We investigate the noise-induced transitions between the oscillatory s
teady slates of a class of weakly nonlinear oscillators excited by res
onant harmonic forcing. We begin by deriving a set of averaged equatio
ns governing slow variables of the system when the latter is perturbed
by both additive white Gaussian noise and by random phase fluctuation
s of the resonant excitation. We then examine in detail the behavior o
f the reduced system in the case of cubic stiffness and viscous dampin
g forces. Three regimes are examined: the case of weak damping, the ca
se of near-bifurcation and the more general case when neither of the f
irst two situations apply, la each case we predict the quasi-stationar
y probability density of the response and the mean time taken by the t
rajectories to pass from one basin of attraction to the other. These t
heoretical predictions are based on averaging of a near-Hamiltonian sy
stem in the weak damping limit, on center-manifold theory in the near-
bifurcation case, or on Wentzell-Kramers-Brillouin (WKB) singular pert
urbation expansions in the more general case. These predictions are co
mpared with digital simulations which show excellent agreement We can
then determine the probability of a transition for each state and for
all parameter values. For this, we compute contour curves of the activ
ation energy of each attractor in the parameter plane to yield a compl
ete picture of the survivability of the system subject to random pertu
rbations.