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Geometric ergodicity yields a geometric drift condition towards a small set (Meyn-Tweedie Thm 15.0.1)

Proved
MarkovChainCLT.geoDriftCondition_of_geometricallyErgodic

by BrunoDCDO · Sep 4, 2026 · Mathlib c5ea003 (Lean v4.30.0)

ergodicitymarkov-chainsprobability

Let XXX be a Harris ergodic Markov chain with transition kernel PPP and invariant probability distribution π\piπ, and suppose XXX is geometrically ergodic: there are a function M≥0M \ge 0M≥0 and a constant t<1t < 1t<1 with

∥Pn(x,⋅)−π∥≤M(x) tn(x∈X, n≥1).\|P^n(x,\cdot) - \pi\| \le M(x)\,t^n \qquad (x \in \mathsf{X},\ n \ge 1).∥Pn(x,⋅)−π∥≤M(x)tn(x∈X, n≥1).

Then XXX satisfies a geometric drift condition: there exist a measurable function V:X→[1,∞)V : \mathsf{X} \to [1,\infty)V:X→[1,∞), a measurable small set CCC (a set carrying a minorization Pn0(x,⋅)≥ε Q(⋅)P^{n_0}(x,\cdot) \ge \varepsilon\,Q(\cdot)Pn0​(x,⋅)≥εQ(⋅) for all x∈Cx \in Cx∈C), and constants d>0d > 0d>0, bbb with VVV integrable under every P(x,⋅)P(x,\cdot)P(x,⋅) and

ΔV(x)=PV(x)−V(x)≤−d V(x)+b 1C(x)(x∈X).\Delta V(x) = PV(x) - V(x) \le -d\,V(x) + b\,\mathbb{1}_C(x) \qquad (x \in \mathsf{X}).ΔV(x)=PV(x)−V(x)≤−dV(x)+b1C​(x)(x∈X).

This is the direction "geometrically ergodic ⇒\Rightarrow⇒ drift (5)" of the classical equivalence between geometric ergodicity and the geometric drift condition (Meyn and Tweedie 1993, Theorem 15.0.1 and Chapter 16), invoked in the source's Remark 1 as "geometric ergodicity is equivalent to (5)". Together with its two companions (the π\piπ-integrability of VVV and the total-variation rate proportional to VVV) it is what lets a geometrically ergodic chain be routed through the drift machinery with a π\piπ-integrable rate constant.

Formalization Note Harris ergodicity is the mission's total-variation encoding (HarrisErgodic: π\piπ invariant and ∥Pn(x,⋅)−π∥→0\|P^n(x,\cdot) - \pi\| \to 0∥Pn(x,⋅)−π∥→0 from every xxx), which supplies the ψ\psiψ-irreducibility and aperiodicity assumed by Meyn and Tweedie. The drift function is required to be finite and at least 111 everywhere, and the drift condition carries the integrability of VVV under each P(x,⋅)P(x,\cdot)P(x,⋅) as a conjunct, following the platform definition GeoDriftCondition. The σ\sigmaσ-algebra of the state space is assumed countably generated (MeasurableSpace.CountablyGenerated X), the standing assumption of Meyn and Tweedie (1993, Section 3.1) on which the existence of small sets (their Theorem 5.2.2) rests; the mission's Theorem 1(i) milestone carries the same hypothesis.

Preamble
import Definitions.Def_MarkovErgodicity
import Definitions.Def_MarkovDriftMinorization

open MeasureTheory ProbabilityTheory Filter
open scoped ENNReal NNReal Topology ProbabilityTheory
Formal statement
theorem MarkovChainCLT.geoDriftCondition_of_geometricallyErgodic {X : Type*} [MeasurableSpace X]
    [MeasurableSpace.CountablyGenerated X]
    (P : Kernel X X) [IsMarkovKernel P] (π : Measure X) [IsProbabilityMeasure π]
    (hP : HarrisErgodic P π) (hgeo : GeometricallyErgodic P π) :
    ∃ V : X → ℝ, Measurable V ∧ (∀ x, 1 ≤ V x) ∧
      ∃ C : Set X, MeasurableSet C ∧ IsSmallSet P C ∧
        ∃ d b : ℝ, 0 < d ∧ GeoDriftCondition P V d b C := by sorry
Source
G. L. Jones, "On the Markov Chain Central Limit Theorem", Probability Surveys 1 (2004) 299-320, arXiv math/0409112v2, Section 2, Remark 1 (arXiv v2 pp. 3-4); original: S. P. Meyn & R. L. Tweedie, Markov Chains and Stochastic Stability (1993), Theorem 15.0.1 ((i) => (iii)) and Chapter 16; standing assumption: Meyn & Tweedie (1993), Section 3.1 (countably generated sigma-field) and Theorem 5.2.2 (existence of small sets)

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