The Sylvester equation and the elliptic Korteweg-de Vries system

preprint2015arXivOpen access

Abstract

The elliptic Korteweg-de Vries (KdV) system is a multi-component generalization of the lattice potential KdV equation, whose soliton solutions are associated with an elliptic Cauchy kernel (i.e., a Cauchy kernel on the torus). In this paper we generalize the class of solutions by using a Sylvester type matrix equation and rederiving the system from the associated Cauchy matrix. Our starting point is the Sylvester equation in the form of  kM+Mk=rcT−gK−1rcTK−1~\boldsymbol{k} \boldsymbol{M}+ \boldsymbol{M} \boldsymbol{k} = \boldsymbol{r} {\boldsymbol{c}}^{T}-g\boldsymbol{K}^{-1} \boldsymbol{r} {\boldsymbol{c}}^{T} \boldsymbol{K}^{-1} where k\boldsymbol{k} and K\boldsymbol{K} are commutative matrices and obey the matrix relation k2=K+3e1I+gK−1{\boldsymbol{k}}^2=\boldsymbol{K}+3e_1\boldsymbol{I}+g{\boldsymbol{K}}^{-1}. The obtained elliptic equations, both discrete and continuous, are formulated by the scalar function S(i,j)S^{(i,j)} which is defined using (k,K,M,r,c)(\boldsymbol{k},\boldsymbol{K}, \boldsymbol{M}, \boldsymbol{r},\boldsymbol{c}) and constitute an infinite size symmetric matrix. Lax pairs for both the discrete and continuous system are derived. The explicit solution M\boldsymbol{M} of the Sylvester equation and generalized solutions of the obtained elliptic equations are presented according to the canonical forms of matrix k\boldsymbol{k}.

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