2005
DOI: 10.1007/bf02704570
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Homoclinic bifurcation in Chua’s circuit

Abstract: Abstract. We report our experimental observations of the Shil'nikov-type homoclinic chaos in asymmetry-induced Chua's oscillator. The asymmetry plays a crucial role in the related homoclinic bifurcations. The asymmetry is introduced in the circuit by forcing a DC voltage. For a selected asymmetry, when a system parameter is controlled, we observed transition from large amplitude limit cycle to homoclinic chaos via a sequence of periodic mixed-mode oscillations interspersed by chaotic states. Moreover, we obser… Show more

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Cited by 30 publications
(8 citation statements)
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“…The time spent during spiraling out varies and it depends on how close the reinjected trajectory reaches a vicinity of the saddle focus and thereby it makes a large variation in the number of small oscillations that makes irregular return time of the large events. A tendency to develop a homoclinic chaos with a local instability of the saddle focus is seen here, but the typical global stability of homoclinic chaos [39] is never achieved due to the presence of a channel like structure. The trajectory revolves around the saddle focus for quite some time due to local instability (attracted along the stable eigendirection, pushed away along the unstable eigenplane of the saddle focus) while a globally instability due to the channel-like structure induces a variation of the return path (global excursion) of the trajectory making a wide variation in both the amplitude and return time of large spikes.…”
Section: Complex Dynamics Of Enso Modelmentioning
confidence: 67%
“…The time spent during spiraling out varies and it depends on how close the reinjected trajectory reaches a vicinity of the saddle focus and thereby it makes a large variation in the number of small oscillations that makes irregular return time of the large events. A tendency to develop a homoclinic chaos with a local instability of the saddle focus is seen here, but the typical global stability of homoclinic chaos [39] is never achieved due to the presence of a channel like structure. The trajectory revolves around the saddle focus for quite some time due to local instability (attracted along the stable eigendirection, pushed away along the unstable eigenplane of the saddle focus) while a globally instability due to the channel-like structure induces a variation of the return path (global excursion) of the trajectory making a wide variation in both the amplitude and return time of large spikes.…”
Section: Complex Dynamics Of Enso Modelmentioning
confidence: 67%
“…fundamental features of spiking and bursting in a neuron. Bursting is also observed in physical systems like CO 2 lasers [12], an asymmetric Chua oscillator [13] and forced Josephson junctions [14].…”
Section: Introductionmentioning
confidence: 93%
“…3 are strongly dependent on initial conditions. 47,48 It should be emphasized that we only considered the autonomous case of the Chua's circuit with a piecewise linear element. Other variants of the Chua's circuit with smooth nonlinearity and/or forcing functions, e.g., the MLC non-autonomous circuit 49 can have very rich varieties of dynamical phenomena and several ubiquitous routes to chaos such as quasiperiodicity, intermittency, period doubling, period-adding Farey sequence, and others.…”
Section: The Chua's Circuitmentioning
confidence: 99%