Anisotropic Spectra of Acoustic TurbulenceWe found universal anizopropic spectra of acoustic turbulence with the linear dispersion law ω(k) =ck within the framework of generalized kinetic equation which takes into account the finite…V. S L'vov, Yu. V. L'vov, A. Pomyalov·May 19, 1999SaveLearn
Temporal surrogates of spatial turbulent statistics: the Taylor hypothesis revistedThe Taylor hypothesis which allows surrogating spatial measurements requiring many experimental probes by time series from one or two probes is examined on the basis of a simple analytic model of…Victor S. L'vov, Anna Pomyalov, Itamar Procaccia·May 19, 1999SaveLearn
Hyperbolic Billiards on Surfaces of Constant CurvatureWe establish sufficient conditions for the hyperbolicity of the billiard dynamics on surfaces of constant curvature. This extends known results for planar billiards. Using these conditions, we…B. Gutkin, U. Smilansky, E. Gutkin·May 18, 1999SaveLearn
Distributions of Transition Matrix Elements in Classically Mixed Quantum SystemsThe quantitative contributions of a mixed phase-space to the mean characterizing the distribution of diagonal transition matrix elements and to the variance characterizing the distributions of…D. Boose, J. Main·May 18, 1999SaveLearn
Influence of compressibility on scaling regimes of strongly anisotropic fully developed turbulenceStatistical model of strongly anisotropic fully developed turbulence of the weakly compressible fluid is considered by means of the field theoretic renormalization group. The corrections due to…N. V. Antonov, M. Hnatič, M. Yu. Nalimov·May 18, 1999SaveLearn
Lagrangian Tetrad Dynamics and the Phenomenology of TurbulenceA new phenomenological model of turbulent fluctuations is constructed by considering the Lagrangian dynamics of 4 points (the tetrad). The closure of the equations of motion is achieved by…Michael Chertkov, Alain Pumir, Boris I. Shraiman·May 18, 1999SaveLearn
Quantum-limited linewidth of a chaotic laser cavityA random-matrix theory is presented for the linewidth of a laser cavity in which the radiation is scattered chaotically. The linewidth is enhanced above the Schawlow-Townes value by the Petermann…M. Patra, H. Schomerus, C. W. J. Beenakker·May 18, 1999SaveLearn
Ergodic and chaotic hypotheses: nonequilibrium ensembles in statistical mechanics and turbulenceThe ergodic hypothesis outgrew from the ancient conception of motion as periodic or quasi periodic. It did cause a revision of our views of motion, particularly through Boltzmann and Poincaré: we…Giovanni Gallavotti·May 17, 1999SaveLearn
Experimental Generation and Observation of Intrinsic Localized Spin Wave Modes in an AntiferromagnetBy driving with a microwave pulse the lowest frequency antiferromagnetic resonance of the quasi 1-D biaxial antiferromagnet (C2 H5 NH3)2 CuCl4 into an unstable region intrinsic localized spin…U. T. Schwarz, L. Q. English, A. J. Sievers·May 16, 1999SaveLearn
Fluctuation-Response Relations for Multi-Time CorrelationsWe show that time-correlation functions of arbitrary order for any random variable in a statistical dynamical system can be calculated as higher-order response functions of the mean history of the…Gregory L. Eyink·May 14, 1999SaveLearn
Self-organization in nonlinear wave turbulenceWe present a statistical equilibrium model of self-organization in a class of focusing, nonintegrable nonlinear Schrodinger (NLS) equations. The theory predicts that the asymptotic-time behavior of…Richard Jordan, Christophe Josserand·May 14, 1999SaveLearn
Noise-induced flow in quasigeostrophic turbulence with bottom frictionRandomly-forced fluid flow in the presence of scale-unselective dissipation develops mean currents following topographic contours. Known mechanisms based on the scale-selective action of damping…A. Alvarez, E. Hernandez-Garcia, J. Tintore·May 14, 1999SaveLearn
Detection of Aliasing in Persistent SignalsWe explain why aliasing can be detected in a generic temporally-sampled stationary signal process. We then define a concept of stationarity that makes sense for single waveforms. (This is done…Kevin R. Vixie, David E. Sigeti, Murray Wolinsky·May 14, 1999SaveLearn
