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Interval formulas and atoms for a Lebesgue-Stieltjes measure

Statement

Assume the Axiom of Countable Choice. Let F:RR be nondecreasing and right-continuous, and let μF be its Lebesgue-Stieltjes measure. Then for every a<b,

μF((a,b))=F(b)F(a),

μF([a,b])=F(b)F(a),

μF([a,b))=F(b)F(a),

and

μF({a})=F(a)F(a).

Consequently a is an atom of μF in the sense of An atom of a measure on R if and only if F(a)>F(a), and the set of atoms of μF is at most countable.

Facts & Assumptions

Given: The Axiom of Countable Choice, a nondecreasing right-continuous function F:RR, its Lebesgue-Stieltjes measure μF, and real numbers a<b.

[L1]

Assuming Countable Choice, the measure μF satisfies μF((u,v])=F(v)F(u) for all u<v. (Assuming countable choice, finite-on-compacts Borel measures on R correspond to nondecreasing right-continuous functions modulo constants)

[L2]

Measures are continuous from below along increasing set limits; they are continuous from above along decreasing set limits when one set has finite measure (Continuity from below for measures, Continuity from above when one set has finite measure).

[L3]

For a bounded-variation function on a compact interval, every well-posed one-sided limit exists, every discontinuity is of the first kind, and there are at most countably many discontinuities (A bounded-variation function has at most countably many discontinuities, all of the first kind).

[L4]

Assuming Countable Choice, a countable union of at most countable sets is at most countable (Countable unions of at most countable sets, assuming ACω).

[L5]

A point x is an atom of a Borel measure μ exactly when μ({x})>0 (An atom of a measure on R).

[L6]

If AB are measurable and μ(B)<+, then μ(BA)=μ(B)μ(A) (Measure of a set difference when the smaller set has finite measure).

Proof

technique · direct
1.1

Put tn:=b(ba)/(n+2). Then a<tn<b for every n and tnb.

L1L2L3algebra

Because (a,b)=n(a,tn], continuity from below and [L1] give

μF((a,b))=limnμF((a,tn])=limn(F(tn)F(a))=F(b)F(a).

Here F[a,b] has bounded variation because it is nondecreasing, so [L3] ensures that the displayed left limit exists. [L1, L2, L3, algebra]

2.1

Put sn:=a1/(n+1). Then sn<a and sna, while the intervals (sn,b] decrease to [a,b].

step 1.1L1L2L3

The first interval has finite measure because F is real-valued, so continuity from above and [L1] give

μF([a,b])=limnμF((sn,b])=limn(F(b)F(sn))=F(b)F(a).

The restriction F[a1,a] has bounded variation because it is nondecreasing, so [L3] ensures that the displayed left limit exists. [L1, L2, L3, algebra]

3.1

The intervals (sn,a] decrease to {a}, and continuity from above gives μF({a})=F(a)F(a).

step 2.1L1L2L3

Indeed, (s0,a] has finite measure and μF({a})=limnμF((sn,a])=limn(F(a)F(sn))=F(a)F(a). [step 2.1, L1, L2, L3]

The same argument gives μF({b})=F(b)F(b). Therefore

μF([a,b))=μF([a,b])μF({b})=F(b)F(a).

Together with step 1.1, this proves all four interval formulas. [step 1.1, step 2.1, step 3.1, L1, L6, algebra]

4.1

By step 3.1 and [L5], the point a is an atom of μF exactly when μF({a})=F(a)F(a)>0, which is exactly the jump condition F(a)>F(a).

step 3.1L5
5.1

Fix m1. The restriction F[m,m] is nondecreasing, hence of bounded variation on [m,m].

step 4.1L3

So [L3] makes its discontinuity set at most countable. Every atom of μF in (m,m) is an interior jump point by step 4.1, hence lies in that countable discontinuity set. Therefore the atoms in (m,m) are at most countable. By [L4], their union over m1 is at most countable, and this union contains every atom of μF. [given, step 4.1, L3, L4]

6.1

Steps 1.1 through 5.1 prove the claimed interval formulas, the atom criterion, and the countability of the atom set.

step 1.1step 2.1step 3.1step 4.1step 5.1

[step 1.1, step 2.1, step 3.1, step 4.1, step 5.1] ∎

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