type and type transition for random walks on randomly
play

Type and type transition for random walks on randomly directed - PowerPoint PPT Presentation

Generalities on random walks Algebraic and probabilistic structures Directed lattices Sketch of proofs Type and type transition for random walks on randomly directed lattices To Iain MacPhee, in memoriam Dimitri Petritis Joint work with


  1. Generalities on random walks Algebraic and probabilistic structures Directed lattices Sketch of proofs Type and type transition for random walks on randomly directed lattices To Iain MacPhee, in memoriam Dimitri Petritis Joint work with Massimo Campanino Institut de recherche mathématique Université de Rennes 1 and CNRS (UMR 6625) France Aspects of random walks 1 April 2014 Durham, 1 April 2014 Random walks on directed lattices

  2. Generalities on random walks Algebraic and probabilistic structures Introduction and motivation Directed lattices And when X is not a group? Sketch of proofs What is the type problem for random walks? How often does a random walker on a denumerably infinite graph X returns to its starting point? It depends on X and on the law of jumps. Typically a dichotomy either almost surely infinitely often (recurrence), or almost surely finitely many times (transience). Durham, 1 April 2014 Random walks on directed lattices

  3. Generalities on random walks Algebraic and probabilistic structures Introduction and motivation Directed lattices And when X is not a group? Sketch of proofs Recall the case X = Z d X = Z d is an Abelian group with generating set, e.g. the minimal generating set A = { e 1 , − e 1 , . . . , e d , − e d } ; card A = 2 d . µ probability on A ⇒ probability on X with supp µ = A . 1 1 Uniform: ∀ x ∈ A : µ ( x ) ≡ card A = 2 d . Symmetric: ∀ x ∈ A : µ ( x ) = µ ( − x ) . Zero mean: � x ∈ A x µ ( x ) = 0. ξ = ( ξ n ) n ∈ N i.i.d. sequence with ξ 1 ∼ µ . Define X 0 = x ∈ X and X n + 1 = X n + ξ n + 1 . Then P ( x , y ) = P ( X n + 1 = y | X n = x ) = P ( ξ n + 1 = y − x ) = µ ( y − x ) . Simple ( = uniform on the minimal generating set) random walk on X the X -valued Markov chain ( X n ) n ∈ N of MC ( X , P , ǫ x ) Durham, 1 April 2014 Random walks on directed lattices

  4. Generalities on random walks Algebraic and probabilistic structures Introduction and motivation Directed lattices And when X is not a group? Sketch of proofs Recall the case X = Z d ? (cont’d) Theorem (Georg Pólya a ) a Über eine Aufgabe der Wahrscheinlichkeitsrechnung betreffend die Irrfahrt im Straßennetz, Ann. Math. (1921) For X = Z d with uniform jumps on n.n. d ≥ 3: transcience, d = 1 , 2: recurrence. Proof by direct combinatorial and Fourier estimates. P n ( x , y ) := � x 1 ,... x n − 1 P ( X 0 = x , X 1 = x 1 , . . . , X n = y ) = µ ∗ n ( y − x ) . For ξ ∼ µ and µ uniform, x exp ( i � t | x � ) µ ( x ) = 1 � d χ ( t ) = E exp ( i � t | ξ � ) = � k = 1 cos ( t k ) . d � 2 n � � d c d 1 1 P 2 n ( 0 , 0 ) ∼ � d d t ∼ k = 1 cos ( t k ) n d / 2 as ( 2 π ) d [ − π,π ] d d n → ∞ . Conclude by Borel-Cantelli ( d ≥ 3) or renewal theorem ( d ≤ 2). Durham, 1 April 2014 Random walks on directed lattices

  5. Generalities on random walks Algebraic and probabilistic structures Introduction and motivation Directed lattices And when X is not a group? Sketch of proofs Why simple random walk are studied? Mathematical interest: simple models with three interwoven structures: low-level algebraic structure conveying combinatorial information, high-level algebraic structure conveying geometric information, stochastic structure adapted to the two previous structures. Discretised (in time/space) versions of stochastic processes, numerous interesting mathematical problems still open. Modelling transport (of energy, information, charge, etc.) phenomena in crystals (metals, semiconductors, ionic conductors, etc.) or on networks. Intervening in models described by PDE’s involving a Laplacian hence in harmonic analysis classical electrodynamics, statistical mechanics, quantum mechanics, quantum field theory, etc Durham, 1 April 2014 Random walks on directed lattices

  6. Generalities on random walks Algebraic and probabilistic structures Introduction and motivation Directed lattices And when X is not a group? Sketch of proofs Short algebraic reminder Groups, groupoids and semigroupoids Definition Let Γ � = ∅ . (Γ , · ) is a semigroup monoid group semigroupoid groupoid if ∃ Γ 2 ⊆ Γ × Γ and · : Γ 2 → Γ if · : Γ × Γ → Γ and ∀ a , b , c ∈ Γ ( c , b ) , ( b , a ) ∈ Γ 2 ⇒ ( cb ) a = c ( ba ) ( cb , a ) , ( c , ba ) ∈ Γ 2 and ( cb ) a = c ( ba ) ∃ ! e ∈ Γ : ea = ae = a units not necessarily unique, ∃ a − 1 ∈ Γ : aa − 1 = a − 1 a = e ∃ a − 1 : ( a − 1 ) − 1 = a , ( a , a − 1 ) , ( a − 1 , a ) ∈ Γ 2 and ( a , b ) ∈ Γ 2 ⇒ a − 1 ( ab ) = b ; ( b , a ) ∈ Γ 2 ⇒ ( ba ) a − 1 = b . Durham, 1 April 2014 Random walks on directed lattices

