1995
DOI: 10.1103/physreve.52.115
|View full text |Cite
|
Sign up to set email alerts
|

Coupled map lattices as models of deterministic and stochastic differential delay equations

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

0
10
0

Year Published

1997
1997
2020
2020

Publication Types

Select...
4
3
1

Relationship

0
8

Authors

Journals

citations
Cited by 21 publications
(10 citation statements)
references
References 30 publications
0
10
0
Order By: Relevance
“…Thus the second eigenvalue of the product of the SPTOs reflects the contribution of the past activity to the present density as shown in Eq. (11). The modulus of the second eigenvalue shows an overall decreasing trend with increasing number of impulses and its angle alternates between 0 and π in the 2:1 stochastic phase-locking region.…”
Section: Numerical Resultsmentioning
confidence: 88%
See 1 more Smart Citation
“…Thus the second eigenvalue of the product of the SPTOs reflects the contribution of the past activity to the present density as shown in Eq. (11). The modulus of the second eigenvalue shows an overall decreasing trend with increasing number of impulses and its angle alternates between 0 and π in the 2:1 stochastic phase-locking region.…”
Section: Numerical Resultsmentioning
confidence: 88%
“…Markov operators have a wide range of applications; for example, they can be applied to analyses of coupled map lattices [11,12], nonlinear oscillators driven by stochastic inputs [5,6,13,14], neuronal dynamics [15][16][17][18][19][20][21], and neural networks [22]. * yamanobe@med.hokudai.ac.jp Markov operators can be constructed using stochastic kernels, which are transition densities corresponding to the given stochastic differential equations.…”
Section: Introductionmentioning
confidence: 99%
“…From a modeling perspective, the interaction of differential delay with noise leads one to study stochastic effects on infinite dimensional systems. In approximating the phase space, finite dimensional formulations based on coupled map lattices were use to initially examine approximations to steady state densities [16]. Here the authors employ a high dimensional Perron-Frobenius formulation to extract the density in the thermodynamic limit.…”
Section: Introductionmentioning
confidence: 99%
“…To properly understand the significance of the two quantities that we intend to calculate (information capacity and locking time), and understand how these two quantities can compete with each other, it is instructive to review the properties of the isolated tent map S(x), and, by simple a generalization, of the CML with = 0 (more information can be found in [5][6][7]). More specifically, we have that the dynamics of the tent map alone are characterized by a Lyapunov exponent equal to ln a.…”
mentioning
confidence: 99%
“…Thus, for 0 < a < 1, all orbits of the map converge to the unique fixed point x * = 0 independent of the value of the initial conditions, while for a = 1, all initial points of the map are fixed points. When 1 < a ≤ 2, the dynamics of the tent map switches abruptly to a chaotic regime (see Behind the chaotic behaviour of the temporal trajectory, the underlying regularity of the dynamics apparent in the banded structure of the bifurcation diagram is the signature of a property called statistical periodicity which can be observed in the density distribution of an ensemble of tent maps [2,6,7,9]. Specifically, for 2 1/2 1/(n+1) < a ≤ 2 1/2 1/n , the densities of the tent map have periodicity with period T = (n + 1) for n = 1, 2, · · · .…”
mentioning
confidence: 99%