As recognized almost immediately following the design of the first laser [1, 2], lasers are
dynamical systems capable of exhibiting a wide variety of nonlinear dynamics. For many …

We report on the bifurcation analysis of an extended Hindmarsh–Rose (eHR) neuronal
oscillator. We prove that Hopf bifurcation occurs in this system, when an appropriate chosen …

By utilizing a memristor to substitute a coupling resistor in the realization circuit of a three-
dimensional chaotic system having one saddle and two stable node-foci, a novel memristive …

In recent years, tremendous research efforts have been devoted to simple chaotic oscillators
based on jerk equation that involves a third-time derivative of a single variable. In the …

Hidden attractors have received considerable interest in physics, mechanics and other
dynamical areas recently. This paper introduces a novel autonomous system with hidden …

In this contribution, a novel memristor-based oscillator, obtained from Shinriki's circuit by
substituting the nonlinear positive conductance with a first order memristive diode bridge, is …

A novel memristor-based oscillator derived from the autonomous jerk circuit (Sprott in IEEE
Trans Circuits Syst II Express Briefs 58: 240–243, 2011) is proposed. A first-order memristive …

In the present paper, a new memristor based oscillator is obtained from the autonomous
Jerk circuit [Kengne et al., Nonlinear Dynamics (2016) 83: 751̶765] by substituting the …

A new 4D chaotic system with infinitely many equilibria is proposed using a linear state
feedback controller in the Sprott C system. Although the new 4D chaotic system has only two …

We characterize the chaotic dynamics of semiconductor lasers subject to either optical or
electrooptical feedback modeled by Lang-Kobayashi and Ikeda equations, respectively. This …