Hopf bifurcation with additive noise

Autor: Maximilian Engel, Martin Rasmussen, Thai Son Doan, Jeroen S. W. Lamb
Přispěvatelé: Engineering & Physical Science Research Council (EPSRC), Commission of the European Communities
Rok vydání: 2018
Předmět:
RANDOM DIFFEOMORPHISMS
Dynamical systems theory
37C75
37D45
37G35
37H10
37H15

random attractor
General Mathematics
Mathematics
Applied

General Physics and Astronomy
dichotomy spectrum
Dynamical Systems (math.DS)
Lyapunov exponent
01 natural sciences
symbols.namesake
0102 Applied Mathematics
0103 physical sciences
Attractor
FOS: Mathematics
Hopf bifurcation
Mathematics - Dynamical Systems
0101 mathematics
STOCHASTIC DUFFING-VAN
Mathematical Physics
Mathematics
Science & Technology
Applied Mathematics
Physics
random dynamical system
Probability (math.PR)
010102 general mathematics
Mathematical analysis
Statistical and Nonlinear Physics
White noise
Nonlinear Sciences::Chaotic Dynamics
Physics
Mathematical

stochastic bifurcation
EQUILIBRIUM
Ordinary differential equation
Physical Sciences
symbols
ATTRACTOR
010307 mathematical physics
DYNAMICAL-SYSTEMS
Random dynamical system
Mathematics - Probability
Linear stability
Popis: We consider the dynamics of a two-dimensional ordinary differential equation exhibiting a Hopf bifurcation subject to additive white noise and identify three dynamical phases: (I) a random attractor with uniform synchronisation of trajectories, (II) a random attractor with non-uniform synchronisation of trajectories and (III) a random attractor without synchronisation of trajectories. The random attractors in phases (I) and (II) are random equilibrium points with negative Lyapunov exponents while in phase (III) there is a so-called random strange attractor with positive Lyapunov exponent. We analyse the occurrence of the different dynamical phases as a function of the linear stability of the origin (deterministic Hopf bifurcation parameter) and shear (amplitude-phase coupling parameter). We show that small shear implies synchronisation and obtain that synchronisation cannot be uniform in the absence of linear stability at the origin or in the presence of sufficiently strong shear. We provide numerical results in support of a conjecture that irrespective of the linear stability of the origin, there is a critical strength of the shear at which the system dynamics loses synchronisation and enters phase (III).
Databáze: OpenAIRE