6,896 research outputs found

    Analytic Tate spaces and reciprocity laws

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    We consider a functional analytic variant of the notion of Tate space, namely the category of those topological vector spaces which have a direct sum decomposition where one summand is nuclear Frechet space and the other is the dual of a nuclear Frechet. We show that, both in the complex and in the p-adic setting, one can use this formalism to define symbols for analytic functions which satisfy Weil-type reciprocity laws

    On a twisted Reidemeister torsion

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    Given a finite simplicial complex, a unimodular representation of its fundamental group and a closed twisted cochain of odd degree, we define a twisted version of the Reidemeister torsion, extending a previous definition of V. Mathai and S. Wu. The main tool is a complex of piecewise smooth currents, defined by J. Dupont.Comment: References added, some points clarifie

    Shannon information, LMC complexity and Renyi entropies: a straightforward approach

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    The LMC complexity, an indicator of complexity based on a probabilistic description, is revisited. A straightforward approach allows us to establish the time evolution of this indicator in a near-equilibrium situation and gives us a new insight for interpreting the LMC complexity for a general non equilibrium system. Its relationship with the Renyi entropies is also explained. One of the advantages of this indicator is that its calculation does not require a considerable computational effort in many cases of physical and biological interest.Comment: 11 pages, 0 figure

    An approach to the problem of generating irreducible polynomials over the finite field GF(2) and its relationship with the problem of periodicity on the space of binary sequences

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    A method for generating irreducible polynomials of degree n over the finite field GF(2) is proposed. The irreducible polynomials are found by solving a system of equations that brings the information on the internal properties of the splitting field GF(2^n) . Also, the choice of a primitive normal basis allows us to build up a natural representation of GF(2^n) in the space of n-binary sequences. Illustrative examples are given for the lowest orders.Comment: 22 pages, 6 tables, 0 figure

    Complex Systems with Trivial Dynamics

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    In this communication, complex systems with a near trivial dynamics are addressed. First, under the hypothesis of equiprobability in the asymptotic equilibrium, it is shown that the (hyper) planar geometry of an NN-dimensional multi-agent economic system implies the exponential (Boltzmann-Gibss) wealth distribution and that the spherical geometry of a gas of particles implies the Gaussian (Maxwellian) distribution of velocities. Moreover, two non-linear models are proposed to explain the decay of these statistical systems from an out-of-equilibrium situation toward their asymptotic equilibrium states.Comment: 9 gaes, 0 figures; Contributed Talk to ECCS'12 (European Conference of Complex Systems, Brussels, September, 2012

    A motivation for some local cohomologies

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    We explain how some results of M. Nori (on motives) and F. Ivorra (on perverse motives) can be used to define "motivic" versions of Lyubeznik numbers, a set of numerical invariants for local rings. We also discuss on additional structures that might be put on some local cohomology modules (besides those of D- or F-module). This note is mainly expository, it is an expanded version of my talk at the FACARD workshop in Barcelona, on January 2019

    Bifurcation Curves of Limit Cycles in some Lienard Systems

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    Lienard systems of the form x¨+ϵf(x)x˙+x=0\ddot{x}+\epsilon f(x)\dot{x}+x=0, with f(x) an even continous function, are considered. The bifurcation curves of limit cycles are calculated exactly in the weak (ϵ→0\epsilon\to 0) and in the strongly (ϵ→∞\epsilon\to\infty) nonlinear regime in some examples. The number of limit cycles does not increase when ϵ\epsilon increases from zero to infinity in all the cases analyzed.Comment: 25 pages, 0 figures. Published in Int. Journal of Bifurcation and Chaos, vol. 10, 971-980 (2001

    On exponential sums

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    Let f be a polinomial with coefficients in a finite field F. Let Ψ:F→C∗\Psi : F \to C^{\ast} be a non-trivial additive character. In this paper we give bounds for the exponential sums ∑x∈FnΨ(TrF/Fp(f(x)))\sum_{x\in F^n} \Psi (Tr_{F/F_p} (f(x))) in some cases where the highest degree form of f defines a singular projective hypersurface X (e.g. when X is an arrangement of lines in P^2). The bound involves the Milnor numbers of the singularities of X. The proof goes via the classical cohomological interpretation of this exponential sums through Grothendieck's trace formula.Comment: Latex 2.09, 15 page

    The Limit Cycles of Lienard Equations in the Weakly Nonlinear Regime

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    Li\'enard equations of the form x¨+ϵf(x)x˙+x=0\ddot{x}+\epsilon f(x)\dot{x}+x=0, with f(x)f(x) an even function, are considered in the weakly nonlinear regime (ϵ→0\epsilon\to 0). A perturbative algorithm for obtaining the number, amplitude and shape of the limit cycles of these systems is given. The validity of this algorithm is shown and several examples illustrating its application are given. In particular, an O(ϵ8){\mathcal O}(\epsilon^8) approximation for the amplitude of the van der Pol limit cycle is explicitly obtained.Comment: 17 text-pages, 1 table, 6 figure

    Symmetry induced Dynamics in four-dimensional Models deriving from the van der Pol Equation

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    Different models of self-excited oscillators which are four-dimensional extensions of the van der Pol system are reported. Their symmetries are analyzed. Three of them were introduced to model the release of vortices behind circular cylinders with a possible transition from a symmetric to an antisymmetric Benard-von Karman vortex street. The fourth reported self-excited oscillator is a new model which implements the breaking of the inversion symmetry. It presents the phenomenon of second harmonic generation in a natural way. The parallelism with second harmonic generation in nonlinear optics is discussed. There is also a small region in the parameter space where the dynamics of this system is quasiperiodic or chaotic.Comment: 14 pages, 0 figure
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