387 research outputs found

    Feynman integrals for a class of exponentially growing potentials

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    We construct the Feynman integrands for a class of exponentially growing time-dependent potentials as white noise functionals. We show that they solve the Schroedinger equation. The Morse potential is considered as a special case

    The truncated discrete moment problem from one to infinite dimensions

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    The discrete truncated moment problem considers the question whether given a discrete subsets KRK \subset \mathbb{R} and a sequence of real numbers one can find a measure supported on KK whose (power) moments are exactly these numbers. The truncated moment is a challenging problem. We derive a minimal set of necessary and sufficient conditions. This simple problem is surprisingly hard and not treatable with known techniques. Applications to the truncated moment problem for point processes, the so-called relizability or representability problem are given. This is a joint work with M. Infusino, J. Lebowitz and E. Speer

    Marked Gibbs measures via cluster expansion

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    We give a sufficiently detailed account on the construction of marked Gibbs measures in the high temperature and low fugacity regime. This is proved for a wide class of underlying spaces and potentials such that stability and integrability conditions are satisfied. That is, for state space we take a locally compact separable metric space XX and a separable metric space SS for the mark space. This framework allowed us to cover several models of classical and quantum statistical physics. Furthermore, we also show how to extend the construction for more general spaces as e.g., separable standard Borel spaces. The construction of the marked Gibbs measures is based on the method of cluster expansion.Comment: 51 page

    Towards a General Theory of Extremes for Observables of Chaotic Dynamical Systems

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    In this paper we provide a connection between the geometrical properties of a chaotic dynamical system and the distribution of extreme values. We show that the extremes of so-called physical observables are distributed according to the classical generalised Pareto distribution and derive explicit expressions for the scaling and the shape parameter. In particular, we derive that the shape parameter does not depend on the chosen observables, but only on the partial dimensions of the invariant measure on the stable, unstable, and neutral manifolds. The shape parameter is negative and is close to zero when high-dimensional systems are considered. This result agrees with what was derived recently using the generalized extreme value approach. Combining the results obtained using such physical observables and the properties of the extremes of distance observables, it is possible to derive estimates of the partial dimensions of the attractor along the stable and the unstable directions of the flow. Moreover, by writing the shape parameter in terms of moments of the extremes of the considered observable and by using linear response theory, we relate the sensitivity to perturbations of the shape parameter to the sensitivity of the moments, of the partial dimensions, and of the Kaplan-Yorke dimension of the attractor. Preliminary numerical investigations provide encouraging results on the applicability of the theory presented here. The results presented here do not apply for all combinations of Axiom A systems and observables, but the breakdown seems to be related to very special geometrical configurations.Comment: 16 pages, 3 Figure

    Linear and fractional response for the SRB measure of smooth hyperbolic attractors and discontinuous observables

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    We consider a smooth one-parameter family t(ft:MM)t\mapsto (f_t:M\to M) of diffeomorphisms with compact transitive Axiom A attractors Λt\Lambda_t, denoting by dρtd \rho_t the SRB measure of ftΛtf_t|_{\Lambda_t}. Our first result is that for any function θ\theta in the Sobolev space Hpr(M)H^r_p(M), with 1<p<1<p<\infty and 0<r<1/p0<r<1/p, the map tθdρtt\mapsto \int \theta\, d\rho_t is α\alpha-H\"older continuous for all α<r\alpha <r. This applies to θ(x)=h(x)Θ(g(x)a)\theta(x)=h(x)\Theta(g(x)-a) (for all α<1\alpha <1) for hh and gg smooth and Θ\Theta the Heaviside function, if aa is not a critical value of gg. Our second result says that for any such function θ(x)=h(x)Θ(g(x)a)\theta(x)=h(x)\Theta(g(x)-a) so that in addition the intersection of {xg(x)=a}\{ x\mid g(x)=a\} with the support of hh is foliated by ``admissible stable leaves'' of ftf_t, the map tθdρtt\mapsto \int \theta\, d\rho_t is differentiable. (We provide distributional linear response and fluctuation-dissipation formulas for the derivative.) Obtaining linear response or fractional response for such observables θ\theta is motivated by extreme-value theory

    Translation invariant realizability problem on the d-dimensional lattice: an explicit construction

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    We consider a particular instance of the truncated realizability problem on the d−dimensional lattice. Namely, given two functions ρ1(i) and ρ2(i,j) non-negative and symmetric on Zd, we ask whether they are the first two correlation functions of a translation invariant point process. We provide an explicit construction of such a realizing process for any d ≥ 2 when the radial distribution has a specific form. We also derive from this construction a lower bound for the maximal realizable density and compare it with the already known lower bounds
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