  7. Generalities on random walks Algebraic and probabilistic structures Introduction and motivation Directed lattices And when X is not a group? Sketch of proofs Monoidal closure of A A = { E , N , W , S } ; A ∗ = ∪ ∞ n = 0 A n , A 0 = { ε } , A n = { α = ( α 1 , . . . , α n ) , α i ∈ A } N FA 1 = W E S Proposition ( A ∗ , ◦ ) is a monoid, the monoidal closure of A . α ◦ ε = ε ◦ α = α . If α = EENNESW ; β = WSN then α ◦ β = EENNESWWSN � = WSNEENNESW = β ◦ α . Durham, 1 April 2014 Random walks on directed lattices

  8. Generalities on random walks Algebraic and probabilistic structures Introduction and motivation Directed lattices And when X is not a group? Sketch of proofs Combinatorial information � = geometric information A ∗ ≃ path space. Combinatorial information encoded into the finite automaton FA. Paths define a regular language recognised by FA 1 . Road map needed to translate into geometric information E = a , W = a − 1 ; N = b , S = b − 1 and relations on reduced words. Example Z 2 = � A |R 1 � : R 1 = { aba − 1 b − 1 = e } (Abelian). F 2 = � A |R 2 � : R 2 = ∅ (free). Z 2 and F 2 have same combinatorial description but are very different groups. Geometric information encoded into the group structure Γ = � A |R� . Natural surjection g : A ∗ ։ Γ . Durham, 1 April 2014 Random walks on directed lattices

  9. Generalities on random walks Algebraic and probabilistic structures Introduction and motivation Directed lattices And when X is not a group? Sketch of proofs The Cayley graph of finitely generated groups Definition Let Γ = � A | R � . The Cayley graph Cayley (Γ , A ) is the graph vertex set Γ and edge set the pairs ( x , y ) ∈ Γ 2 such that y = ax for some a ∈ A . Remark Since A symmetric, graph undirected. Example For A = { a , b , a − 1 , b − 1 } , Cayley ( F 2 , A ) is the homogeneous tree of degree 4, Cayley ( Z 2 , A ) is the standard Z 2 lattice with edges over n.n. Durham, 1 April 2014 Random walks on directed lattices

  10. Generalities on random walks Algebraic and probabilistic structures Introduction and motivation Directed lattices And when X is not a group? Sketch of proofs The probabilistic structure µ := ( p 1 , . . . , p card A ) ∈ M 1 ( A ) transforms FA into PFA. Path space A ∗ acquires natural probability P µ ( { α } ) = � | α | i = 1 p α i . Due to the surjection g , PFA induces natural Markov chain ( X n ) : P ( X n + 1 = y | X n = x ) = µ ( { x − 1 y } ) = p x − 1 y , x , y ∈ Γ . Probabilistic structure adapted to combinatorial/geometric structure if supp µ = A . When µ replaced by family ( µ x ) x ∈ Γ not necessarily supp µ x = A , ∀ x ∈ Γ (i.e. ellipticity can fail). Suppose there exist a ∈ A and x , y ∈ Γ , with x � = y , such that µ x ( { a } ) = 0 and µ y ( { a } ) � = 0 . Then combinatorial structure must be modified for ( µ x ) x ∈ Γ to remain adapted. The resulting Γ may not be a group any longer. Durham, 1 April 2014 Random walks on directed lattices

  11. Generalities on random walks Algebraic and probabilistic structures Introduction and motivation Directed lattices And when X is not a group? Sketch of proofs How can we generalise? Distinctive property of simple r.w. on Z d : Abelian group of finite type generated by supp µ , i.e. graph on which r.w. evolves = Cayley ( Z d , supp µ ) . Generalisation to non-commutative groups: The three interwoven structures and harmonic analysis survive. Very active domain (e.g. products of fixed size random matrices, random dynamical systems, amenability issues, etc.). Space inhomogeneity: family of probabilities ( µ x ) x ∈ X , with µ x ∈ M 1 ( A ) ≃ { p ∈ R card A a ∈ A p a = 1 } . : � + P ( X n + 1 = y | X n = x ) = µ x ( y − x ) . (e.g. i.i.d. random probabilities ( µ x ) ). Combinatorial and geometric structures survive. If uniform ellipticity, probabilistic structure remains adapted. But harmonic analysis (if any) very cumbersome. Durham, 1 April 2014 Random walks on directed lattices

  12. Generalities on random walks Algebraic and probabilistic structures Introduction and motivation Directed lattices And when X is not a group? Sketch of proofs And when the graph is not a group? R.w. on quasi-periodic tilings of R d of Penrose type: the groupoid case Transport properties on quasi-periodic structures 1 . Spectral properties of Schrödinger operators on quasi-periodic structures. Random walks on groupoids, non-random inhomogeneity. 1 Introduced as mathematical curiosities by Sir Roger Penrose (1974–1976), observed in nature as crystalline structures of Al-Mn alloys by Shechtman (1982) - Nobel Prize in Chemistry 2011, obtained by an algorithmically much more efficient way by Duneau-Katz (1985). Durham, 1 April 2014 Random walks on directed lattices

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend