Classical limit of quantum chaos
β Scribed by Mario Feingold; Nimrod Moiseyev; Asher Peres
- Publisher
- Elsevier Science
- Year
- 1985
- Tongue
- English
- Weight
- 300 KB
- Volume
- 117
- Category
- Article
- ISSN
- 0009-2614
No coin nor oath required. For personal study only.
β¦ Synopsis
When a quantum system has a ciassieally chaotic analog, the expce~atlon value (E[AlE> of any dynamical variable A. for an energy eigenstare IE). lends to tie ciassiul microcanonical average of the analog variable A. 01 the Same energy E Some numerical examples are discti. Although there is no consensus on the definition ornature ofquantum chaos, nor even on its existence, there appears to be a growing body of theoretical [l-71 and numerical [S-12] evidence in support of the followmg property: If a quantum system has a classically chaotic analog, then, in the semiclassical limit fi --f 0, the energy eigenfunctions fill the entire accessible phase space and, moreover, their Wigner distributions [13] ffuctuate around the classical microcanonical phase space density. * This result was pre&ctcd by Berry 1261. An interesting problem, which we did not solve, is to estimate the deviahon of the. quantum results from the classical ones. It probably behawx as a power of 7l_ 346
π SIMILAR VOLUMES
In this paper a formulation of classical mechanics is given with the help of linear operators in HILBERT space, which is different from the formalism of v. NEUMANN and KOOPMAN, i.e. the observables are represented by selfadjoint operators instead of real functions. It is shown that classical mechani