Homepage Solution manuals Terence Tao An Introduction to Measure Theory Exercise 1.2.16 (Equivalent formulations of finite Lebesgue measurability)

Exercise 1.2.16 (Equivalent formulations of finite Lebesgue measurability)

Let E d. Then the following are equivalent:

(i)
E is Lebesgue measurable with finite measure
(ii)
(Outer approximation by open) For every 𝜖 > 0, one can contain E in an open set U of finite measure with m(UE) 𝜖.
(iii)
(Almost open bounded) E differs from a bounded open set by a set of arbitrarily small Lebesgue outer measure. (In other words, for every 𝜖 > 0, there exists a bounded open set U such that m(EU) 𝜖.)
(iv)
(Inner approximation by compact) For every 𝜖 > 0, one can find a compact set F contained in E with m(EF) 𝜖.
(v)
(Almost compact) E differs from a compact set by a set of arbitrarily small Lebesgue outer measure.
(vi)
(Almost bounded measurable) E differs from a bounded Lebesgue measurable set by a set of arbitrarily small Lebesgue outer measure.
(vii)
(Almost finite measure) E differs from a Lebesgue measurable set with finite measure by a set of arbitrarily small Lebesgue outer measure.
(viii)
(Almost elementary) E differs from an elementary set by a set of arbitrarily small Lebesgue outer measure.
(ix)
(Almost dyadically elementary) For every 𝜖 > 0, there exists an integer n and a finite union F of closed dyadic cubes of sidelength 2n such that m(EF) 𝜖.

Answers

We use the chain of implications to demonstrate (i)(ii)(iii) first.

  • (i)(ii)
    By Lebesgue measurability we can find an open set U such that m(UE) 𝜖. By countable additivity m(U) m(E) + 𝜖. Since m(E) and 𝜖 are both finite, m(U) must be finite too. In other words, our usual choice of the open set U from the definition is already sufficient.
  • (ii)(iii)
    Pick an arbitrary 𝜖 > 0. By (ii) we can find an open set U O(d) : E U such that m(UE) = m(UE) 𝜖3. We do not, however, know whether U is bounded or not. This is easily fixable by cutting out its "small" (in measure theoretic sense) unbounded part as follows. For all r let Ur := U (r,r)d where each Ur is open and bounded. Let us look closely at EUr

    • item We obviously have U1E U2E and r=1UrE = UE. Thus, by Exercise 1.2.11 we have

      lim rm(U rE) = m(UE)

      Pick an r1 large enough such that 𝜖3 m(UE) m(UrE); in other words, m(UrE) m(UE) + 𝜖3.

    • Similarly notice that EU1 EU2 and r=1EUr = EU = . Again, by Exercise 1.2.11 we have

      lim rm(EU r) = m(EU) = 0

      In other words, we can pick r2 large enough so that m(EUr) 𝜖3.

    Set r := max {r1,r2}; then

    m(EU r) = m(EU r) + m(U rE) 𝜖 3 + m(UE) + 𝜖 3 𝜖

    as desired.

  • (iii)(i)
    Pick an arbitrary 𝜖 > 0 and choose U O(d) such that m(UE) = m(UE) + m(EU) 𝜖3. Notice that U is already almost sufficient for us - the only problem is a possible part of E not covered by U, i.e., EU. Since it is not very big (m(EU) 𝜖) we can choose a small open set U1 to cover EU, and then simply take U := U U1. This is possible by outer regularity of the Lebesgue outer measure (Lemma 1.2.12): we can always find an open outer cover U1 of EU such that m(U1) m(EU) 𝜖3. Then we obviously have E U U1, the latter being open. Thus,

    m(UE) = m((U U 1)E) m(UE) + m(U 1E) 𝜖 3 + m(U 1E) 𝜖 3 + m(U1) 𝜖 3 + m(EU) + 𝜖 3 𝜖

    and we also have m(U) m(U) + m(U1) < .

