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Showing papers by "Jean-Pierre Eckmann published in 1999"


Journal ArticleDOI
TL;DR: In this paper, the authors studied the statistical mechanics of a finite-dimensional non-linear Hamiltonian system coupled to two heat baths and proved the existence of steady states under suitable assumptions on the potential and the coupling between the chain and the heat baths.
Abstract: We study the statistical mechanics of a finite-dimensional non-linear Hamiltonian system (a chain of anharmonic oscillators) coupled to two heat baths (described by wave equations). Assuming that the initial conditions of the heat baths are distributed according to the Gibbs measures at two different temperatures we study the dynamics of the oscillators. Under suitable assumptions on the potential and on the coupling between the chain and the heat baths, we prove the existence of an invariant measure for any temperature difference, i.e., we prove the existence of steady states. Furthermore, if the temperature difference is sufficiently small, we prove that the invariant measure is unique and mixing. In particular, we develop new techniques for proving the existence of invariant measures for random processes on a non-compact phase space. These techniques are based on an extension of the commutator method of Hormander used in the study of hypoelliptic differential operators.

335 citations


Journal ArticleDOI
TL;DR: In this paper, the authors consider a finite chain of nonlinear oscillators coupled at its ends to two infinite heat baths which are at different temperatures and show rigorously that for arbitrary temperature differences and arbitrary couplings, such a system has a unique stationary state.
Abstract: We consider a finite chain of nonlinear oscillators coupled at its ends to two infinite heat baths which are at different temperatures. Using our earlier results about the existence of a stationary state, we show rigorously that for arbitrary temperature differences and arbitrary couplings, such a system has a unique stationary state. (This extends our earlier results for small temperature differences.) In all these cases, any initial state will converge (at an unknown rate) to the stationary state. We show that this stationary state continually produces entropy. The rate of entropy production is strictly negative when the temperatures are unequal and is proportional to the mean energy flux through the system

164 citations


Journal ArticleDOI
TL;DR: In this paper, the authors consider the global attracting set (i.e., the forward map of the set of bounded initial data), and restrict it to a cube Q L of side L. The set of solutions of the complex Ginzburg-Landau equation in R d, d < 3.
Abstract: We study the set of solutions of the complex Ginzburg–Landau equation in R d , d <3. We consider the global attracting set (i.e., the forward map of the set of bounded initial data), and restrict it to a cube Q L of side L. We cover this set by a (minimal) number N Q L (ɛ) of balls of radius ɛ in $L infin(Q L ). We show that the Kolmogorov ɛ-entropy per unit length, \(\) exists. In particular, we bound \(\) by \(\), which shows that the attracting set is smaller than the set of bounded analytic functions in a strip. We finally give a positive lower bound: \(\).

42 citations


Posted Content
TL;DR: In this article, the authors study the implications of translation invariance on the tangent dynamics of extended dynamical systems, within a random matrix approximation, and show the existence of hydrodynamic modes in the slowly growing part of the Lyapunov spectrum.
Abstract: We study the implications of translation invariance on the tangent dynamics of extended dynamical systems, within a random matrix approximation. In a model system, we show the existence of hydrodynamic modes in the slowly growing part of the Lyapunov spectrum, which are analogous to the hydrodynamic modes discovered numerically by [Dellago, Ch., Posch, H.A., Hoover, W.G., Phys. Rev. E 53, 1485 (1996)]. The hydrodynamic Lyapunov vectors loose the typical random structure and exhibit instead the structure of weakly perturbed coherent long wavelength waves. We show further that the amplitude of the perturbations vanishes in the thermodynamic limit, and that the associated Lyapunov exponents are universal.

41 citations


Journal ArticleDOI
TL;DR: The topological entropy per unit volume in parabolic PDEs such as the complex Ginzburg-Landau equation is defined, and it is shown that it exists and is bounded by the upper Hausdorff dimension times the maximal expansion rate.
Abstract: We define the topological entropy per unit volume in parabolic PDEs such as the complex Ginzburg-Landau equation, and show that it exists and is bounded by the upper Hausdorff dimension times the maximal expansion rate. We then give a constructive implementation of a bound on the inertial range of such equations. Using this bound, we are able to propose a finite sampling algorithm which allows (in principle) to measure this entropy from experimental data. AMS classification number: 35B37

33 citations


Journal ArticleDOI
TL;DR: In this article, it was shown that on the global attracting set $G$ the topological entropy of damped hyperbolic equations on the infinite line exists in the topology of a bounded domain in position space and for large momenta.
Abstract: We study damped hyperbolic equations on the infinite line. We show that on the global attracting set $G$ the $\epsilon$-entropy (per unit length) exists in the topology of $W^{1,\infty}$. We also show that the topological entropy per unit length of $G$ exists. These results are shown using two main techniques: Bounds in bounded domains in position space and for large momenta, and a novel submultiplicativity argument in $W^{1,\infty}$.

14 citations


Journal ArticleDOI
TL;DR: In this paper, the authors studied the model of a strongly non-linear chain of particles coupled to two heat baths at different temperatures and proved the existence and uniqueness of a stationary state at all temperatures.
Abstract: We study the model of a strongly non-linear chain of particles coupled to two heat baths at different temperatures. Our main result is the existence and uniqueness of a stationary state at all temperatures. This result extends those of Eckmann, Pillet, Rey-Bellet to potentials with essentially arbitrary growth at infinity. This extension is possible by introducing a stronger version of H\"ormander's theorem for Kolmogorov equations to vector fields with polynomially bounded coefficients on unbounded domains.

5 citations


Book ChapterDOI
TL;DR: In this article, the authors explain the implications of a mathematical theory (by the same authors) of holes in fractals and their relation to dimension for measurements, and consider the fractal measure on a set rather than just the support of that measure.
Abstract: This paper explains the implications of a mathematical theory (by the same authors) of holes in fractals and their relation to dimension for measurements The novelty of our approach is to consider the fractal measure on a set rather than just the support of that measure This should take into account in a more precise way the distribution of data points in measured sets, such as the distribution of galaxies

1 citations


Journal ArticleDOI
TL;DR: In this paper, the authors introduce a concept of porosity for measures and study relations between dimensions and porosities for two classes of measures: measures on $R^n$ which satisfy the doubling condition and strongly porous measures on$R$
Abstract: We introduce a concept of porosity for measures and study relations between dimensions and porosities for two classes of measures: measures on $R^n$ which satisfy the doubling condition and strongly porous measures on $R$.