It is nice to know that the computer understands the problem.
But I would like to understand it, too. EUGENE P. WIGNER Physics Today 46 (1993) 38 |
The kicked rotor plays a key role in the field of quantum chaos. On the one hand the 1979 paper by CASATI, CHIRIKOV, IZRAELEV and FORD [CCIF79] marks the starting point of the systematic analysis of the quantum dynamics of classically chaotic dynamical systems; in this study characteristic differences between the classical and quantum behaviours of the same model systems were found for the first time. In particular, the numerical investigation of the quantum kicked rotor for certain parameter values clearly yielded localized quantum states, whereas the classical counterpart of the system exhibited unbounded diffusive dynamics with respect to the energy in sharp contrast to the quantum result that established an upper limit for the energy.
On the other hand, the theoretical explanation of this observation was given in 1982 by FISHMAN, GREMPEL and PRANGE [FGP82,GFP82,PGF83], who showed that the quantum kicked rotor can be mapped onto a well-known model of solid state physics. This model, the ANDERSON model [And58,And61,And78], is characterized by pronounced localization phenomena of the quantum states, provided certain conditions are met that I discuss below. Localization in the ANDERSON model thus carries over to the quantum kicked rotor and provides the desired explanation.
In the present chapter I analyze the
nonresonant
(with respect to )
quantum kicked harmonic oscillator
along
lines similar to those
sketched above with respect to the quantum kicked
rotor. In this way,
by making contact between the quantum kicked harmonic oscillator and the
ANDERSON model,
I provide a novel theoretical explanation for the
suppressed diffusion that
is
numerically found to be typical for the quantum dynamics
in the absence of stochastic
webs as discussed in the previous chapter.
Section 5.1 is dedicated to the exposition of the
theory of ANDERSON localization
in its well-established area of application, the quantum kicked
rotor. In this context I also briefly summarize the most important
properties of the ANDERSON model of disordered solids, as far as
these properties are needed for the present discussion.
In section 5.2 I present
numerical
evidence for localization phenomena in the quantum kicked harmonic
oscillator
for nonresonant values of , i.e. in the absence of
quantum stochastic webs as discussed in the previous chapter.
In section 5.3 I then show analytically that the
nonresonant
quantum kicked oscillator exhibits ANDERSON localization.