2014
DOI: 10.1587/nolta.5.252
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Basin-filling Peano omega-branches and structural stability of a chaotic attractor

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Cited by 5 publications
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“…Instead, chaotic attractors have physical reality in the sense that their geometrical structures can be reproducibly observed with a probability of unity. These observations appear to be consistent with Ueda's theory of chaos [13,14], wherein chaotic dynamical behavior represents a manifestation of random transitions, triggered by experimental perturbations or numerical roundoff, between (infinitely many) unstable periodic orbits accompanying (infinitely many) homoclinic points in the chaotic attractors [15]. Ueda referred to such dynamical behavior as randomly transitional oscillations [13].…”
Section: Introductionsupporting
confidence: 77%
“…Instead, chaotic attractors have physical reality in the sense that their geometrical structures can be reproducibly observed with a probability of unity. These observations appear to be consistent with Ueda's theory of chaos [13,14], wherein chaotic dynamical behavior represents a manifestation of random transitions, triggered by experimental perturbations or numerical roundoff, between (infinitely many) unstable periodic orbits accompanying (infinitely many) homoclinic points in the chaotic attractors [15]. Ueda referred to such dynamical behavior as randomly transitional oscillations [13].…”
Section: Introductionsupporting
confidence: 77%