On the self-similar solutions of normality equation in two-dimensional caseThe integrability in quadratures of normality equation for spatially homogeneous dynamical systems in two-dimensional space is shown. The classical symmetries of this equation are calculated and the…A. Yu. Boldin·Jul 25, 1993SaveLearn
One parameter family of Compacton Solutions in a class of Generalized Korteweg-DeVries EquationsWe study the generalized Korteweg-DeVries equations derivable from the Lagrangian: $ L(l,p) = ∫ ( 12 φx φt - (φx)l l(l-1) + α(φx)p (φxx)2 )…Avinash Khare, Fred Cooper·Jul 21, 1993SaveLearn
A quantitative measurement of spatial order in ventricular fibrillationAs an objective measurement of spatial order in ventricular fibrillation (VF), spatial correlation functions and their characteristic lengths were estimated from epicardial electrograms of pigs in…P. V. Bayly, E. E. Johnson, P. D. Wolf et al.·Jul 18, 1993SaveLearn
Dissipative Boussinesq System of Equations in the Bénard-Marangoni PhenomenonBy using the long-wave approximation, a system of coupled evolution equations for the bulk velocity and the surface perturbations of a Bénard-Marangoni system is obtained. It includes nonlinearity,…R. A. Kraenkel, S. M. Kurcbart, J. G. Pereira et al.·Jun 28, 1993SaveLearn
Discrete Breathers and Energy Localization in Nonlinear LatticesWe discuss the process by which energy, initially evenly distributed in a nonlinear lattice, can localize itself into large amplitude excitations. We show that, the standard modulational instability…T. Dauxois, M. Peyrard·Jun 25, 1993SaveLearn
A New Class of Nonsingular Exact Solutions for Laplacian Pattern FormationWe present a new class of exact solutions for the so-called Laplacian Growth Equation describing the zero-surface-tension limit of a variety of 2D pattern formation problems. Contrary to common…Mark B. Mineev-Weinstein, Silvina Ponce Dawson·May 26, 1993SaveLearn
Nonequilibrium Phenomena in Liquid CrystalsThis paper summarizes a talk presented at the April NATO ASI on Spatiotemporal Chaos in Complex Fluids, in Santa Fe, NM. The paper gives reasons that make complex fluids good material systems for…John Bechhoefer·May 21, 1993SaveLearn
Phase Transitions In Two-Dimensional Traffic Flow ModelsWe introduce two simple two-dimensional lattice models to study traffic flow in cities. We have found that a few basic elements give rise to the characteristic phase diagram of a first-order phase…José A. Cuesta, Froilán C. Martínez, Juan M. Molera et al.·May 19, 1993SaveLearn
Pattern Formation in Dissipative Nonvariational Systems: The Effects of Front BifurcationsPatterns in reaction-diffusion systems often contain two spatial scales; a long scale determined by a typical wavelength or domain size, and a short scale pertaining to front structures separating…Aric Hagberg, Ehud Meron·May 19, 1993SaveLearn
Spiral Defect Chaos in Large Aspect Ratio Rayleigh-Benard ConvectionWe report experiments on convection patterns in a cylindrical cell with a large aspect ratio. The fluid had a Prandtl number of approximately 1. We observed a chaotic pattern consisting of many…Stephen W. Morris, Eberhard Bodenschatz, David S. Cannell et al.·May 18, 1993SaveLearn
Solitary Waves and Compactons in a class of Generalized Korteweg-DeVries EquationsWe study the class of generalized Korteweg-DeVries equations derivable from the Lagrangian: $ L(l,p) = ∫ ( 12 x t - (x)l l(l-1) + α(x)p…Fred Cooper, Harvey Shepard, Pasquale Sodano·May 18, 1993SaveLearn
Spiral defect chaos in a model of Rayleigh-Benard convectionA numerical solution of a generalized Swift-Hohenberg equation in two dimensions reveals the existence of a spatio-temporal chaotic state comprised of a large number of rotating spirals. This state…Hao-wen Xi, J. D. Gunton, Jorge Vinals·May 14, 1993SaveLearn
