Direct Numerical Simulations of the Kraichnan Model: Scaling Exponents and Fusion RulesWe present results from direct numerical simulations of the Kraichnan model for passive scalar advection by a rapidly-varying random scaling velocity field for intermediate values of the velocity…Adrienne L. Fairhall, Barak Galanti, Victor S. L'vov et al.·Jul 1, 1997SaveLearn
Algebraic approximations to bifurcation curves of limit cycles for the Lienard equationIn this paper, we study the bifurcation of limit cycles in Lienard systems of the form dot(x)=y-F(x), dot(y)=-x, where F(x) is an odd polynomial that contains, in general, several free parameters. By…Hector Giacomini, Sebastien Neukirch·Jun 30, 1997SaveLearn
Comment on "Optimal Periodic Orbits of Chaotic Systems"In a recent Letter, Hunt and Ott argued that SHORT-period unstable periodic orbits (UPOs) would be the invariant sets associated with a chaotic attractor that are most likely to optimize the time…Scott M. Zoldi, Henry S. Greenside·Jun 27, 1997SaveLearn
Slow Manifold Structure and the Emergence of Mixed-Mode OscillationsA detailed study of the slow manifold of a model exhibiting mixed-mode oscillations is presented. A scenario for the emergence of mixed-mode states which does not involve phase locking on a 2-torus…Andrei Goryachev, Peter Strizhak, Raymond Kapral·Jun 26, 1997SaveLearn
Chaotic Scattering on a BilliardWe investigate chaotic scattering on an attractive step potential with a quadrupolar deformation. The phase space features of the bound billiard are studied by using the notion of symmetry lines to…Vincent J. Daniels, Michel Vallieres, Jian Min Yuan·Jun 26, 1997SaveLearn
Lasing Threshold and Mode Competition in Chaotic CavitiesThe lasing threshold is studied of a multi-mode chaotic cavity (linear size D >> wavelength λ) coupled to the outside through a small hole (linear size d << λ). For sufficiently weak absorption by…T. Sh. Misirpashaev, C. W. J. Beenakker·Jun 25, 1997SaveLearn
Spontaneous Emission in Chaotic CavitiesThe spontaneous emission rate Γof a two-level atom inside a chaotic cavity fluctuates strongly from one point to another because of fluctuations in the local density of modes. For a cavity with…T. Sh. Misirpashaev, P. W. Brouwer, C. W. J. Beenakker·Jun 25, 1997SaveLearn
Wave Dynamical Chaos in a Superconducting Three-Dimensional Sinai BilliardBased on very accurate measurements performed on a superconducting microwave resonator shaped like a desymmetrized three-dimensional (3D) Sinai billiard, we investigate for the first time spectral…H. Alt, C. Dembowski, H. -D. Graef et al.·Jun 25, 1997SaveLearn
Quantitative study of scars in the boundary section of the stadium billiardWe construct a semiclassically invariant function on the boundary of the billiard, taken as the Poincare section in Birkhoff coordinates, based on periodic orbit information, as an ansatz for the…Fernando P. Simonotti, Eduardo Vergini, Marcos Saraceno·Jun 24, 1997SaveLearn
New Universal Aspects of Diffusion in Strongly Chaotic SystemsWe study some new universal aspects of diffusion in chaotic systems, especially such having very large Lyapunov coefficients on the chaotic (indecomposable, topologically transitive) component. We do…Marko Robnik, Jure Dobnikar, Andrea Rapisarda et al.·Jun 24, 1997SaveLearn
Directed Percolation Universality in Asynchronous Evolution of Spatio-Temporal IntermittencyWe present strong evidence that a coupled-map-lattice model for spatio-temporal intermittency belongs to the universality class of directed percolation when the updating rules are asynchronous, i.e.…Juri Rolf, Tomas Bohr, Mogens H. Jensen·Jun 23, 1997SaveLearn
Comment on Energy Level Statistics in the Mixed RegimeWe comment on the recent paper by Abul-Magd (J.Phys.A: Math.Gen. 29 (1996) 1) concerning the energy level statistics in the mixed regime, i.e. such having the mixed classical dynamics where regular…Marko Robnik, Tomaz Prosen·Jun 23, 1997SaveLearn
