Quantum effects of the transition to chaos of an (almost) classical dynamical system are studied by renormalization-group methods. Planck's constant is a relevant variable which determines the time tₕ∝^-1γ at which the system crosses over to quantal behavior. The exponent γ is 6.039 for the limit of period-doubling bifurcations and is 3.04 for the disappearance of the final Kolmogorov-Arnold-Moser trajectory in the standard map. For the standard map the scaling of the energy diffusion coefficient is also calculated.
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Grempel et al. (1984) studied this question.
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