Periodic orbits

Topics: Symbolic dynamics, Inverse quantum chaology, General approach to symbolic dynamics, Bifurcations

Symbolic dynamics

The Gutzwiller trace formula provides a fundamental relationship between the quantum mechanical density of states and a sum over all periodic orbits of the classical system.
Thus it is of vital importance to have a detailed knowledge of the periodic orbits of the system; usually this is achieved by finding a symbolic dynamics, i.e. an encoding of the dynamical system in terms of a (preferably) finite alphabet.

In the paper Symbolic dynamics and periodic orbits for the cardioid billiard a symbolic dynamics for the cardioid billiard with just two symbols was established. This allowed to determine all periodic orbits with up to 20 reflections, e.g.:

periodic orbits, cardioid billiard


Inverse quantum chaology

Using a Fourier transform of the quantum mechanical density of states the periodic orbits show up as peaks at the places of their geometric length L:

trace of the cosine modulated heat kernel, cardioid billiard

See the paper Spectral statistics in the quantized cardioid billiard for further details.

General approach to symbolic dynamics in billiards

More generally, one can prove that in a wide class of hyperbolic billiards with singularities a symbolic dynamics with a finite number of symbols can be found, see the paper Generating partitions for two-dimensional hyperbolic maps for details.

The result for example applies to the cardioid billiard, dispersing billiards and the stadium billiard. For the stadium billiard a symbolic dynamics with 16 symbols is obtained. Fortunately, this can be reduced to one with 5 symbols.
generating partition, stadium billiard


Periodic orbits and bifurcations in mixed systems

In systems with mixed phase space periodic orbits can bifurcate when one varies some external parameter. For the family of limaçon billiards this was studied in detail in the paper About ergodicity in the family of limaçon billiards. In addition to the question on the density of bifurcations and stability intervals it was demonstrated that arbitrarily close to the cardioid one can find stable periodic orbits.

Parameter of creation of AnBB orbits:
parameter at which AnBB is created


Example of an island close to the cardioid at ε=0.93395:
stability island near the cardioid


References:


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