Surface tension and dynamics of fingering patternsWe study the minimal class of exact solutions of the Saffman-Taylor problem with zero surface tension, which contains the physical fixed points of the regularized (non-zero surface tension) problem.…F. X. Magdaleno, J. Casademunt·Jul 25, 1997SaveLearn
Universal algebraic relaxation of fronts propagating into an unstable stateWe analyze ``pulled'' or ``linearly marginally stable'' fronts propagating into unstable states. While ``pushed'' fronts into meta- and unstable states relax exponentially,…Ute Ebert, Wim van Saarloos·Jul 16, 1997SaveLearn
Breaking the symmetry in bimodal frequency distributions of globally coupled oscillatorsThe mean-field Kuramoto model for synchronization of phase oscillators with an asymmetric bimodal frequency distribution is analyzed. Breaking the reflection symmetry facilitates oscillator…J. A. Acebron, L. L. Bonilla, S. De Leo et al.·Jul 11, 1997SaveLearn
Nonequilibrium phase separation in traffic flowsTraffic jam in an optimal velocity model with the backward reference function is analyzed. An analytic scaling solution is presented near the critical point of the phase separation. The validity of…H. Hayakawa, K. Nakanishi·Jul 8, 1997SaveLearn
Optical characterization of chevron texture formation in nematic electroconvectionWe characterize the director structures in electroconvection patterns of nematic liquid crystals by means of polarising microscopy. This study was stimulated by a theory put forward by Rossberg et…H. Amm, R. Stannarius, A. G. Rossberg·Jul 3, 1997SaveLearn
Phenomenological Theory for Spatiotemporal Chaos in Rayleigh-Benard ConvectionWe present a phenomenological theory for spatiotemporal chaos (STC) in Rayleigh-Benard convection, based on the generalized Swift-Hohenberg model. We apply a random phase approximation to STC and…Xiao-jun Li, Hao-wen Xi, J. D. Gunton·Jun 18, 1997SaveLearn
Fingering Instability in a Water-Sand MixtureThe temporal evolution of a water-sand interface driven by gravity is experimentally investigated. By means of a Fourier analysis of the evolving interface the growth rates are determined for the…A. Lange, M. Schröter, M. A. Scherer et al.·Jun 16, 1997SaveLearn
Weakly nonlinear analysis in spatially extended systems as a formal perturbation schemeThe well known concept, to reduce the spatio-temporal dynamics beyond instabilities of trivial states to amplitude modulated patterns, is reviewed from the point of view of a formal perturbation…Wolfram Just, Frank Matth"aus, Hans Rainer V"olger et al.·Jun 16, 1997SaveLearn
Time-periodic phases in populations of nonlinearly coupled oscillators with bimodal frequency distributionsThe mean field Kuramoto model describing the synchronization of a population of phase oscillators with a bimodal frequency distribution is analyzed (by the method of multiple scales) near regions in…L. L. Bonilla, C. J. Perez Vicente, R. Spigler·Jun 16, 1997SaveLearn
Asymptotic description of transients and synchronized states of globally coupled oscillatorsA two-time scale asymptotic method has been introduced to analyze the multimodal mean-field Kuramoto-Sakaguchi model of oscillator synchronization in the high-frequency limit. The method allows to…J. A. Acebron, L. L. Bonilla·Jun 13, 1997SaveLearn
Phase Space Derivation of a Variational Principle for One Dimensional Hamiltonian SystemsWe consider the bifurcation problem u'' + λu = N(u) with two point boundary conditions where N(u) is a general nonlinear term which may also depend on the eigenvalue λ. A new derivation of a…R. D. Benguria, M. C. Depassier·Jun 10, 1997SaveLearn
Amplitude Equations for Electrostatic Waves: multiple speciesThe amplitude equation for an unstable electrostatic wave is analyzed using an expansion in the mode amplitude A(t). In the limit of weak instability, i.e. γ 0+ where γ is the linear growth…John David Crawford, Anandhan Jayaraman·Jun 10, 1997SaveLearn
