Chaotic Dynamics of Binary SystemsWe propose a theory of chaos for discrete systems, based on their representation in a space of ``binary histories'', B∞ . We show that B∞ is a metrizable Cantor…H. Waelbroeck, F. Zertuche·Jun 1, 1995SaveLearn
Evolution of Liouville density of a chaotic systemAn area-preserving map of the unit sphere, consisting of alternating twists and turns, is mostly chaotic. A Liouville density on that sphere is specified by means of its expansion into spherical…Asher Peres, Daniel Terno·May 31, 1995SaveLearn
Chaotic principle: some applications to developed turbulenceSome models for developed turbulence are considered; they are shown to obey a large fluctuations theorem, and one among them also obeys a response reciprocity relation of Onsager's type. This…Giovanni Gallavotti·May 27, 1995SaveLearn
Thermodynamic Description of the Relaxation of Two-Dimensional Euler Turbulence Using Tsallis StatisticsEuler turbulence has been experimentally observed to relax to a metaequilibrium state that does not maximize the Boltzmann entropy, but rather seems to minimize enstrophy. We show that a recent…Bruce M. Boghosian·May 23, 1995SaveLearn
Diffractive orbits in quantum billiardsWe study diffractive effects in two dimensional polygonal billiards. We derive an analytical trace formula accounting for the role of non-classical diffractive orbits in the quantum spectrum. As an…Nicolas Pavloff, Charles Schmit·May 18, 1995SaveLearn
Disorder in the 1D spinless Holstein modelWe investigate a spinless fermion system on a one dimensional lattice interacting locally with the optical modes of a quantized phonon field: the Holstein model. The system is shown to have a…G. Benfatto, G. Gallavotti, L. Lebowitz·May 16, 1995SaveLearn
Trace formula for an ensemble of bumpy billiards.We study the semiclassical quantization of an ensemble of billiards with a small random shape deformation. We derive a trace formula averaged over shape disorder. The results are illustrated by the…Nicolas Pavloff·May 16, 1995SaveLearn
THE CONVERGENCE OF CHAOTIC INTEGRALSWe review the convergence of chaotic integrals computed by Monte Carlo simulation, the trace method, dynamical zeta function, and Fredholm determinant on a simple one-dimensional example: the…Oliver Bauer, Ronnie Mainieri·May 12, 1995SaveLearn
The Origin of Non-chaotic Behavior in Identically Driven SystemsRecently it has been found that different physical systems driven by identical random noise behave exactly identical after a long time. It is also suggested that this is an outcome of finite…P. M. Gade, Chaitali Basu·May 12, 1995SaveLearn
Universal Behavior of Lyapunov Exponents in Unstable SystemsWe calculate the Lyapunov exponents in a classical molecular dynamics framework. The system is composed of few hundreds particles interacting either through Yukawa (Nuclear) or Slater-Kirkwood…A. Bonasera, V. Latora, A. Rapisarda·May 10, 1995SaveLearn
Predictability in Systems with Many Characteristic Times: The Case of TurbulenceIn chaotic dynamical systems, an infinitesimal perturbation is exponentially amplified at a time-rate given by the inverse of the maximum Lyapunov exponent λ. In fully developed turbulence, λ…E. Aurell, G. Boffetta, A. Crisanti et al.·May 10, 1995SaveLearn
Optimized Periodic Control of Chaotic SystemsIn this work, we demonstrate the open-loop control of chaotic systems by means of optimized periodic signals. The use of such signals enables us to reduce control power significantly in comparison to…Robert Mettin, Thomas Kurz·May 9, 1995SaveLearn
The Schroedinger Problem, Levy Processes Noise in Relativistic Quantum MechanicsThe main purpose of the paper is an essentially probabilistic analysis of relativistic quantum mechanics. It is based on the assumption that whenever probability distributions arise, there exists a…P. Garbaczewski, J. R. Klauder, R. Olkiewicz·May 9, 1995SaveLearn
