A new class of chaotic circuit

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Adaptive backstepping control, synchronization and circuit simulation of a 3-D novel jerk chaotic system with two hyperbolic sinusoidal nonlinearities (2014, background): “x +Aẍ+ ẋ = G(x), (3) where G is a nonlinear function having some special properties [69].”
Finite-time synchronization of complex networks with nonidentical discontinuous nodes (2013, methodology): “They include almost all the well-known chaotic systems with discontinuous functions, such as discontinuous Sprott circuit [42], discontinuous Chua circuit [32, 43], discontinuous Chen system [44], and neural networks with discontinuous activation functions [31, 35].”
Chaotic hyperjerk systems (2006, neutral): “One particularly simple example of such a system is [7,8] d(3)x dt3 þ a d (2)x dt2 þ dx dt 1⁄4 gðxÞ ð2Þ”
Algebraically Simple Chaotic Flows (2000, background): “One of the active integrators can be replaced with a passive integrator, and one of the diodes can be eliminated, resulting in a circuit with fifteen components rather than eighteen [50].”
Chaos in fractional-order autonomous nonlinear systems (2003, methodology): “focus on two types of autonomous chaotic systems that are of practical interest: an electronic chaotic oscillator model [10], and a mechanical chaotic ‘‘jerk’’ model [11,12].”