Anomalies of Transport in Reflectionally Noninvariant TurbulenceWe consider the transport of passive admixture in locally homogeneous isotropic reflectionally noninvariant turbulence of incompressible fluid. It is shown that anomalous convective flow appears…A. V. Chechkin, A. V. Tur, V. V. Yanovsky·Jun 6, 1997SaveLearn
Resonant Collisions in Four Dimensional Reversible Maps: A Description of ScenariosWe define a resonant collision of order k(geq 1) in a family of four-dimensional reversible maps. For any specified k, the bifurcation secnario is the collection of the different possible types of…A. Lahiri, A. Bhowal, T. K. Roy·Jun 6, 1997SaveLearn
A KAM type theorem for systems with round-off errorsPerturbations due to round-off errors in computer modeling are discontinuous and therefore one cannot use results like KAM theory about smooth perturbations of twist maps. We elaborate a special…M. Blank, T. Kruger, L. Pustyl'nikov·Jun 4, 1997SaveLearn
Entropy potential and Lyapunov exponentsAccording to a previous conjecture, spatial and temporal Lyapunov exponents of chaotic extended systems can be obtained from derivatives of a suitable function: the entropy potential. The validity…Stefano Lepri, Antonio Politi, Alessandro Torcini·Jun 3, 1997SaveLearn
Structure and convergence of Poincare-like normal formsThe general term of the Poincare normalizing series is explicitly constructed for non-resonant systems of ODE's in a large class of equations. In the resonant case, a non-local transformation is…S. Louies, L. Brenig·Jun 3, 1997SaveLearn
Diffusion Process in a FlowWe establish circumstances under which the dispersion of passive contaminants in a forced, deterministic or random, flow can be consistently interpreted as a Markovian diffusion process. In case of…P. Garbaczewski·Jun 2, 1997SaveLearn
Quadratic Volume Preserving MapsWe study quadratic, volume preserving diffeomorphisms whose inverse is also quadratic. Such maps generalize the Henon area preserving map and the family of symplectic quadratic maps studied by Moser.…H. E. Lomeli, J. D. Meiss·May 30, 1997SaveLearn
Communication with Chaos over Band-Limited ChannelsMethods of communications using chaotic signals use an ability of a chaos generator (encoder) and matched response system (decoder) to behave identically despite the instability of chaotic…Nikolai F. Rulkov, Lev S. Tsimring·May 28, 1997SaveLearn
Ultrametric structure of multiscale energy correlations in turbulent modelsUltrametric structure of the energy cascade process in a dynamical model of turbulence is studied. The tree model we use can be viewed as an approximated one-dimensional truncation of the wavelets…R. Benzi, L. Biferale, E. Trovatore·May 23, 1997SaveLearn
Exact Result for the 3rd Order Correlations of Velocity in Turbulence with HelicityAll statistical models of turbulence take into account Kolmogorov's exact result known as the "4/5 law" which stems from energy conservation. This law states that the energy flux…Victor S. L'vov, Evgenii Podivilov, Itamar Procaccia·May 22, 1997SaveLearn
Active control of ionized boundary layersThe challenging problems, in the field of control of chaos or of transition to chaos, lie in the domain of infinite-dimensional systems. Access to all variables being impossible in this case and the…R. Vilela Mendes·May 22, 1997SaveLearn
Quantum mechanical time-delay matrix in chaotic scatteringWe calculate the probability distribution of the matrix Q = -i S-1 dS/dE for a chaotic system with scattering matrix S at energy E. The eigenvalues τj of Q are the so-called proper delay…P. W. Brouwer, K. M. Frahm, C. W. J. Beenakker·May 20, 1997SaveLearn
Criteria for the onset of chaos in finite Fermi systemsThe paper in its present form has been withdrawn.V. V. Flambaum, G. F. Gribakin, O. P. Sushkov·May 17, 1997SaveLearn
Unpredictability, information, and chaosA source of unpredictability is equivalent to a source of information: unpredictability means not knowing which of a set of alternatives is the actual one; determining the actual alternative yields…Carlton M. Caves, Ruediger Schack·May 15, 1997SaveLearn
Random Quantum BilliardsWe present a random matrix model suitable for the quantum mechanical description of a particle confined to move inside a two-dimensional domain. Here, the ensemble average corresponds to an average…Henrik J. Pedersen, A. D. Jackson·May 13, 1997SaveLearn
Chaos properties and localization in Lorentz lattice gasesThe thermodynamic formalism of Ruelle, Sinai, and Bowen, in which chaotic properties of dynamical systems are expressed in terms of a free energy-type function - called the topological pressure - is…C. Appert, M. H. Ernst·May 12, 1997SaveLearn
Low-Dimensional Modelling of Dynamical SystemsConsider briefly the equations of fluid dynamics-they describe the enormous wealth of detail in all the interacting physical elements of a fluid flow-whereas in applications we want to deal with a…A. J. Roberts·May 9, 1997SaveLearn
New Universality of Lyapunov Spectra in Hamiltonian SystemsA new universality of Lyapunov spectra λi is shown for Hamiltonian systems. The universality appears in middle energy regime and is different from another universality which can be reproduced by…Yoshiyuki Y. Yamaguchi·May 6, 1997SaveLearn
Distribution of the wave function inside chaotic partially open systemsWe demonstrate both theoretically and experimentally that the distribution of the wavefunction inside a partially open chaotic timereversal symmetric system displays significant deviations from the…P. Seba, F. Haake, M. Kus et al.·May 6, 1997SaveLearn
Numerical study of scars in a chaotic billiardWe study numerically the scaling properties of scars in stadium billiard. Using the semiclassical criterion, we have searched systematically the scars of the same type through a very wide range, from…Baowen Li·May 1, 1997SaveLearn
Singularities in droplet pinching with vanishing viscosityA slender-jet model for the pinching of a liquid column is considered in the limit of vanishing viscosity. We find the model to develop a singularity in the gradients of the local radius and the…Jens Eggers·Apr 30, 1997SaveLearn
On the number of limit cycles of the Lienard equationIn this paper, we study a Lienard system of the form dotx=y-F(x), doty=-x, where F(x) is an odd polynomial. We introduce a method that gives a sequence of algebraic approximations to the equation…H. Giacomini, S. Neukirch·Apr 30, 1997SaveLearn
Pseudochaos in Statistical PhysicsA new generic dynamical phenomenon of pseudochaos and its relevance to the statistical physics both modern as well as traditional one are considered and explained in some detail. The pseudochaos is…Boris Chirikov·Apr 30, 1997SaveLearn
Linear and Nonlinear Dynamical ChaosInterrelations between dynamical and statistical laws in physics, on the one hand, and between the classical and quantum mechanics, on the other hand, are discussed with emphasis on the new…Boris Chirikov·Apr 30, 1997SaveLearn
On the low-dimensional modelling of Stratonovich stochastic differential equationsWe develop further ideas on how to construct low-dimensional models of stochastic dynamical systems. The aim is to derive a consistent and accurate model from the originally high-dimensional system.…Chao Xu, A. J. Roberts·Apr 30, 1997SaveLearn