Abstract
Using a combination of analytical and numerical techniques, we show that chaos in globally coupled identical dynamical systems, whether dissipative or Hamiltonian, is both extensive and subextensive: their spectrum of Lyapunov exponents is asymptotically flat (thus extensive) at the value given by a single unit forced by the mean field, but sandwiched between subextensive bands containing typically exponents whose values vary as with .
- Received 23 March 2011
DOI:https://doi.org/10.1103/PhysRevLett.107.124101
© 2011 American Physical Society