433 related articles for article (PubMed ID: 25679700)
1. Generalized Lyapunov exponent as a unified characterization of dynamical instabilities.
Akimoto T; Nakagawa M; Shinkai S; Aizawa Y
Phys Rev E Stat Nonlin Soft Matter Phys; 2015 Jan; 91(1):012926. PubMed ID: 25679700
[TBL] [Abstract][Full Text] [Related]
2. Subexponential instability in one-dimensional maps implies infinite invariant measure.
Akimoto T; Aizawa Y
Chaos; 2010 Sep; 20(3):033110. PubMed ID: 20887050
[TBL] [Abstract][Full Text] [Related]
3. Lyapunov exponents from unstable periodic orbits.
Franzosi R; Poggi P; Cerruti-Sola M
Phys Rev E Stat Nonlin Soft Matter Phys; 2005 Mar; 71(3 Pt 2A):036218. PubMed ID: 15903557
[TBL] [Abstract][Full Text] [Related]
4. An Improved Calculation Formula of the Extended Entropic Chaos Degree and Its Application to Two-Dimensional Chaotic Maps.
Inoue K
Entropy (Basel); 2021 Nov; 23(11):. PubMed ID: 34828209
[TBL] [Abstract][Full Text] [Related]
5. The largest Lyapunov exponent of chaotic dynamical system in scale space and its application.
Liu HF; Yang YZ; Dai ZH; Yu ZH
Chaos; 2003 Sep; 13(3):839-44. PubMed ID: 12946175
[TBL] [Abstract][Full Text] [Related]
6. Exact invariant measures: How the strength of measure settles the intensity of chaos.
Venegeroles R
Phys Rev E Stat Nonlin Soft Matter Phys; 2015 Jun; 91(6):062914. PubMed ID: 26172779
[TBL] [Abstract][Full Text] [Related]
7. Noise-induced unstable dimension variability and transition to chaos in random dynamical systems.
Lai YC; Liu Z; Billings L; Schwartz IB
Phys Rev E Stat Nonlin Soft Matter Phys; 2003 Feb; 67(2 Pt 2):026210. PubMed ID: 12636779
[TBL] [Abstract][Full Text] [Related]
8. Analysis of Chaotic Dynamics by the Extended Entropic Chaos Degree.
Inoue K
Entropy (Basel); 2022 Jun; 24(6):. PubMed ID: 35741547
[TBL] [Abstract][Full Text] [Related]
9. Separation of trajectories and its relation to entropy for intermittent systems with a zero Lyapunov exponent.
Korabel N; Barkai E
Phys Rev E Stat Nonlin Soft Matter Phys; 2010 Jul; 82(1 Pt 2):016209. PubMed ID: 20866709
[TBL] [Abstract][Full Text] [Related]
10. Lyapunov exponent of ion motion in microplasmas.
Gaspard P
Phys Rev E Stat Nonlin Soft Matter Phys; 2003 Nov; 68(5 Pt 2):056209. PubMed ID: 14682873
[TBL] [Abstract][Full Text] [Related]
11. Lyapunov Exponent and Out-of-Time-Ordered Correlator's Growth Rate in a Chaotic System.
Rozenbaum EB; Ganeshan S; Galitski V
Phys Rev Lett; 2017 Feb; 118(8):086801. PubMed ID: 28282154
[TBL] [Abstract][Full Text] [Related]
12. Infinite ergodicity that preserves the Lebesgue measure.
Okubo KI; Umeno K
Chaos; 2021 Mar; 31(3):033135. PubMed ID: 33810722
[TBL] [Abstract][Full Text] [Related]
13. Exponential localization of singular vectors in spatiotemporal chaos.
Pazó D; López JM; Rodríguez MA
Phys Rev E Stat Nonlin Soft Matter Phys; 2009 Mar; 79(3 Pt 2):036202. PubMed ID: 19392030
[TBL] [Abstract][Full Text] [Related]
14. OBSERVING LYAPUNOV EXPONENTS OF INFINITE-DIMENSIONAL DYNAMICAL SYSTEMS.
Ott W; Rivas MA; West J
J Stat Phys; 2015 Dec; 161(5):1098-1111. PubMed ID: 28066028
[TBL] [Abstract][Full Text] [Related]
15. Lyapunov exponent diagrams of a 4-dimensional Chua system.
Stegemann C; Albuquerque HA; Rubinger RM; Rech PC
Chaos; 2011 Sep; 21(3):033105. PubMed ID: 21974640
[TBL] [Abstract][Full Text] [Related]
16. Hydrodynamic Lyapunov modes and strong stochasticity threshold in the dynamic XY model: an alternative scenario.
Yang HL; Radons G
Phys Rev E Stat Nonlin Soft Matter Phys; 2008 Jan; 77(1 Pt 2):016203. PubMed ID: 18351922
[TBL] [Abstract][Full Text] [Related]
17. The transition between strong and weak chaos in delay systems: Stochastic modeling approach.
Jüngling T; D'Huys O; Kinzel W
Phys Rev E Stat Nonlin Soft Matter Phys; 2015 Jun; 91(6):062918. PubMed ID: 26172783
[TBL] [Abstract][Full Text] [Related]
18. Using recurrences to characterize the hyperchaos-chaos transition.
Souza EG; Viana RL; Lopes SR
Phys Rev E Stat Nonlin Soft Matter Phys; 2008 Dec; 78(6 Pt 2):066206. PubMed ID: 19256924
[TBL] [Abstract][Full Text] [Related]
19. Distinguishing chaos from noise by scale-dependent Lyapunov exponent.
Gao JB; Hu J; Tung WW; Cao YH
Phys Rev E Stat Nonlin Soft Matter Phys; 2006 Dec; 74(6 Pt 2):066204. PubMed ID: 17280136
[TBL] [Abstract][Full Text] [Related]
20. Strong and weak chaos in networks of semiconductor lasers with time-delayed couplings.
Heiligenthal S; Jüngling T; D'Huys O; Arroyo-Almanza DA; Soriano MC; Fischer I; Kanter I; Kinzel W
Phys Rev E Stat Nonlin Soft Matter Phys; 2013 Jul; 88(1):012902. PubMed ID: 23944533
[TBL] [Abstract][Full Text] [Related]
[Next] [New Search]
