Quantization of a billiard model for interacting particlesWe consider a billiard model of a self-bound, interacting three-body system in two spatial dimensions. Numerical studies show that the classical dynamics is chaotic. The corresponding quantum system…Thomas Papenbrock, Tomaz Prosen·May 6, 1999SaveLearn
Intermittency corrections to the mean square particle acceleration in high Reynolds number turbulenceThe mean square particle acceleration in high Reynolds number turbulence is dominated by the mean square pressure gradient. Recent experiments by Voth et al [Phys. Fluids 10, 2268 (1998)]…Mark Nelkin, Shiyi Chen·May 5, 1999SaveLearn
Correlations of electromagnetic fields in chaotic cavitiesWe consider the fluctuations of electromagnetic fields in chaotic microwave cavities. We calculate the transversal and longitudinal correlation function based on a random wave assumption and compare…B. Eckhardt, U. Dörr, U. Kuhl et al.·May 5, 1999SaveLearn
Stationarity and Redundancy of Multichannel EEG Data Recorded During Generalized Tonic-Clonic SeizuresA prerequisite for applying some signal analysis methods to electroencephalographic (EEG) data is that the data be statistically stationary. We have investigated the stationarity of 21-electrode…Scott M. Zoldi, Andrew Krystal, Henry S. Greenside·May 4, 1999SaveLearn
The Control of high-dimensional Chaos in Time-Delay SystemsWe present the control of the high-dimensional chaos, with possibly a large number of positive Lyapunov-exponents, of unknown time-delay systems to an arbitrary goal dynamics. We give an…M. J. Bünner·May 3, 1999SaveLearn
Stability Exponents, Separation of Variables, and Lyapunov TransformsThe problem of formulating self-consistent local and global stability exponents is shown to require global separation of variables. Posing the separation of variable problem, we see that many such…William E. Wiesel·May 3, 1999SaveLearn
Deciphering Secure Chaotic CommunicationA simple technique for decoding an unknown modulated chaotic time-series is presented. We point out that, by fitting a polynomial model to the modulated chaotic signal, the error in the fit gives…C. Mathiazhagan·May 3, 1999SaveLearn
Non Asymptotic Properties of Transport and MixingWe study relative dispersion of passive scalar in non-ideal cases, i.e. in situations in which asymptotic techniques cannot be applied; typically when the characteristic length scale of the Eulerian…G. Boffetta, A. Celani, M. Cencini et al.·Apr 29, 1999SaveLearn
Transition to turbulence in a shear flowWe analyze the properties of a 19 dimensional Galerkin approximation to a parallel shear flow. The laminar flow with a sinusoidal shape is stable for all Reynolds numbers Re. For sufficiently large…Bruno Eckhardt, Alois Mersmann·Apr 28, 1999SaveLearn
Distribution of Husimi Zeroes in Polygonal BilliardsThe zeroes of the Husimi function provide a minimal description of individual quantum eigenstates and their distribution is of considerable interest. We provide here a numerical study for pseudo-…Debabrata Biswas, Sudeshna Sinha·Apr 26, 1999SaveLearn
Random Roughness of Boundary Increases Turbulent Convection Scaling ExponentThe influence of the boundary layer properties on the heat transport in turbulent thermal convection is experimentally investigated in a cell with a rough bottom plate.It is shown that the standard…S. Ciliberto, C. Laroche·Apr 26, 1999SaveLearn
Extracting and Stabilizing the Unstable State of Hysteresis LoopA novel perturbation method for the stabilization of unstable intermediate states of hysteresis loop (i.e. S-shaped curve) is proposed. This method only needs output signals of the system to…Liu Yaowen, Ping Huican, Zhao Hong et al.·Apr 25, 1999SaveLearn
