Domain Structures in Fourth-Order Phase and Ginzburg-Landau EquationsIn pattern-forming systems, competition between patterns with different wave numbers can lead to domain structures, which consist of regions with differing wave numbers separated by domain walls. For…David Raitt, Hermann Riecke·Feb 18, 1994SaveLearn
SUSY-Based Variational Method for the Anharmonic OscillatorUsing a newly suggested algorithm of Gozzi, Reuter, and Thacker for calculating the excited states of one dimensional systems, we determine approximately the eigenvalues and eigenfunctions of the…Fred Cooper, John Dawson, Harvey Shepard·Feb 17, 1994SaveLearn
Structure And Dynamics Of Modulated Traveling Waves In Cellular FlamesWe describe spatial and temporal patterns in cylindrical premixed flames in the cellular regime, Le < 1, where the Lewis number Le is the ratio of thermal to mass diffusivity of a deficient…A. Bayliss, B. J. Matkowsky, H. Riecke·Feb 4, 1994SaveLearn
Front Structures in a Real Ginzburg-Landau Equation Coupled to a Mean FieldLocalized traveling wave trains or pulses have been observed in various experiments in binary mixture convection. For strongly negative separation ratio, these pulse structures can be described as…Henar Herrero, Hermann Riecke·Jan 28, 1994SaveLearn
Kink stability, propagation, and length scale competition in the periodically modulated sine-Gordon equationWe have examined the dynamical behavior of the kink solutions of the one-dimensional sine-Gordon equation in the presence of a spatially periodic parametric perturbation. Our study clarifies and…Angel Sanchez, A R Bishop, Francisco Dominguez-Adame·Jan 24, 1994SaveLearn
Domain Structures and Zig-Zag Patterns Modeled by a Fourth-Order Ginzburg-Landau EquationDomain walls between spatially periodic patterns with different wave numbers, can arise in pattern-forming systems with a neutral curve that has a double minimum. Within the framework of the phase…David Raitt, Hermann Riecke·Jan 24, 1994SaveLearn
Soliton solutions of the Hamiltonian DSI and DSIII equationsBy introducing generalized Backlund Transformations depending on arbitrary functions, wave and localized soliton solutions of the Davey- Stewartson equations are generated. Moreover explicit soliton…Flora Pempinelli·Jan 10, 1994SaveLearn
From Labyrinthine Patterns to Spiral TurbulenceA new mechanism for spiral vortex nucleation in nongradient reaction diffusion systems is proposed. It involves two key ingredients: An Ising-Bloch type front bifurcation and an instability of a…Aric Hagberg, Ehud Meron·Jan 5, 1994SaveLearn
Hydrothermal Surface-Wave Instability and the Kuramoto-Sivashinsky EquationWe consider a system formed by an infinite viscous liquid layer with a constant horizontal temperature gradient, and a basic nonlinear bulk velocity profile. In the limit of long-wavelength and large…R. A. Kraenkel, J. G. Pereira, M. A. Manna·Jan 4, 1994SaveLearn
Multiple Front Propagation into Unstable StatesThe dynamics of transient patterns formed by front propagation in extended nonequilibrium systems is considered. Under certain circumstances, the state left behind a front propagating into an…R. Montagne, A. Amengual, E. Hernandez-Garcia et al.·Dec 10, 1993SaveLearn
Dual Fronts Propagating into an Unstable StateThe interface between an unstable state and a stable state usually develops a single confined front travelling with constant velocity into the unstable state. Recently, the splitting of such an…F. J. Elmer, J. -P. Eckmann, G. Hartsleben·Nov 26, 1993SaveLearn
Solitons in the Camassa-Holm Shallow Water EquationWe study the class of shallow water equations of Camassa and Holm derived from the Lagrangian: $ L= ∫ ( 12 (φxxx-φx )φt - 1 2 (φx)3 - 1 …Fred Cooper, Harvey Shepard·Nov 22, 1993SaveLearn
