Heterogeneity Induced Order in Globally Coupled Chaotic SystemsCollective behavior is studied in globally coupled maps with distributed nonlinearity. It is shown that the heterogeneity enhances regularity in the collective dynamics. Low-dimensional quasiperiodic…Tatsuo Shibata, Kunihiko Kaneko·Apr 29, 1996SaveLearn
Inflation of Hamiltonian System: The Spinning Top in Projective SpaceWe present a method to enlarge the phase space of a canonical Hamiltonian System in order to remove coordinate singularities arising from a nontrivial topology of the configuration space. This…Holger R. Dullin·Apr 26, 1996SaveLearn
Low-Dimensional Modelling of Dynamics via Computer AlgebraI describe a method, particularly suitable to implementation by computer algebra, for the derivation of low-dimensional models of dynamical systems. The method is systematic and is based upon centre…A. J. Roberts·Apr 22, 1996SaveLearn
A New Method for Computing Topological PressureThe topological pressure introduced by Ruelle and similar quantities describe dynamical multifractal properties of dynamical systems. These are important characteristics of mesoscopic systems in the…Péter Pollner, Gábor Vattay·Apr 18, 1996SaveLearn
Coherent States Measurement EntropyCoherent states (CS) quantum entropy can be split into two components. The dynamical entropy is linked with the dynamical properties of a quantum system. The measurement entropy, which tends to zero…Jaroslaw Kwapien, Wojciech Slomczynski, Karol Zyczkowski·Apr 18, 1996SaveLearn
Transitions and Probes in Turbulent HeliumPrevious analysis of a Paris turbulence experiment zoc94,tab95 shows a transition at the Taylor Reynolds number ≈ 700. Here correlation function data is analyzed which gives…V. Emsellem, L. Kadanoff, D. Lohse et al.·Apr 18, 1996SaveLearn
Non-equilibrium Thermodynamics approach to Transport Processes in Gas MixturesThe thermodynamic approach to non-equilibrium dynamics describes the state of macroscopic systems by means of a collection of intensities or intensive variables. The latter are by definition the…Z. Hens, X. de Hemptinne·Apr 16, 1996SaveLearn
Growth of non-infinitesimal perturbations in turbulenceWe discuss the effects of finite perturbations in fully developed turbulence by introducing a measure of the chaoticity degree associated to a given scale of the velocity field. This allows one to…E. Aurell, G. Boffetta, A. Crisanti et al.·Apr 15, 1996SaveLearn
Equivalence of dynamical ensembles and Navier Stokes equationsA reversible version of the Navier Stokes equation is studied. A conjecture emerges stating the equivalence between the reversible equation and the usual Navier Stokes equation. The latter appears as…Giovanni Gallavotti·Apr 12, 1996SaveLearn
Localization in Strongly Chaotic SystemsWe show that, in the semiclassical limit and whenever the elements of the Hamiltonian matrix are random enough, the eigenvectors of strongly chaotic time-independent systems in ordered bases can on…Mario Feingold·Apr 12, 1996SaveLearn
Long-time unbreaking correlations in the large number of degrees of freedom Hamiltonian systemA behaviour of molecular cluster with Lennard-Jones potential of interactions as Hamiltonian system is studied by computer simulation (molecular dynamics method). It is shown that complex periodic…O. I. Gorsky, Yu. P Kuchugurny·Apr 11, 1996SaveLearn
Winding number instability in the phase-turbulence regime of the Complex Ginzburg-Landau EquationWe give a statistical characterization of states with nonzero winding number in the Phase Turbulence (PT) regime of the one-dimensional Complex Ginzburg-Landau equation. We find that states with…R. Montagne, E. Hernandez-Garcia, M. San Miguel·Apr 10, 1996SaveLearn
Anomalous scaling of triple correlation function of white-advected passive scalarFor a short-correlated Gaussian velocity field the problem of a passive scalar with the imposed constant gradient is considered. It is shown that the scaling of three-point correlation function is…D. Gutman, E. Balkovsky·Apr 9, 1996SaveLearn
