Abstract:In this paper, we show that the expansion of linear problems of the Painlevé equation in powers of the spectral variable can be used to derive hierarchies of ordinary differential equations. We applied this approach to linear problems of the first, second, third and fourth Painlevé equations. We derived a new hierarchy of the third Painlevé equation and rederived known hierarchies of the other equations. Moreover some special solutions of the hierarchies of the second, third and fourth Painlevé equations are a… Show more
“…The rogue wave of order k = 0 coincides with the background solution. Indeed, if k = 0, then the solution of Riemann-Hilbert Problem 1 is In verifying the jump condition (11) one should make use of the fact that the first three factors appearing on the second line of the right-hand side in (15) combine, perhaps despite appearances, to form an entire function U(λ; x, t) of λ: noting that analyticity follows because sin(θ)/θ and cos(θ) are even in θ and hence entire functions of θ 2 = (λ 2 + 1)(x + λt) 2 . Applying the formula (14) for k = 0 then gives (17) In [1], the conditions of Riemann-Hilbert Problem 1 were translated into a finite-dimensional linear algebra problem via a suitable rational ansatz for the matrix M (k) (λ; x, t)E(λ) −1 in the exterior domain that builds in poles of order n at λ = ±i (only visible upon analytic continuation into the interior domain through Σ • ).…”
We study the fundamental rogue wave solutions of the focusing nonlinear Schrödinger equation in the limit of large order. Using a recently-proposed Riemann-Hilbert representation of the rogue wave solution of arbitrary order k, we establish the existence of a limiting profile of the rogue wave in the large-k limit when the solution is viewed in appropriate rescaled variables capturing the near-field region where the solution has the largest amplitude. The limiting profile is a new particular solution of the focusing nonlinear Schrödinger equation in the rescaled variables -the rogue wave of infinite order -which also satisfies ordinary differential equations with respect to space and time. The spatial differential equations are identified with certain members of the Painlevé-III hierarchy. We compute the far-field asymptotic behavior of the near-field limit solution and compare the asymptotic formulae with the exact solution with the help of numerical methods for solving Riemann-Hilbert problems. In a certain transitional region for the asymptotics the near field limit function is described by a specific globally-defined tritronquée solution of the Painlevé-II equation. These properties lead us to regard the rogue wave of infinite order as a new special function.
“…The rogue wave of order k = 0 coincides with the background solution. Indeed, if k = 0, then the solution of Riemann-Hilbert Problem 1 is In verifying the jump condition (11) one should make use of the fact that the first three factors appearing on the second line of the right-hand side in (15) combine, perhaps despite appearances, to form an entire function U(λ; x, t) of λ: noting that analyticity follows because sin(θ)/θ and cos(θ) are even in θ and hence entire functions of θ 2 = (λ 2 + 1)(x + λt) 2 . Applying the formula (14) for k = 0 then gives (17) In [1], the conditions of Riemann-Hilbert Problem 1 were translated into a finite-dimensional linear algebra problem via a suitable rational ansatz for the matrix M (k) (λ; x, t)E(λ) −1 in the exterior domain that builds in poles of order n at λ = ±i (only visible upon analytic continuation into the interior domain through Σ • ).…”
We study the fundamental rogue wave solutions of the focusing nonlinear Schrödinger equation in the limit of large order. Using a recently-proposed Riemann-Hilbert representation of the rogue wave solution of arbitrary order k, we establish the existence of a limiting profile of the rogue wave in the large-k limit when the solution is viewed in appropriate rescaled variables capturing the near-field region where the solution has the largest amplitude. The limiting profile is a new particular solution of the focusing nonlinear Schrödinger equation in the rescaled variables -the rogue wave of infinite order -which also satisfies ordinary differential equations with respect to space and time. The spatial differential equations are identified with certain members of the Painlevé-III hierarchy. We compute the far-field asymptotic behavior of the near-field limit solution and compare the asymptotic formulae with the exact solution with the help of numerical methods for solving Riemann-Hilbert problems. In a certain transitional region for the asymptotics the near field limit function is described by a specific globally-defined tritronquée solution of the Painlevé-II equation. These properties lead us to regard the rogue wave of infinite order as a new special function.
“…. defined by R p j (x) p ℓ (x)|x| 2α e − dx = h j (n, k, α)δ jℓ 23[1, Appendix B] and[17, Exercise 4.4]): p 2j (u; 2n, k, α) = p j (u 2 ; n, k, α − 1/2), (7.27) p 2j+1 (u; 2n, k, α) = up j (u 2 ; n, k, α + 1/2).…”
We study unitary invariant random matrix ensembles with singular potentials. We obtain asymptotics for the partition functions associated to the Laguerre and Gaussian Unitary Ensembles perturbed with a pole of order k at the origin, in the double scaling limit where the size of the matrices grows, and at the same time the strength of the pole decreases at an appropriate speed. In addition, we obtain double scaling asymptotics of the correlation kernel for a general class of ensembles of positive-definite Hermitian matrices perturbed with a pole. Our results are described in terms of a hierarchy of higher order analogues to the Painlevé III equation, which reduces to the Painlevé III equation itself when the pole is simple.
“…In the present article, we generalize known Bäcklund transformations of the first and second Painlevé equations to the first and second Painlevé hierarchies given in [6,11]. We give a Bäcklund transformation between the considered first Painlevé hierarchy and a new hierarchy of Painlevé-type equations.…”
Section: Introductionmentioning
confidence: 94%
“…Moreover its members may define new transcendental functions. The PI hierarchy (2.1) can be written in the following form [11]…”
Section: Bäcklund Transformations For Pi Hierarchymentioning
Abstract. We give Bäcklund transformations for first and second Painlevé hierarchies. These Bäcklund transformations are generalization of known Bäcklund transformations of the first and second Painlevé equations and they relate the considered hierarchies to new hierarchies of Painlevé-type equations.
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