Lebesgue Measure

Basis
Last updated: Tags: Measure Theory

You now have all the pieces: outer measure builds a size function λ\lambda^* on every subset of R\mathbb{R}, and Carathéodory’s criterion isolates the sets on which λ\lambda^* becomes a genuine, countably additive measure. Putting them together yields the Lebesgue measure — the canonical notion of length on R\mathbb{R}.

The Lebesgue σ-algebra and Lebesgue measure

Definition. The Lebesgue σ-algebra L\mathcal{L} is the collection of all sets ERE \subseteq \mathbb{R} that are Carathéodory-measurable with respect to the Lebesgue outer measure λ\lambda^*:

L    {ER:λ(A)=λ(AE)+λ(AEc) for all AR}.(1)\mathcal{L} \;\coloneqq\; \{E \subseteq \mathbb{R} : \lambda^*(A) = \lambda^*(A \cap E) + \lambda^*(A \cap E^c) \text{ for all } A \subseteq \mathbb{R}\}. \tag{1}

The Lebesgue measure is the restriction

λ    λL ⁣:L[0,+].(2)\lambda \;\coloneqq\; \lambda^*\restriction_{\mathcal{L}} \colon \mathcal{L} \to [0, +\infty]. \tag{2}

By Carathéodory’s theorem, L\mathcal{L} is a σ-algebra, and λ\lambda is a complete, countably additive measure on L\mathcal{L}.

Every open set is Lebesgue measurable

The first task is to verify that the Lebesgue measure captures ordinary geometry — that is, that every open interval, and hence every open set, is in L\mathcal{L}.

Claim. Every open interval (a,b)(a, b) is in L\mathcal{L}.

Proof. You need to show that for any test set AA,

λ(A)λ(A(a,b))+λ(A(a,b)c).\lambda^*(A) \geq \lambda^*(A \cap (a,b)) + \lambda^*(A \cap (a,b)^c).

Fix a countable cover of AA by open intervals {Ik}\{I_k\} with kIkλ(A)+ε\sum_k |I_k| \leq \lambda^*(A) + \varepsilon. For each kk, split IkI_k into Ik(a,b)I_k \cap (a, b) and Ik(a,b)I_k \setminus (a, b) (the latter being at most two intervals). These splits give covers of A(a,b)A \cap (a, b) and A(a,b)cA \cap (a, b)^c respectively, with total lengths summing to Ik|I_k|. Adding over kk:

λ(A(a,b))+λ(A(a,b)c)kIkλ(A)+ε.\lambda^*(A \cap (a,b)) + \lambda^*(A \cap (a,b)^c) \leq \sum_k |I_k| \leq \lambda^*(A) + \varepsilon.

Since ε\varepsilon is arbitrary, the claim follows.

Because every open set in R\mathbb{R} is a countable union of disjoint open intervals (a fact from real analysis), and L\mathcal{L} is closed under countable unions, every open set is in L\mathcal{L}. By taking complements, every closed set is also in L\mathcal{L}.

The Borel sets are Lebesgue measurable

Since L\mathcal{L} contains all open sets and is a σ-algebra, it must contain the smallest σ-algebra generated by the open sets — the Borel σ-algebra B(R)\mathcal{B}(\mathbb{R}) from σ-Algebra:

B(R)    L.(3)\mathcal{B}(\mathbb{R}) \;\subseteq\; \mathcal{L}. \tag{3}

The inclusion is strict: L\mathcal{L} contains some non-Borel sets (the subsets of Borel null sets, which land in L\mathcal{L} by completeness but may not be Borel). In particular, every Borel set is Lebesgue measurable, but the Lebesgue σ-algebra is strictly larger than B(R)\mathcal{B}(\mathbb{R}).

Basic computations

Intervals

For any bounded interval II with endpoints aba \leq b,

λ(I)=ba,(4)\lambda(I) = b - a, \tag{4}

regardless of whether the endpoints are included. This is equation (5) from Outer Measure, applied to an element of L\mathcal{L}.