Turbulent-like Diffusion in Complex Quantum SystemsWe study a quantum particle propagating through a ``quantum mechanically chaotic'' background, described by parametric random matrices with only short range spatial correlations. The particle…Dimitri Kusnezov, Aurel Bulgac, Gui Do Dang·Jun 22, 1997SaveLearn
The Kolmogorov-Sinai Entropy for Dilute Gases in EquilibriumWe use the kinetic theory of gases to compute the Kolmogorov-Sinai entropy per particle for a dilute gas in equilibrium. For an equilibrium system, the KS entropy, hKS is the sum of all of the…H. van Beijeren, J. R. Dorfman, H. A. Posch et al.·Jun 18, 1997SaveLearn
Invariants for Correlations of Velocity Differences in Turbulent FieldsThe phenomenology of the scaling behavior of higher order structure functions of velocity differences across a scale R in turbulence should be built around the irreducible representations of the…Victor S. L'vov, Evgenii Podivilov, Itamar Procaccia·Jun 13, 1997SaveLearn
Inverse cascade and intermittency of passive scalar in 1d smooth flowRandom advection of Lagrangian tracer scalar field θ(t,x) by a one-dimensional, spatially smooth and short-correlated in time velocity field is considered. Scalar fluctuations are maintained by a…M. Chertkov, I. Kolokolov, M. Vegrassola·Jun 12, 1997SaveLearn
Inverse versus direct cascades in turbulent advectionA model of scalar turbulent advection in compressible flow is analytically investigated. It is shown that, depending on the dimensionality d of space and the degree of compressibility of the smooth…M. Chertkov, I. Kolokolov, M. Vegrassola·Jun 12, 1997SaveLearn
An Exact Renormalization Group analysis of 3-d Well Developed turbulenceWe take advantage of peculiar properties of three dimensional incompressible turbulence to introduce a nonstandard Exact Renormalization Group method. A Galilean invariance preserving regularizing…Paolo Tomassini·Jun 11, 1997SaveLearn
Towards a two-fluid picture of intermittency in shell models of turbulenceIntermittency in the Gledzer-Okhitani-Yamada (GOY) model of turbulence is explained in terms of collisions of coherent soliton-like structures with a random background issuing from the desintegration…J. L. Gilson, T. Dombre·Jun 11, 1997SaveLearn
On the triple correlations in helical turbulenceThe evolution of correlation characteristics in homogeneous helical turbulence is considered. Additional K'arm'an-Howarth type equations, describing the evolution of the mixed correlation…Otto Chkhetiani·Jun 11, 1997SaveLearn
Coarsening by Ginzburg-Landau DynamicsWe study slowly moving solutions of the real Ginzburg-Landau equation on the line, by a method due to J. Carr and R.L. Pego. These are functions taking alternately positive or negative values on…J. -P. Eckmann, J. Rougemont·Jun 10, 1997SaveLearn
Curvature fluctuations and Lyapunov exponent at MeltingWe calculate the maximal Lyapunov exponent in constant-energy molecular dynamics simulations at the melting transition for finite clusters of 6 to 13 particles (model rare-gas and metallic systems)…Vishal Mehra, Ramakrishna Ramaswamy·Jun 10, 1997SaveLearn
The Limits of Mathematics -- A course on information theory and the limits of formal reasoningThis book is the final version of a course on algorithmic information theory and the epistemology of mathematics and physics. This is camera-ready copy prepared for publication as a book, but at the…G. J. Chaitin·Jun 7, 1997SaveLearn
Observing the Symmetry of AttractorsWe show how the symmetry of attractors of equivariant dynamical systems can be observed by equivariant projections of the phase space. Equivariant projections have long been used, but they can give…Jeffrey H. Schenker, James W. Swift·Jun 6, 1997SaveLearn
A Solvable Model for Spatiotemporal ChaosWe show that the dynamical behavior of a coupled map lattice where the individual maps are Bernoulli shift maps can be solved analytically for integer couplings. We calculate the invariant density of…R. O. Grigoriev, H. G. Schuster·Jun 6, 1997SaveLearn