Amplitude Equation for Lattice Maps, a Renormalization Group ApproachWe consider the development of instabilities of homogeneous stationary solutions of discrete time lattice maps. Under some generic hypothesis we derive an amplitude equation which is the space-time…P. Collet·May 22, 1997SaveLearn
Stability of a Nonequilibrium Interface in a Driven Phase Segregating SystemWe investigate the dynamics of a nonequilibrium interface between coexisting phases in a system described by a Cahn-Hilliard equation with an additional driving term. By means of a matched asymptotic…Claude A. Laberge, Sven Sandow·May 20, 1997SaveLearn
Stretching of vortex lines and generation of vorticity in the three-dimensional complex Ginzburg-Landau EquationThe dynamics of curved vortex filaments is studied analytically and numerically in the framework of a three-dimensional complex Ginzburg-Landau equation (CGLE). It is proved that a straight vortex…Igor Aranson, Alan Bishop·May 19, 1997SaveLearn
Existence and Stability of Propagating Fronts for an Autocatalytic Reaction-Diffusion SystemWe study a one-dimensional reaction-diffusion system which describes an isothermal autocatalytic chemical reaction involving both a quadratic (A + B -> 2B) and a cubic (A + 2B -> 3B) autocatalysis.…Stephane Focant, Thierry Gallay·May 16, 1997SaveLearn
On Envelope Dynamics In 2D Faraday WavesA weakly nonlinear model for two-dimensional Faraday waves over infinite depth is derived and studied. Sideband instability of monochromatic standing waves as well as non-monochromatic solutions are…I. Keller, A. Oron, P. Z. Bar-Yoseph·May 15, 1997SaveLearn
The branching structure of diffusion-limited aggregatesI analyze the topological structures generated by diffusion-limited aggregation (DLA), using the recently developed "branched growth model". The computed bifurcation number B for DLA in two…Thomas C. Halsey·May 8, 1997SaveLearn
Unicellular algal growth: A biomechanical approach to cell wall dynamicsWe present a model for unicellular algal growth as motivated by several experiments implicating the importance of calcium ions and ``loosening'' enzymes in morphogenesis. A growing cell at…Royce Kam, Herbert Levine·May 7, 1997SaveLearn
Dynamical Reduction of Discrete Systems Based on the Renormalization Group MethodThe renormalization group (RG) method is extended for global asymptotic analysis of discrete systems. We show that the RG equation in the discretized form leads to difference equations corresponding…T. Kunihiro, J. Matsukidaira·May 7, 1997SaveLearn
Selection of the Saffman-Taylor Finger Width in the Absence of Surface Tension: an Exact ResultUsing our exact time-depending solutions, we solve the Saffman-Taylor finger selection problem in the absence of surface tension by showing that an arbitrary interface in a Hele-Shaw cell evolves to…Mark Mineev-Weinstein·May 6, 1997SaveLearn
A Lubrication Model of Coating Flows over a Curved Substrate in SpaceConsider the three-dimensional flow of a viscous Newtonian fluid upon an abitrarily curved substrate when the fluid film is thin as occurs in many draining, coating and biological flows. We derive a…R. Valery Roy, A. J. Roberts, M. E. Simpson·May 1, 1997SaveLearn
Phase Segregation Dynamics In Particle Systems with Long Range Interactions II: Interface motionWe study properties of the solutions of a family of second order integro-differential equations, which describe the large scale dynamics of a class of microscopic phase segregation models with…G. Giacomin, J. L. Lebowitz·Apr 29, 1997SaveLearn
Spiral Dynamics in Pattern-Forming Systems: Mean Flow EffectsMean flow effects are discussed for two different pattern-forming systems: Rayleigh-Benard convection and Faraday instability in viscous fluid. In both systems spirals are observed in certain…Lev S. Tsimring·Apr 21, 1997SaveLearn
Onset of oscillatory instabilities under stochastic modulationWe study the effect of external stochastic modulation on a system with O(2) symmetry that exhibits a Hopf or oscillatory instability in the absence of modulation. The study includes a random…Francois Drolet, Jorge Vinals·Apr 21, 1997SaveLearn