Period p-tuplings in coupled mapsWe study the critical behavior (CB) of all period p-tuplings (p \!=\!2,3,4,…) in N (N \!=\! 2,3,4,…) symmetrically coupled one-dimensional maps. We first investigate the CB for the…Sang-Yoon Kim·Apr 5, 1996SaveLearn
Quantum Chaotic Dynamics and Random PolynomialsWe investigate the distribution of roots of polynomials of high degree with random coefficients which, among others, appear naturally in the context of "quantum chaotic dynamics". It is shown…E. Bogomolny, O. Bohigas, P. Leboeuf·Apr 5, 1996SaveLearn
Phase Diffusion in Localized Spatio-Temporal Amplitude ChaosWe present numerical simulations of coupled Ginzburg-Landau equations describing parametrically excited waves which reveal persistent dynamics due to the occurrence of phase slips in sequential…Glen D. Granzow, Hermann Riecke·Apr 4, 1996SaveLearn
Energy-Conserving Truncations for Convection with Shear FlowA method is presented for making finite Fourier mode truncations of the Rayleigh--Benard convection system that preserve invariants of the full partial differential equations in the dissipationless…Jean-Luc Thiffeault, Wendell Horton·Apr 3, 1996SaveLearn
Burgers Velocity Fields and the Electromagnetic Forcing in Schroedinger's Interpolating DynamicsWe explore a connection of the deterministically forced Burgers equation for local velocity fields with probabilistic solutions of the Schrödinger boundary data problem. An issue of deducing the most…P. Garbaczewski, G. Kondrat, R. Olkiewicz·Apr 3, 1996SaveLearn
Dynamical Zeta Functions, Nielsen theory and Reidemeister torsionThe paper consists of four parts. Part I presents a brief survey of the Nielsen fixed point theory. Part II deals with dynamical zeta functions connected with Nielsen fixed point theory. Part III is…Alexander Fel'shtyn·Apr 2, 1996SaveLearn
Three disks in a row: A two-dimensional scattering analog of the double-well problemWe investigate the scattering off three nonoverlapping disks equidistantly spaced along a line in the two-dimensional plane with the radii of the outer disks equal and the radius of the inner disk…Andreas Wirzba, Per. E Rosenqvist·Apr 2, 1996SaveLearn
Viscous Instanton for Burgers' TurbulenceWe consider the tails of probability density functions (PDF) for different characteristics of velocity that satisfies Burgers equation driven by a large-scale force. The saddle-point approximation is…E. Balkovsky, G. Falkovich, I. Kolokolov et al.·Mar 31, 1996SaveLearn
WKB expansion for the angular momentum and the Kepler problem: from the torus quantization to the exact oneWe calculate the WKB series for the angular momentum and the non--relativistic 3-dim Kepler problem. This is the first semiclassical treatment of the angular momentum for terms beyond the leading WKB…Marko Robnik, Luca Salasnich·Mar 29, 1996SaveLearn
Spatial chaos in weakly dispersive and viscous media: a nonperturbative theory of the driven KdV-Burgers equationThe asymptotic travelling wave solution of the KdV-Burgers equation driven by the long scale periodic driver is constructed. The solution represents a shock-train in which the quasi-periodic sequence…M. A. Malkov·Mar 29, 1996SaveLearn
Gaussian Fluctuations in Chaotic EigenstatesWe study the fluctuations that are predicted in the autocorrelation function of an energy eigenstate of a chaotic, two-dimensional billiard by the conjecture (due to Berry) that the eigenfunction is…Mark Srednicki, Frank Stiernelof·Mar 28, 1996SaveLearn
Scaling and Linear Response in the GOY Turbulence modelThe GOY model is a model for turbulence in which two conserved quantities cascade up and down a linear array of shells. When the viscosity parameter, ν, is small the model has a qualitative…Leo Kadanoff, Detlef Lohse, Norbert Schorghofer·Mar 27, 1996SaveLearn