Computing the Scaling Exponents in Fluid Turbulence from First Principles: Demonstration of Multi-scalingThis manuscript is a draft of work in progress, meant for network distribution only. It will be updated to a formal preprint when the numerical calculations will be accomplished. In this draft we…Victor I. Belinicher, Victor S. L'vov, Itamar Procaccia·Aug 5, 1997SaveLearn
Chaos and Lyapunov exponents in classical and quantal distribution dynamicsWe analytically establish the role of a spectrum of Lyapunov exponents in the evolution of phase-space distributions ρ(p,q). Of particular interest is λ2, an exponent which quantifies the rate…Arjendu K. Pattanayak, Paul Brumer·Aug 5, 1997SaveLearn
Single-point velocity distribution in turbulenceWe show that the tails of the single-point velocity probability distribution function (PDF) are generally non-Gaussian in developed turbulence. By using instanton formalism for the Navier-Stokes…Gregory Falkovich, Vladimir Lebedev·Aug 1, 1997SaveLearn
Modulational Estimate for Fermi-Pasta-Ulam Chain Lyapunov ExponentsIn the framework of the Fermi-Pasta-Ulam (FPU) model, we show a simple method to give an accurate analytical estimation of the maximal Lyapunov exponent at high energy density. The method is based on…Thierry Dauxois, Stefano Ruffo, Alessandro Torcini·Aug 1, 1997SaveLearn
Lyapunov instability and finite size effects in a system with long-range forcesWe study the largest Lyapunov exponent λ and the finite size effects of a system of N fully-coupled classical particles, which shows a second order phase transition. Slightly below the critical…Vito Latora, Andrea Rapisarda, Stefano Ruffo·Jul 30, 1997SaveLearn
Three applications of scaling to inhomogeneous, anisotropic turbulenceThe energy spectrum in three examples of inhomogeneous, anisotropic turbulence, namely, purely mechanical wall turbulence, the Bolgiano-Obukhov cascade and helical turbulence, is analyzed. As one…Piero Olla·Jul 28, 1997SaveLearn
Nonlinear hydrodynamic stabilityThe variational principle of V. I. Arnold [J. Appl. Math. Mech. Vol. 29, P. 1002 (1965)] is extended to the general conservative inhomogeneous, compressible, and conducting fluid. The concept of…M. B. Isichenko·Jul 28, 1997SaveLearn
Exact Eigenfunctions of a Chaotic SystemThe interest in the properties of quantum systems, whose classical dynamics are chaotic, derives from their abundance in nature. The spectrum of such systems can be related, in the semiclassical…O. M. Auslaender, S. Fishman·Jul 26, 1997SaveLearn
Experimental Study of Bifurcations in A Parametrically Forced PendulumAn experimental study of bifurcations associated with stability of stationary points (SP's) in a parametrically forced magnetic pendulum and a comparison of its results with numerical results are…Sang-Yoon Kim, S. H. Shin, J. Yi et al.·Jul 23, 1997SaveLearn
Controlling Physical Systems with SymmetriesSymmetry properties of the evolution equation and the state to be controlled are shown to determine the basic features of the linear control of unstable orbits. In particular, the selection of…R. O. Grigoriev, M. C. Cross·Jul 21, 1997SaveLearn
Helicity Transfer in Turbulent ModelsHelicity transfer in a shell model of turbulence is investigated. We show that a Reynolds-independent helicity flux is present in the model when the large scale forcing breaks inversion symmetry. The…L. Biferale, D. Pierotti, F. Toschi·Jul 21, 1997SaveLearn
The problem of quantum chaotic scattering with direct processes reduced to the one withoutWe show that the study of the statistical properties of the scattering matrix S for quantum chaotic scattering in the presence of direct processes (charaterized by a nonzero average S matrix <S>) can…Victor A. Gopar, Pier A. Mello·Jul 20, 1997SaveLearn
