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Volumn 60, Issue 6, 1999, Pages 6402-6406

Nonequilibrium noise in coupled phase oscillators

Author keywords

[No Author keywords available]

Indexed keywords

ARTICLE;

EID: 0001551482     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.60.6402     Document Type: Article
Times cited : (72)

References (17)
  • 1
    • 0343684694 scopus 로고
    • C. Vidal, A. Pacault, Springer, Berlin Nonequilibrium Dynamics in Chemical Systems ibid 1981;
    • G. Nicolis and I. Prigogine, Self Organization in Nonequilibrium Systems, edited by C. Vidal and A. Pacault (Springer, Berlin, 1981);Nonequilibrium Dynamics in Chemical Systems, ibid 1981
    • (1981) Self Organization in Nonequilibrium Systems
    • Nicolis, G.1    Prigogine, I.2
  • 4
    • 0003886783 scopus 로고
    • Springer, Berlin S.H. Strogatz in Frontiers in Mathematical Biology, edited by S. Levine (Springer, Berlin, 1994), and further references therein
    • Y. Kuramoto, Chemical Oscillations, Waves, and Turbulence (Springer, Berlin, 1984);S.H. Strogatz in Frontiers in Mathematical Biology, edited by S. Levine (Springer, Berlin, 1994), and further references therein.
    • (1984) Chemical Oscillations, Waves, and Turbulence
    • Kuramoto, Y.1
  • 5
    • 85036422429 scopus 로고    scopus 로고
    • Since the unperturbed frequencies (Formula presented) are not required to be large in comparison with the interaction and the noise in (1), a transformation to an effective state-independent noise by “phase-averaging” 2 is not possible in our case. We further note that the factor (Formula presented) in (2) can equivalently be absorbed as “multiplicative noise” (Formula presented) in (1). The latter is to be understood in the physically relevant sense of Stratonovich 5
    • Since the unperturbed frequencies (Formula presented) are not required to be large in comparison with the interaction and the noise in (1), a transformation to an effective state-independent noise by “phase-averaging” 2 is not possible in our case. We further note that the factor (Formula presented) in (2) can equivalently be absorbed as “multiplicative noise” (Formula presented) in (1). The latter is to be understood in the physically relevant sense of Stratonovich 5.
  • 13
    • 85036386787 scopus 로고    scopus 로고
    • Note that Q can be absorbed into the time-scale in (1), thus (Formula presented) depends only on (Formula presented) and (Formula presented)
    • Note that Q can be absorbed into the time-scale in (1), thus (Formula presented) depends only on (Formula presented) and (Formula presented)
  • 17
    • 85036400634 scopus 로고    scopus 로고
    • For (Formula presented) it can be shown rigorously that (Formula presented)
    • For (Formula presented) it can be shown rigorously that (Formula presented)


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