782 research outputs found

    Longitudinal Losses Due to Breathing Mode Excitation in Radiofrequency Linear Accelerators

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    Transverse breathing mode oscillations in a particle beam can couple energy into longitudinal oscillations in a bunch of finite length and cause significant losses. We develop a model that illustrates this effect and explore the dependence on mismatch size, space-charge tune depression, longitudinal focusing strength, bunch length, and RF bucket length

    Glycine/Glycolic acid based copolymers

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    Glycine/glycolic acid based biodegradable copolymers have been prepared by ring-opening homopolymerization of morpholine-2,5-dione, and ring-opening copolymerization of morpholine-2,5-dione and glycolide. The homopolymerization of morpholine-2,5-dione was carried out in the melt at 200°C for 3 min using stannous octoate as an initiator, and continued at lower reaction temperatures (100-160°C) for 2-48 h. The highest yields (60%) and intrinsic viscosities ([] = 0.50 dL/g; DMSO, 25°C) were obtained after 3 min reaction at 200°C and 17 h at 130°C using a molar ratio of monomer and initiator of 1000. The polymer prepared by homopolymerization of morpholine-2,5-dione was composed of alternating glycine and glycolic acid residues, and had a glass transition temperature of 67°C and a melting temperature of 199°C. Random copolymers of glycine and glycolic acid were synthesized by copolymerization of morpholine-2,5-dione and glycolide in the melt at 200°C, followed by 17 h reaction at 130°C using stannous octoate as an initiator. The morphology of the copolymers varied from semi-crystalline to amorphous, depending on the mole fraction of glycolic acid residues incorporated

    Total destruction of invariant tori for the generalized Frenkel-Kontorova model

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    We consider generalized Frenkel-Kontorova models on higher dimensional lattices. We show that the invariant tori which are parameterized by continuous hull functions can be destroyed by small perturbations in the CrC^r topology with r<1r<1

    Chaotic versus stochastic behavior in active-dissipative nonlinear systems

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    We study the dynamical state of the one-dimensional noisy generalized Kuramoto-Sivashinsky (gKS) equation by making use of time-series techniques based on symbolic dynamics and complex networks. We focus on analyzing temporal signals of global measure in the spatiotemporal patterns as the dispersion parameter of the gKS equation and the strength of the noise are varied, observing that a rich variety of different regimes, from high-dimensional chaos to pure stochastic behavior, emerge. Permutation entropy, permutation spectrum, and network entropy allow us to fully classify the dynamical state exposed to additive noise

    On the importance of nonlinear modeling in computer performance prediction

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    Computers are nonlinear dynamical systems that exhibit complex and sometimes even chaotic behavior. The models used in the computer systems community, however, are linear. This paper is an exploration of that disconnect: when linear models are adequate for predicting computer performance and when they are not. Specifically, we build linear and nonlinear models of the processor load of an Intel i7-based computer as it executes a range of different programs. We then use those models to predict the processor loads forward in time and compare those forecasts to the true continuations of the time seriesComment: Appeared in "Proceedings of the 12th International Symposium on Intelligent Data Analysis

    Topological properties and fractal analysis of recurrence network constructed from fractional Brownian motions

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    Many studies have shown that we can gain additional information on time series by investigating their accompanying complex networks. In this work, we investigate the fundamental topological and fractal properties of recurrence networks constructed from fractional Brownian motions (FBMs). First, our results indicate that the constructed recurrence networks have exponential degree distributions; the relationship between HH and canberepresentedbyacubicpolynomialfunction.Wenextfocusonthemotifrankdistributionofrecurrencenetworks,sothatwecanbetterunderstandnetworksatthelocalstructurelevel.Wefindtheinterestingsuperfamilyphenomenon,i.e.therecurrencenetworkswiththesamemotifrankpatternbeinggroupedintotwosuperfamilies.Last,wenumericallyanalyzethefractalandmultifractalpropertiesofrecurrencenetworks.Wefindthattheaveragefractaldimension can be represented by a cubic polynomial function. We next focus on the motif rank distribution of recurrence networks, so that we can better understand networks at the local structure level. We find the interesting superfamily phenomenon, i.e. the recurrence networks with the same motif rank pattern being grouped into two superfamilies. Last, we numerically analyze the fractal and multifractal properties of recurrence networks. We find that the average fractal dimension of recurrence networks decreases with the Hurst index HH of the associated FBMs, and their dependence approximately satisfies the linear formula ≈2−H \approx 2 - H. Moreover, our numerical results of multifractal analysis show that the multifractality exists in these recurrence networks, and the multifractality of these networks becomes stronger at first and then weaker when the Hurst index of the associated time series becomes larger from 0.4 to 0.95. In particular, the recurrence network with the Hurst index H=0.5H=0.5 possess the strongest multifractality. In addition, the dependence relationships of the average information dimension andtheaveragecorrelationdimension and the average correlation dimension on the Hurst index HH can also be fitted well with linear functions. Our results strongly suggest that the recurrence network inherits the basic characteristic and the fractal nature of the associated FBM series.Comment: 25 pages, 1 table, 15 figures. accepted by Phys. Rev.

    Hopf Bifurcations in a Watt Governor With a Spring

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    This paper pursues the study carried out by the authors in "Stability and Hopf bifurcation in a hexagonal governor system", focusing on the codimension one Hopf bifurcations in the hexagonal Watt governor differential system. Here are studied the codimension two, three and four Hopf bifurcations and the pertinent Lyapunov stability coefficients and bifurcation diagrams, ilustrating the number, types and positions of bifurcating small amplitude periodic orbits, are determined. As a consequence it is found an open region in the parameter space where two attracting periodic orbits coexist with an attracting equilibrium point.Comment: 30 pages and 7 figure

    Classical field theory. Advanced mathematical formulation

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    In contrast with QFT, classical field theory can be formulated in strict mathematical terms of fibre bundles, graded manifolds and jet manifolds. Second Noether theorems provide BRST extension of this classical field theory by means of ghosts and antifields for the purpose of its quantization.Comment: 30 p

    A Tool to Recover Scalar Time-Delay Systems from Experimental Time Series

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    We propose a method that is able to analyze chaotic time series, gained from exp erimental data. The method allows to identify scalar time-delay systems. If the dynamics of the system under investigation is governed by a scalar time-delay differential equation of the form dy(t)/dt=h(y(t),y(t−τ0))dy(t)/dt = h(y(t),y(t-\tau_0)), the delay time τ0\tau_0 and the functi on hh can be recovered. There are no restrictions to the dimensionality of the chaotic attractor. The method turns out to be insensitive to noise. We successfully apply the method to various time series taken from a computer experiment and two different electronic oscillators

    Symmetries of degenerate center singularities of plane vector fields

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    Let DD be a closed unit 22-disk on the plane centered at the origin OO, and FF be a smooth vector field such that OO is a unique singular point of FF and all other orbits of FF are simple closed curves wrapping once around OO. Thus topologically OO is a "center" singularity. Let also Diff(F)\mathrm{Diff}(F) be the group of all diffeomorphisms of DD which preserve orientation and orbits of FF. In arXiv:0907.0359 the author described the homotopy type of Diff(F)\mathrm{Diff}(F) under assumption that the 11-jet of FF at OO is non-degenerate. In this paper degenerate case is considered. Under additional "non-degeneracy assumptions" on FF the path components of Diff(F)\mathrm{Diff}(F) with respect to distinct weak topologies are described.Comment: 21 page, 3 figure
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