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Total variation bounds differences of integrals of [0,1][0,1][0,1]-valued functions

Proved
MarkovChainCLT.abs_integral_sub_le_tvDist

by LukeBernese · Aug 15, 2026 · Mathlib c5ea003 (Lean v4.30.0)

markov-chainmeasure-theoryprobabilitytotal-variation

Let μ,ν\mu, \nuμ,ν be finite measures on a measurable space X\mathsf{X}X and let f:X→Rf : \mathsf{X} \to \mathbb{R}f:X→R be measurable with 0≤f≤10 \le f \le 10≤f≤1 everywhere. Then

∣∫f dμ−∫f dν∣  ≤  ∥μ−ν∥  :=  sup⁡A measurable∣μ(A)−ν(A)∣.\left| \int f \,\mathrm{d}\mu - \int f \,\mathrm{d}\nu \right| \;\le\; \|\mu - \nu\| \;:=\; \sup_{A \text{ measurable}} \bigl|\mu(A) - \nu(A)\bigr|.​∫fdμ−∫fdν​≤∥μ−ν∥:=A measurablesup​​μ(A)−ν(A)​.

What it upgrades. The total variation distance is defined as a supremum over measurable sets — equivalently, over indicator functions. This theorem says the same bound holds for every measurable function with values in [0,1][0,1][0,1]. The set version is the special case f=1Af = \mathbf{1}_Af=1A​; the function version is what is actually needed, and it does not follow formally from the definition.

Why it is indispensable for Markov chains. Every quantitative mixing estimate has the same shape: one has a rate ∥Pn(x,⋅)−π∥≤C\|P^n(x,\cdot) - \pi\| \le C∥Pn(x,⋅)−π∥≤C and wants to conclude that some functional of the chain started at xxx differs from the same functional under stationarity by at most CCC. The functional in question is almost never an indicator of a set in X\mathsf{X}X — it is x↦K(x,B)x \mapsto K(x, B)x↦K(x,B) for a kernel KKK and a set BBB in a different space, typically path space. Concretely, for a Markov kernel KKK and measurable BBB,

∣(K∘μ)(B)−(K∘ν)(B)∣=∣∫K(x,B) dμ(x)−∫K(x,B) dν(x)∣  ≤  ∥μ−ν∥,\bigl|(K \circ \mu)(B) - (K \circ \nu)(B)\bigr| = \left|\int K(x,B)\,\mathrm{d}\mu(x) - \int K(x,B)\,\mathrm{d}\nu(x)\right| \;\le\; \|\mu - \nu\|,​(K∘μ)(B)−(K∘ν)(B)​=​∫K(x,B)dμ(x)−∫K(x,B)dν(x)​≤∥μ−ν∥,

since x↦K(x,B)x \mapsto K(x,B)x↦K(x,B) takes values in [0,1][0,1][0,1]. That is the data-processing inequality: applying a Markov kernel cannot increase total variation distance. It is the step that transports a rate of convergence on the state space to a bound on path-space events, and hence the step that turns an ergodicity hypothesis into a mixing-coefficient bound.

Proof. The definition of ∥μ−ν∥\|\mu-\nu\|∥μ−ν∥ as a supremum over sets gives no direct handle on integrals; the bridge is the unsigned Hahn decomposition. Choose a measurable sss with ν≤μ\nu \le \muν≤μ on subsets of sss and μ≤ν\mu \le \nuμ≤ν on subsets of scs^{c}sc; equivalently, as measures, ν∣s≤μ∣s\nu|_s \le \mu|_sν∣s​≤μ∣s​ and μ∣sc≤ν∣sc\mu|_{s^c} \le \nu|_{s^c}μ∣sc​≤ν∣sc​. Split each integral over sss and scs^csc. On scs^csc the difference ∫scf dμ−∫scf dν\int_{s^c} f\,\mathrm{d}\mu - \int_{s^c} f\,\mathrm{d}\nu∫sc​fdμ−∫sc​fdν is ≤0\le 0≤0 because f≥0f \ge 0f≥0 and μ≤ν\mu \le \nuμ≤ν there. On sss, applying the same monotonicity to 1−f≥01 - f \ge 01−f≥0 gives

∫s(1−f) dν  ≤  ∫s(1−f) dμ,i.e.∫sf dμ−∫sf dν  ≤  μ(s)−ν(s).\int_s (1-f)\,\mathrm{d}\nu \;\le\; \int_s (1-f)\,\mathrm{d}\mu, \qquad\text{i.e.}\qquad \int_s f\,\mathrm{d}\mu - \int_s f\,\mathrm{d}\nu \;\le\; \mu(s) - \nu(s).∫s​(1−f)dν≤∫s​(1−f)dμ,i.e.∫s​fdμ−∫s​fdν≤μ(s)−ν(s).

Adding the two gives ∫f dμ−∫f dν≤μ(s)−ν(s)≤∥μ−ν∥\int f\,\mathrm{d}\mu - \int f\,\mathrm{d}\nu \le \mu(s) - \nu(s) \le \|\mu-\nu\|∫fdμ−∫fdν≤μ(s)−ν(s)≤∥μ−ν∥. The reverse inequality is the same argument with the roles of μ\muμ and ν\nuν exchanged and sss replaced by scs^csc. Note the two applications of "1−f1-f1−f rather than fff" are what make the bound μ(s)−ν(s)\mu(s)-\nu(s)μ(s)−ν(s) appear rather than the useless ∫sf dμ\int_s f \,\mathrm{d}\mu∫s​fdμ.

Preamble
import Definitions.Def_TotalVariationDist
import Mathlib.MeasureTheory.Measure.Decomposition.Hahn
import Mathlib.MeasureTheory.Integral.Bochner.Set

open MeasureTheory
open MarkovChainCLT
Formal statement
theorem MarkovChainCLT.abs_integral_sub_le_tvDist {X : Type*} [MeasurableSpace X]
    (μ ν : Measure X) [IsFiniteMeasure μ] [IsFiniteMeasure ν]
    (f : X → ℝ) (hf : Measurable f) (h0 : ∀ x, 0 ≤ f x) (h1 : ∀ x, f x ≤ 1) :
    |∫ x, f x ∂μ - ∫ x, f x ∂ν| ≤ tvDist μ ν := by sorry
Source
H. Hahn, "Über die Integrale des Herrn Hellinger und die Orthogonalinvarianten der quadratischen Formen von unendlich vielen Veränderlichen", Monatsh. Math. Phys. 23 (1912) 161-224; D. A. Levin and Y. Peres, Markov Chains and Mixing Times, 2nd ed., AMS 2017, Proposition 4.5 and Lemma 4.11; S. P. Meyn and R. L. Tweedie, Markov Chains and Stochastic Stability, 2nd ed., Cambridge 2009, Ch. 16.

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