Pattern Formation from Defect Chaos --- A Theory of ChevronsFor over 25 years it is known that the roll structure of electroconvection (EC) in the dielectric regime in planarly aligned nematic liquid crystals has, after a transition to defect chaos, the…A. G. Rossberg, L. Kramer·Jan 9, 1997SaveLearn
Diffusive Boundary Layers in the Free-Surface Excitable Medium SpiralSpiral waves are a ubiquitous feature of the nonequilibrium dynamics of a great variety of excitable systems. In the limit of a large separation in timescale between fast excitation and slow…David A. Kessler, Herbert Levine·Jan 8, 1997SaveLearn
Energy thresholds for discrete breathers in one-, two- and three-dimensional latticesDiscrete breathers are time-periodic, spatially localized solutions of equations of motion for classical degrees of freedom interacting on a lattice. They come in one-parameter families. We report on…S. Flach, K. Kladko, R. S. MacKay·Jan 6, 1997SaveLearn
Bistability of Slow and Fast Traveling Waves in Fluid MixturesThe appearence of a new type of fast nonlinear traveling wave states in binary fluid convection with increasing Soret effect is elucidated and the parameter range of their bistability with the common…St. Hollinger, P. Buechel, M. Luecke·Jan 3, 1997SaveLearn
Worm Structure in Modified Swift-Hohenberg Equation for ElectroconvectionA theoretical model for studying pattern formation in electroconvection is proposed in the form of a modified Swift-Hohenberg equation. A localized state is found in two dimension, in agreement with…Yuhai Tu·Jan 2, 1997SaveLearn
Optical Solitary Waves in the Higher Order Nonlinear Schrodinger EquationWe study solitary wave solutions of the higher order nonlinear Schrodinger equation for the propagation of short light pulses in an optical fiber. Using a scaling transformation we reduce the…M. Gedalin, T. C. Scott, Y. B. Band·Dec 25, 1996SaveLearn
Sources and sinks separating domains of left- and right-traveling waves: Experiment versus amplitude equationsIn many pattern forming systems that exhibit traveling waves, sources and sinks occur which separate patches of oppositely traveling waves. We show that simple qualitative features of their dynamics…Roberto Alvarez, Martin van Hecke, Wim van Saarloos·Dec 23, 1996SaveLearn
Geometric Stability Analysis for Periodic Solutions of the Swift-Hohenberg EquationIn this paper we describe invariant geometrical ~structures in the phase space of the Swift-Hohenberg equation in a neighborhood of its periodic stationary states. We show that in spite of the fact…J. -P. Eckmann, C. E. Wayne, P. Wittwer·Dec 20, 1996SaveLearn
A Mechanism for Spatio-Temporal Disorder in Bistable Reaction-Diffusion SystemsIn bistable systems, the stability of front structures often influences the dynamics of extended patterns. We show how the combined effect of an instability to curvature modulations and proximity to…Aric Hagberg, Ehud Meron·Dec 10, 1996SaveLearn
The Dynamics of Curved Fronts: Beyond GeometryWe derive a new set of kinematic equations for front motion in two-dimensional bistable media. The equations generalize the geometric approach by complementing the equation for the front curvature…Aric Hagberg, Ehud Meron·Nov 14, 1996SaveLearn
Vortex Dynamics in Dissipative SystemsWe derive the exact equation of motion for a vortex in two- and three- dimensional non-relativistic systems governed by the Ginzburg-Landau equation with complex coefficients. The velocity is given…Ola Tornkvist, Elsebeth Schroder·Nov 5, 1996SaveLearn
Solvable Optimal Velocity Models and Asymptotic TrajectoryIn the Optimal Velocity Model proposed as a new version of Car Following Model, it has been found that a congested flow is generated spontaneously from a homogeneous flow for a certain range of the…K. Nakanishi, K. Itoh, Y. Igarashi et al.·Oct 23, 1996SaveLearn
Solitary vortex couples in viscoelastic Couette flowWe report experimental observation of a localized structure, which is of a new type for dissipative systems. It appears as a solitary vortex couple ("diwhirl") in Couette flow with highly…Alexander Groisman, Victor Steinberg·Oct 22, 1996SaveLearn
