Reversible centered-indicator decay bounds one-step maximal correlation
OpenMarkovChainCLT.rhoMixingCoef_one_le_of_reversible_indicator_even_decaymarkov-chainmaximal-correlationreversibilityspectral-gap
Let be a stationary Markov kernel reversible with respect to the probability law , and let . Assume there is a finite constant such that every centered event indicator has exponentially decaying even-lag correlation:
for every measurable and every . Then the stationary chain's one-step maximal-correlation coefficient obeys
The centered indicators span a dense subspace of centered . Reversibility makes the Markov operator self-adjoint, so the displayed even moments control its centered spectrum. The Markov reduction then identifies that operator norm with the one-step maximal correlation.
Preamble
import Definitions.Def_MarkovErgodicity import Definitions.Def_MarkovChainPathMeasure import Definitions.Def_MixingCoefficients open MeasureTheory ProbabilityTheory Filter open scoped ENNReal NNReal Topology ProbabilityTheory
Formal statement
theorem MarkovChainCLT.rhoMixingCoef_one_le_of_reversible_indicator_even_decay
{X : Type*} [MeasurableSpace X]
(P : Kernel X X) [IsMarkovKernel P]
(pi : Measure X) [IsProbabilityMeasure pi]
(hinv : Kernel.Invariant P pi)
(t : ℝ) (ht_nonneg : 0 ≤ t) (ht_lt : t < 1)
(hrev : Kernel.IsReversible P pi)
(hdecay : ∃ C : ℝ, 0 ≤ C ∧
∀ (A : Set X), MeasurableSet A → ∀ n : ℕ, 1 ≤ n →
|∫ x,
((A.indicator (fun _ => (1 : ℝ))) x - pi.real A) *
(((iterKernel P (2 * n)) x A).toReal - pi.real A) ∂pi| ≤
C * t ^ (2 * n)) :
rhoMixingCoef (chainMeasure P pi) (fun i omega => omega i) 1 ≤ t := by sorrySource
G. O. Roberts and J. S. Rosenthal, Geometric Ergodicity and Hybrid Markov Chains, Electronic Communications in Probability 2 (1997), Theorem 2 and proof, pp. 7-9, https://www.probability.ca/jeff/ftpdir/hybrid.pdf; Richard C. Bradley, On Mixing Properties of Reversible Markov Chains, arXiv:1403.4895v1, p. 4, eq. (1.10), https://arxiv.org/abs/1403.4895.