75 research outputs found

    Quasi-linear Stokes phenomenon for the second Painlev\'e transcendent

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    Using the Riemann-Hilbert approach, we study the quasi-linear Stokes phenomenon for the second Painlev\'e equation yxx=2y3+xy−αy_{xx}=2y^3+xy-\alpha. The precise description of the exponentially small jump in the dominant solution approaching α/x\alpha/x as ∣x∣→∞|x|\to\infty is given. For the asymptotic power expansion of the dominant solution, the coefficient asymptotics is found.Comment: 19 pages, LaTe

    Quasi-linear Stokes phenomenon for the Painlev\'e first equation

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    Using the Riemann-Hilbert approach, the Ψ\Psi-function corresponding to the solution of the first Painleve equation, yxx=6y2+xy_{xx}=6y^2+x, with the asymptotic behavior y∼±−x/6y\sim\pm\sqrt{-x/6} as ∣x∣→∞|x|\to\infty is constructed. The exponentially small jump in the dominant solution and the coefficient asymptotics in the power-like expansion to the latter are found.Comment: version accepted for publicatio

    Viscous shocks in Hele-Shaw flow and Stokes phenomena of the Painleve I transcendent

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    In Hele-Shaw flows at vanishing surface tension, the boundary of a viscous fluid develops cusp-like singularities. In recent papers [1, 2] we have showed that singularities trigger viscous shocks propagating through the viscous fluid. Here we show that the weak solution of the Hele-Shaw problem describing viscous shocks is equivalent to a semiclassical approximation of a special real solution of the Painleve I equation. We argue that the Painleve I equation provides an integrable deformation of the Hele-Shaw problem which describes flow passing through singularities. In this interpretation shocks appear as Stokes level-lines of the Painleve linear problem.Comment: A more detailed derivation is include

    On the location of poles for the Ablowitz-Segur family of solutions to the second Painlev\'e equation

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    Using a simple operator-norm estimate we show that the solution to the second Painlev\'e equation within the Ablowitz-Segur family is pole-free in a well defined region of the complex plane of the independent variable. The result is illustrated with several numerical examples.Comment: 8 pages, to appear in Nonlinearit

    Phase Shift in the Whitham Zone for the Gurevich-Pitaevskii Special Solution of the Korteweg-de Vries Equation

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    We get the leading term of the Gurevich-Pitaevskii special solution to the KdV equation in the oscillation zone without using averaging methods.Comment: 13 pages, 3 figure

    On the Linearization of the First and Second Painleve' Equations

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    We found Fuchs--Garnier pairs in 3X3 matrices for the first and second Painleve' equations which are linear in the spectral parameter. As an application of our pairs for the second Painleve' equation we use the generalized Laplace transform to derive an invertible integral transformation relating two its Fuchs--Garnier pairs in 2X2 matrices with different singularity structures, namely, the pair due to Jimbo and Miwa and the one found by Harnad, Tracy, and Widom. Together with the certain other transformations it allows us to relate all known 2X2 matrix Fuchs--Garnier pairs for the second Painleve' equation with the original Garnier pair.Comment: 17 pages, 2 figure

    Hard loss of stability in Painlev\'e-2 equation

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    A special asymptotic solution of the Painlev\'e-2 equation with small parameter is studied. This solution has a critical point t∗t_* corresponding to a bifurcation phenomenon. When t<t∗t<t_* the constructed solution varies slowly and when t>t∗t>t_* the solution oscillates very fast. We investigate the transitional layer in detail and obtain a smooth asymptotic solution, using a sequence of scaling and matching procedures

    Asymptotics for a special solution to the second member of the Painleve I hierarchy

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    We study the asymptotic behavior of a special smooth solution y(x,t) to the second member of the Painleve I hierarchy. This solution arises in random matrix theory and in the study of Hamiltonian perturbations of hyperbolic equations. The asymptotic behavior of y(x,t) if x\to \pm\infty (for fixed t) is known and relatively simple, but it turns out to be more subtle when x and t tend to infinity simultaneously. We distinguish a region of algebraic asymptotic behavior and a region of elliptic asymptotic behavior, and we obtain rigorous asymptotics in both regions. We also discuss two critical transitional asymptotic regimes.Comment: 19 page
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