Nonlinear Modulation of Travelling Rolls in MagnetoconvectionModulational dynamics of oscillatory travelling rolls in magnetoconvection is studied near the onset of a Hopf bifurcation. Using weakly nonlinear analysis, we derive an envelope equation of…Ken-ichi Matsuba, Kenji Imai, Kazuhiro Nozaki·Oct 8, 1996SaveLearn
An analytical stability theory for Faraday waves and the observation of the harmonic surface responseWe present an analytical stability theory for the onset of the Faraday instability, applying over a wide frequency range between shallow water gravity and deep water capillary waves. For sufficiently…H. W. Mueller, H. Wittmer, C. Wagner et al.·Oct 8, 1996SaveLearn
Direct Transition to Spatiotemporal Chaos in Low Prandtl Number FluidsWe present the first large scale numerical simulation of three-dimensional Rayleigh-Bénard convection near onset, under free-free boundary conditions for a fluid of Prandtl number σ=0.5. We find…Hao-wen Xi, Xiao-jun Li, J. D. Gunton·Oct 7, 1996SaveLearn
Influence of boundaries on pattern selection in through-flowThe problem of pattern selection in absolutely unstable open flow systems is investigated by considering the example of Rayleigh-Bénard convection. The spatiotemporal structure of convection rolls…D. Roth, P. Buechel, M. Luecke et al.·Sep 30, 1996SaveLearn
Stationary planar domain walls of a classical spin chainDomain walls of a discrete model of an anisotropic ferromagnet are studied. They can be described by sequences of two reversible mappings. Competition between the length scale of spatial structures…Benno Rumpf·Sep 30, 1996SaveLearn
Influence of through-flow on linear pattern formation properties in binary mixture convectionWe investigate how a horizontal plane Poiseuille shear flow changes linear convection properties in binary fluid layers heated from below. The full linear field equations are solved with a shooting…Ch. Jung, M. Luecke, P. Buechel·Sep 30, 1996SaveLearn
Pattern selection as a nonlinear eigenvalue problemA unique pattern selection in the absolutely unstable regime of driven, nonlinear, open-flow systems is reviewed. It has recently been found in numerical simulations of propagating vortex structures…P. Buechel, M. Luecke·Sep 30, 1996SaveLearn
Extended Symbolic Dynamics in Bistable CML: Existence and Stability of FrontsWe consider a diffusive Coupled Map Lattice (CML) for which the local map is piece-wise affine and has two stable fixed points. By introducing a spatio-temporal coding, we prove the one-to-one…R. Coutinho, B. Fernandez·Sep 25, 1996SaveLearn
A domain wall between single-mode and bimodal states and its transition to dynamical behavior in inhomogeneous systemsWe consider domain walls (DW's) between single-mode and bimodal states that occur in coupled nonlinear diffusion (NLD), real Ginzburg-Landau (RGL), and complex Ginzburg-Landau (CGL) equations…M. van Hecke, B. A. Malomed·Sep 13, 1996SaveLearn
Convection in rotating annuli: Ginzburg-Landau equations with tunable coefficientsThe coefficients of the complex Ginzburg-Landau equations that describe weakly nonlinear convection in a large rotating annulus are calculated for a range of Prandtl numbers σ. For fluids with…Martin van Hecke, Wim van Saarloos·Sep 12, 1996SaveLearn
Structure of Complex-Periodic and Chaotic Media with Spiral WavesThe spatiotemporal structure of reactive media supporting a solitary spiral wave is studied for systems where the local reaction law exhibits a period-doubling cascade to chaos. This structure is…Andrei Goryachev, Raymond Kapral·Sep 9, 1996SaveLearn
Dynamical Properties of Multi-Armed Global Spirals in Rayleigh-Benard ConvectionExplicit formulas for the rotation frequency and the long-wavenumber diffusion coefficients of global spirals with m arms in Rayleigh-Benard convection are obtained. Global spirals and parallel…Xiao-jun Li, Hao-wen Xi, J. D. Gunton·Aug 28, 1996SaveLearn