topological dynamics
Symbolic Dynamics
You should know: discrete maps, ergodic theory ds
Overview
Symbolic dynamics encodes the orbits of a dynamical system using sequences over a finite alphabet, reducing continuous or differentiable dynamics to combinatorics on symbol sequences. A partition of the phase space into regions labeled 0, 1, ..., k-1 assigns to each orbit the sequence of labels it visits -- its itinerary. The set of allowed itineraries forms a shift-invariant subspace of the full shift A^Z. Subshifts of finite type (SFTs), defined by a finite list of forbidden words, model Markov systems. Sofic shifts generalise SFTs and arise from finite automata.
Intuition
Imagine tracking whether a pendulum swings left (L) or right (R) at each second. The resulting infinite sequence of L's and R's is the symbolic orbit. If the system is chaotic, the set of all possible symbolic orbits is huge -- essentially all sequences of L's and R's. If the system is constrained (e.g., you can never have LL), the allowed sequences form a subshift of finite type. The beauty of symbolic dynamics is that many dynamical questions (periodicity, topological entropy, mixing) become purely combinatorial questions about the shift.
Formal Definition
Let A = {0,...,k-1} be a finite alphabet. The full shift is (A^Z, sigma) where A^Z is the set of bi-infinite sequences and sigma is the left shift: sigma(x)_n = x_{n+1}. A subshift is a closed, shift-invariant subset X of A^Z. A subshift of finite type (SFT) is defined by a finite set F of forbidden words: X = {x in A^Z : no word in F appears in x}. Every SFT is conjugate to a Markov shift defined by a transition matrix A: X_A = {x : A_{x_n, x_{n+1}} = 1 for all n}.
Notation
| Notation | Meaning |
|---|---|
| Full shift over alphabet A | |
| Left shift map | |
| Set of allowed words of length n in subshift X | |
| Topological entropy of subshift X |
Theorems
Worked Examples
- 1
The golden mean shift is an SFT with transition matrix A = [[1,1],[1,0]] (states 0 and 1, with transitions: from 0 can go to 0 or 1; from 1 can only go to 0).
- 2
Characteristic polynomial: det(A - lambda*I) = (1-lambda)(0-lambda) - 1 = lambda^2 - lambda - 1.
- 3
Largest eigenvalue: rho(A) = (1 + sqrt(5))/2 = phi (golden ratio).
- 4
Topological entropy: h = log(phi) = log((1+sqrt(5))/2) approx 0.481 bits.
✓ Answer
The topological entropy of the golden mean shift is log(phi) where phi = (1+sqrt(5))/2 is the golden ratio.
Practice Problems
Define a subshift of finite type and explain how to compute its topological entropy from the transition matrix.
Common Mistakes
Thinking every closed shift-invariant set is a subshift of finite type.
SFTs are a special subclass defined by finitely many forbidden words. Sofic shifts (defined by finite automata, not finite forbidden words) and more general subshifts exist that are not SFTs.
Quiz
Historical Background
Symbolic dynamics originated with Hadamard (1898), who encoded geodesics on surfaces of negative curvature by sequences of symbols corresponding to fundamental domain crossings. Morse and Hedlund systematically developed the theory in the 1930s-40s. The connection to hyperbolic dynamics via Markov partitions was established by Adler-Weiss (1970) and Sinai, and extended to Axiom A systems by Bowen.
- 1898
Hadamard encodes geodesics on hyperbolic surfaces using symbolic sequences
Jacques Hadamard
- 1938
Morse and Hedlund develop symbolic dynamics systematically
Marston Morse, Gustav Hedlund
- 1970
Adler and Weiss construct Markov partitions for hyperbolic toral automorphisms
Roy Adler, Benjamin Weiss
- 1975
Bowen constructs Markov partitions for Axiom A diffeomorphisms
Rufus Bowen
Summary
- Symbolic dynamics encodes orbits as infinite sequences over a finite alphabet, reducing dynamics to combinatorics.
- Subshifts of finite type (SFTs) are defined by transition matrices; their entropy is the log of the spectral radius.
- The Curtis-Lyndon-Hedlund theorem characterises conjugacies between subshifts as sliding block codes.
- Symbolic dynamics is the framework for analysing hyperbolic and chaotic systems via Markov partitions.
References
- BookLind, D. and Marcus, B. An Introduction to Symbolic Dynamics and Coding. Cambridge, 1995.
- BookKatok, A. and Hasselblatt, B. Introduction to the Modern Theory of Dynamical Systems. Cambridge, 1995.
Mathematics