2001
DOI: 10.1142/s0129183101002073
|View full text |Cite
|
Sign up to set email alerts
|

Chaotic Behavior and Chaos Control for a Class of Complex Partial Differential Equations

Abstract: Systems of complex partial differential equations, which include the famous nonlinear Schrödinger, complex Ginzburg–Landau and Nagumo equations, as examples, are important from a practical point of view. These equations appear in many important fields of physics. The goal of this paper is to concentrate on this class of complex partial differential equations and study the fixed points and their stability analytically, the chaotic behavior and chaos control of their unstable periodic solutions. The presence of … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
4
1

Citation Types

0
15
0

Year Published

2003
2003
2017
2017

Publication Types

Select...
8

Relationship

1
7

Authors

Journals

citations
Cited by 17 publications
(15 citation statements)
references
References 11 publications
0
15
0
Order By: Relevance
“…[6][7][8][9][10] These systems have wide applications in physics, in areas as diverse as fluids, quantum mechanics, superconductivity, plasma physics, optical systems, astrophysics, and high-energy accelerators. 3,[11][12][13][14][15] Motivated by this more recent trend in research, and in line with previous work searching for simple systems of a given form that exhibit chaotic behavior, [16][17][18][19][20] this work began with a search for simple driven chaotic oscillators with a complex variable z, of the form ż + f͑z͒ = e i⍀t . This form is equivalent, with z = x + iy and f͑z͒ = u͑x , y͒ + iv͑x , y͒, where u and v are real functions, to the driven two-dimensional system, ẋ = − u͑x,y͒ + cos ⍀t, ͑1͒ ẏ = − v͑x,y͒ + sin ⍀t, which can be recast as the autonomous three-dimensional system, ẋ = − u͑x,y͒ + cos ⍀t, ẏ = − v͑x,y͒ + sin ⍀t, ͑2͒ ṫ = 1.…”
Section: Introductionmentioning
confidence: 99%
“…[6][7][8][9][10] These systems have wide applications in physics, in areas as diverse as fluids, quantum mechanics, superconductivity, plasma physics, optical systems, astrophysics, and high-energy accelerators. 3,[11][12][13][14][15] Motivated by this more recent trend in research, and in line with previous work searching for simple systems of a given form that exhibit chaotic behavior, [16][17][18][19][20] this work began with a search for simple driven chaotic oscillators with a complex variable z, of the form ż + f͑z͒ = e i⍀t . This form is equivalent, with z = x + iy and f͑z͒ = u͑x , y͒ + iv͑x , y͒, where u and v are real functions, to the driven two-dimensional system, ẋ = − u͑x,y͒ + cos ⍀t, ͑1͒ ẏ = − v͑x,y͒ + sin ⍀t, which can be recast as the autonomous three-dimensional system, ẋ = − u͑x,y͒ + cos ⍀t, ẏ = − v͑x,y͒ + sin ⍀t, ͑2͒ ṫ = 1.…”
Section: Introductionmentioning
confidence: 99%
“…In this field, several theoretical studies have been developed (involving nonlinear oscillators, often with periodic forcing) [31]- [33]. There are a number of applications in physics, in areas as diverse as fluids, quantum mechanics, superconductivity, plasma physics, optical systems, astrophysics, and high-energy accelerators, that can be described by this class of systems [29], [34], [35].…”
Section: B Complex-valued Chaotic Examplementioning
confidence: 99%
“…In recent years chaotic and hyperchaotic dissipative complex nonlinear systems have been proposed and studied in the literature [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16]18]. However, there also are many interesting cases of conservative complex nonlinear systems have not yet been as actively explored.…”
Section: Introductionmentioning
confidence: 99%