384 research outputs found

    Super-resolution in turbulent videos: making profit from damage

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    It is shown that one can make use of local instabilities in turbulent video frames to enhance image resolution beyond the limit defined by the image sampling rate. The paper outlines the processing algorithm, presents its experimental verification on simulated and real-life videos and discusses its potentials and limitations.Comment: 11 pages, 2 figures. Submitted to Optics Letters, 10-07-0

    Dressing chain for the acoustic spectral problem

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    The iterations are studied of the Darboux transformation for the generalized Schroedinger operator. The applications to the Dym and Camassa-Holm equations are considered.Comment: 16 pages, 6 eps figure

    Discrete Darboux transformation for discrete polynomials of hypergeometric type

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    Darboux Transformation, well known in second order differential operator theory, is applied here to the difference equation satisfied by the discrete hypergeometric polynomials(Charlier, Meixner-Krawchuk, Hahn)

    Complete list of Darboux Integrable Chains of the form t1x=tx+d(t,t1)t_{1x}=t_x+d(t,t_1)

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    We study differential-difference equation of the form ddxt(n+1,x)=f(t(n,x),t(n+1,x),ddxt(n,x)) \frac{d}{dx}t(n+1,x)=f(t(n,x),t(n+1,x),\frac{d}{dx}t(n,x)) with unknown t(n,x)t(n,x) depending on continuous and discrete variables xx and nn. Equation of such kind is called Darboux integrable, if there exist two functions FF and II of a finite number of arguments xx, {t(n±k,x)}k=−∞∞\{t(n\pm k,x)\}_{k=-\infty}^\infty, dkdxkt(n,x)k=1∞{\frac{d^k}{dx^k}t(n,x)}_{k=1}^\infty, such that DxF=0D_xF=0 and DI=IDI=I, where DxD_x is the operator of total differentiation with respect to xx, and DD is the shift operator: Dp(n)=p(n+1)Dp(n)=p(n+1). Reformulation of Darboux integrability in terms of finiteness of two characteristic Lie algebras gives an effective tool for classification of integrable equations. The complete list of Darboux integrable equations is given in the case when the function ff is of the special form f(u,v,w)=w+g(u,v)f(u,v,w)=w+g(u,v)

    Discrete symmetry's chains and links between integrable equations

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    The discrete symmetry's dressing chains of the nonlinear Schrodinger equation (NLS) and Davey-Stewartson equations (DS) are consider. The modified NLS (mNLS) equation and the modified DS (mDS) equations are obtained. The explicitly reversible Backlund auto-transformations for the mNLS and mDS equations are constructed. We demonstrate discrete symmetry's conjugate chains of the KP and DS models. The two-dimensional generalization of the P4 equation are obtained.Comment: 20 page

    Nonlocal symmetries of integrable two-field divergent evolutionary systems

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    Nonlocal symmetries for exactly integrable two-field evolutionary systems of the third order have been computed. Differentiation of the nonlocal symmetries with respect to spatial variable gives a few nonevolutionary systems for each evolutionary system. Zero curvature representations for some new nonevolution systems are presented

    Towards the theory of integrable hyperbolic equations of third order

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    The examples are considered of integrable hyperbolic equations of third order with two independent variables. In particular, an equation is found which admits as evolutionary symmetries the Krichever--Novikov equation and the modified Landau--Lifshitz system. The problem of choice of dynamical variables for the hyperbolic equations is discussed.Comment: 22
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