For λ({a})=0\lambda(\{a\}) = 0: a singleton can be covered by (aε,a+ε)(a - \varepsilon, a + \varepsilon) for any ε>0\varepsilon > 0, giving λ({a})2ε\lambda^*(\{a\}) \leq 2\varepsilon; hence λ({a})=0\lambda(\{a\}) = 0. The formulas for open and closed intervals then follow from countable additivity.

Countable sets are null

A set NN is called a null set (or measure-zero set) when λ(N)=0\lambda(N) = 0. Any countable set is a null set:

λ ⁣({x1,x2,x3,})=k=1λ({xk})=k=10=0.(5)\lambda\!\left(\{x_1, x_2, x_3, \ldots\}\right) = \sum_{k=1}^{\infty} \lambda(\{x_k\}) = \sum_{k=1}^{\infty} 0 = 0. \tag{5}

This confirms the intuition from Introduction to Measure: λ(Q[0,1])=0\lambda(\mathbb{Q} \cap [0,1]) = 0, even though the rationals are dense in [0,1][0,1].

Open and closed sets in [0,1][0,1]

The measure of an open set UU decomposes cleanly. Every open U[0,1]U \subseteq [0,1] can be written as a countable disjoint union of open intervals U=k(ak,bk)U = \bigsqcup_k (a_k, b_k), so

λ(U)=k(bkak).(6)\lambda(U) = \sum_{k} (b_k - a_k). \tag{6}

Its closed complement F=[0,1]UF = [0,1] \setminus U satisfies λ(F)=1λ(U)\lambda(F) = 1 - \lambda(U), by the countable additivity of λ\lambda on the disjoint decomposition [0,1]=FU[0,1] = F \sqcup U.

The Cantor set is a striking example. Start from [0,1][0,1]; at each stage remove the open middle third of every remaining interval. After countably many steps, what remains is a closed set CC with λ(C)=0\lambda(C) = 0 (because the removed intervals account for total length 1/3+2/9+4/27+=11/3 + 2/9 + 4/27 + \cdots = 1). Yet CC is uncountable — it has the cardinality of R\mathbb{R}.

Translation invariance

Theorem. For any ELE \in \mathcal{L} and tRt \in \mathbb{R}, the translate E+t{x+t:xE}E + t \coloneqq \{x + t : x \in E\} satisfies E+tLE + t \in \mathcal{L} and

λ(E+t)=λ(E).(7)\lambda(E + t) = \lambda(E). \tag{7}

Why. Translating a cover by intervals of EE by tt gives a cover of E+tE + t with the same total length. So λ(E+t)=λ(E)\lambda^*(E + t) = \lambda^*(E). The Carathéodory measurability of E+tE + t follows similarly.

Translation invariance (7)(7) is a defining geometric property of length: the size of a set does not depend on where it sits on the line. Together with countable additivity and the normalization λ([0,1])=1\lambda([0,1]) = 1, this uniquely characterises Lebesgue measure among all measures on B(R)\mathcal{B}(\mathbb{R}) that are finite on bounded sets.

Summary

  • The Lebesgue σ-algebra L\mathcal{L} (equation (1)(1)) is the collection of Carathéodory-measurable sets for λ\lambda^*; the Lebesgue measure λ\lambda (equation (2)(2)) is λ\lambda^* restricted to L\mathcal{L}.
  • λ\lambda is a complete, countably additive measure, by Carathéodory’s theorem.
  • Every open set, and therefore every Borel set, belongs to L\mathcal{L} — inclusion (3)(3). The Lebesgue σ-algebra is strictly larger than B(R)\mathcal{B}(\mathbb{R}).
  • On intervals, λ\lambda agrees with length: λ(I)=ba\lambda(I) = b - a — equation (4)(4).
  • Countable sets are null sets — equation (5)(5); in particular λ(Q[0,1])=0\lambda(\mathbb{Q} \cap [0,1]) = 0.
  • The Cantor set is a closed, uncountable null set: a striking example of the subtlety of measure zero.
  • Translation invariance λ(E+t)=λ(E)\lambda(E + t) = \lambda(E) — equation (7)(7) — reflects that length is a geometric (not positional) property of a set.