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Measure Theory 20 | Outer measures - Part 1 [dark version] thumbnail

Measure Theory 20 | Outer measures - Part 1 [dark version]

4 min read

Based on The Bright Side of Mathematics's video on YouTube. If you like this content, support the original creators by watching, liking and subscribing to their content.

TL;DR

An outer measure Φ is defined on all subsets of a set X (the power set) and takes values in nonnegative extended reals.

Briefing

Outer measures provide a flexible way to assign “volumes” to *all* subsets of a space without requiring a sigma-algebra up front. Instead of starting with measurable sets, an outer measure is defined on the full power set of a fixed set X and satisfies three core properties: it assigns 0 to the empty set, it is monotone (if A ⊆ B then Φ(A) ≤ Φ(B)), and it is countably sub-additive (Φ(⋃_{n} A_n) ≤ Σ_{n} Φ(A_n)). This combination captures the intuition that unions can’t have more “size” than the sum of the sizes of their parts, even when overlaps occur.

The motivation matters because many standard measure-theoretic constructions fail on arbitrary subsets. In particular, countable additivity—where Φ(⋃ A_n) equals Σ Φ(A_n)—does not hold for general outer measures. The transcript highlights this by contrasting sub-additivity with the stronger “sigma additivity” property expected from a genuine measure. Since equality can break down on the whole power set, the path forward is to identify which subsets behave well enough for additivity to work.

That leads to the key next step: restricting attention to “good” sets, called Φ-measurable sets. A set A is Φ-measurable if it splits every other set Q into two parts—Q ∩ A and Q  A—such that Φ(Q) equals Φ(Q ∩ A) + Φ(Q  A). Geometrically, A acts like a boundary that doesn’t distort the outer-measure accounting when sets are decomposed. The transcript also notes a common variation in definitions across textbooks: some use an inequality direction (≥) instead of equality, but for outer measures the conditions end up equivalent.

The payoff comes in the form of a proposition: the collection of all Φ-measurable sets forms a sigma algebra. Once that structure is in place, the outer measure can be converted into an ordinary measure. Specifically, defining μ(A) = Φ(A) for measurable sets A produces a true measure on that sigma algebra. This is the foundation needed to prove major theorems later—especially those that rely on extending pre-measures—because it shows how outer-measure constructions can be turned into bona fide measures once the right sets are identified.

In short, outer measures start as a coarse tool defined everywhere, then Φ-measurability selects the subsets where additivity becomes exact. The resulting sigma algebra supports a genuine measure, setting up the technical machinery for the next stage of measure theory.

Cornell Notes

Outer measures assign nonnegative extended real values to every subset of a fixed set X, using three rules: Φ(∅)=0, monotonicity (A ⊆ B ⇒ Φ(A) ≤ Φ(B)), and countable sub-additivity (Φ(⋃ A_n) ≤ Σ Φ(A_n)). Because sub-additivity is weaker than countable additivity, an outer measure typically cannot serve as a measure on the whole power set. The remedy is to focus on Φ-measurable sets: A is Φ-measurable if every set Q splits into Q∩A and Q\A with Φ(Q)=Φ(Q∩A)+Φ(Q\A). The key result is that all Φ-measurable sets form a sigma algebra, and restricting Φ to that sigma algebra yields an ordinary measure μ(A)=Φ(A).

Why isn’t countable sub-additivity enough to make an outer measure a measure on all subsets?

A measure needs countable additivity: Φ(⋃_{n} A_n) should equal Σ_{n} Φ(A_n). Outer measures only guarantee the inequality Φ(⋃_{n} A_n) ≤ Σ_{n} Φ(A_n), because overlaps among the A_n can cause “double counting” on the right-hand side. The transcript emphasizes that equality (sigma additivity) generally fails on the full power set, so additional structure is required.

What does monotonicity mean for an outer measure, and why is it natural?

Monotonicity says that if A ⊆ B, then Φ(A) ≤ Φ(B). The intuition is straightforward: a subset cannot have larger “volume” than the set that contains it. This property mirrors what happens for ordinary measures and is one of the three defining axioms of an outer measure.

How does Φ-measurability turn an outer measure into something additive?

A set A is Φ-measurable if for every set Q, the outer measure of Q splits exactly across the partition induced by A: Φ(Q)=Φ(Q∩A)+Φ(Q\A). This condition ensures that decomposing Q into the part inside A and the part outside A does not introduce the inequality gap that sub-additivity allows.

Why does the collection of Φ-measurable sets matter structurally?

The transcript states that all Φ-measurable sets form a sigma algebra. That matters because sigma algebras are the domains where measures are defined and where countable operations behave consistently. Once the measurable sets form a sigma algebra, defining μ(A)=Φ(A) on that collection produces a genuine measure.

What is the practical conversion from an outer measure Φ to an ordinary measure μ?

After identifying the Φ-measurable sets, define μ on that sigma algebra by μ(A)=Φ(A). The proposition guarantees that this restriction satisfies the measure axioms, turning the initial “everywhere-defined” outer measure into a proper measure on a well-behaved family of sets.

Review Questions

  1. State the three defining properties of an outer measure Φ and explain how sub-additivity differs from additivity.
  2. Give the definition of a Φ-measurable set A in terms of how it partitions an arbitrary set Q.
  3. What proposition links Φ-measurable sets to sigma algebras, and how does it produce an ordinary measure μ?

Key Points

  1. 1

    An outer measure Φ is defined on all subsets of a set X (the power set) and takes values in nonnegative extended reals.

  2. 2

    Outer measures satisfy Φ(∅)=0, monotonicity (A ⊆ B ⇒ Φ(A) ≤ Φ(B)), and countable sub-additivity (Φ(⋃ A_n) ≤ Σ Φ(A_n)).

  3. 3

    Outer measures generally fail to be measures on the whole power set because countable additivity (equality) need not hold.

  4. 4

    A set A is Φ-measurable if every set Q splits as Φ(Q)=Φ(Q∩A)+Φ(Q\A).

  5. 5

    All Φ-measurable sets form a sigma algebra.

  6. 6

    Restricting Φ to the sigma algebra of Φ-measurable sets via μ(A)=Φ(A) yields an ordinary measure μ.

Highlights

Outer measures start with three axioms—zero on the empty set, monotonicity, and countable sub-additivity—without requiring any sigma algebra.
Countable sub-additivity is weaker than countable additivity, so equality can fail on arbitrary subsets.
Φ-measurability is the exact condition that restores additivity when sets are split by A.
Once Φ-measurable sets form a sigma algebra, defining μ(A)=Φ(A) turns the outer measure into a true measure.

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