30 research outputs found

    Upgrading the Local Ergodic Theorem for planar semi-dispersing billiards

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    The Local Ergodic Theorem (also known as the `Fundamental Theorem') gives sufficient conditions under which a phase point has an open neighborhood that belongs (mod 0) to one ergodic component. This theorem is a key ingredient of many proofs of ergodicity for billiards and, more generally, for smooth hyperbolic maps with singularities. However the proof of that theorem relies upon a delicate assumption (Chernov-Sinai Ansatz), which is difficult to check for some physically relevant models, including gases of hard balls. Here we give a proof of the Local Ergodic Theorem for two dimensional billiards without using the Ansatz.Comment: 17 pages, 2 figure

    The characteristic exponents of the falling ball model

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    We study the characteristic exponents of the Hamiltonian system of nn (2\ge 2) point masses m1,,mnm_1,\dots,m_n freely falling in the vertical half line {qq0}\{q|\, q\ge 0\} under constant gravitation and colliding with each other and the solid floor q=0q=0 elastically. This model was introduced and first studied by M. Wojtkowski. Hereby we prove his conjecture: All relevant characteristic (Lyapunov) exponents of the above dynamical system are nonzero, provided that m1mnm_1\ge\dots\ge m_n (i. e. the masses do not increase as we go up) and m1m2m_1\ne m_2

    Heat conduction and diffusion of hard disks in a narrow channel

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    Using molecular dynamics we study heat conduction and diffusion of hard disks in one dimensional narrow channels. When collisions preserve momentum the heat conduction κ\kappa diverges with the number of disks NN as κNα\kappa\sim N^\alpha (α1/3)(\alpha \approx 1/3). Such a behaviour is seen both when the ordering of disks is fixed ('pen-case' model), and when they can exchange their positions. Momentum conservation results also in sound-wave effects that enhance diffusive behaviour and on an intermediate time scale (that diverges in the thermodynamic limit) normal diffusion takes place even in the 'pen-case' model. When collisions do not preserve momentum, κ\kappa remains finite and sound-wave effects are absent.Comment: 4 pages, accepted in Phys.Rev.

    Proving The Ergodic Hypothesis for Billiards With Disjoint Cylindric Scatterers

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    In this paper we study the ergodic properties of mathematical billiards describing the uniform motion of a point in a flat torus from which finitely many, pairwise disjoint, tubular neighborhoods of translated subtori (the so called cylindric scatterers) have been removed. We prove that every such system is ergodic (actually, a Bernoulli flow), unless a simple geometric obstacle for the ergodicity is present.Comment: 24 pages, AMS-TeX fil

    On the complexity of curve fitting algorithms

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    We study a popular algorithm for fitting polynomial curves to scattered data based on the least squares with gradient weights. We show that sometimes this algorithm admits a substantial reduction of complexity, and, furthermore, find precise conditions under which this is possible. It turns out that this is, indeed, possible when one fits circles but not ellipses or hyperbolas.Comment: 8 pages, no figure

    Stable regimes for hard disks in a channel with twisting walls

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    We study a gas of NN hard disks in a box with semi-periodic boundary conditions. The unperturbed gas is hyperbolic and ergodic (these facts are proved for N=2 and expected to be true for all N2N\geq 2). We study various perturbations by twisting the outgoing velocity at collisions with the walls. We show that the dynamics tends to collapse to various stable regimes, however we define the perturbations and however small they are.Comment: 30 pages, final version to appear in "Chaos

    Approximating multi-dimensional Hamiltonian flows by billiards

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    Consider a family of smooth potentials VϵV_{\epsilon}, which, in the limit ϵ0\epsilon\to0, become a singular hard-wall potential of a multi-dimensional billiard. We define auxiliary billiard domains that asymptote, as ϵ0\epsilon\to0 to the original billiard, and provide asymptotic expansion of the smooth Hamiltonian solution in terms of these billiard approximations. The asymptotic expansion includes error estimates in the CrC^{r} norm and an iteration scheme for improving this approximation. Applying this theory to smooth potentials which limit to the multi-dimensional close to ellipsoidal billiards, we predict when the separatrix splitting persists for various types of potentials

    On the work distribution for the adiabatic compression of a dilute classical gas

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    We consider the adiabatic and quasi-static compression of a dilute classical gas, confined in a piston and initially equilibrated with a heat bath. We find that the work performed during this process is described statistically by a gamma distribution. We use this result to show that the model satisfies the non-equilibrium work and fluctuation theorems, but not the flucutation-dissipation relation. We discuss the rare but dominant realizations that contribute most to the exponential average of the work, and relate our results to potentially universal work distributions.Comment: 4 page

    Rotation sets of billiards with one obstacle

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    We investigate the rotation sets of billiards on the mm-dimensional torus with one small convex obstacle and in the square with one small convex obstacle. In the first case the displacement function, whose averages we consider, measures the change of the position of a point in the universal covering of the torus (that is, in the Euclidean space), in the second case it measures the rotation around the obstacle. A substantial part of the rotation set has usual strong properties of rotation sets
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