Abstract:
A Hamiltonian system on a Poisson manifold $M$ is called integrable if it
possesses sufficiently many commuting first integrals $f_1, \dots f_s$
which are functionally independent on $M$ almost everywhere. We study
the structure of the singular set $K$ where the differentials $df_1,
\dots, df_s$ become linearly dependent and show that in the case of
bi-Hamiltonian systems this structure is closely related to the
properties of the corresponding pencil of compatible Poisson brackets.
The main goal of the paper is to illustrate this relationship and to show
that the bi-Hamiltonian approach can be extremely effective in the study
of singularities of integrable systems, especially in the case of many
degrees of freedom when using other methods leads to serious
computational problems. Since in many examples the underlying
bi-Hamiltonian structure has a natural algebraic interpretation, the
technology developed in this paper allows one to reformulate analytic and
topological questions related to the dynamics of a given system into pure
algebraic language, which leads to simple and natural answers.