Abstract
Chaotic diffusion in periodic Hamiltonian maps is studied by the introduction of a sequence of Markov models of transport based on the partition of phase space into resonances. The transition probabilities are given by turnstile overlap areas. The master equation has a Bloch band spectrum. A general exact expression for the diffusion coefficient D is derived. The behavior of D is examined for the sawtooth map. We find a critical scaling law for D, extending a result of Cary and Meiss. The critical scaling emerges as a collective effect of many resonances, in contrast with the standard map.
| Original language | English |
|---|---|
| Pages (from-to) | 233-236 |
| Number of pages | 4 |
| Journal | Physical Review Letters |
| Volume | 62 |
| Issue number | 3 |
| DOIs | |
| State | Published - 1989 |
| Externally published | Yes |