-
1
-
-
12944275674
-
-
10.1103/PhysRevLett.85.461.
-
Schreiber T. Phys. Rev. Lett. 2000, 85:461. 10.1103/PhysRevLett.85.461.
-
(2000)
Phys. Rev. Lett.
, vol.85
, pp. 461
-
-
Schreiber, T.1
-
2
-
-
36148985016
-
-
10.1103/PhysRevLett.99.204101
-
Frenzel S. Pompe B. Phys. Rev. Lett. 2007, 99:204101. 10.1103/PhysRevLett.99.204101, and.
-
(2007)
Phys. Rev. Lett.
, vol.99
, pp. 204101
-
-
Frenzel, S.1
Pompe, B.2
-
11
-
-
78049318729
-
Phase coupling estimation from multivariate phase statistics
-
10.1162/NECO_a_00048, and
-
Cadieu C.F. Koepsell K. Phase coupling estimation from multivariate phase statistics. Neural Comput. 2010, 22(12):3107. 10.1162/NECO_a_00048, and .
-
(2010)
Neural Comput.
, vol.22
, Issue.12
, pp. 3107
-
-
Cadieu, C.F.1
Koepsell, K.2
-
13
-
-
37649029497
-
-
10.1103/PhysRevE.67.055201
-
Paluŝ M. Stefanovska A. Phys. Rev. E 2003, 67:055201. 10.1103/PhysRevE.67.055201, and.
-
(2003)
Phys. Rev. E
, vol.67
, pp. 055201
-
-
Paluŝ, M.1
Stefanovska, A.2
-
14
-
-
40549145872
-
-
10.1103/PhysRevE.77.026214
-
Vejmelka M. Paluš M. Phys. Rev. E 2008, 77:026214. 10.1103/PhysRevE.77.026214, and.
-
(2008)
Phys. Rev. E
, vol.77
, pp. 026214
-
-
Vejmelka, M.1
Paluš, M.2
-
18
-
-
0344118112
-
-
10.1143/PTPS.150.22
-
Cimponeriu L. Rosenblum M.G. Fieseler T. Dammers J. Schiek M. Majtanik M. Morosan P. Bezerianos A. Tass P.A. Prog. Theor. Phys. Suppl. 2003, 150:22. 10.1143/PTPS.150.22, and.
-
(2003)
Prog. Theor. Phys. Suppl.
, vol.150
, pp. 22
-
-
Cimponeriu, L.1
Rosenblum, M.G.2
Fieseler, T.3
Dammers, J.4
Schiek, M.5
Majtanik, M.6
Morosan, P.7
Bezerianos, A.8
Tass, P.A.9
-
24
-
-
84958264229
-
-
See for "The matlab implementation of the algorithms."
-
See for "The matlab implementation of the algorithms.".
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-
-
-
28
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-
84958264231
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The coupling strength ε should be smaller than the absolute values of negative Lyapunov exponents of the limit cycles. Physically, it means that the deviations of the motion of each system from its limit cycle can be considered as enslaved by the phase dynamics.
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The coupling strength ε should be smaller than the absolute values of negative Lyapunov exponents of the limit cycles. Physically, it means that the deviations of the motion of each system from its limit cycle can be considered as enslaved by the phase dynamics.
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29
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84958264232
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Note
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In case of a cross-coupling, the terms, depending on three and more phases, appear already in the first approximation in ε.
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-
30
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0000248127
-
-
10.1103/PhysRevLett.81.3291
-
Tass P. Rosenblum M.G. Weule J. Kurths J. Pikovsky A.S. Volkmann J. Schnitzler A. Freund H.-J. Phys. Rev. Lett. 1998, 81:3291. 10.1103/PhysRevLett.81.3291, and.
-
(1998)
Phys. Rev. Lett.
, vol.81
, pp. 3291
-
-
Tass, P.1
Rosenblum, M.G.2
Weule, J.3
Kurths, J.4
Pikovsky, A.S.5
Volkmann, J.6
Schnitzler, A.7
Freund, H.-J.8
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