Band Husimi Distributions and the Classical-Quantum Correspondence on the TorusBand Husimi distributions (BHDs) are introduced in the quantum-chaos problem on a toral phase space. In the framework of this phase space, a quantum state must satisfy Bloch boundary conditions (BCs)…Itzhack Dana, Yaakov Rutman, Mario Feingold·Sep 27, 1998SaveLearn
Weak Quantum ErgodicityWe examine the consequences of classical ergodicity for the localization properties of individual quantum eigenstates in the classical limit. We note that the well known Schnirelman result is a…L. Kaplan, E. J. Heller·Sep 25, 1998SaveLearn
Instability and Chaos in Non-Linear Wave Interaction: a simple modelWe analyze stability of a system which contains an harmonic oscillator non-linearly coupled to its second harmonic, in the presence of a driving force. It is found that there always exists a critical…I. M. Khalatnikov, M. Kroyter·Sep 23, 1998SaveLearn
Maps for analysis of nonlinear dynamicsArea preserving maps provide the simplest and most accurate means to visualize and quantify the behavior of nonlinear systems. Convenience of the mapping equations of motion for investigation of…B. Kaulakys·Sep 23, 1998SaveLearn
Normal forms and complex periodic orbits in semiclassical expansions of Hamiltonian systemsBifurcations of periodic orbits as an external parameter is varied are a characteristic feature of generic Hamiltonian systems. Meyer's classification of normal forms provides a powerful tool to…P. Leboeuf, A. Mouchet·Sep 18, 1998SaveLearn
Critical Behavior of Period Doublings in Coupled Inverted PendulumsWe study the critical behaviors of period doublings in N (N=2,3,4,...) coupled inverted pendulums by varying the driving amplitude A and the coupling strength c. It is found that the critical…Sang-Yoon Kim, Bambi Hu·Sep 17, 1998SaveLearn
Scar and Antiscar Quantum Effects in Open Chaotic SystemsWe predict and numerically observe strong periodic orbit effects in the properties of open quantum systems with a chaotic classical limit. Antiscars lead to a large number of exponentially narrow…L. Kaplan·Sep 12, 1998SaveLearn
Wavefunction Intensity Statistics from Unstable Periodic OrbitsWe examine the effect of short unstable periodic orbits on wavefunction statistics in a classically chaotic system, and find that the tail of the wavefunction intensity distribution in phase space is…L. Kaplan·Sep 12, 1998SaveLearn
Linear and Nonlinear Theory of Eigenfunction ScarsThe theory of scarring of eigenfunctions of classically chaotic systems by short periodic orbits is extended in several ways. The influence of short-time linear recurrences on correlations and…L. Kaplan, E. J. Heller·Sep 11, 1998SaveLearn
Passive advection in nonlinear mediumForced advection of passive tracer, θ, in nonlinear relaxational medium by large scale (Batchelor problem) incompressible velocity field at scales less than the correlation length of the flow and…Michael Chertkov·Sep 11, 1998SaveLearn
Correspondence between classical dynamics and energy level spacing distribution in the transition billiard systemsThe Robnik billiard is investigated in detail both classically and quantally in the transition range from integrable to almost chaotic system. We find out that a remarkable correspondence between…Soo-Young Lee, Sunghwan Rim, Eui-Soon Yim et al.·Sep 5, 1998SaveLearn
Overcoming the wall in the semiclassical baker's mapA major barrier in semiclassical calculations is the sheer number of terms that contribute as time increases; for classically chaotic dynamics, the proliferation is exponential. We have been able to…L. Kaplan, E. J. Heller·Sep 4, 1998SaveLearn
Semiclassical dynamical localization and the multiplicative semiclassical propagatorWe describe an iterative approach to computing long-time semiclassical dynamics in the presence of chaos, which eliminates the need for summing over an exponentially large number of classical paths,…L. Kaplan·Sep 4, 1998SaveLearn
Multiplicative semiclassical dynamics and the quantization timeWe study smooth, caustic-free, chaotic semiclassical dynamics on two-dimensional phase space and find that the dynamics can be approached by an iterative procedure which constructs an approximation…L. Kaplan·Sep 4, 1998SaveLearn
Eigenvalue statistics in quantum ideal gasesThe eigenvalue statistics of quantum ideal gases with single particle energies en=nα are studied. A recursion relation for the partition function allows to calculate the mean density of states…B. Eckhardt·Sep 4, 1998SaveLearn
Spectral properties of non-hydrogenic atoms in weak external fieldsWe study how the ionic core in a non-hydrogenic atom modifies the dynamics of a Rydberg electron in the presence of a weak static external field. We show that such a system is neither regular nor…T. Jonckheere, B. Gremaud, D. Delande·Sep 2, 1998SaveLearn
Cantorian Fractal Spacetime and Quantum-like Chaos in Neural Networks of the Human BrainThe neural networks of the human brain act as very efficient parallel processing computers co-ordinating memory related responses to a multitude of input signals from sensory organs. Information…A. M. Selvam·Sep 2, 1998SaveLearn
A Cell Dynamical System Model for Thundercloud ElectrificationA cell dynamical system model is developed for thundercloud electrification by consideration of microscopic domain eddy dynamical processes in the atmospheric boundary layer (ABL). This…A. M. Selvam·Sep 1, 1998SaveLearn
Expansion-modificaction systems: an explanation for long range correlations in DNABased on a model first studied in [Physical Review A, vol. 43, 5240-5260,1991] properties of correlation function for expansion-modification systems are developed. The existence of several…R. Mansilla, G. Cocho·Aug 31, 1998SaveLearn
A Langevin equation for the energy cascade in fully-developed turbulenceExperimental data from a turbulent jet flow is analysed in terms of an additive, continuous stochastic process where the usual time variable is replaced by the scale. We show that the energy transfer…Philippe Marcq, Antoine Naert·Aug 25, 1998SaveLearn
On the Heat Transfer in Rayleigh-Benard systemsIn this paper we discuss some theoretical aspects concerning the scaling laws of the Nusselt number versus the Rayleigh number in a Rayleigh-Benard cell. We present a new set of numerical simulations…R. Benzi, F. Toschi, R. Tripiccione·Aug 23, 1998SaveLearn
Transitions to quantum chaos in a generic one-parameter family of billiardsGeneric one-parameter billiards are studied both classically and quantally. The classical dynamics for the billiards makes a transition from regular to fully chaotic motion through intermediary soft…Sunghwan Rim, Soo-Young Lee, Eui-Soon Yim et al.·Aug 21, 1998SaveLearn
Hyperchaos synchronization with a zero driving variableFor the first time an example of hyperchaos synchronization with a zero driving variable using the system's parameters changes, proposed by L.Zonghua and C.Shigang (Phys.Rev.E, 55, 6651 (1997))…E. M. Shahverdiev·Aug 20, 1998SaveLearn
Frustrated synchronization in competing drive-response coupled chaotic systemsChaotic systems can be synchronized by linking them to a common signal, subject to certain conditions. However, the presence of multiple driving signals coming from different systems, give rise to…Sitabhra Sinha·Aug 19, 1998SaveLearn
Border Collision Bifurcations in Two Dimensional Piecewise Smooth MapsRecent investigations on the bifurcations in switching circuits have shown that many atypical bifurcations can occur in piecewise smooth maps which can not be classified among the generic cases like…Soumitro Banerjee, Celso Grebogi·Aug 14, 1998SaveLearn