Levy Diffusion and Classes of Universal Parametric CorrelationsA general formulation of translationally invariant, parametrically correlated random matrix ensembles, is used to classify universality in correlation functions. Surprisingly, the range of possible…Dimitri Kusnezov, Caio H. Lewenkopf·Apr 11, 1995SaveLearn
Collective patterns arising out of spatio-temporal chaosWe present a simple mathematical model in which a time averaged pattern emerges out of spatio-temporal chaos as a result of the collective action of chaotic fluctuations. Our evolution equation…Shin-ichi Sasa·Apr 10, 1995SaveLearn
Chronotopic Lyapunov Analysis: (I) a Comprehensive Characterization of 1D SystemsInstabilities in 1D spatially extended systems are studied with the aid of both temporal and spatial Lyapunov exponents. A suitable representation of the spectra allows a compact description of all…Stefano Lepri, Antonio Politi, Alessandro Torcini·Apr 7, 1995SaveLearn
Basis functions for strongly correlated Fermi systemsA general method to construct basis functions for fermionic systems which account for the SU(2) symmetry and for the translational invariance of the Hamiltonian is presented. The method does not…Mario Salerno·Apr 5, 1995SaveLearn
Guessing probability distributions from small samplesWe propose a new method for the calculation of the statistical properties, as e.g. the entropy, of unknown generators of symbolic sequences. The probability distribution p(k) of the elements k of…Thorsten Pöschel, Werner Ebeling, Helge Rosé·Apr 4, 1995SaveLearn
Universality in Turbulence: an Exactly Soluble ModelThe present note contains the text of lectures discussing the problem of universality in fully developed turbulence. After a brief description of Kolmogorov's 1941 scaling theory of turbulence…Krzysztof Gawedzki, Antti Kupiainen·Apr 3, 1995SaveLearn
The Source of Irreversibility in Macroscopic DynamicsThe dynamics of irreversible relaxation of non-equilibrium macroscopic systems is discussed. Arguments are developed showing that the general process is supported by two independent successive…X de Hemptinne·Mar 31, 1995SaveLearn
On multiplicities in length spectra of arithmetic hyperbolic three-orbifoldsAsymptotic laws for mean multiplicities of lengths of closed geodesics in arithmetic hyperbolic three-orbifolds are derived. The sharpest results are obtained for non-compact orbifolds associated…J. Marklof·Mar 30, 1995SaveLearn
Ionization of Rydberg atoms in a low frequency field: modelling by maps of transition to chaotic behaviorWe investigate a microwave ionization of highly excited atom in a low frequency field and show that such a process may be studied on the bases of map for the electron energy change during the period…B. Kaulakys, G. Vilutis·Mar 27, 1995SaveLearn
On the Quantum Baker's Map and its Unusual TracesThe quantum baker's map is the quantization of a simple classically chaotic system, and has many generic features that have been studied over the last few years. While there exists a…Arul Lakshminarayan·Mar 25, 1995SaveLearn
Decoherence, Delocalization and Irreversibility in Quantum Chaotic SystemsDecoherence in quantum systems which are classically chaotic is studied. The Arnold cat map and the quantum kicked rotor are chosen as examples of linear and nonlinear chaotic systems. The…K. Shiokawa, B. L. Hu·Mar 23, 1995SaveLearn
Quantum Surface of Section Method: Eigenstates and Unitary Quantum Poincare EvolutionThe unitary representation of exact quantum Poincare mapping is constructed. It is equivalent to the compact representation in a sense that it yields equivalent quantization condition with important…Tomaz Prosen·Mar 22, 1995SaveLearn
Lindstedt series and Kolmogorov theoremThe KAM theorem from a combinatorial viewpoint.Giovanni Gallavotti·Mar 21, 1995SaveLearn
Stochastic Shell Model: a model of anomalous scaling and non-Gaussian distribution in turbulenceWe propose a simple stochastic model of cascading transport in wave number space to clarify the origin of intermittent behavior of fully-developed fluid turbulence. In spite of lack of nonlinearity…Hideki Takayasu, Y-h. Taguchi, Tomoo Katsuyama·Mar 17, 1995SaveLearn
The entropy of ``strange'' billiards inside n-simplexesIn the present work we investigate a new type of billiards defined inside of n--simplex regions. We determine an invariant ergodic (SRB) measure of the dynamics for any dimension. In using symbolic…Thomas Schürmann, Ingo Hoffmann·Mar 17, 1995SaveLearn
Controlling Neuronal Noise Using Chaos ControlChaos control techniques have been applied to a wide variety of experimental systems, including magneto-elastic ribbons, lasers, chemical reactions, arrhythmic cardiac tissue, and spontaneously…David J. Christini, James J. Collins·Mar 15, 1995SaveLearn
Evidence for the Validity of the Berry-Robnik Surmise in a Periodically Pulsed Spin SystemWe study the statistical properties of the spectrum of a quantum dynamical system whose classical counterpart has a mixed phase space structure consisting of two regular regions separated by a…PH. Jacquod, J. -P. Amiet·Mar 9, 1995SaveLearn
Normal and Anomalous Scaling of the Fourth-Order Correlation Function of a Randomly Advected Passive ScalarFor a delta-correlated velocity field, simultaneous correlation functions of a passive scalar satisfy closed equations. We analyze the equation for the four-point function. To describe a solution…M. Chertkov, G. Falkovich, I. Kolokolov et al.·Mar 6, 1995SaveLearn
Do Spectral Trace Formulae Converge?We evaluate the Gutzwiller trace formula for the level density of classically chaotic systems by considering the level density in a bounded energy range and truncating its Fourier integral. This…Eyal Doron·Mar 2, 1995SaveLearn
Chaos induced by Pauli blockingDynamics of classical scattering in the system of fermions is studied. The model is based on the coherent state representation and the equations of motion for fermions are derived from the…S. Drożdż, J. Okołowicz, M. Ploszajczak et al.·Mar 2, 1995SaveLearn
Geometrization of spin systems using cycle expansionsIt is shown that a spin system with long range interactions can be converted into a chaotic dynamical system that is differentiable and low-dimensional. The thermodynamic limit of the spin system is…Ronnie Mainieri·Mar 1, 1995SaveLearn
Quantized chaotic dynamics and non-commutative KS entropyWe study the quantization of two examples of classically chaotic dynamics, the Anosov dynamics of "cat maps" on a two dimensional torus, and the dynamics of baker's maps. Each of these…S. Klimek, A. Lesniewski·Feb 28, 1995SaveLearn
Dynamical Simulation of Fluidized Beds --- Hydrodynamically Interacting Granular ParticlesA numerical simulation of a gas-fluidized bed is performed without introduction of any empirical parameters. Realistic bubbles and slugs are observed in our simulation. It is found that the…Kengo Ichiki, Hisao Hayakawa·Feb 28, 1995SaveLearn
Localized States in the Chaotic Ce AtomWe show that the energy averaged entropy localization length for the eigenstates of the Ce atom is well approximated by the prediction of the Wigner ensemble.Mario Feingold, Oreste Piro·Feb 27, 1995SaveLearn
Quantization of Sinai's Billiard - A Scattering ApproachWe obtained the spectrum of the Sinai billiard as the zeroes of a secular equation, which is based on the scattering matrix of a related scattering problem. We show that this quantization method…Holger Schanz, Uzy Smilansky·Feb 25, 1995SaveLearn