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Том 196, № 2 (2018)

Article

Nonlocal Symmetries of Integrable Linearly Degenerate Equations: A Comparative Study

Baran H., Krasilshchik I., Morozov O., Vojčák P.

Аннотация

We continue the study of Lax integrable equations. We consider four three-dimensional equations: (1) the rdDym equation uty = uxuxy − uyuxx, (2) the Pavlov equation uyy = utx + uyuxx − uxuxy, (3) the universal hierarchy equation uyy = utuxy − uyutx, and (4) the modified Veronese web equation uty = utuxy − uyutx. For each equation, expanding the known Lax pairs in formal series in the spectral parameter, we construct two differential coverings and completely describe the nonlocal symmetry algebras associated with these coverings. For all four pairs of coverings, the obtained Lie algebras of symmetries manifest similar (but not identical) structures; they are (semi)direct sums of the Witt algebra, the algebra of vector fields on the line, and loop algebras, all of which contain a component of finite grading. We also discuss actions of recursion operators on shadows of nonlocal symmetries.

Theoretical and Mathematical Physics. 2018;196(2):1089-1110
pages 1089-1110 views

Zeros of Entire Functions and Related Systems of Infinitely Many Nonlinearly Coupled Evolution Equations

Calogero F.

Аннотация

Recent findings concerning the zeros of generic polynomials are extended to entire functions featuring infinitely many distinct zeros, and related systems of infinitely many nonlinearly coupled evolution ODEs and PDEs are identified, the solutions of which display interesting properties.

Theoretical and Mathematical Physics. 2018;196(2):1111-1128
pages 1111-1128 views

Higher-Order Dispersive Deformations of Multidimensional Poisson Brackets of Hydrodynamic Type

Casati M.

Аннотация

The theory of multidimensional Poisson vertex algebras provides a completely algebraic formalism for studying the Hamiltonian structure of partial differential equations for any number of dependent and independent variables. We compute the cohomology of the Poisson vertex algebras associated with twodimensional, two-component Poisson brackets of hydrodynamic type at the third differential degree. This allows obtaining their corresponding Poisson–Lichnerowicz cohomology, which is the main building block of the theory of their deformations. Such a cohomology is trivial neither in the second group, corresponding to the existence of a class of nonequivalent infinitesimal deformations, nor in the third group, corresponding to the obstructions to extending such deformations.

Theoretical and Mathematical Physics. 2018;196(2):1129-1149
pages 1129-1149 views

Skyrmion States in Chiral Liquid Crystals

De Matteis G., Martina L., Turco V.

Аннотация

We analyze static configurations for chiral liquid crystals in the framework of the Oseen–Frank theory. In particular, we find numerical solutions for localized axisymmetric states in confined chiral liquid crystals with weak homeotropic anchoring at the boundaries. These solutions describe the distortions of twodimensional skyrmions, known as either spherulites or cholesteric bubbles, which have been observed experimentally in these systems. We outline relations to nonlinear integrable equations and use the relations to study the asymptotic behavior of the solutions. Using analytic methods, we build approximate solutions of the equilibrium equations and analyze the generation and stabilization of these states in relation to the material parameters, external fields, and anchoring boundary conditions.

Theoretical and Mathematical Physics. 2018;196(2):1150-1163
pages 1150-1163 views

Matrix Kadomtsev–Petviashvili Equation: Tropical Limit, Yang–Baxter and Pentagon Maps

Dimakis A., Müller-Hoissen F.

Аннотация

In the tropical limit of matrix KP-II solitons, their support at a fixed time is a planar graph with “polarizations” attached to its linear parts. We explore a subclass of soliton solutions whose tropical limit graph has the form of a rooted and generically binary tree and also solutions whose limit graph comprises two relatively inverted such rooted tree graphs. The distribution of polarizations over the lines constituting the graph is fully determined by a parameter-dependent binary operation and a Yang–Baxter map (generally nonlinear), which becomes linear in the vector KP case and is hence given by an R-matrix. The parameter dependence of the binary operation leads to a solution of the pentagon equation, which has a certain relation to the Rogers dilogarithm via a solution of the hexagon equation, the next member in the family of polygon equations. A generalization of the R-matrix obtained in the vector KP case also solves a pentagon equation. A corresponding local version of the latter then leads to a new solution of the hexagon equation.

Theoretical and Mathematical Physics. 2018;196(2):1164-1173
pages 1164-1173 views

Multiparametric Families of Solutions of the Kadomtsev–Petviashvili-I Equation, the Structure of Their Rational Representations, and Multi-Rogue Waves

Gaillard P.

Аннотация

We construct solutions of the Kadomtsev–Petviashvili-I equation in terms of Fredholm determinants. We deduce solutions written as a quotient of Wronskians of order 2N. These solutions, called solutions of order N, depend on 2N−1 parameters. They can also be written as a quotient of two polynomials of degree 2N(N +1) in x, y, and t depending on 2N−2 parameters. The maximum of the modulus of these solutions at order N is equal to 2(2N + 1)2. We explicitly construct the expressions up to the order six and study the patterns of their modulus in the plane (x, y) and their evolution according to time and parameters.

Theoretical and Mathematical Physics. 2018;196(2):1174-1199
pages 1174-1199 views

A Direct Algorithm for Constructing Recursion Operators and Lax Pairs for Integrable Models

Habibullin I., Khakimova A.

Аннотация

We suggest an algorithm for seeking recursion operators for nonlinear integrable equations. We find that the recursion operator R can be represented as a ratio of the form R = L1−1 L2, where the linear differential operators L1 and L2 are chosen such that the ordinary differential equation (L2 −λL1)U = 0 is consistent with the linearization of the given nonlinear integrable equation for any value of the parameter λ ∈ C. To construct the operator L1, we use the concept of an invariant manifold, which is a generalization of a symmetry. To seek L2, we then take an auxiliary linear equation related to the linearized equation by a Darboux transformation. It is remarkable that the equation L1\(\tilde U\) = L2U defines a B¨acklund transformation mapping a solution U of the linearized equation to another solution \(\tilde U\) of the same equation. We discuss the connection of the invariant manifold with the Lax pairs and the Dubrovin equations.

Theoretical and Mathematical Physics. 2018;196(2):1200-1216
pages 1200-1216 views

Haantjes Manifolds with Symmetry

Magri F.

Аннотация

We introduce the definition of Haantjes manifolds with symmetry and explain why these manifolds appear in the theory of integrable systems of hydrodynamic type and in topological field theories.

Theoretical and Mathematical Physics. 2018;196(2):1217-1229
pages 1217-1229 views

Integrable Nonautonomous Liénard-Type Equations

Sinelshchikov D., Kudryashov N.

Аннотация

We study a family of nonautonomous generalized Liénard-type equations. We consider the equivalence problem via the generalized Sundman transformations between this family of equations and type-I Painlevé–Gambier equations. As a result, we find four criteria of equivalence, which give four integrable families of Liénard-type equations. We demonstrate that these criteria can be used to construct general traveling-wave and stationary solutions of certain classes of diffusion–convection equations. We also illustrate our results with several other examples of integrable nonautonomous Liénard-type equations.

Theoretical and Mathematical Physics. 2018;196(2):1230-1240
pages 1230-1240 views