In this paper, we focus on distinguishing between the types of dynamical
behavior that occur for typical one- and two-dimensional torus maps, in
particular without the assumption of invertibility. We use three fast and
accurate numerical methods: weighted Birkhoff averages, Farey trees, and
resonance orders. The first of these allows us to distinguish between chaotic
and regular orbits, as well as to calculate the frequency vectors for the
regular case to high precision. The second method allows us to distinguish
between the periodic and quasiperiodic orbits, and the third allows us to
distinguish among the quasiperiodic orbits to determine the dimension the
resulting attracting tori. We first consider the well-studied Arnold circle
map, comparing our results to the universal power law of Jensen and Ecke. We
next consider quasiperiodically forced circle maps, inspired by models
introduced by Ding, Grebogi, and Ott. We use the Birkhoff average to
distinguish between "strong" chaos (positive Lyapunov exponents) and "weak"
chaos (strange nonchaotic attractors). Finally, we apply our methods to 2D
torus maps, building on the work of Grebogi, Ott, and Yorke. We distinguish
incommensurate, resonant, periodic, and chaotic orbits and accurately compute
the proportions of each as the strength of the nonlinearity grows. We compute
generalizations of Arnold tongues corresponding to resonances and to periodic
orbits, and we show that chaos typically begins before the map becomes
noninvertible. We show that the proportion of nonresonant orbits does not obey
a universal power law like that seen in the 1D case.Comment: Keywords: Circle maps, Quasiperiodic forcing, Arnold tongues,
Resonance, Birkhoff averages, Strange nonchaotic attractor