Yet another look at Harris' ergodic theorem for Markov chains

Martin Hairer, Jonathan C. Mattingly

Setting and main result

Throughout this note, we fix a measurable space X\mathbf{X} and a Markov transition kernel P(x,⋅)\mathcal{P}(x,\cdot) on X\mathbf{X}. We will use the notation P\mathcal{P} for the operators defined as usual on both the set of bounded measurable functions and the set of measures of finite mass by

Hence we are using P\mathcal{P} both to denote the action on functions and its duel action on measure. Note that P\mathcal{P} extends trivially to measurable functions φ ⁣:X→[0,+∞]\varphi\colon\mathbf{X}\to[0,+\infty]. We first assume that P\mathcal{P} satisfies the following geometric drift condition:

There exists a function V:X→[0,∞)V:\mathbf{X}\rightarrow[0,\infty) and constants K≥0K\geq 0 and γ∈(0,1)\gamma\in(0,1) such that