Mean dimension

In mathematics, the mean (topological) dimension of a topological dynamical system is a non-negative extended real number that is a measure of the complexity of the system. Mean dimension was first introduced in 1999 by Gromov.[1] Shortly after it was developed and studied systematically by Lindenstrauss and Weiss.[2] In particular they proved the following key fact: a system with finite topological entropy has zero mean dimension. For various topological dynamical systems with infinite topological entropy, the mean dimension can be calculated or at least bounded from below and above. This allows mean dimension to be used to distinguish between systems with infinite topological entropy. Mean dimension is also related to the problem of embedding topological  dynamical systems in shift spaces (over Euclidean cubes).

  1. ^ Gromov, Misha (1999). "Topological invariants of dynamical systems and spaces of holomorphic maps I". Mathematical Physics, Analysis and Geometry. 2 (4): 323–415. doi:10.1023/A:1009841100168. S2CID 117100302.
  2. ^ Cite error: The named reference LindenstraussWeiss2000 was invoked but never defined (see the help page).