On the Rate of Quantum Ergodicity on hyperbolic Surfaces and BilliardsThe rate of quantum ergodicity is studied for three strongly chaotic (Anosov) systems. The quantal eigenfunctions on a compact Riemannian surface of genus g=2 and of two triangular billiards on a…R. Aurich, M. Taglieber·Jul 17, 1997SaveLearn
Computing the Scaling Exponents in Fluid Turbulence from First Principles: the Formal SetupWe propose a scheme for the calculation from the NS equations of the scaling exponents ζn of the nth order correlators in fully developed hydrodynamic turbulence. The scheme is nonperturbative…Victor S. L'vov, Itamar Procaccia·Jul 17, 1997SaveLearn
Reaction-diffusion fronts under stochastic advectionWe study front propagation in stirred media using a simplified modelization of the turbulent flow. Computer simulations reveal the existence of the two limiting propagation modes observed in recent…A. C. Marti, F. Sagues, J. M. Sancho·Jul 17, 1997SaveLearn
Double Phase Slips and Bound Defect Pairs in Parametrically Driven WavesSpatio-temporal chaos in parametrically driven waves is investigated in one and two dimensions using numerical simulations of Ginzburg-Landau equations. A regime is identified in which in one…Hermann Riecke, Glen D. Granzow·Jul 11, 1997SaveLearn
Search for Low-Dimensional Chaos in Observational DataWe introduce the reader to the "global flow reconstruction method". The purpose of the method is to see if a given temporal sequence has been generated by a low dimensional dynamics, and to…J. Robert Buchler·Jul 9, 1997SaveLearn
Scale-dependent functions in statistical hydrodynamics: a functional analysis point of viewMost of dynamic systems which exhibit chaotic behavior are also known to posses self-similarity and manifest strong fluctuations of all possible scales.The meaning of this terms is not always same.…Mikhail V. Altaisky·Jul 7, 1997SaveLearn
The Building Blocks of Spatiotemporal IntermittencyWe obtain a family of uniformly propagating hole-solutions to the complex Ginzburg-Landau equation which differ from the well-known Nozaki-Bekki holes. They describe the spatial organization and…Martin van Hecke·Jul 7, 1997SaveLearn
A Geometrical Model for Stagnant Motion in Hamiltonian Systems with Many Degrees of FreedomWe introduce a model of Poincaré mappings which represents hierarchical structure of phase spaces for systems with many degrees of freedom. The model yields residence time distribution of power type,…Yoshiyuki Y. Yamaguchi, Tetsuro Konishi·Jul 4, 1997SaveLearn
Fractals in Linear Ordinary Differential EquationsWe prove the existence of fractal solutions to a class of linear ordinary differential equations.This reveals the possibility of chaos in the very short time limit of the evolution even of a linear…Dhurjati Prasad Datta·Jul 4, 1997SaveLearn
Mean dynamical entropy of quantum system tends to infinity in the semiclassical limitWe show that the mean dynamical entropy of a quantum map on the sphere is positive and tends logarithmically to infinity in the semiclassical limit. A link between chaotic dynamics of classical…Wojciech Slomczynski, Karol Zyczkowski·Jul 4, 1997SaveLearn
Composed ensembles of random unitary matricesComposed ensembles of random unitary matrices are defined via products of matrices, each pertaining to a given canonical circular ensemble of Dyson. We investigate statistical properties of spectra…Marcin Pozniak, Karol Zyczkowski, Marek Kus·Jul 3, 1997SaveLearn
Dynamical Tunneling in Mixed SystemsWe study quantum-mechanical tunneling in mixed dynamical systems between symmetry-related phase space tori separated by a chaotic layer. Considering e.g. the annular billiard we decompose…Steffen D. Frischat, Eyal Doron·Jul 3, 1997SaveLearn
Nonlinear Dynamics of Dry FrictionThe dynamical behavior caused by dry friction is studied for a spring-block system pulled with constant velocity over a surface. The dynamical consequences of a general type of phenomenological…Franz-Josef Elmer·Jul 1, 1997SaveLearn