2001
DOI: 10.1002/cta.141
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A systematic procedure for synthesizing two‐terminal devices with polynomial non‐linearity

Abstract: SUMMARYIn this paper, a systematic procedure for synthesizing two-terminal devices with polynomial non-linearity is proposed. A two-terminal, or one-port, device with an arbitrary polynomial non-linearity can be designed using the proposed procedure in a step-by-step systematic manner. A variety of drivingpoint characteristics of two-terminal devices with synthesized polynomial non-linearity, both numerically calculated and experimentally measured, are demonstrated.

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Cited by 6 publications
(3 citation statements)
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“…Due to the fundamental properties of the chaotic signals each chaotic oscillator contains at least one energy source and one nonlinear element. Thus, with a view to achieving simplicity, it could be a good idea to combine both requirements and implement it as a single active two-port device [99], [100].…”
Section: Description Of Sub-circuitsmentioning
confidence: 99%
“…Due to the fundamental properties of the chaotic signals each chaotic oscillator contains at least one energy source and one nonlinear element. Thus, with a view to achieving simplicity, it could be a good idea to combine both requirements and implement it as a single active two-port device [99], [100].…”
Section: Description Of Sub-circuitsmentioning
confidence: 99%
“…Of course, it is also possible to build both analog networks provided in Figure 1 directly. Instead of nonlinear two-ports we must construct a couple of resistors with polynomial AVC; systematic design towards these network elements can be found in [39,40]. Circuitry realization of original MVMS with state vector x = (v 1 , v 2 , i) T is demonstrated by means of Figure 10; i.e., the state variables are voltages across grounded capacitors and current flowing through the inductor.…”
Section: Circuitry Realization Of Mvms-based Chaotic Oscillatorsmentioning
confidence: 99%
“…This resistor can be piecewise linear; for example, where a third-order admittance network contains both capacitors and inductors as functional accumulation elements is provided in [ 1 ], while an RC passive ladder network connected as a load for active nonlinear resistors is the primary subject of [ 2 ]. Polynomial resistors with arbitrary degrees [ 3 ] can be connected in parallel with a third-order fully passive admittance network to obtain a robust chaotic oscillator [ 4 , 5 ] as well. Moreover, higher-order polynomial resistors can be used to approximate goniometric functions and connected as the fundamental nonlinearity inside suitable circuit topology to generate the so-called multiscroll [ 6 , 7 , 8 ] or multigrid strange attractors [ 9 , 10 ].…”
Section: Introductionmentioning
confidence: 99%