It is show that the quantum relaxation process in a classically chaotic
open dynamical system is characterized by a quantum relaxation time
scale [95].
This scale is much shorter than the Heisenberg time and much larger than
the Ehrenfest time:
where
is the conductance
of the system and the exponent
is close to
. As a result,
quantum and classical decay probabilities remain close up to values
similarly to the case of
open disordered systems. The analysis of this behaviour was done for
the kicked rotator model with absorption which was introduced in [50].
Later this result was confirmed by methods of random
matrix theory (D.Savin and V.Sokolov) and by supersymmetry approach
(K.Frahm). This result can be also understand on the basis of weak
localization correction to diffusion in disordered
systems (A.Mirlin, B.Muzikantskii and D.Khmelnitskii).
In the chaotic regime the quantum eigenstates of nonunitary evolution operator reveal a fractal structure in the phase space [97] corresponding to a underlying classical strange repeller. An example of such fractal quantum eigenstate in Husimi representation is shown at the frontal page of this report (the color changes from red (maximal probability) to blue (zero probability)). It is conjectured that quantum strange attractors, once identified, should have a similar structure.
The quantum effects for Poincaré recurrences in divided
phase space (see sections 3.2.1 and 3.6.1) are investigated in [100].
It is shown that quantum effects modify the decay rate of Poincaré
recurrences in classical chaotic systems with hierarchical
structure of phase space.
The exponent
of
the algebraic decay
is shown to have the
universal value
due to tunneling and localization effects.
Experimental evidence of such decay should be observable in mesoscopic
systems, Rydberg and cold atoms.
This direction of research forms the basis of the thesis "Quantum chaos in open systems" of G.Maspero (Univ. of Milano at Como) finished in January 1999.