Secondary Instabilities and Spatiotemporal Chaos in Parametric Surface WavesA two dimensional model is introduced to study pattern formation, secondary instabilities and the transition to spatiotemporal chaos (weak turbulence) in parametric surface waves. The stability of a…Wenbin Zhang, Jorge Vinals·Nov 19, 1993SaveLearn
D4+ T2 Mode Interactions and Hidden Rotational SymmetryBifurcation problems in which periodic boundary conditions or Neumann boundary conditions are imposed often involve partial differential equations that have Euclidean symmetry. As a result the normal…John David Crawford·Nov 14, 1993SaveLearn
Properties Of Solutions Of The Kpi EquationThe Kadomtsev--Petviashvili I (KPI) is considered as a useful laboratory for experimenting new theoretical tools able to handle the specific features of integrable models in 2+1 dimensions. The…M. Boiti, F. Fempinelli·Nov 12, 1993SaveLearn
Multidimensional Localized SolitonsRecently it has been discovered that some nonlinear evolution equations in 2+1 dimensions, which are integrable by the use of the Spectral Transform, admit localized (in the space) soliton solutions.…M. Boiti, L. Martina, F. Pempinelli·Nov 12, 1993SaveLearn
Oscillatory instability of crack propagations in quasi-static fractureCrack propagations in quasi-static fracture are studied theoretically. The Griffith theory is applied to discuss a crack extension condition and motion of crack tips in straight propagations.…Shin-ichi Sasa, Ken Sekimoto·Nov 5, 1993SaveLearn
On the existence of monotonic fronts for a class of physical problems described by the equation λu''' + u' = f(u)We obtain an upper bound on the value of λ for which monotonic front solutions of the equation λu''' + u' = f(u) with λ> 0 may exist.R. D. Benguria, M. C. Depassier·Nov 4, 1993SaveLearn
D4-symmetric Maps with Hidden Euclidean SymmetryBifurcation problems in which periodic boundary conditions (PBC) or Neumann boundary conditions (NBC) are imposed often involve partial differential equations that have Euclidean symmetry. In this…John David Crawford·Nov 2, 1993SaveLearn
Amplitude Expansions for Instabilities in Populations of Globally-Coupled OscillatorsWe analyze the nonlinear dynamics near the incoherent state in a mean-field model of coupled oscillators. The population is described by a Fokker-Planck equation for the distribution of phases, and…John David Crawford·Oct 28, 1993SaveLearn
Exact Solutions of the One-Dimensional Quintic Complex Ginzburg-Landau EquationExact solitary wave solutions of the one-dimensional quintic complex Ginzburg-Landau equation are obtained using a method derived from the Painlevé test for integrability. These solutions are…Philippe Marcq, Hugues Chate', Robert Conte·Oct 22, 1993SaveLearn
Temporal Forcing of Small-Amplitude Waves in Anisotropic SystemsWe investigate the effect of resonant temporal forcing on an anisotropic system that exhibits a Hopf bifurcation to obliquely traveling waves in the absence of this forcing. We find that the forcing…Hermann Riecke, Mary Silber, Lorenz Kramer·Oct 15, 1993SaveLearn
Thermodynamic Limit Of The Ginzburg-Landau EquationsWe investigate the existence of a global semiflow for the complex Ginzburg-Landau equation on the space of bounded functions in unbounded domain. This semiflow is proven to exist in dimension 1 and 2…P. Collet·Oct 14, 1993SaveLearn
Disordered Regimes of the one-dimensional complex Ginzburg-Landau equationI review recent work on the ``phase diagram'' of the one-dimensional complex Ginzburg-Landau equation for system sizes at which chaos is extensive. Particular attention is paid to a detailed…Hugues Chate'·Oct 12, 1993SaveLearn
Nonradial Solutions of a Semilinear Elliptic Equation in Two Dimensions: We establish existence of an infinite family of exponentially-decaying non-radial C2 solutions to the equation Δu + f(u) = 0 on R2 for a large class of nonlinearities f. These solutions…Joseph Iaia, Henry Warchall·Sep 13, 1993SaveLearn