Reading guide · Proof index

Jordan measurable sets

Jiří Lebl, Basic Analysis I–II, version 6.3. Free author edition of this section. Selection and attribution · Notation.

L10.5.1: Jordan measurability iff null boundary, using an interior containing rectangle.

Proof.

Suppose RR is a closed rectangle such that SS is contained in the interior of R.R\text{.} If x∈∂S,x \in \partial S\text{,} then for every δ>0,\delta > 0\text{,} the sets S∩B(x,δ)S \cap B(x,\delta) (where χS\chi_S is 1) and the sets (R∖S)∩B(x,δ)(R \setminus S) \cap B(x,\delta) (where χS\chi_S is 0) are both nonempty. So χS\chi_S is not continuous at x.x\text{.} If xx is either in the interior of SS or in the complement of the closure S‾,\widebar{S}\text{,} then χS\chi_S is either identically 1 or identically 0 in a whole neighborhood of xx and hence χS\chi_S is continuous at x.x\text{.} Therefore, the set of discontinuities of χS\chi_S is precisely the boundary ∂S.\partial S\text{.} The proposition follows.

L10.5.3: Full equality of Jordan volume and outer measure, with the finite-disjoint-rectangle and empty-family steps supplied.

Proof.

Given ϵ>0,\epsilon > 0\text{,} let RR be a closed rectangle that contains S.S\text{.} Let PP be a partition of RR such that
U(P,χS)≤(∫RχS)+ϵ=V(S)+ϵandL(P,χS)≥(∫RχS)−ϵ=V(S)−ϵ.\begin{equation*} U(P,\chi_S) \leq \left( \int_R \chi_S \right) + \epsilon = V(S) + \epsilon \qquad \text{and} \qquad L(P,\chi_S) \geq \left( \int_R \chi_S \right) - \epsilon = V(S)-\epsilon. \end{equation*}
Let R1,R2,…,RkR_1,R_2,\ldots,R_k be all the subrectangles of PP such that χS\chi_S is not identically zero on each Rj.R_j\text{.} That is, there is some point x∈Rjx \in R_j such that x∈Sx \in S (i.e. χS(x)=1\chi_S(x)=1). Let OjO_j be an open rectangle such that Rj⊂OjR_j \subset O_j and V(Oj)<V(Rj)+ϵ ⁣/ ⁣k.V(O_j) < V(R_j) + \nicefrac{\epsilon}{k}\text{.} Notice that S⊂⋃jOj.S \subset \bigcup_j O_j\text{.} Then
U(P,χS)=∑j=1kV(Rj)>(∑j=1kV(Oj))−ϵ≥m∗(S)−ϵ.\begin{equation*} U(P,\chi_S) = \sum_{j=1}^k V(R_j) > \left(\sum_{j=1}^k V(O_j)\right) - \epsilon \geq m^*(S) - \epsilon . \end{equation*}
As U(P,χS)≤V(S)+ϵ,U(P,\chi_S) \leq V(S) + \epsilon\text{,} then m∗(S)−ϵ≤V(S)+ϵ,m^*(S) - \epsilon \leq V(S) + \epsilon\text{,} or in other words m∗(S)≤V(S).m^*(S) \leq V(S)\text{.}
Let R1′,R2′,…,Rℓ′R'_1,R'_2,\ldots,R'_\ell be all the subrectangles of PP such that χS\chi_S is identically one on each Rj′.R'_j\text{.} In other words, these are the subrectangles contained in S.S\text{.} The interiors of the subrectangles Rj′∘R'^\circ_j are disjoint and V(Rj′∘)=V(Rj′).V(R'^\circ_j) = V(R'_j)\text{.} Via Exercise 10.3.16,
m∗(⋃j=1ℓRj′∘)=∑j=1ℓV(Rj′∘).\begin{equation*} m^*\Bigl(\bigcup_{j=1}^\ell R'^\circ_j\Bigr) = \sum_{j=1}^\ell V(R'^\circ_j) . \end{equation*}
Hence
m∗(S)≥m∗(⋃j=1ℓRj′)≥m∗(⋃j=1ℓRj′∘)=∑j=1ℓV(Rj′∘)=∑j=1ℓV(Rj′)=L(P,χS)≥V(S)−ϵ.\begin{equation*} m^*(S) \geq m^*\Bigl(\bigcup_{j=1}^\ell R'_j\Bigr) \geq m^*\Bigl(\bigcup_{j=1}^\ell R'^\circ_j\Bigr) = \sum_{j=1}^\ell V(R'^\circ_j) = \sum_{j=1}^\ell V(R'_j) = L(P,\chi_S) \geq V(S) - \epsilon . \end{equation*}
Therefore m∗(S)≥V(S)m^*(S) \geq V(S) as well.

L10.5.5: Every bounded continuous function on a bounded Jordan set is Riemann integrable; full proof.

Proof.

Define the function f~\widetilde{f} as above for some closed rectangle RR with S⊂R.S \subset R\text{.} If x∈R∖S‾,x \in R \setminus \widebar{S}\text{,} then f~\widetilde{f} is identically zero in a neighborhood of x.x\text{.} Similarly, if xx is in the interior of S,S\text{,} then f~=f\widetilde{f} = f on a neighborhood of xx and ff is continuous at x.x\text{.} Therefore, f~\widetilde{f} is only ever possibly discontinuous at ∂S,\partial S\text{,} which is a set of measure zero, and we are finished.

L10.5.9: Full compact Jordan image theorem, with the local inverse theorem already closed; source f|V is the map g|V.

Proof.

Let T≔g(S).T \coloneqq g(S)\text{.} By Lemma 7.5.5, the set TT is also compact and so closed and bounded. We claim ∂T⊂g(∂S).\partial T \subset g(\partial S)\text{.} Suppose the claim is proved. As SS is Jordan measurable, ∂S\partial S is measure zero. Then g(∂S)g(\partial S) is measure zero by Proposition 10.3.10. As ∂T⊂g(∂S),\partial T \subset g(\partial S)\text{,} then TT is Jordan measurable.
It is therefore left to prove the claim. As TT is closed, ∂T⊂T.\partial T \subset T\text{.} Suppose y∈∂T.y \in \partial T\text{.} There must exist an x∈Sx \in S such that g(x)=y,g(x) = y\text{,} and by hypothesis Jg(x)≠0.J_g(x) \neq 0\text{.} We use the inverse function theorem (Theorem 8.5.1). We find a neighborhood V⊂UV \subset U of xx and an open set WW such that the restriction f∣Vf|_V is a one-to-one and onto function from VV to WW with a continuously differentiable inverse. In particular, g(x)=y∈W.g(x) = y \in W\text{.} As y∈∂T,y \in \partial T\text{,} there exists a sequence {yk}k=1∞\{ y_k \}_{k=1}^\infty in WW with lim⁡k→∞yk=y\lim_{k\to\infty} y_k = y and yk∉T.y_k \notin T\text{.} As g∣Vg|_V is invertible and in particular has a continuous inverse, there exists a sequence {xk}k=1∞\{ x_k \}_{k=1}^\infty in VV such that g(xk)=ykg(x_k) = y_k and lim⁡k→∞xk=x.\lim_{k\to\infty} x_k = x\text{.} Since yk∉T=g(S),y_k \notin T = g(S)\text{,} clearly xk∉S.x_k \notin S\text{.} Since x∈S,x \in S\text{,} we conclude that x∈∂S.x \in \partial S\text{.} The claim is proved: ∂T⊂g(∂S).\partial T \subset g(\partial S)\text{.}