22,088 research outputs found

    An Averaging Theorem for Perturbed KdV Equation

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    We consider a perturbed KdV equation: [\dot{u}+u_{xxx} - 6uu_x = \epsilon f(x,u(\cdot)), \quad x\in \mathbb{T}, \quad\int_\mathbb{T} u dx=0.] For any periodic function u(x)u(x), let I(u)=(I1(u),I2(u),...)R+I(u)=(I_1(u),I_2(u),...)\in\mathbb{R}_+^{\infty} be the vector, formed by the KdV integrals of motion, calculated for the potential u(x)u(x). Assuming that the perturbation ϵf(x,u())\epsilon f(x,u(\cdot)) is a smoothing mapping (e.g. it is a smooth function ϵf(x)\epsilon f(x), independent from uu), and that solutions of the perturbed equation satisfy some mild a-priori assumptions, we prove that for solutions u(t,x)u(t,x) with typical initial data and for 0tϵ10\leqslant t\lesssim \epsilon^{-1}, the vector I(u(t))I(u(t)) may be well approximated by a solution of the averaged equation.Comment: 25 page

    On long time dynamics of perturbed KdV equations

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    Consider perturbed KdV equations: ut+uxxx6uux=ϵf(u()),xT=R/Z,  Tu(x,t)dx=0,u_t+u_{xxx}-6uu_x=\epsilon f(u(\cdot)),\quad x\in\mathbb{T}=\mathbb{R}/\mathbb{Z},\;\int_{\mathbb{T}}u(x,t)dx=0, where the nonlinearity defines analytic operators u()f(u())u(\cdot)\mapsto f(u(\cdot)) in sufficiently smooth Sobolev spaces. Assume that the equation has an ϵ\epsilon-quasi-invariant measure μ\mu and satisfies some additional mild assumptions. Let uϵ(t)u^{\epsilon}(t) be a solution. Then on time intervals of order ϵ1\epsilon^{-1}, as ϵ0\epsilon\to0, its actions I(uϵ(t,))I(u^{\epsilon}(t,\cdot)) can be approximated by solutions of a certain well-posed averaged equation, provided that the initial datum is μ\mu-typical

    Long-time dynamics of resonant weakly nonlinear CGL equations

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    Consider a weakly nonlinear CGL equation on the torus~Td\mathbb{T}^d: u_t+i\Delta u=\epsilon [\mu(-1)^{m-1}\Delta^{m} u+b|u|^{2p}u+ ic|u|^{2q}u].\eqno{(*)} Here u=u(t,x)u=u(t,x), xTdx\in\mathbb{T}^d, 0<ϵ<<10<\epsilon<<1, μ0\mu\geqslant0, b,cRb,c\in\mathbb{R} and m,p,qNm,p,q\in\mathbb{N}. Define \mbox{I(u)=(I_{\dk},\dk\in\mathbb{Z}^d)}, where I_{\dk}=v_{\dk}\bar{v}_{\dk}/2 and v_{\dk}, \dk\in\mathbb{Z}^d, are the Fourier coefficients of the function~uu we give. Assume that the equation ()(*) is well posed on time intervals of order ϵ1\epsilon^{-1} and its solutions have there a-priori bounds, independent of the small parameter. Let u(t,x)u(t,x) solve the equation ()(*). If ϵ\epsilon is small enough, then for tϵ1t\lesssim\epsilon^{-1}, the quantity I(u(t,x))I(u(t,x)) can be well described by solutions of an {\it effective equation}: ut=ϵ[μ(1)m1Δmu+F(u)],u_t=\epsilon[\mu(-1)^{m-1}\Delta^m u+ F(u)], where the term F(u)F(u) can be constructed through a kind of resonant averaging of the nonlinearity bu2p+icu2qub|u|^{2p}+ ic|u|^{2q}u

    KdV equation under periodic boundary conditions and its perturbations

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    In this paper we discuss properties of the KdV equation under periodic boundary conditions, especially those which are important to study perturbations of the equation. Next we review what is known now about long-time behaviour of solutions for perturbed KdV equations

    Story Ending Generation with Incremental Encoding and Commonsense Knowledge

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    Generating a reasonable ending for a given story context, i.e., story ending generation, is a strong indication of story comprehension. This task requires not only to understand the context clues which play an important role in planning the plot but also to handle implicit knowledge to make a reasonable, coherent story. In this paper, we devise a novel model for story ending generation. The model adopts an incremental encoding scheme to represent context clues which are spanning in the story context. In addition, commonsense knowledge is applied through multi-source attention to facilitate story comprehension, and thus to help generate coherent and reasonable endings. Through building context clues and using implicit knowledge, the model is able to produce reasonable story endings. context clues implied in the post and make the inference based on it. Automatic and manual evaluation shows that our model can generate more reasonable story endings than state-of-the-art baselines.Comment: Accepted in AAAI201

    Nearly circular domains which are integrable close to the boundary are ellipses

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    The Birkhoff conjecture says that the boundary of a strictly convex integrable billiard table is necessarily an ellipse. In this article, we consider a stronger notion of integrability, namely integrability close to the boundary, and prove a local version of this conjecture: a small perturbation of an ellipse of small eccentricity which preserves integrability near the boundary, is itself an ellipse. This extends the result in [1], where integrability was assumed on a larger set. In particular, it shows that (local) integrability near the boundary implies global integrability. One of the crucial ideas in the proof consists in analyzing Taylor expansion of the corresponding action-angle coordinates with respect to the eccentricity parameter, deriving and studying higher order conditions for the preservation of integrable rational caustics.Comment: 64 pages, 3 figures. Final revised version, to appear on Geometric and Functional Analysis (GAFA

    A Three-Pole Substrate Integrated Waveguide Bandpass Filter Using New Coupling Scheme

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    A novel three-pole substrate integrated waveguide (SIW) bandpass filter (BPF) using new coupling scheme is proposed in this paper. Two high order degenerate modes (TE102 and TE201) of a square SIW cavity and a dominant mode (TE101) of a rectangular SIW cavity are coupled to form a three-pole SIW BPF. The coupling scheme of the structure is given and analyzed. Due to the coupling between two cavities, as well as the coupling between source and load, three transmission zeros are created in the stopband of the filter. The proposed three-pole SIW BPF is designed and fabricated. Good agreement between simulated and measured results verifies the validity of the design methodology well
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