TY - JOUR
T1 - The complex Ginzburg-Landau equation
T2 - An introduction
AU - García-Morales, Vladimir
AU - Krischer, Katharina
N1 - Funding Information:
The authors gratefully acknowledge Kathrin Kostorz and Lennart Schmidt for their comments on the manuscript. Financial support from the cluster of excellence Nanosystems Initiative Munich (NIM) is gratefully acknowledged. V.G.-M. acknowledges also financial support from the Technische Universität München – Institute for Advanced Study, funded by the German Excellence Initiative.
PY - 2012/3
Y1 - 2012/3
N2 - The complex Ginzburg-Landau equation (CGLE), probably the most celebrated nonlinear equation in physics, describes generically the dynamics of oscillating, spatially extended systems close to the onset of oscillations. Using symmetry arguments, this article gives an easy access to this equation and an introduction into the rich spatio-temporal behaviour it describes. Starting out from the familiar linear oscillator, we first show how the generic model for an individual nonlinear oscillator, the so-called Stuart-Landau equation, can be derived from symmetry arguments. Then, we extend our symmetry considerations to spatially extended systems, arriving at the CGLE. A comparison of diffusively coupled linear and nonlinear oscillators makes apparent the source of instability in the latter systems. A concise survey of the most typical patterns in 1D and 2D is given. Finally, more recent extensions of the CGLE are discussed that comprise external, time-periodic forcing as well as nonlocal and global spatial coupling.
AB - The complex Ginzburg-Landau equation (CGLE), probably the most celebrated nonlinear equation in physics, describes generically the dynamics of oscillating, spatially extended systems close to the onset of oscillations. Using symmetry arguments, this article gives an easy access to this equation and an introduction into the rich spatio-temporal behaviour it describes. Starting out from the familiar linear oscillator, we first show how the generic model for an individual nonlinear oscillator, the so-called Stuart-Landau equation, can be derived from symmetry arguments. Then, we extend our symmetry considerations to spatially extended systems, arriving at the CGLE. A comparison of diffusively coupled linear and nonlinear oscillators makes apparent the source of instability in the latter systems. A concise survey of the most typical patterns in 1D and 2D is given. Finally, more recent extensions of the CGLE are discussed that comprise external, time-periodic forcing as well as nonlocal and global spatial coupling.
KW - nonlinear physics
KW - oscillations
KW - resonant forcing
KW - spatial coupling
KW - spatially extended systems
KW - turbulence
UR - http://www.scopus.com/inward/record.url?scp=84857964225&partnerID=8YFLogxK
U2 - 10.1080/00107514.2011.642554
DO - 10.1080/00107514.2011.642554
M3 - Article
AN - SCOPUS:84857964225
SN - 0010-7514
VL - 53
SP - 79
EP - 95
JO - Contemporary Physics
JF - Contemporary Physics
IS - 2
ER -