We study the time dependence of the ionization probability of Rydberg atoms
driven by a microwave field, both in classical and in quantum mechanics. T
he quantum survival probability follows the classical one up to the Heisenb
erg time and then decays algebraically as P(t) proportional to 1/t. This de
cay law derives from the exponentially long times required to escape from s
ome region of the phase space, due to tunneling and localization effects. W
e also provide parameter values which should allow one to observe such deca
y in laboratory experiments.