# Random physics

Alberto Verga, research notebook


»chaos

The idea that the complex spectrum of heavy nucleons could be associated with a random (and correlated) distribution of levels given by the eigenvalues of a random matrix Hamiltonian, comes back to Wigner and Landau in the fifties:

From very general considerations one expects that levels with the same spin are distributed in such a way that the probability of a very small spacing will be very small—the levels act as though repelling each other. This problem merits investigation (Landau & Smorodinsky).

The important point about this idea is that it relates deterministic quantum systems (Hamiltonian) to a seemingly stochastic behavior (energy spectrum and eventually, dynamics). Random behavior of deterministic systems is usually referred as chaos.

However, the first investigations of chaos in quantum systems dealt with systems whose corresponding classical companions were chaotic. The question was about the existence (or not) of quantum signatures of classical chaos. This bridge between quantum and classical systems can be defined, in principle, only in the semiclassical limit. In fact even in this limit essential differences may arise: chaotic classical systems can correspond to regular quantum systems, and classical integrable systems may have irregular quantum counterparts. Two conjectures guided the early research for chaos in quantum systems:

• The level spacings distribution of a quantum system close to an integrable classical system, is Poissonian (Berry & Tabor).
• For quantum systems corresponding to chaotic classical systems, the irregular part of the spectrum is well described by the random matrix ensembles (Bohigas et al.).

We first investigate the relationship between classical and quantum chaos through the simple kicked rotator model. The kicked rotator exhibits a rich phenomenology, and in particular, contrary to the standard map in the global chaotic regime for which the particle undergoes a diffusive motion, the spreading of the quantum particle is stopped by a dynamical localization effect, analogous to the Anderson localization metal-insulator transition of a particle in a disordered potential. We end with a discussion of the random matrices ensembles, in order to relate the symmetry properties of the quantum hamiltonian to the statistical properties of its spectrum.