Searcharxiv⌕ Search

arXiv · nlin/0606069

Coisotropic deformations of associative algebras and dispersionless integrable hierarchies

Abstract

The paper is an inquiry of the algebraic foundations of the theory of dispersionless integrable hierarchies, like the dispersionless KP and modified KP hierarchies and the universal Whitham's hierarchy of genus zero. It stands out for the idea of interpreting these hierarchies as equations of coisotropic deformations for the structure constants of certain associative algebras. It discusses the link between the structure constants and the Hirota's tau function, and shows that the dispersionless Hirota's bilinear equations are, within this approach, a way of writing the associativity conditions for the structure constants in terms of the tau function. It also suggests a simple interpretation of the algebro-geometric construction of the universal Whitham's equations of genus zero due to Krichever.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

B. G. Konopelchenko, F. Magri. 2006-07-04. Coisotropic deformations of associative algebras and dispersionless integrable hierarchies. https://doi.org/10.1007/s00220-007-0295-2

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

The $\mathrm{al}_{ab}$ functions of hyperelliptic curves: a generalization of Jacobi's elliptic functions and explicit solutions of a degenerate Krichever-Novikov equation

The Jacobi elliptic functions $\mathrm{sn}$, $\mathrm{cn}$, $\mathrm{dn}$ and their ratios are expressed by Weierstrass's functions $\mathrm{al}_a=\sqrt{x-b_a}$ of an elliptic curve. For a hyperelliptic curve of genus $g$, Weierstrass's $\mathrm{al}_a$ functions generalize $\mathrm{sn}$, $\mathrm{cn}$ and $\mathrm{dn}$, and the modified Korteweg-de Vries and sine-Gordon equations stand behind them. In this paper we study the $\mathrm{al}_{ab}$ functions, which are defined by the sigma function shifted by the sum of two half-periods and which, together with the ratios of the $\mathrm{al}_a$ functions, generalize the remaining Jacobi elliptic functions. We determine the exact lattice of periods of $\mathrm{al}_{12}$ and show that it is single-valued on the unramified double covering of the Jacobian corresponding to the double covering $\hat{w}^2=(x-b_1)(x-b_2)$ of the curve. We show that $\mathrm{al}_{12}$ is the Wronskian of the band-edge eigenfunctions $\mathrm{al}_1$ and $\mathrm{al}_2$, so that the half-period translations realize Darboux transformations. As the main result, $\mathrm{al}_{12}$, $\mathrm{al}_2/\mathrm{al}_1$ and $1/\mathrm{al}_{12}$ satisfy one and the same degenerate Krichever-Novikov equation, whose polynomial has the double roots $0$ and $\infty$, and the half-periods act on these solutions as the Möbius symmetries of the equation. Thus the Krichever-Novikov equation stands behind the $\mathrm{al}_{ab}$ functions. In genus one these functions reduce to $\mathrm{sn}$, $\mathrm{ns}$ and $\mathrm{dc}$.

nlin.SI↗

The integer spectrum of a superintegrable quantum field theory

In our previous article CMP 407 (2026) 131, we explored the rich algebraic structures arising from a specific quantum many-body Hamiltonian quartic in the bosonic creation-annihilation operators. This Hamiltonian originated from the works of Gérard and Grellier on classical turbulent energy transfer in a Lax-integrable setting, and its quantum version respects hierarchies of polynomial conservation laws all of which possess purely integer spectra, as does the Hamiltonian itself. The latter feature, known from numerical studies, has previously remained unproved. Here, we present an elementary solution of the quantum Gérard-Grellier Hamiltonian. The eigenstates are labelled by partitions and the corresponding eigenvalues admit simple explicit expressions in terms of the principal hook lengths. The key ingredient in this construction is a specific basis we introduce, inspired by the classical multisoliton coherent states, in which the Hamiltonian is upper-triangular. The expressions for the eigenvalues then immediately follow, while the full eigenbasis can be recovered via a Gram-Schmidt procedure.

nlin.SI↗

The \texorpdfstring{$\mathbf N$-soliton}{N-soliton} solution formula for the Kaup--Kupershmidt equation

An explicit formula is presented for the $\mathbf N$-soliton solution to the Kaup--Kupershmidt equation, for any positive integer $\mathbf N,$ by using the input data set consisting of $\mathbf N$ distinct positive $p_j$-values and $\mathbf N$ arbitrarily chosen positive $c_j$-values. The formula is derived from the solution to the inverse scattering problem for a third-order linear operator in the reflectionless case with the $p_j$-values related to the bound-state poles of a transmission coefficient and the $c_j$-values related to the bound-state dependency constants. It is indicated how the formula is constructed from the solution to a Riemann--Hilbert problem and from the solution to a Marchenko integral equation used in the formulation of the aforementioned inverse scattering problem.

nlin.SI↗