwise disjoint members of B(Rn)\mathcal{B}(\mathbb{R}^{n}) with union BB, each of measure hnh^{n}, the ll-th coordinate of a point of Qm,jQ_{m,j} lying in [βˆ’R+(jlβˆ’1)h,Β βˆ’R+jlh)[-R+(j_{l}-1)h,\ -R+j_{l}h).

Let J={j∈[m]n:Qm,jβˆ©Ξ£β‰ βˆ…}J=\{j\in[m]^{n}:Q_{m,j}\cap\Sigma\ne\varnothing\} and choose wj∈Qm,j∩Σw^{j}\in Q_{m,j}\cap\Sigma for each j∈Jj\in J. Since Σ∩B\Sigma\cap B is covered by the cells of the grid, Σ∩BβŠ†β‹ƒj∈JQm,j\Sigma\cap B\subseteq\bigcup_{j\in J}Q_{m,j}.

Fix a tuple ΞΉ=(ΞΉl)lβ‰ i\iota=(\iota_{l})_{l\ne i} of elements of [m][m] indexed by {1,…,n}βˆ–{i}\{1,\dots,n\}\setminus\{i\} and put JΞΉ={j∈J:jl=ΞΉlΒ forΒ everyΒ lβ‰ i}J_{\iota}=\{j\in J: j_{l}=\iota_{l}\text{ for every }l\ne i\}. Suppose JΞΉβ‰ βˆ…J_{\iota}\ne\varnothing. For lβ‰ il\ne i set Ξ²l=βˆ’R+(ΞΉlβˆ’12)h\beta_{l}=-R+(\iota_{l}-\tfrac12)h, the midpoint of the ll-th coordinate interval, so that ∣wljβˆ’Ξ²lβˆ£β‰€h/2|w^{j}_{l}-\beta_{l}|\le h/2 for every j∈JΞΉj\in J_{\iota}. Put

Ξ³=βˆ’1Ξ½iβˆ‘lβ‰ iΞ½lΞ²l,\gamma=-\frac{1}{\nu_{i}}\sum_{l\ne i}\nu_{l}\beta_{l},

which is well defined because Ξ½iβ‰ 0\nu_{i}\ne 0. For j∈JΞΉj\in J_{\iota} we have βˆ£Ξ½β‹…wjβˆ£β‰€Ξ΄|\nu\cdot w^{j}|\le\delta, hence

∣νiβˆ£β€‰βˆ£wijβˆ’Ξ³βˆ£=∣νiwij+βˆ‘lβ‰ iΞ½lΞ²lβˆ£β‰€βˆ£Ξ½β‹…wj∣+βˆ‘lβ‰ i∣νlβˆ£β€‰βˆ£Ξ²lβˆ’wljβˆ£β‰€Ξ΄+h2βˆ‘lβ‰ i∣νlβˆ£β‰€Ξ΄+Οƒnh2,|\nu_{i}|\,|w^{j}_{i}-\gamma|=\Bigl|\nu_{i}w^{j}_{i}+\sum_{l\ne i}\nu_{l}\beta_{l}\Bigr|\le|\nu\cdot w^{j}|+\sum_{l\ne i}|\nu_{l}|\,|\beta_{l}-w^{j}_{l}|\le\delta+\frac{h}{2}\sum_{l\ne i}|\nu_{l}|\le\delta+\frac{\sigma_{n}h}{2},

using Step 2. Since ∣νi∣β‰₯1/Οƒn|\nu_{i}|\ge1/\sigma_{n} this gives ∣wijβˆ’Ξ³βˆ£β‰€ΟƒnΞ΄+Οƒn2h/2|w^{j}_{i}-\gamma|\le\sigma_{n}\delta+\sigma_{n}^{2}h/2. Every x∈Qm,jx\in Q_{m,j} has ∣xiβˆ’wijβˆ£β‰€h|x_{i}-w^{j}_{i}|\le h, because both coordinates lie in an interval of length hh; therefore

∣xiβˆ’Ξ³βˆ£β‰€ΟƒnΞ΄+12Οƒn2h+hforΒ everyΒ j∈JΞΉΒ andΒ x∈Qm,j.|x_{i}-\gamma|\le\sigma_{n}\delta+\tfrac12\sigma_{n}^{2}h+h\qquad\text{for every }j\in J_{\iota}\text{ and }x\in Q_{m,j}.

