Fractal tracer distributions in turbulent field theoriesWe study the motion of passive tracers in a two-dimensional turbulent velocity field generated by the Kuramoto-Sivashinsky equation. By varying the direction of the velocity-vector with respect to…Jonas Lundbek Hansen, Tomas Bohr·Sep 9, 1997SaveLearn
Non-normal parameter blowout bifurcation: an example in a truncated mean field dynamo modelWe examine global dynamics and bifurcations occurring in a truncated model of a stellar mean field dynamo. This model has symmetry-forced invariant subspaces for the dynamics and we find examples of…Eurico Covas, Peter Ashwin, Reza Tavakol·Sep 8, 1997SaveLearn
Vorticity alignment results for the three-dimensional Euler and Navier-Stokes equationsWe address the problem in Navier-Stokes isotropic turbulence of why the vorticity accumulates on thin sets such as quasi-one-dimensional tubes and quasi-two-dimensional sheets. Taking our motivation…B. Galanti, J. D. Gibbon, M. Heritage·Sep 4, 1997SaveLearn
An Infinite Step BilliardA class of non-compact billiards is introduced, namely the infinite step billiards, i.e., systems of a point particle moving freely in the domain Ω= n∈ [n,n+1] × [0,pn], with…Mirko Degli Esposti, Gianluigi Del Magno, Marco Lenci·Sep 3, 1997SaveLearn
Intermittent dissipation of a passive scalar in turbulenceProbability density function (PDF) of passive scalar dissipation P (ε) is found analytically in the limit of large Peclet and Prandtl numbers (Batchelor-Kraichnan regime) in two dimensions.…M. Chertkov, G. Falkovich, I. Kolokolov·Sep 2, 1997SaveLearn
Pendulum: separatrix splittingAn exact expression for the determinant of the splitting matrix is derived: it allows us to analyze the asympotic behaviour needed to amend the large angles theorem proposed in Ann. Inst. H.…G. Gallavotti, G. Gentile, V. Mastropietro·Sep 2, 1997SaveLearn
Relationships among coefficients in deterministic and stochastic transient diffusionSystems are studied in which transport is possible due to large extension with open boundaries in certain directions but the particles responsible for transport can disappear from it by leaving it in…Z. Kaufmann·Sep 1, 1997SaveLearn
The Quantum Adiabatic Approximation in Chaotic SystemsQuantum systems with chaotic classical counterparts cannot be treated by perturbative techniques or any kind of adiabatic approximations. This is so, in spite of the quantum suppression of classical…G. Abal, A. J. Pereira, A. Romanelli et al.·Aug 29, 1997SaveLearn
Probability density and scaling exponents of the moments of longitudinal velocity difference in strong turbulenceWe consider a few cases of homogeneous and isotropic turbulence differing by the mechanisms of turbulence generation. The advective terms in the Navier-Stokes and Burgers equations are similar. It is…Victor Yakhot·Aug 28, 1997SaveLearn
Invariant Measures in Generic Dynamical SystemsIrreversible thermodynamics of simple fluids have been connected recently to the theory of dynamical systems and some interesting assumptions have been made about the nature of the associated…Jean-Pierre Eckmann, Itamar Procaccia·Aug 27, 1997SaveLearn
Structure of Eigenstates and Local Spectral Density of States: A Three-Orbital Schematic Shell ModelThe average shape of the Spectral Local Density of States (LDOS) and eigenfunctions (EFs) has been studied numerically for a conservative dynamical model (three-orbital Lipkin-Meshkov-Glick model)…Wen-ge Wang, F. M. Izrailev, G. Casati·Aug 26, 1997SaveLearn
Orbital measures in non-equilibrium statistical mechanics: the Onsager relationsWe assume that the properties of nonequilibrium stationary states of systems of particles can be expressed in terms of weighted orbital measures, i.e. through periodic orbit expansions. This allows…L. Rondoni, E. G. D. Cohen·Aug 26, 1997SaveLearn
