Noise-correlation-time-mediated localization in random nonlinear dynamical systemsWe investigate the behavior of the residence times density function for different nonlinear dynamical systems with limit cycle behavior and perturbed parametrically with a colored noise. We present…Juan L. Cabrera, J. Gorro~nogoitia, F. J. de la Rubia·Mar 10, 1999SaveLearn
Transport in finite size systems: an exit time approachIn the framework of chaotic scattering we analyze passive tracer transport in finite systems. In particular, we study models with open streamlines and a finite number of recirculation zones. In the…P. Castiglione, M. Cencini, A. Vulpiani et al.·Mar 9, 1999SaveLearn
Disentangling Scaling Properties in Anisotropic and Inhomogeneous TurbulenceWe address scaling in inhomogeneous and anisotropic turbulent flows by decomposing structure functions into their irreducible representation of the SO(3) symmetry group which are designated by j,m…I. Arad, L. Biferale, I. Mazzitelli et al.·Mar 9, 1999SaveLearn
Defect-freezing and Defect-unbinding in the Vector Complex Ginzburg-Landau EquationWe describe the dynamical behavior found in numerical solutions of the Vector Complex Ginzburg-Landau equation in parameter values where plane waves are stable. Topological defects in the system are…Miguel Hoyuelos, Emilio Hernandez-Garcia, Pere Colet et al.·Mar 8, 1999SaveLearn
Past events never come backTime can be defined as the duration between events. It is irreversible. When used as a variable in quantifying the changing properties of matter, this irreversibility of time is incompatible with…X. de Hemptinne·Mar 8, 1999SaveLearn
Improvement of SNR with Chaotic Spreading Sequences for CDMAWe show that chaotic spreading sequences generated by ergodic mappings of Chebyshev orthogonal polynomials have better correlation properties for CDMA(code division multiple access) than the optimal…Ken Umeno, Ken-ichi Kitayama·Mar 8, 1999SaveLearn
Chaotic Dynamics in Iterated Map Neural Networks with Piecewise Linear Activation FunctionThe paper examines the discrete-time dynamics of neuron models (of excitatory and inhibitory types) with piecewise linear activation functions, which are connected in a network. The properties of a…Sitabhra Sinha·Mar 6, 1999SaveLearn
A hypothesis concerning "quantal" Hilbert space criterion of chaos in nonlinear dynamical systemsBased on the Hilbert space approach to the theory of nonlinear dynamical systems developed by the author a hypothesis is formulated concerning the "quantal" criterion for classical ordinary…Krzysztof Kowalski·Mar 6, 1999SaveLearn
Spectral reduction: a statistical description of turbulenceA method is described for predicting statistical properties of turbulence. Collections of Fourier amplitudes are represented by nonuniformly spaced modes with enhanced coupling coefficients. The…John C. Bowman, B. A. Shadwick, P. J. Morrison·Mar 5, 1999SaveLearn
Statistical Theory of Energy Transfer to Small and Chaotic Quantum Systems Induced by a Slowly-Varying External FieldWe study nonequilibrium properties of small and chaotic quantum systems, i.e., non-integrable systems whose size is small in the sense that the separations of energy levels are non-negligible as…Yasuhiro Higashiyama, Akira Shimizu·Mar 4, 1999SaveLearn
Quantum chaos of a kicked particle in a 1D infinite square potential wellWe study quantum chaos in a non-KAM system, i.e. a kicked particle in a one-dimensional infinite square potential well. Within the perturbative regime the classical phase space displays stochastic…Baowen Li, Jie Liu, Yan Gu et al.·Mar 3, 1999SaveLearn
Energy Absorption and Storage in a Hamiltonian System in Partial Contact with a Heat BathTo understand the mechanism allowing for long-term storage of excess energy in proteins, we study a Hamiltonian system consisting of several coupled pendula in partial contact with a heat bath. It is…Naoko Nakagawa, Kunihiko Kaneko·Mar 2, 1999SaveLearn