Signatures of Classical Periodic Orbits on a Smooth Quantum SystemGutzwiller's trace formula and Bogomolny's formula are applied to a non--specific, non--scalable Hamiltonian system, a two--dimensional anharmonic oscillator. These semiclassical theories…Daniel Provost·May 8, 1995SaveLearn
Pitch Perception of Complex Sounds: Nonlinearity RevisitedThe ability of the auditory system to perceive the fundamental frequency of a sound even when this frequency is removed from the stimulus is an interesting phenomenon related to the pitch of complex…D. L. Gonzalez, L. Morettini, F. Sportolari et al.·May 5, 1995SaveLearn
Magnetic Field Effect in a Two-dimensional Array of Short Josephson JunctionsWe study analytically the effect of a constant magnetic field on the dynamics of a two dimensional Josephson array. The magnetic field induces spatially dependent states and coupling between rows,…G. Filatrella, K. Wiesenfeld·May 3, 1995SaveLearn
ERROR PROPAGATION IN EXTENDED CHAOTIC SYSTEMSA strong analogy is found between the evolution of localized disturbances in extended chaotic systems and the propagation of fronts separating different phases. A condition for the evolution to be…A. Torcini, P. Grassberger, A. Politi·May 2, 1995SaveLearn
Chaotic Scattering Theory, Thermodynamic Formalism, and Transport CoefficientsThe foundations of the chaotic scattering theory for transport and reaction-rate coefficients for classical many-body systems are considered here in some detail. The thermodynamic formalism of Sinai,…P. Gaspard, J. R. Dorfman, .·Apr 25, 1995SaveLearn
High Temperature Expansions and Dynamical SystemsWe develop a resummed high-temperature expansion for lattice spin systems with long range interactions, in models where the free energy is not, in general, analytic. We establish uniqueness of the…J. Bricmont, A. Kupiainen·Apr 25, 1995SaveLearn
Experimental studies of Chaos and Localization in Quantum WavefunctionsWavefunctions in chaotic and disordered quantum billiards are studied experimentally using thin microwave cavities. The chaotic wavefunctions display universal density distributions and density…A. Kudrolli, V. Kidambi, S. Sridhar·Apr 21, 1995SaveLearn
Chaotic advection in three-dimensional unsteady incompressible laminar flowWe discuss chaotic advection in three-dimensional unsteady incompressible laminar flow, and analyse in detail the most important novel advection phenomenon in these flows; the global dispersion of…Julyan H. E. Cartwright, Mario Feingold, Oreste Piro·Apr 18, 1995SaveLearn
Bubble Shape Oscillations and the Onset of SonoluminescenceAn air bubble trapped in water by an oscillating acoustic field undergoes either radial or nonspherical pulsations depending on the strength of the forcing pressure. Two different instability…Michael P. Brenner, Detlef Lohse, T. F. Dupont·Apr 13, 1995SaveLearn
Anomalous Scaling in a Model of Passive Scalar Advection: Exact ResultsKraichnan's model of passive scalar advection in which the driving velocity field has fast temporal decorrelation is studied as a case model for understanding the appearance of anomalous scaling…A. Fairhall, O. Gat, V. S. L'vov et al.·Apr 12, 1995SaveLearn
Transition to nonchaotic behavior in a Brownian-type motionA theoretical and numerical analysis of the transition from chaotic to nonchaotic behavior in an ensemble of particles with different initial conditions which move according to Newton's equations…B. Kaulakys, G. Vektaris·Apr 12, 1995SaveLearn
Belavkin-Kolkoltsov watch-dog effects in interactively controlled stochastic computer-graphic dynamic systems. A mathematical studyStochastic properties of the long-time behaviour of a continuously observed (and interactively controlled) quantum-field top are investigated mathematically. Applications to interactively controlled…Denis Juriev·Apr 11, 1995SaveLearn