An integrable shallow water equation with peaked solitonsWe derive a new completely integrable dispersive shallow water equation that is biHamiltonian and thus possesses an infinite number of conservation laws in involution. The equation is obtained by…Roberto Camassa, Darryl D. Holm·May 13, 1993SaveLearn
Pattern formation during Rayleigh-Bénard convection in non-Boussinesq fluidsMotivated by recent experimental studies of Bodenschatz et al. [E. Bodenschatz, J.R. de Bruyn, G. Ahlers and D.S. Cannell, Phys. Rev. Lett. 67, 3078 (1991) ], we present a numerical study of a…Hao-wen Xi, J. D. Gunton, Jorge Vinals·May 4, 1993SaveLearn
Solitons and 1/f Noise in Molecular ChainsDavydov's model of solitons in alpha-helix protein chains is shown to display features of self-organized criticality (SOC), i.e., power law behaviour of correlations in space and 1/f-noise, as a…H. Rosu, E. Canessa·Apr 20, 1993SaveLearn
Complex Patterns in a Simple SystemNumerical simulations of a simple reaction--diffusion model reveal a surprising variety of irregular spatio--temporal patterns. These patterns arise in response to finite--amplitude perturbations.…John E. Pearson·Apr 17, 1993SaveLearn
Domain Walls in Non-Equilibrium Systems and the Emergence of Persistent PatternsDomain walls in equilibrium phase transitions propagate in a preferred direction so as to minimize the free energy of the system. As a result, initial spatio-temporal patterns ultimately decay toward…Aric Hagberg, Ehud Meron·Apr 9, 1993SaveLearn
Multidimensional Dynamical Systems Accepting the Normal ShiftThe dynamical systems of the form r= F ( r, r) in Rn accepting the normal shift are considered. The concept of weak normality for them is introduced. The…A. Yu. Boldin, R. A. Sharipov·Apr 4, 1993SaveLearn
Threshold-Range Scaling of Excitable Cellular AutomataEach cell of a two-dimensional lattice is painted one of k colors, arranged in a "color wheel." The colors advance (0 to k-1 mod k) either automatically or by contact with at least a…Robert Fisch, Janko Gravner, David Griffeath·Apr 2, 1993SaveLearn
Metastability in the Greenberg-Hastings ModelThe Greenberg-Hastings Model (GHM) is a family of multitype cellular automata that emulate excitable media, exhibiting the nucleation and spiral formation characteristic of such complex systems. In…Robert Fisch, Janko Gravner, David Griffeath·Mar 23, 1993SaveLearn
Threshold Growth DynamicsWe study the asymptotic shape of the occupied region for monotone deterministic dynamics in d-dimensional Euclidean space parametrized by a threshold theta, and a Borel set N with positive and finite…Janko Gravner, David Griffeath·Mar 23, 1993SaveLearn
Solitons and Long Josephson JunctionsMagnetic flux quanta, of value h/2e, in long Josephson junctions behave as (quasi) solitons. Fluxon dynamical states are well described by a perturbed sine-Gordon equation model, with boundary…R. D. Parmentier·Mar 23, 1993SaveLearn
Asymptotic Behavior of Excitable Cellular AutomataWe study two families of excitable cellular automata known as the Greenberg-Hastings Model (GHM) and the Cyclic Cellular Automaton (CCA). Each family consists of local deterministic oscillating…Richard Durrett, David Griffeath·Mar 22, 1993SaveLearn
Localized States in Discrete Nonlinear Schrödinger EquationsA new 1-D discrete nonlinear Schrödinger (NLS) Hamiltonian is introduced which includes the integrable Ablowitz-Ladik system as a limit. The symmetry properties of the system are studied. The…David Cai, A. R. Bishop, Niels Grønbech-Jensen·Mar 14, 1993SaveLearn
Rotating Rayleigh-Bénard Convection: Aspect Ratio Dependence of the Initial BifurcationsThe initial bifurcations in rotating Rayleigh-Bénard convection are studied in the range of dimensionless rotation rate 0 < Ω< 2150 for an aspect-ratio-2.5 cylindrical cell. We used simultaneous…Li Ning, Robert E. Ecke·Mar 11, 1993SaveLearn