Vibrating soap films: An analog for quantum chaos on billiardsWe present an experimental setup based on the normal modes of vibrating soap films which shows quantum features of integrable and chaotic billiards. In particular, we obtain the so-called scars…E. Arcos, G. Baez, P. A. Cuatlayol et al.·Mar 2, 1999SaveLearn
Chaotic Monte Carlo computation: a dynamical effect of random-number generationsIt is shown that superefficient Monte Carlo computations can be carried out by using chaotic dynamical systems as non-uniform random-number generators. Here superefficiency means that the expectation…Ken Umeno·Mar 2, 1999SaveLearn
A semiclassical theory of dissipative Henon-Heiles systemA semiclassical theory of dissipative Henon-Heiles system is proposed. Based on -scaling of an equation for evolution of Wigner quasiprobability distribution function in presence of…Bidhan Chandra Bag, Deb Shankar Ray·Feb 27, 1999SaveLearn
Periodic Orbit Quantization of Mixed Regular Chaotic SystemsA general technique for the periodic orbit quantization of systems with near-integrable to mixed regular-chaotic dynamics is introduced. A small set of periodic orbits is sufficient for the…J. Main, G. Wunner·Feb 27, 1999SaveLearn
A unifying definition of synchronization for dynamical systemsWe propose a unified definition for synchronization. By example we show that the synchronization phenomena discussed in the dynamical systems literature can be described within the framework of this…Reggie Brown, Ljupco Kocarev·Feb 27, 1999SaveLearn
Spatiotemporal Chaos, Localized Structures and Synchronization in the Vector Complex Ginzburg-Landau EquationWe study the spatiotemporal dynamics, in one and two spatial dimensions, of two complex fields which are the two components of a vector field satisfying a vector form of the complex Ginzburg-Landau…Emilio Hernandez-Garcia, Miguel Hoyuelos, Pere Colet et al.·Feb 24, 1999SaveLearn
Trace Formulas and Bogomolny's Transfer OperatorThe trace formulas commonly used in discussing spectral properties of quantum or wave systems are derived simply and directly from the Bogomolny transfer operator. Special cases are the Gutzwiller…Oleg Zaitsev, R. Narevich, R. E. Prange·Feb 23, 1999SaveLearn
Comment on "Entropy Generation in Computation and the Second law of Thermodynamics", by S. Ishioka and N. FuchikamiThis brief note argues that, contrary to the claim of Ishioka and Fuchikami (chao-dyn/9902012), Landauer's principle is concerned a priori with entropy generation in computing processes. The…Hugo Touchette·Feb 19, 1999SaveLearn
Localization and Fluctuations in Quantum Kicked RotorsWe address the issue of fluctuations, about an exponential lineshape, in a pair of one-dimensional kicked quantum systems exhibiting dynamical localization. An exact renormalization scheme…Indubala I. Satija, Bala Sundaram, Jukka A. Ketoja·Feb 18, 1999SaveLearn
Direct Numerical Simulations of the Navier-Stokes Alpha ModelWe explore the utility of the recently proposed alpha equations in providing a subgrid model for fluid turbulence. Our principal results are comparisons of direct numerical simulations of fluid…Shiyi Chen, Darryl D. Holm, Len G. Margolin et al.·Feb 18, 1999SaveLearn
Entropy Generation in Computation and the Second Law of ThermodynamicsLandauer discussed the minimum energy necessary for computation and stated that erasure of information is accompanied by heat generation to the amount of kT ln2/bit. Modifying the above statement, we…Shunya Ishioka, Nobuko Fuchikami·Feb 17, 1999SaveLearn
Renormalization group method and canonical perturbation theoryRenormalization group method is one of the most powerful tool to obtain approximate solutions to differential equations. We apply the renormalization group method to Hamiltonian systems whose…Yoshiyuki Y. Yamaguchi, Yasusada Nambu·Feb 16, 1999SaveLearn
Passive scalar intermittency in compressible flowA compressible generalization of the Kraichnan model (Phys. Rev. Lett. 72, 1016 (1994)) of passive scalar advection is considered. The dynamical role of compressibility on the intermittency of the…A. Celani, A. Lanotte, A. Mazzino·Feb 12, 1999SaveLearn