Next we verify (i)(iv)(v)

  • (i)(iv)
    Since E is Lebesgue measurable, we can find a closed set F E such that m(EF) = m(E) m(F) 𝜖2. If E is bounded, then F is bounded also, and we are done. If E is not bounded, notice that we can make F bounded by approximating it using the sequence Fr := F B(0,r) for any r . By Exercise 1.2.11 by F1 F2 and r=1Fr = F we have lim rm(Fr) = m(F). Thus, pick r large enough so that m(F) m(Fr) 𝜖2, i.e., m(Fr) m(F) + 𝜖2. We then obtain

    m(EFr) = m(E) m(Fr) m(E) m(F) + 𝜖2 𝜖

  • (iv)(v)
    Follows directly by taking the same E for (v) as the E for (iv).
  • (v)(vi)
    Follows trivially from (v) since any compact set is automatically a bounded Lebesgue measurable set.
  • (vi)(vii)
    Follows trivially, since any bounded Lebesgue measurable set can be contained in a ball B(0,r) for some r large enough; by m(F) m(B(0,r) < it must have a finite Lebesgue measure.
  • (vii)(i)
    Pick an arbitrary 𝜖 > 0, and take a measurable set E𝜖 such that m(EE𝜖) 𝜖3 as in (vii). On one hand, notice that we can replace the measurable set E𝜖 by an open set U1 E𝜖 such that m(U1) m(E𝜖) 𝜖3. On the other hand, by Lemma 1.2.12 we can replace EE𝜖 by an open set U2 such that m(U2) m(EE𝜖) 𝜖3. Then we have an open set U := U1 U2 such that E U and

    m(UE) m(U 1E) + m(U 2E) = m(U 1E) + 𝜖 3 m((U 1E𝜖 E𝜖)E) + 𝜖 3 m(U 1E𝜖E) + m(E 𝜖E) + 𝜖 3 m(U 1E𝜖) + m(E 𝜖E) + 𝜖 3 𝜖

    Where it is easy to verify that m(U) < .

Now we demonstrate the equivalence of the "pixelation" criteria (i)(viii)(ix).

  • (i)(viii)
    By the definition of Lebesgue measure we have

    m(E) = { n=1|B n| : Bn are boxes E n=1Bn } <

    Pick an arbitrary (Bn)n such that n=1|Bn| m(E) 𝜖2. For each N define FN := n=1NBn. Notice that

    • em The set EF1 EF2 , and we have N=1EFn = ; thus lim Nm(EFN) = 0 by Exercise 1.2.11. Pick an N1 large enough such that m(EFN1) 𝜖2.
    • The set F1E F2E , and we have N=1FNE = n=1BnE; thus, lim Nm(FNE) = m( n=1BnE) = m( n=1Bn) m(E) 𝜖3. Pick an N2 large enough such that m(FN2E) 𝜖2.

    Now set N = max {N1,N2}, and we have

    m(EFN) m(EFN) + m(FNE) 𝜖2 + 𝜖2 = 𝜖

    as desired.

  • (viii)(ix)
    We use the following lemma:

    Lemma 1. Let A,B,C d be sets such that A approximates B in measure m(AB) 𝜖, and B approximates C in measure m(BC) 𝜖. Then A approximates C in measure m(AC) 𝜖.

    Proof. Since we can represent both sets disjointly as A = (A B) (AB) and B = (B C) (BC) by monotonicity of the Lebesgue outer measure it follows that

    m(AC) m(AC) + m(CA) m((A B)C) + m((AB)C) + m((B C)A) + m((BC)A) m((A B)C) + m(AB) + m((B C)A) + m(BC) m((A B)C) + 𝜖 + m((B C)A) + 𝜖 = m(AC BC) + 𝜖 + m(BA CA) + 𝜖 m(BC) + 𝜖 + m(BA) + 𝜖 4𝜖.

    Now we have by theorem assumption an elementary set F that approximates E, i.e., m(FE) 𝜖. But F is an elementary (Jordan measurable) set. Thus, by Exercise 1.1.14 we can find a n large enough so that the measure of all dyadic cubes Q := i=1E(F,2n) Qn of sidelength 2n contained in F satisfies m(F) m(Q) = m(FQ) = m(FQ) 𝜖. By the previous lemma, from m(EF) 𝜖 and m(FQ) 𝜖) we deduce m(EQ) 𝜖.

  • (ix)(i)
    Since the union of dyadic cubes Q is a finitely measurable set, and since E differs from Q by an arbitrarily small Lebesgue outer measure, by part (vii) E must be measurable too, with finite measure.
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2020-05-30 00:00
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