  A quantum system can be driven by either sinusoidal, rectangular, or noisy
signals. In the literature, these regimes are referred to as
Landau-Zener-Stuckelberg-Majorana (LZSM) interferometry, latching modulation,
and motional averaging, respectively. We demonstrate that these pronounced and
interesting effects are also inherent in the dynamics of classical two-state
systems. We discuss how such classical systems are realized using either
mechanical, electrical, or optical resonators. In addition to the fundamental
interest of such dynamical phenomena linking classical and quantum physics, we
believe that these are attractive for the classical analogue simulation of
quantum systems.
