Numerical studies were performed for a system of two vibrational modes
coupled by two Fermi resonances in order to investigate its classical
and quantum chaotic behavior. Thirteen different expressions were use
d for the second Fermi resonance Hamiltonian. Examination of the stati
stical properties of the spectra showed that, when treated quantum mec
hanically, this model differs substantially from random matrices becau
se (i) the first Fermi resonance is integrable and its nondiagonal ter
ms cannot create level repulsion, spacing correlations, etc. and (ii)
for the same value of the coupling strength, each coupling Hamiltonian
has a different ability to induce quantum chaos, depending on its exp
ression and on the levels it connects. Computation of the largest Lyap
unov exponent for trajectories in the classical phase space showed tha
t the quantum and the classical systems behave similarly: the quicker
a coupling Hamiltonian induces quantum chaos, the quicker the trajecto
ries become unstable in the classical phase space.