Stochastic Resonance in a Bistable System Subject to Non-Gaussian and Gaussian Noises

In this paper,we consider the phenomenon of stochastic resonance(SR)in a quartic bistable system underthe simultaneous action of a multiplicative non-Gaussian and an additive Gaussian noises and a weak periodic signalThe expression of the signal-to-noise ratio R is derived by applying the two-state theory in adiabatic limit.We discussthe effects of the parameter q indicating the departure of the non-Gaassian noise from the Gaussian noise,the correlationtime Τ of the non-Gaussian noise,and coupling intensity λ between two noise terms on the stochastic resonance.It isfound that the signal-to-noise ratio of the system,as a function of the additive noise intensity,undergoes the transitionfrom having one peak to having two peaks,and then to having one peak again when the parameter q or the noisecorrelation time Τ is increased.The parameter q and Τ play opposite roles in the SR of the system.

In this paper, we consider the phenomenon of stochastic resonance （SR） in a quartic bistable system under the simultaneous action of a multiplicative non-Gaussian and an additive Gaussian noises and a weak periodic signal. The expression of the signal-to-noise ratio R is derived by applying the two-state theory in adiabatic limit. We discuss the effects of the parameter q indicating the departure of the non-Gaussian noise from the Gaussian noise, the correlation time r of the non-Gaussian noise, and coupling intensity A between two noise terms on the stochastic resonance. It is found that the signM-to-noise ratio of the system, as a function of the additive noise intensity, undergoes the transition from having one peak to having two peaks, and then to having one peak again when the parameter q or the noise correlation time τ is increased. The parameter q and τ play opposite roles in the SR of the system.