19 research outputs found

    Performance Analysis of Classification Algorithms for Activity Recognition using Micro-Doppler Feature

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    Classification of different human activities using micro-Doppler data and features is considered in this study, focusing on the distinction between walking and running. 240 recordings from 2 different human subjects were collected in a series of simulations performed in the real motion data from the Carnegie Mellon University Motion Capture Database. The maximum the micro-Doppler frequency shift and the period duration are utilized as two classification criterions. Numerical results are compared against several classification techniques including the Linear Discriminant Analysis (LDA), Naïve Bayes (NB), K-nearest neighbors (KNN), Support Vector Machine(SVM) algorithms. The performance of different classifiers is discussed aiming at identifying the most appropriate features for the walking and running classification

    Lyapunov exponents of the half-line SHE

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    We consider the half-line stochastic heat equation (SHE) with Robin boundary parameter A=−12A = -\frac{1}{2}. Under narrow wedge initial condition, we compute every positive (including non-integer) Lyapunov exponents of the half-line SHE. As a consequence, we prove a large deviation principle for the upper tail of the half-line KPZ equation under Neumann boundary parameter A=−12A = -\frac{1}{2} with rate function Φ+hf(s)=23s32\Phi_+^{\text{hf}} (s) = \frac{2}{3} s^{\frac{3}{2}}. This confirms the prediction of [Krajenbrink and Le Doussal 2018] and [Meerson, Vilenkin 2018] for the upper tail exponent of the half-line KPZ equation.Comment: 25 page

    KPZ equation with a small noise, deep upper tail and limit shape

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    In this paper, we consider the KPZ equation under the weak noise scaling. That is, we introduce a small parameter ε\sqrt{\varepsilon} in front of the noise and let ε→0\varepsilon \to 0. We prove that the one-point large deviation rate function has a 32\frac{3}{2} power law in the deep upper tail. Furthermore, by forcing the value of the KPZ equation at a point to be very large, we prove a limit shape of the KPZ equation as ε→0\varepsilon \to 0. This confirms the physics prediction in Kolokolov and Korshunov (2007), Kolokolov and Korshunov (2009), Meerson, Katzav, and Vilenkin (2016), Kamenev, Meerson, and Sasorov (2016), and Le Doussal, Majumdar, Rosso, and Schehr (2016).Comment: 22 pages, 1 figur
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