Universal long-time properties of Lagrangian statistics in the Batchelor regime and their application to the passive scalar problemWe consider transport of dynamically passive quantities in the Batchelor regime of smooth in space velocity field. For the case of arbitrary temporal correlations of the velocity we formulate the…E. Balkovsky, A. Fouxon·May 13, 1999SaveLearn
Anomalous spatio-temporal chaos in a two-dimensional system of non-locally coupled oscillatorsA two-dimensional system of non-locally coupled complex Ginzburg-Landau oscillators is investigated numerically for the first time. As already known for the one-dimensional case, the system exhibits…Hiroya Nakao·May 13, 1999SaveLearn
Instanton Calculus in Shell Models of TurbulenceIt has been shown recently that intermittency of the Gledzer Ohkitani Yamada (GOY) shell model of turbulence has to be related to singular structures whose dynamics in the inertial range includes…I. Daumont, T. Dombre, J. -L. Gilson·May 12, 1999SaveLearn
Pulses in the Zero-Spacing Limit of the GOY ModelWe study the propagation of localised disturbances in a turbulent, but momentarily quiescent and unforced shell model (an approximation of the Navier-Stokes equations on a set of exponentially spaced…K. H. Andersen, T. Bohr, M. H. Jensen et al.·May 12, 1999SaveLearn
Chaotic eigenfunctions in momentum spaceWe study eigenstates of chaotic billiards in the momentum representation and propose the radially integrated momentum distribution as useful measure to detect localization effects. For the momentum…Arnd Bäcker, Roman Schubert·May 11, 1999SaveLearn
The Radiative Kicked Oscillator: A Stochastic Web or Chaotic Attractor ?A relativistic charged particle moving in a uniform magnetic field and kicked by an electric field is considered. Under the assumption of small magnetic field, an iterative map is developed. We…Y. Ashkenazy, L. P. Horwitz·May 11, 1999SaveLearn
Quasilinear theory of collisionless Fermi acceleration in a multicusp magnetic confinement geometryParticle motion in a cylindrical multiple-cusp magnetic field configuration is shown to be highly (though not completely) chaotic, as expected by analogy with the Sinai billiard. This provides a…Robert L. Dewar, Carmen I. Ciubotariu·May 10, 1999SaveLearn
The Construction of a Quantum Markov PartitionWe present a method for constructing a quantum Markov partition. Its elements are obtained by quantizing the characteristic function of the classical rectangles. The result is a set of quantum…Raul O. Vallejos, Marcos Saraceno·May 8, 1999SaveLearn
Decomposition of Resonant Scatterers by Surfaces of SectionScattering on the energy shell is viewed here as the relation between the bound states of the Hamiltonian, restricted to sections on leads that are asymptotically independent, far away from the…Raul O. Vallejos, Alfredo M. Ozorio de Almeida·May 8, 1999SaveLearn
Poincare's Recurrence Theorem and the Unitarity of the S matrixA scattering process can be described by suitably closing the system and considering the first return map from the entrance onto itself. This scattering map may be singular and discontinuous, but it…Alfredo M. Ozorio de Almeida, Raul O. Vallejos·May 8, 1999SaveLearn
Characterization of the long-time and short-time predictability of low-order models of the atmosphereMethods to quantify predictability properties of atmospheric flows are proposed. The ``Extended Self Similarity'' (ESS) technique, recently employed in turbulence data analysis, is used to…R. Benzi, M. Marrocu, A. Mazzino et al.·May 8, 1999SaveLearn
Collective and chaotic motion in self-bound many-body systemsWe investigate the interplay of collective and chaotic motion in a classical self-bound N-body system with two-body interactions. This system displays a hierarchy of three well separated time scales…Thomas Papenbrock·May 6, 1999SaveLearn