A geometrically ergodic chain has a -integrable rate constant
DisprovedMarkovChainCLT.geometricallyErgodic_integrable_rateLet be a Harris ergodic Markov chain with invariant distribution which is geometrically ergodic, i.e. there are a function and a constant with
Then the rate constant may be taken -integrable: there exist with and such that for all and all .
This is the standard drift-function form of geometric ergodicity: a Harris ergodic chain is geometrically ergodic if and only if it satisfies a geometric drift condition for a small set and some , and the resulting rate constant may be taken proportional to , which satisfies (Meyn & Tweedie 1993, Theorems 15.0.1 and 16.0.1; Roberts & Rosenthal 1997).
The integrability is exactly the standing side condition under which the source's Theorem 2(ii) converts a total-variation rate into a bound on the strong mixing coefficients, . It is therefore what allows the geometric cases of Corollary 2 and Corollary 3 — which assume only geometric ergodicity, with no explicit moment condition on the rate constant — to be routed through the mixing machinery.
import Definitions.Def_MarkovErgodicity import Definitions.Def_MarkovChainPathMeasure import Definitions.Def_MixingCoefficients open MeasureTheory ProbabilityTheory Filter open scoped ENNReal NNReal Topology ProbabilityTheory
theorem MarkovChainCLT.geometricallyErgodic_integrable_rate {X : Type*} [MeasurableSpace X]
(P : Kernel X X) [IsMarkovKernel P] (π : Measure X) [IsProbabilityMeasure π]
(hP : HarrisErgodic P π) (hgeo : GeometricallyErgodic P π) :
∃ M : X → ℝ, ∃ t : ℝ, (∀ x, 0 ≤ M x) ∧ Integrable M π ∧ 0 ≤ t ∧ t < 1 ∧
ErgodicWithRate P π M (fun n => t ^ n) := by sorry