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Finite measures are determined by their averaged open and closed interval masses

Proved
MeasureTheory.Measure.eq_of_interval_average

by Mazecto · Oct 5, 2026 · Mathlib 0df444a (Lean v4.33.1)

complex-analysismeasure-theoryspectral-theory

Let μ,ν\mu,\nuμ,ν be finite Borel measures on R\mathbb RR. Suppose that for every a<ba<ba<b,

μ((a,b))+μ([a,b])2=ν((a,b))+ν([a,b])2.\frac{\mu((a,b))+\mu([a,b])}{2}=\frac{\nu((a,b))+\nu([a,b])}{2}.2μ((a,b))+μ([a,b])​=2ν((a,b))+ν([a,b])​.

Then μ=ν\mu=\nuμ=ν. No assumption that either measure has no atoms is needed. This is the measure-determination step in Stieltjes inversion.

Preamble
import Mathlib.Analysis.SpecialFunctions.Integrals.Basic
import Mathlib.MeasureTheory.Integral.DominatedConvergence
import Mathlib.MeasureTheory.Integral.Prod
import Mathlib.MeasureTheory.Constructions.BorelSpace.Order
import Mathlib.Tactic.FieldSimp
import Mathlib.Tactic.Ring
import Mathlib.Tactic.Linarith
import Mathlib.Tactic.Positivity
import Mathlib.Tactic.FunProp
import Mathlib.Tactic.SplitIfs
import Mathlib.Tactic.NormNum

open MeasureTheory Filter Set
open scoped Topology

Formal statement
theorem MeasureTheory.Measure.eq_of_interval_average (μ ν : Measure ℝ) [IsFiniteMeasure μ] [IsFiniteMeasure ν]
    (h : ∀ a b : ℝ, a < b →
      ((μ (Ioo a b)).toReal + (μ (Icc a b)).toReal) / 2 =
      ((ν (Ioo a b)).toReal + (ν (Icc a b)).toReal) / 2) : μ = ν := by sorry
Source
G. Teschl, Mathematical Methods in Quantum Mechanics, AMS GSM 99 (2009), p. 108, Theorem 3.21 and its proof, Eq. (3.89); https://www.mat.univie.ac.at/~gerald/ftp/book-schroe/schroe.pdf (PDF p. 119).

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