Harmonic functions: Lemma 3.1.6 Introduction and main results

One can find a few more examples of diffusion matrices satisfying the assumptions in Theorem 3.1.5, but it turns out that these are mainly trivial variations on the two examples mentioned above. The message of Theorem 3.1.5 is that all these examples fall into the same framework. The common property that unites them is the stability of the boundary distribution against a linear drift. In fact, we conjecture that this property is a necessary condition for the uni- versality of the long-time distribution. If the boundary distribution is not stable against a linear drift, it seems likely that still X t converges weakly to some limit as t → ∞, although we do not know how to prove this for infinite . But we believe that in this case the law of X ∞ will depend on the choice of the recur- rent kernel a S and the Abelian group . However, we have at present very little knowledge about the nature of this dependence. In conclusion, we have found that the ‘duality comparison argument’ devel- oped in [6] is linked to universality of the long-time distribution of solutions to 3.1.2. A similar relation between comparison arguments and universality has been found for models on the hierarchical group N with N large in [1, 10, 21]. There, the system in 3.1.2 is studied by means of a renormalization transforma- tion acting on diffusion matrices. Under iteration of the transformation, the renor- malized diffusion matrices converge to a limit. In the clustering case a comparison argument shows that this limit is universal within a large ‘universality class’ of ma- trices. This has been worked out for 2-type models in [1] and for isotropic models in [21]. The universal limit that is found is exactly the w ∗ in formula 3.1.52. The conclusion we can draw from Theorem 3.1.5 is that the correct ‘universality classes’ of diffusion matrices one should look at are formed by all diffusion matri- ces w that share the same boundary distribution Ŵ x x ∈K . Furthermore, universal behavior can be expected only if this boundary distribution is stable against a linear drift.

3.2 Proofs of Theorems 3.1.1 and 3.1.2

3.2.1 Proof of Theorem 3.1.1

If ⊂ is finite then C 2 K is the space of real functions on K that have a C 2 -extension to all of R d . C 2 fin K consists of all functions that are the lifting to the larger space K of a function in C 2 K for some finite ⊂ . Lemma 3.2.1 The operator A in 3.1.10 with domain D A in 3.1.12 is a densely defined linear operator on the Banach space C K , and satisfies the max- imum principle. Proof of Lemma 3.2.1: By the Stone-Weierstrass theorem, C 2 K is dense in C K for each finite ⊂ . Pick a bijection between and the positive integers and fix a point z ∈ K . Define, for x ∈ K , π n x : = x 1 , x 2 , . . . , x n , z, z, . . .. 3.2.1 The sets πK are uniformly dense in K , and since each f ∈ C K is uni- formly continuous, it is the uniform limit of functions f n x : = f π n x 3.2.2 depending on finitely many coordinates. Hence C fin K is dense in C K . To see that A satisfies the maximum principle, fix f ∈ C 2 fin K and suppose that f assumes its maximum in a point x. Fix an i ∈ . Keeping all x j j =i fixed, f assumes its maximum as a function of the remaining variable in the point x i . By the convexity of K it is easily checked that j α a j − ix α j − x α i ∂ ∂ x α i f x ≤ 0. 3.2.3 Condition 3.1.8 ensures that αβ w αβ x i ∂ 2 ∂ x α i ∂ x β i f x ≤ 0, 3.2.4 as can be seen by writing the matrix wx in diagonal form: αβ w αβ x i ∂ 2 ∂ x α i ∂ x β i f x = ˜α λ ˜α x ∂ 2 ∂ x ˜α 2 f x 3.2.5 for an appropriate orthonormal basis x ˜α of R d . By condition 3.1.8, the only non-zero terms in 3.2.5 occur for directions that lie in the space I x , and for such directions the second derivative is non-positive. We equip K with the Borel σ -field generated by the open sets. We write D K [0, ∞ for the cadlag functions from [0, ∞ to K , equipped with the metric d from chapter 3, section 5 of [16], which generates the Skorohod topology. By C K [0, ∞ we denote the continuous functions from [0, ∞ to K . On D K [0, ∞ we choose the Borel σ -field generated by the open sets of this topology. We equip the space of probability measures on D K [0, ∞ with the topology of weak con- vergence and we denote weak convergence of the laws of processes with sample paths in D K [0, ∞ by ⇒. Thus X n ⇒ X means that E[ f X n ] → E[ f X] as n → ∞ 3.2.6 for all bounded continuous real functions f on D K [0, ∞. By a solution to the martingale problem we always mean a solution with sample paths in D K [0, ∞.

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