Existence and uniqueness: Theorems 3.1.1 and
3.1.5 Clustering: Theorem 3.1.3
In order to state our first result, we introduce the symmetrized kernel a S i : = ai + a−i i ∈ . 3.1.26 By the random walk with kernel a S we mean a continuous-time random walk on that jumps from a point j to a point i with rate a S j − i. By ⇒ we denote weak convergence of the laws of processes as probability measures on K . Theorem 3.1.3 Let X be a shift-invariant solution to 3.1.2 and assume that there exists a K -valued random variable X ∞ such that X t ⇒ X ∞ as t → ∞. 3.1.27 If the random walk with kernel a S is recurrent, then i P[X i ∞ ∈ ∂ w K ∀i ∈ ] = 1 ii P[X i ∞ = X j ∞ ∀i, j ∈ ] = 1. 3.1.28 If the random walk with kernel a S is transient, E[X 0] ∈ ∂ w K and L X 0 is spatially ergodic, then i P[X i ∞ ∈ ∂ w K ] 1 ∀i ∈ ii P[X i ∞ = X j ∞] 1 ∀i = j ∈ . 3.1.29 Note that Theorem 3.1.3 makes a statement about the possible properties of a lim- iting distribution X ∞, but that it does not answer the question whether such a limiting distribution actually exists. Provided we know in some way that X t converges weakly to a limit, Theorem 3.1.3 says the following. In the recurrent case, the configuration in any finite window ⊂ after a sufficiently long time becomes almost flat. At large but finite time in the system there are regions, called ‘clusters’, of typical sizes that grow with time, in which all components are almost equal. This behavior is called ‘clustering’. The behavior is similar to that of the voter model in low d ≤ 2 dimension. In fact, 2-type models as in 3.1.16 are believed to be asymptotically equivalent, in some sense, to the voter model on the same lattice. See [7] for some pictures of simulations of the clustering voter model on Z 2 . In the transient case, such clustering behavior cannot occur. Instead, the system converges to a ‘true’ equilibrium X ∞. We refer to this as ‘stable’ behavior. Although it seems hard to imagine a shift-invariant solution to 3.1.2 that does not converge as t → ∞, the convergence in 3.1.27 is in general hard to prove. For finite , one may exploit the fact that i X i t is a bounded martingale to get the convergence in 3.1.27, not only in the sense of weak convergence, but also in L 2 -norm. 1 For infinite , convergence in L 2 -norm in general does not hold. 1 For the interested reader we have added a proof of this fact in section 3.6.Parts
» largspscb. 826KB Jun 04 2011 12:09:08 AM
» The diffusion limit Particle models and diffusion limits
» Examples Particle models and diffusion limits
» The p-type q-tuple model with migration
» Uniqueness problems Particle models and diffusion limits
» Interacting p-type q-tuple models
» Other models Particle models and diffusion limits
» Renormalization theory Overview of the three articles
» Renormalization of interacting diffusions
» A renormalization transformation Overview of the three articles
» Higher-dimensional generalizations Overview of the three articles
» Renormalization of isotropic diffusions
» Non-isotropic models Overview of the three articles
» Harmonic functions and clustering
» Doing the iterations at once
» Non-invariant harmonics Open problems
» Renormalization on other lattices Discrete models
» Outlook and conclusion Open problems
» The hierarchical model Introduction
» The local mean-field limit N
» The renormalization transformation Introduction
» Multiple space-time scale analysis
» Large space-time behavior and universality
» Generalizations to different state spaces
» Isotropic models Renormalization in d
» Two renormalization classes: Theorems 2.2.5–2.2.10
» Difficulties for d Results for d
» Notation Preliminaries The renormalization transformation
» Proof of Theorem 2.2.1 The renormalization transformation
» Proof of Theorems 2.2.2–2.2.4 The renormalization transformation
» Ergodicity: Proof of Theorem 2.2.5
» Existence: Proof of Theorem 2.2.6 Strong uniqueness: Proof of Theorem 2.2.9
» Weak uniqueness: Proof of Theorem 2.2.10
» Definitions Introduction and main results
» Existence and uniqueness: Theorems 3.1.1 and
» Biological background Introduction and main results
» The non-interacting model Introduction and main results
» Clustering: Theorem 3.1.3 Introduction and main results
» Covariance calculations: Lemma 3.1.4 Introduction and main results
» Universality of the long-time distribution: Theorem 3.1.5
» Harmonic functions: Lemma 3.1.6 Introduction and main results
» Special models: Corollary 3.1.7 Examples
» Proof of Theorem 3.1.1 Proofs of Theorems 3.1.1 and 3.1.2
» Proof of Theorem 3.1.2 Proofs of Theorems 3.1.1 and 3.1.2
» Proof of Lemma 3.1.4 Proofs of Theorem 3.1.3 and Lemma 3.1.4
» Random walk representations Proofs of Theorem 3.1.3 and Lemma 3.1.4
» Spatially ergodic measures Proofs of Theorem 3.1.3 and Lemma 3.1.4
» Proof of Theorem 3.1.3 Proofs of Theorem 3.1.3 and Lemma 3.1.4
» Potential theory Proofs of Theorem 3.1.5, Lemma 3.1.6
» Infinite-dimensional differentiation Proofs of Theorem 3.1.5, Lemma 3.1.6
» Proof of Lemma 3.1.6 Proofs of Theorem 3.1.5, Lemma 3.1.6
» Proof of Theorem 3.1.5 Proofs of Theorem 3.1.5, Lemma 3.1.6
» Proof of Corollary 3.1.7 Proofs of Theorem 3.1.5, Lemma 3.1.6
» Finite largspscb. 826KB Jun 04 2011 12:09:08 AM
» Definitions Introduction and main result
» Main scaling theorem Introduction and main result
» Identification of the drift and diffusion rate of ˆ
» Definitions Convergence of the diffusion rate
» Block immobility Convergence of the diffusion rate
» An approximate equilibrium equation
» Equilibrium calculations Convergence of the diffusion rate
» Asymptotics of the scaling factor µ
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