Generalized Couplings and Ergodic Rates for SPDEs and Other Markov Models: A Generalized Coupling and a Lyapunov Function Give a Unique Invariant Measure and Wasserstein Ergodic RatesResearch Paper
Motivation
Many Markov processes that arise as solutions of stochastic partial differential equations, stochastic delay equations, or other infinite-dimensional models are not strong Feller: their transition probabilities from two nearby starting points can be mutually singular. For such processes convergence to equilibrium cannot hold in total variation, and the classical Harris theorem (a Lyapunov function plus a minorization on a small set) does not apply. Hairer, Mattingly and Scheutzow ([23], 2011) replaced total variation by a coupling distance built from a suitable distance-like function , and proved a weak Harris theorem: contraction of on the whole space, -smallness of the level sets of a Lyapunov function, and the Lyapunov drift together give a unique invariant measure and a rate of convergence. Butkovsky ([6], 2014) extended it to subgeometric rates, and Kulik's monograph ([25], 2017) gives a systematic account.
The remaining difficulty is to verify the contraction hypothesis for a concrete model. Butkovsky, Kulik and Scheutzow (arXiv:1806.00395, Ann. Appl. Probab. 2020) show that it suffices to build a generalized coupling: a pair of processes whose first component has the correct law, whose second component is only close in law to the process started at the other point, and whose components approach each other. Their abstract theorem of §2 is the input to the paper's applications to stochastic functional differential equations and to the 2D Navier–Stokes, Euler-type and Boussinesq SPDEs of §4.
Setting
Let be a Polish space with Borel -field , and let be a Markov transition function: Markov kernels with and the Chapman–Kolmogorov identity. Write . The semigroup is Feller if maps bounded continuous functions to continuous functions.
A distance-like function is symmetric, lower semicontinuous and vanishes exactly on the diagonal. A premetric is lower semicontinuous and vanishes exactly on the diagonal, but need not be symmetric. For probability measures , is the set of couplings and
is the total variation distance.
A measurable satisfies the Lyapunov condition if, for a concave differentiable increasing to infinity with and a constant ,
Put for .
Assumption A asks for a non-increasing with , a locally bounded , and for every a pair of processes with ,
Assumption B1 for a set and : for every there is a set with and . Assumption B2 is a generalized-coupling version of B1 on a set . The paper's auxiliary distance is .
Formalization targets
Goal: Theorem 2.5
Assume is Feller, satisfies the Lyapunov condition, , Assumption A holds, and there is such that B1 holds for every level set and . Then has a unique invariant probability measure , and for every there are with
The constants are existential, so the goal survives any improvement of them.
Companion: Theorem 2.6
In the exponential case , hypothesis B1 on all level sets may be replaced by B2 on the single level set ; the same bound then holds and is exponential in .
Milestones
In attack order: is distance-like (2.6); the coupling lemma, the gluing lemma and the reimbursement bound used inside the proof of Theorem 2.3(i); Theorem 2.3(i) (contractivity of under A) and (ii) (-smallness under B1); the remark after Definition 2.2 that contractivity and smallness give (2.3)–(2.4); the non-expansion step of the proof of Theorem 2.5; Proposition 2.1 (cited weak Harris theorem); and, for the companion, Theorem 2.3(iii), Proposition 2.2 (cited) and Theorem 2.6.
Significance
Theorem 2.5 turns the verification of the weak Harris theorem into two checks that can be carried out model by model: construct a controlled process that is close in law to the true one (Assumption A), and check a support condition on level sets (B1). It covers subexponential rates, given by the function of the Lyapunov drift, and the Wasserstein distance it controls metrizes weak convergence. Theorem 2.6 is the abstract result behind the exponential ergodicity statements for SPDEs in §4 of the paper.
The results are proved in the paper; none of them, nor the weak Harris theorems of [6] and [23] they rely on, has a machine-checked proof. Mathlib has Markov kernels, their composition and invariant measures, but no coupling distances for lower semicontinuous costs, no maximal coupling or gluing lemma on Polish spaces, and no weak Harris theorem. Propositions 2.1 and 2.2 are cited by the paper, not proved there; formalizing them is part of the mission.
Difficulty
The obvious route to contraction is a true coupling of and whose components meet or approach. For processes without the strong Feller property, such a coupling is generally not available explicitly; the generalized coupling only gives the second marginal up to a total variation error. Turning the error-in-law bound into a statement about needs a maximal coupling of two laws on a Polish space and a gluing of two couplings along a common marginal, both of which rest on disintegration of measures. The cited Proposition 2.1 is itself a substantial result: existence of an invariant measure needs tightness from the Lyapunov drift and the Feller property, and the subexponential rate needs a careful interpolation between the drift and the contraction.
Formalization scope
The state space is any type with MetricSpace, CompleteSpace, SeparableSpace and the Borel σ-algebra; is dist. Time is ℝ≥0 and is a map ℝ≥0 → Kernel E E with Markov kernels, , Chapman–Kolmogorov, and measurability of , which the time integral in (2.2) presupposes. Expectations, and are lower Lebesgue integrals in , and (2.2) is stated without subtraction (), which is equivalent. A pair of processes is represented by its joint law on path space; is read through the one-dimensional marginals , a weaker hypothesis. Total variation is the published MarkovChainCLT.tvDist, without a factor 2. "Unique invariant measure" means unique among probability measures, with invariance for every . is encoded by quantifying over every with ; such a exists and is unique under the Lyapunov condition. In Proposition 2.1 condition 2 is stated as , which is Proposition 2.1 for the equivalent complete metric and is the form the proof of Theorem 2.5 uses.
No statement relies on a junk value: no Bochner integral of a possibly non-integrable function, no real-valued infimum over a possibly empty or unbounded set, no Measure.map along a non-measurable map, no default-valued inverse of (which would make the bound read ), and "invariant" is never used without "probability".
A complete development needs: Kantorovich-type coupling distances for lower semicontinuous costs, maximal couplings and gluing on Polish spaces, the transfer of -bounds through Markov kernels, and the weak Harris theorem with subexponential rates. All of these are reusable well beyond this mission. Contributions to any milestone, including the cited Propositions 2.1 and 2.2, are welcome.
Selected references
- O. Butkovsky, A. Kulik, M. Scheutzow, Generalized couplings and ergodic rates for SPDEs and other Markov models, Ann. Appl. Probab. 30(1), 2020. arXiv:1806.00395, doi:10.1214/19-AAP1485
- M. Hairer, J. C. Mattingly, M. Scheutzow, Asymptotic coupling and a general form of Harris' theorem with applications to stochastic delay equations, Probab. Theory Related Fields 149, 2011. arXiv:0902.4495
- O. Butkovsky, Subgeometric rates of convergence of Markov processes in the Wasserstein metric, Ann. Appl. Probab. 24(2), 2014. arXiv:1211.4273
- A. Kulik, Ergodic Behavior of Markov Processes, De Gruyter, Berlin, 2017. doi:10.1515/9783110458930
- C. Villani, Optimal Transport: Old and New, Springer, 2009 (coupling lemma, Theorem 4.1; gluing, p. 23). doi:10.1007/978-3-540-71050-9