Titlebook: Microscopic Aspects of Nonlinearity in Condensed Matter; A. R. Bishop,V. L. Pokrovsky,V. Tognetti Book 1991 Plenum Press, New York 1991 co

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Statistical Properties of the Transition to Spatiotemporal Chaosced by the non-linear interaction of a small number of degrees of freedom. In spatially extended systems low dimensional chaos is often associated with relevant spatial effects, such as mode competition, travelling waves, localized oscillations., but the unpredictable time evolution does not influen

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Defects and Order to Disorder Transition in Non-Equilibrium Structuressystem is a convective fluid driven to turbulence. Both the stationary and time-dependent homogeneous ordered states may become unstable against localized perturbations which create defects. Then, the defects may contribute either to the disorganization of the states, or they may mediate rapid trans

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From Chaos to Quasicrystalstiling with 5—fold symmetry has been published years before.. And even very wide popularization of it by M. Gardner in Physics Today. was not enough to convince a lot of crystallographists that the pentagonal tiling exists. We should not forget the unsuccessful efforts of I. Kepler to solve this pro

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A Model of a Catalytic Reaction with Local Interactionsis paper we consider the reaction (1) described by the simple irreversible model: . where. denotes the gaseous species; * stands for an empty site and “_” represents a nearest neighbor (.) bond on the surface (hereafter a square lattice).

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Polarons in Quasi-One-Dimensional Materialsto drag along its polarization cloud. This combined entity of an electron (or hole) and its polarization cloud is commonly refered to as a polaron. The energy gain due to the interaction with the medium is the polaron binding energy and the increased inertia is associated with an increased polaron m