Writing Ο„=ΟƒnΞ΄+12Οƒn2h+h\tau=\sigma_{n}\delta+\tfrac12\sigma_{n}^{2}h+h, we conclude that ⋃j∈JΞΉQm,j\bigcup_{j\in J_{\iota}}Q_{m,j} is contained in the Borel rectangle A1Γ—β‹―Γ—AnA_{1}\times\dots\times A_{n} with Ai=[Ξ³βˆ’Ο„,Ξ³+Ο„]A_{i}=[\gamma-\tau,\gamma+\tau] and Al=[βˆ’R+(ΞΉlβˆ’1)h,Β βˆ’R+ΞΉlh]A_{l}=[-R+(\iota_{l}-1)h,\ -R+\iota_{l}h] for lβ‰ il\ne i. By claim 1 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl\mathbb{R}^l and claim 4 of Existence of Lebesgue Measure on the Real Line that rectangle has measure hnβˆ’1β‹…2Ο„h^{n-1}\cdot 2\tau, so by monotonicity

Ξ»n(⋃j∈JΞΉQm,j)≀2τ hnβˆ’1,\lambda_{n}\Bigl(\bigcup_{j\in J_{\iota}}Q_{m,j}\Bigr)\le 2\tau\,h^{n-1},

an inequality that also holds trivially when JΞΉ=βˆ…J_{\iota}=\varnothing.

As ΞΉ\iota ranges over the mnβˆ’1m^{n-1} tuples in [m][m] indexed by {1,…,n}βˆ–{i}\{1,\dots,n\}\setminus\{i\}, the sets JΞΉJ_{\iota} are pairwise disjoint with union JJ. Hence, by monotonicity and finite subadditivity of Ξ»n\lambda_{n} (claims 2 and 4 of Basic Properties of a Measure),

Ξ»n(Σ∩B)β‰€βˆ‘ΞΉΞ»n(⋃j∈JΞΉQm,j)≀mnβˆ’1hnβˆ’1 2Ο„=(2R)nβˆ’1(2ΟƒnΞ΄+(Οƒn2+2)h),\lambda_{n}(\Sigma\cap B)\le\sum_{\iota}\lambda_{n}\Bigl(\bigcup_{j\in J_{\iota}}Q_{m,j}\Bigr)\le m^{n-1}h^{n-1}\,2\tau=(2R)^{n-1}\bigl(2\sigma_{n}\delta+(\sigma_{n}^{2}+2)h\bigr),

since mh=2Rmh=2R.

Step 5: conclusion. Combining Steps 3 and 4, for every m∈Nm\in\mathbb{N},

Ξ»n(Ξ£)≀2ΟƒnΞ΄(2R)nβˆ’1+(2R)n(Οƒn2+2)1m.\lambda_{n}(\Sigma)\le 2\sigma_{n}\delta(2R)^{n-1}+(2R)^{n}(\sigma_{n}^{2}+2)\frac{1}{m}.

If we had Ξ»n(Ξ£)>2ΟƒnΞ΄(2R)nβˆ’1\lambda_{n}(\Sigma)>2\sigma_{n}\delta(2R)^{n-1}, then by The Archimedean Property of the Real Numbers there would be m∈Nm\in\mathbb{N} with

(2R)n(Οƒn2+2)1m<Ξ»n(Ξ£)βˆ’2ΟƒnΞ΄(2R)nβˆ’1,(2R)^{n}(\sigma_{n}^{2}+2)\frac{1}{m}<\lambda_{n}(\Sigma)-2\sigma_{n}\delta(2R)^{n-1},

contradicting the displayed inequality. Hence Ξ»n(Ξ£)≀2ΟƒnΞ΄(2R)nβˆ’1\lambda_{n}(\Sigma)\le 2\sigma_{n}\delta(2R)^{n-1}.

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