On the deformation of linear Hamiltonian systems

preprint2021arXivOpen access

Abstract

For linear Hamiltonian 2n×2n2n\times 2n systems Jy′(x)=(λW(x)+H(x))y(x)J y'(x) = (λW(x)+H(x))y(x) we investigate the problem how the eigenvalues λλ depend on the entries of the coefficient matrix HH. This question turns into a deformation equation for HH and a partial differential equation for the eigenvalues λλ. We apply our results to various examples, including generalizations of the confluent Heun equation and the Chandrasekhar-Page angular equation. We are mainly concerned with the 2×22\times 2 case, and in order to reduce the degrees of freedom in HH as much as possible, we will first convert such systems into a complementary triangular form, which is a canonical form with a minimum number of free parameters. Furthermore, we discuss relations to monodromy preserving deformations and to matrix Lax pairs.

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