Complex step-size dependences in tracking a simple two-body dynamicsIn molecular simulations, one of the most difficult points is to track the real dynamics of many-body systems from the first principle. The present study shows that step-size dependences have an…Ken Umeno·Aug 25, 1997SaveLearn
Quantal-Classical Duality and the Semiclassical Trace FormulaWe consider Hamiltonian systems which can be described both classically and quantum mechanically. Trace formulas establish links between the energy spectra of the quantum description and the spectrum…Doron Cohen, Harel Primack, Uzy Smilansky·Aug 22, 1997SaveLearn
Strange Attractor in Immunology of Tumor GrowthThe time delayed cytotoxic T-lymphocyte response on the tumor growth has been developed on the basis of discrete approximation (2-dimensional map). The growth kinetic has been described by logistic…Margarita Voitikova·Aug 21, 1997SaveLearn
Front dynamics in turbulent mediaA study of a stable front propagating in a turbulent medium is presented. The front is generated through a reaction-diffusion equation, and the turbulent medium is statistically modeled using a…A. C. Marti, F. Sagues, J. M. Sancho·Aug 21, 1997SaveLearn
Uniform Approximation for Period-Quadrupling BifurcationsWe derive a uniform approximation for semiclassical contributions of periodic orbits to the spectral density which is valid for generic period-quadrupling bifurcations in systems with a mixed phase…Martin Sieber, Henning Schomerus·Aug 21, 1997SaveLearn
Route to Chaos in the 15NH3 far infrared ring laserThe route to chaos as the pump power is raised in the Lorenz-like ammonia laser is studied using transients and compared with the route which is expected in the Lorenz Haken equations. The…R. Dykstra, M. Y. Li, N. R. Heckenberg·Aug 21, 1997SaveLearn
Cycle expansions for intermittent diffusionWe investigate intermittent diffusion using cycle expansions, and show that a truncation based on cycle stability achieves reasonable convergence.Carl Dettmann, Predrag Cvitanovic'·Aug 18, 1997SaveLearn
Cycling chaos: its creation, persistence and loss of stability in a model of nonlinear magnetoconvectionWe examine a model system where attractors may consist of a heteroclinic cycle between chaotic sets; this `cycling chaos' manifests itself as trajectories that spend increasingly long periods…Peter Ashwin, A. M. Rucklidge·Aug 15, 1997SaveLearn
Stellar ArrhythmiasThe light curves of the two large amplitude variable stars, R Scuti and AC Herculis, display irregular pulsation cycles with 'periods' of 75 and 35 days, respectively. We review the evidence…J. Robert Buchler·Aug 13, 1997SaveLearn
Burridge-Knopoff Models as Elastic Excitable MediaWe construct a model of an excitable medium with elastic rather than the usual diffusive coupling. We explore the dynamics of elastic excitable media, which we find to be dominated by low dimensional…Julyan H. E. Cartwright, Emilio Hernández-García, Oreste Piro·Aug 11, 1997SaveLearn
Inert gas accumulation in sonoluminescing bubblesIn this paper we elaborate on the idea [Lohse et al., Phys. Rev. Lett. 78, 1359-1362 (1997)] that (single) sonoluminescing air bubbles rectify argon. The reason for the rectification is that nitrogen…Detlef Lohse, Sascha Hilgenfeldt·Aug 7, 1997SaveLearn
Scaling of the irreducible SO(3)-invariants of velocity correlations in turbulenceThe scaling behavior of the SO(3) irreducible amplitudes dnl(r) of velocity structure tensors (see L'vov, Podivilov, and Procaccia, Phys. Rev. Lett. (1997)) is numerically examined for…Siegfried Grossmann, Detlef Lohse, Achim Reeh·Aug 6, 1997SaveLearn
Symmetry and Dynamics of A Magnetic OscillatorWe consider a permanent magnetic dipole in an oscillating magnetic field. This magnetic oscillator has two dynamical symmetries. With increasing the amplitude A of the magnetic field, dynamical…Sang-Yoon Kim·Aug 6, 1997SaveLearn