메뉴 건너뛰기




Volumn 212, Issue 3-4, 2005, Pages 216-232

Non-transitive maps in phase synchronization

Author keywords

Chaotic phase synchronization; Ergodic Theory; Temporal mappings

Indexed keywords

CHAOS THEORY; OSCILLATORS (ELECTRONIC); REAL TIME SYSTEMS; VECTORS;

EID: 28244433132     PISSN: 01672789     EISSN: None     Source Type: Journal    
DOI: 10.1016/j.physd.2005.10.003     Document Type: Article
Times cited : (17)

References (35)
  • 2
    • 0033609387 scopus 로고    scopus 로고
    • Nature 399 1999 354
    • (1999) Nature , vol.399 , pp. 354
  • 18
    • 28244490111 scopus 로고    scopus 로고
    • note
    • Phase can be defined as a Hilbert transformation of a trajectory component, as the angle of a trajectory point into a special projection of the attractor, as a function that grows by 2 π every time the chaotic trajectory crosses some specific surface, or as the angle of the projected vector field into some subspace with respect to some rotation point
  • 20
    • 28244433016 scopus 로고    scopus 로고
    • note
    • A chaotic set is always transitive through the flow. So, given a set of initial conditions, its evolution through the flow eventually reaches arbitrary open subsets of the original chaotic attractor. However, the conditional Poincaré map might not possess the transitive property. That is, given a set of initial conditions, its evolution through this map might not reach arbitrary open subsets of the special projections of the chaotic attractor; its dynamics stay confined to a subset of the attractor
  • 21
    • 28244478771 scopus 로고    scopus 로고
    • note
    • The results presented here for the sinusoidally forced Chua circuit were also verified in the sinusoidally forced Rössler oscillator
  • 24
    • 28244439675 scopus 로고    scopus 로고
    • note
    • r is considered to be rational. However, as shown in Ref. [23], PS, as defined by the boundedness of the phase difference, was found in two chaotic systems for a finite but very large time interval as r approaches an irrational. Therefore, although in this work we consider r to be rational, we should make the remark that, for the special situation such as that presented in Ref. [23], Eq. (6) can only be satisfied for a finite but large time if r is considered to be irrational
  • 26
    • 28244444356 scopus 로고    scopus 로고
    • note
    • The intermittency observed in the phase difference is characterized as a usual intermittency by the alternation between a laminar regime and a burst regime. If the phase difference remains bounded in the interval [ 0, 〈 Δ φ 1 〉 ], we say that we have a laminar regime. If the phase difference leaves this interval, we have a burst, also known as phase slip. As one approaches the border between the PS and the non-PS region, the laminar regime in the phase difference becomes longer
  • 27
    • 28244437431 scopus 로고    scopus 로고
    • note
    • The choice of these time intervals is not unique. It depends on what type of event one wants to identify in the system. A length-1 basic set is constructed by measuring time intervals between the occurrence of two events of the same type. A length-2 basic set is constructed by measuring the time interval between the occurrence of an event A and the occurrence of an event B, and then between the event B and finally the event A, and so on


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.