A q-anaolg of the sixth Painlevé equationA q-difference analog of the sixth Painlevé equation is presented. It arises as the condition for preserving the connection matrix of linear q-difference equations, in close analogy with the…Michio Jimbo, Hidetaka Sakai·Jul 31, 1995SaveLearn
The Computational Complexity of Symbolic Dynamics at the Onset of ChaosIn a variety of studies of dynamical systems, the edge of order and chaos has been singled out as a region of complexity. It was suggested by Wolfram, on the basis of qualitative behaviour of…Porus Lakdawala·Jul 28, 1995SaveLearn
Fusion Rules in Turbulent Systems with Flux EquilibriumFusion rules in turbulence specify the analytic structure of many-point correlation functions of the turbulent field when a group of coordinates coalesce. We show that the existence of flux…Victor L'vov, Itamar Procaccia·Jul 27, 1995SaveLearn
Exact Resummations in the Theory of Hydrodynamic Turbulence: III. Scenarios for Anomalous Scaling and IntermittencyElements of the analytic structure of anomalous scaling and intermittency in fully developed hydrodynamic turbulence are described. We focus here on the structure functions of velocity differences…Victor L'vov, Itamar Procaccia·Jul 26, 1995SaveLearn
Exact Resummations in the Theory of Hydrodynamic Turbulence: II A Ladder to Anomalous ScalingIn paper I of this series on fluid turbulence we showed that exact resummations of the perturbative theory of the structure functions of velocity differences result in a finite (order by order)…Victor L'vov, Itamar Procaccia·Jul 26, 1995SaveLearn
Exact Resummations in the Theory of Hydrodynamic Turbulence: I The Ball of Locality and Normal ScalingThis paper is the first in a series of three papers that aim at understanding the scaling behaviour of hydrodynamic turbulence. We present in this paper a perturbative theory for the structure…Victor L'vov, Itamar Procaccia·Jul 26, 1995SaveLearn
Collective Behavior of Coupled Chaotic MapsThe collective behavior of a coupled map lattice having unbounded chaotic local dynamics is investigated through the properties of its mean field. The presence of unstable periodic orbits in…M. G. Cosenza·Jul 21, 1995SaveLearn
Alternative method to find orbits in chaotic systemsWe present here a new method which applies well ordered symbolic dynamics to find unstable periodic and non-periodic orbits in a chaotic system. The method is simple and efficient and has been…Kai T. Hansen·Jul 9, 1995SaveLearn
Boundary integral method applied in chaotic quantum billiardsThe boundary integral method (BIM) is a formulation of Helmholtz equation in the form of an integral equation suitable for numerical discretization to solve the quantum billiard. This paper is an…Baowen Li, Marko Robnik·Jul 7, 1995SaveLearn
Universal diffusion near the golden chaos borderWe study local diffusion rate D in Chirikov standard map near the critical golden curve. Numerical simulations confirm the predicted exponent α=5 for the power law decay of D as approaching the…S. Ruffo, D. L. Shepelyansky·Jul 7, 1995SaveLearn
The creation of high-dimensional oscillations from low-dimensional systemsThe complication of chaotic oscillation under its transformation by linear inertial process is discussed. It is shown that such complication is begun from large scales of attractor and is pure…A. A. Kipchatov, L. V. Krasichkov·Jul 4, 1995SaveLearn
Chaotic Spectra of Classically Integrable SystemsWe prove that any spectral sequence obeying a certain growth law is the quantum spectrum of an equivalence class of classically integrable non-linear oscillators. This implies that exceptions to the…P. Crehan·Jul 3, 1995SaveLearn
Sample to sample fluctuations in fragmentation and agglomeration processesThe fluctuations in the particle size distribution for processes of fragmentation and aggregation are studied for stationary state regimes. The system is described in terms of a stochastic process…Piero Olla·Jul 2, 1995SaveLearn
Decay of Classical Chaotic Systems - the Case of the Bunimovich StadiumThe escape of an ensemble of particles from the Bunimovich stadium via a small hole has been studied numerically. The decay probability starts out exponentially but has an algebraic tail. The weight…H. Alt, H. -D. Graef, R. Hofferbert et al.·Jun 30, 1995SaveLearn
Interaction of Nonlinear Schrödinger Solitons with an External PotentialEmploying a particularly suitable higher order symplectic integration algorithm, we integrate the 1-d nonlinear Schrödinger equation numerically for solitons moving in external potentials. In…Helge Frauenkron, Peter Grassberger·Jun 30, 1995SaveLearn
ANOMALOUS SCALING OF THE PASSIVE SCALARWe establish anomalous inertial range scaling of structure functions for a model of advection of a passive scalar by a random velocity field. The velocity statistics is taken gaussian with…Krzysztof Gawedzki, Antti Kupiainen·Jun 30, 1995SaveLearn
Lyapunov spectral analysis of a nonequilibrium Ising-like transitionBy simulating a nonequilibrium coupled map lattice that undergoes an Ising-like phase transition, we show that the Lyapunov spectrum and related dynamical quantities such as the dimension correlation…Corey S. O'Hern, David A. Egolf, Henry S. Greenside·Jun 29, 1995SaveLearn
Information-theoretic characterization of quantum chaosHypersensitivity to perturbation is a criterion for chaos based on the question of how much information about a perturbing environment is needed to keep the entropy of a Hamiltonian system from…R. Schack, C. M. Caves·Jun 28, 1995SaveLearn
Direct Numerical Simulation Tests of Eddy Viscosity in Two DimensionsTwo-parametric eddy viscosity (TPEV) and other spectral characteristics of two-dimensional (2D) turbulence in the energy transfer sub-range are calculated from direct numerical simulation (DNS) with…A. Chekhlov, S. A. Orszag, S. Sukoriansky et al.·Jun 21, 1995SaveLearn
Chaotic hypothesis: Onsager reciprocity and fluctuation-dissipation theoremIt is shown that the "chaoticity hypothesis", analogous to Ruelle's principle for turbulence and recently introduced in statistical mechanics, implies the Onsager reciprocity and the…Giovanni Gallavotti·Jun 18, 1995SaveLearn
Enhancing Efficiency of Mixing in Chaotic FlowsWe propose a mechanism by which the efficiency of mixing in chaotic flows can be enhanced. Our mechanism consists of introducing small changes in the system parameters in regions of phase space where…Neelima Gupte, R. E. Amritkar·Jun 14, 1995SaveLearn
Methods for the analysis of the Lindstedt series for KAM tori and renormalizability in classical mechanicsThis paper consists in a unified exposition of methods and techniques of the renormalization group approach to quantum field theory applied to classical mechanics, and in a review of results: (1) a…G. Gentile, V. Mastropietro·Jun 6, 1995SaveLearn
A New Version of Algorithmic Information TheoryThis material was presented in a series of lectures at the Santa Fe Institute, the Los Alamos National Laboratory, and the University of New Mexico, during a one-month visit to the Santa Fe…G J Chaitin·Jun 5, 1995SaveLearn
Chaos for Liouville probability densitiesUsing the method of symbolic dynamics, we show that a large class of classical chaotic maps exhibit exponential hypersensitivity to perturbation, i.e., a rapid increase with time of the information…R. Schack, C. M. Caves·Jun 5, 1995SaveLearn
Universal bifurcation property of two- or higher-dimensional dissipative systems in parameter space: Why does 1D symbolic dynamics work so well?The universal bifurcation property of the Hénon map in parameter space is studied with symbolic dynamics. The universal-L region is defined to characterize the bifurcation universality. It is found…H. P. Fang·Jun 2, 1995SaveLearn