53,023 research outputs found

    Dynamical Anomalous Subvarieties: Structure and Bounded Height Theorems

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    According to Medvedev and Scanlon, a polynomial f(x)Qˉ[x]f(x)\in \bar{\mathbb Q}[x] of degree d2d\geq 2 is called disintegrated if it is not linearly conjugate to xdx^d or ±Cd(x)\pm C_d(x) (where Cd(x)C_d(x) is the Chebyshev polynomial of degree dd). Let nNn\in\mathbb{N}, let f1,,fnQˉ[x]f_1,\ldots,f_n\in \bar{\mathbb Q}[x] be disintegrated polynomials of degrees at least 2, and let φ=f1××fn\varphi=f_1\times\ldots\times f_n be the corresponding coordinate-wise self-map of (P1)n({\mathbb P}^1)^n. Let XX be an irreducible subvariety of (P1)n({\mathbb P}^1)^n of dimension rr defined over Qˉ\bar{\mathbb Q}. We define the \emph{φ\varphi-anomalous} locus of XX which is related to the \emph{φ\varphi-periodic} subvarieties of (P1)n({\mathbb P}^1)^n. We prove that the φ\varphi-anomalous locus of XX is Zariski closed; this is a dynamical analogue of a theorem of Bombieri, Masser, and Zannier \cite{BMZ07}. We also prove that the points in the intersection of XX with the union of all irreducible φ\varphi-periodic subvarieties of (P1)n({\mathbb P}^1)^n of codimension rr have bounded height outside the φ\varphi-anomalous locus of XX; this is a dynamical analogue of Habegger's theorem \cite{Habegger09} which was previously conjectured in \cite{BMZ07}. The slightly more general self-maps φ=f1××fn\varphi=f_1\times\ldots\times f_n where each fiQˉ(x)f_i\in \bar{\mathbb Q}(x) is a disintegrated rational map are also treated at the end of the paper.Comment: Minor mistakes corrected, slight reorganizatio

    The Yukawa Coupling in Three Dimensions

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    We consider several renormalizable, scale free models in three space-time dimensions which involve scalar and spinor fields. The Yukawa couplings are bilinear in both the spinor and scalar fields and the potential is of sixth order in the scalar field. In a model with a single scalar field and a complex Fermion field in three Euclidean dimensions, the couplings in the theory are both asymptotically free. This property is not retained in 2+1 dimensional Minkowski space, as we illustrate by considering a renormalizable scale-free supersymmetric model. This is on account of the different properties of the Dirac matrices in Euclidean and Minkowski space. We also examine a model in 2+1 dimensional Minkowski space in which two species of Fermions, associated with the two unitarily inequivalent representations of the 2×22 \times 2 Dirac matrices, couple in two different ways to two distinct scalar fields. There are two types of Yukawa couplings in this model, and either one or the other of them can be asymptotically free (but not both simultaneously).Comment: 15 pages RevTex, uses epsfig.st

    Wearable Sensor Data Based Human Activity Recognition using Machine Learning: A new approach

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    Recent years have witnessed the rapid development of human activity recognition (HAR) based on wearable sensor data. One can find many practical applications in this area, especially in the field of health care. Many machine learning algorithms such as Decision Trees, Support Vector Machine, Naive Bayes, K-Nearest Neighbor, and Multilayer Perceptron are successfully used in HAR. Although these methods are fast and easy for implementation, they still have some limitations due to poor performance in a number of situations. In this paper, we propose a novel method based on the ensemble learning to boost the performance of these machine learning methods for HAR

    Coherent coupling between surface plasmons and excitons in semiconductor nanocrystals

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    We present an experimental demonstration of strong coupling between a surface plasmon propagating on a planar silver substrate, and the lowest excited state of CdSe nanocrystals. Variable-angle spectroscopic ellipsometry measurements demonstrated the formation of plasmon-exciton mixed states, characterized by a Rabi splitting of \sim 82 meV at room temperature. Such a coherent interaction has the potential for the development of plasmonic non-linear devices, and furthermore, this system is akin to those studied in cavity quantum electrodynamics, thus offering the possibility to study the regime of strong light-matter coupling in semiconductor nanocrystals at easily accessible experimental conditions.Comment: 12 pages, 4 figure
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