Self-similarity in a system with short-time delayed feedbackUsing the Poincaré section technique, we study in detail the dynamical behaviors of delay differential system and find a new type of solutions Si in short-time delay feedback. Our numerical…Liu Yaowen, Li Haibin, Zhao Hong et al.·Apr 25, 1999SaveLearn
Power Laws in Solar Flares: Self-Organized Criticality or Turbulence?We study the time evolution of Solar Flares activity by looking at the statistics of quiescent times τL between successive bursts. The analysis of 20 years of data reveals a power law…Guido Boffetta, Vincenzo Carbone, Paolo Giuliani et al.·Apr 23, 1999SaveLearn
Microscopic chaos from Brownian motion?A recent experiment on Brownian motion has been interpreted to exhibit direct evidence for microscopic chaos. In this note we demonstrate that virtually identical results can be obtained numerically…C. P. Dettmann, E. G. D. Cohen, H. van Beijeren·Apr 22, 1999SaveLearn
Quantization of multidimensional cat mapsIn this work we study cat maps with many degrees of freedom. Classical cat maps are classified using the Cayley parametrization of symplectic matrices and the closely associated center and chord…A. M. F. Rivas, M. Saraceno, A. M. Ozorio de Almeida·Apr 22, 1999SaveLearn
Semiclassical Non-Trace Type Formulas for Matrix Element Fluctuations and Weighted Densities of StatesDensities of states weighted with the diagonal matrix elements of two operators A and B, i.e., rho(A,B)(E) = sumn <n|A|n><n|B|n> delta(E-En) cannot, in general, be written as a trace formula, and…J. Main, G. Wunner·Apr 22, 1999SaveLearn
Semiclassical quantization with short periodic orbitsWe apply a recently developed semiclassical theory of short peridic orbits to the stadium billiard. We give explicit expresions for the resonances of periodic orbits and for the application of the…Eduardo G. Vergini, Gabriel Carlo·Apr 22, 1999SaveLearn
Semiclassical Theory of Short Periodic Orbits in Quantum ChaosWe have developed a semiclassical theory of short periodic orbits to obtain all quantum information of a bounded chaotic Hamiltonian system. If T1 is the period of the shortest periodic orbit, T2…Eduardo G. Vergini·Apr 22, 1999SaveLearn
Chaos as a basis of new principle for detecting the gravitational wavesA particular example of chaos can be conceived in the interaction of non-linear oscillator with a harmonic gravitational wave. When we replace the linear potential forces by the therm SIN(x), the…G. V. Vlasov·Apr 22, 1999SaveLearn
Influence of Friction on the Direct Cascade of the 2d Forced TurbulenceWe discuss two possible scenario for the direct cascade in two dimensional turbulent systems in presence of friction which differ by the presence or not of enstrophy dissipation in the inviscid…Denis Bernard·Apr 20, 1999SaveLearn
Porosities and dimensions of measures satisfying the doubling conditionSummary of a talk at the conference The Chaotic Universe in Rome, Feb, 1999Jean-Pierre Eckmann, Esa Jarvenpaa, Maarit Jarvenpaa·Apr 20, 1999SaveLearn
KAM Tori for 1D Nonlinear Wave Equations with Periodic Boundary ConditionsIn this paper, one-dimensional (1D) nonlinear wave equations utt -uxx+V(x)u =f(u), with periodic boundary conditions are considered; V is a periodic smooth or analytic function and the…Luigi Chierchia, Jaingong You·Apr 20, 1999SaveLearn
Birth of resonances in the spin-orbit problem of Celestial MechanicsThe behaviour of resonances in the spin-orbit coupling in Celestial Mechanics is investigated. We introduce a Hamiltonian nearly-integrable model describing an approximation of the spin-orbit…Alessandra Celletti, Luigi Chierchia·Apr 20, 1999SaveLearn
Helicoidal model for DNA openingWe present a new dynamical model of DNA. This model has two degrees of freedom per base-pair: one radial variable related to the opening of the hydrogen bonds and an angular one related to the…Maria Barbi, Simona Cocco, Michel Peyrard·Apr 19, 1999SaveLearn