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Bratteli–Vershik diagram

In mathematics, a Bratteli–VerÅ¡ik diagram is an ordered, essentially simple Bratteli diagram (V, E) with a homeomorphism on the set of all infinite paths called the VerÅ¡hik transformation. It is named after Ola Bratteli and Anatoly Vershik.

Definition

Let X&nbsp;=&nbsp;{(e<sub>1</sub>,&nbsp;e<sub>2</sub>,&nbsp;...) | e<sub>i</sub>&nbsp;∈&nbsp;E<sub>i</sub> and r(e<sub>i</sub>)&nbsp;=&nbsp;s(e<sub>i+1</sub>)} be the set of all paths in the essentially simple Bratteli diagram (V,&nbsp;E). Let E<sub>min</sub> be the set of all minimal edges in E, similarly let E<sub>max</sub> be the set of all maximal edges. Let y be the unique infinite path in E<sub>max</sub>. (Diagrams which possess a unique infinite path are called "essentially simple".)

The Veršhik transformation is a homeomorphism φ&nbsp;:&nbsp;X&nbsp;→&nbsp;X defined such that φ(x) is the unique minimal path if x&nbsp;=&nbsp;y. Otherwise x&nbsp;=&nbsp;(e<sub>1</sub>,&nbsp;e<sub>2</sub>,...) | e<sub>i</sub>&nbsp;∈&nbsp;E<sub>i</sub> where at least one e<sub>i</sub>&nbsp;∉&nbsp;E<sub>max</sub>. Let k be the smallest such integer. Then φ(x) =&nbsp;(f<sub>1</sub>, f<sub>2</sub>,&nbsp;...,&nbsp;f<sub>k−1</sub>, e<sub>k</sub>&nbsp;+&nbsp;1, e<sub>k+1</sub>,&nbsp;...&nbsp;), where e<sub>k</sub>&nbsp;+&nbsp;1 is the successor of e<sub>k</sub> in the total ordering of edges incident on r(e<sub>k</sub>) and (f<sub>1</sub>,&nbsp;f<sub>2</sub>,&nbsp;...,&nbsp;f<sub>k−1</sub>) is the unique minimal path to&nbsp;e<sub>k</sub>&nbsp;+&nbsp;1.

The Veršhik transformation allows us to construct a pointed topological system (X,&nbsp;φ,&nbsp;y) out of any given ordered, essentially simple Bratteli diagram. The reverse construction is also defined.

Equivalence

The notion of graph minor can be promoted from a well-quasi-ordering to an equivalence relation if we assume the relation is symmetric. This is the notion of equivalence used for Bratteli diagrams.

The major result in this field is that equivalent essentially simple ordered Bratteli diagrams correspond to topologically conjugate pointed dynamical systems. This allows us apply results from the former field into the latter and vice versa.

See also

Notes

Further reading