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Every finite Borel measure on R has a unique absolutely continuous, discrete, and singular-continuous decomposition

Statement

Assume the Axiom of Choice. Let μ be a finite Borel measure on R. Then there exist unique finite Borel measures μac,μd,μsc such that μ=μac+μd+μsc, where μac≪λ, μd is discrete, and μsc is atomless and singular with respect to Lebesgue measure λ.

Facts & Assumptions

Given: AC and a finite Borel measure μ on R.

[L1]

Under countable choice a finite Borel measure splits as μd(E)=μ(E∩A) and η(E)=μ(E∖A), where A={x:μ({x})>0} is countable and η is atomless. (Every finite Borel measure on R splits as an atomic part plus an atomless part, An atom of a measure on R)

[L3]

Under AC, common-finite-exhaustion Lebesgue decomposition exists, with positive components dominated by the original measure in the positive case. Given two decompositions, their components are unique without any choice hypothesis. (Every sigma-finite signed measure admits a Lebesgue decomposition relative to a sigma-finite positive measure, The Lebesgue decomposition of a sigma-finite signed measure is unique)

[L4]

AC supplies [L3] and implies the countable choice required by [L1] and [L2]. (The Axiom of Choice)

Proof

technique · direct
1.1L1L4given

Apply [L1] to write μ=μd+η. The measure μd is discrete, meaning concentrated on a countable set, and η is atomless. These measures are finite positive Borel measures.

2.1L2L3L4step 1.1construct

On Xn=[−n,n] both λ and η are finite by [L2] and finiteness of η. Under AC, [L3] decomposes η=μac+μsc with positive finite components, μac≪λ and μsc⊥λ. Since η({x})=0, positivity gives μac({x})=μsc({x})=0 for every x. Thus μsc is atomless, proving existence of the claimed three parts.

3.1L2L3step 1.1step 2.1algebra∎

For uniqueness, consider any such three-part decomposition. The absolutely continuous part has zero mass on singletons by [L2], and the singular-continuous part does by atomlessness. Thus the discrete part has singleton mass μ({x}) at every x. A measure concentrated on a countable set is determined by these masses through countable additivity, so this discrete part equals μd from step 1.1. The other two parts therefore sum to the same finite remainder η. The uniqueness clause of [L3] identifies them with μac and μsc.

Depends on

Used by

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Sources