Titlebook: Solitons and Chaos; Ioannis Antoniou,Franklin J. Lambert Conference proceedings 1991 Springer-Verlag Berlin Heidelberg 1991 Chaos.Integrab

五行打油詩

波動

Integrable Supersymmetric Models and Phase Transitions in One Dimensioncal mechanics [1]. In the last cases anticomm Ling variables are first introduced for pure combinatorical reasons, to replace the N→O replica trick. But one might expect the supersymmetry in condensed matter physics to arise as a relation between fermionic and bosonic excitations. Recently there hav

Creatinine-Test

Neonatal

Transition to Turbulence in 1-D Rayleigh-Bénard Convectionh depends on one space variable, may destabilize and become turbulent when a control parameter is varied. The spatio-temporal chaos observed thus stands between the deterministic chaos of confined systems and the developped turbulence of extended ones. Much theoretical and numerical work was devoted

Dictation

隱語

Spatial Coherent Structures in Dissipative Systemsell as in studies of model equations [5–9]. They consist of finite domains in which the system is in one state embedded in a background consisting of another state. These . solitary waves can appear in a uniform environment and their characteristic properties (width, frequency, ...) are entirely det

octogenarian

Conference proceedings 1991 a wide range of topics butshare common mathematical notions and investigationtechniques. An introductory note on eight conceptsofintegrability has been added as a guide for the uninitiatedreader.Both specialists and graduate students will findthis update on the state ofthe art useful.Key points: ch

性滿足

Heisenberg Ferromagnet, Generalized Coherent States and Nonlinear Behaviour solved exactly. Nowadays hamiltonian (1) is of a great interest both from the application point of view and from that of mathematical physics. Indeed, we shall see in what follows that the system governed by (1) displays many interesting and even intriguing features.

占卜者

Flawless

Spatial Coherent Structures in Dissipative Systemsanother state. These . solitary waves can appear in a uniform environment and their characteristic properties (width, frequency, ...) are entirely determined by the parameters of the system. The term . [10] has been coined to characterize these patterns.