Algebraic and geometric properties of quadratic Hamiltonians determined by sectional operators

Following the terminology introduced by V. V. Trofimov and A. T. Fomenko, we say that a self-adjoint operator $\varphi :\mathfrak{g}* \to \mathfrak{g}$ is sectional if it satisfies the identity ad _?x ^* a = ad _β ^* x, $x \in \mathfrak{g}*$ , where $\mathfrak{g}$ is a finite-dimensional Lie algebra and $a \in \mathfrak{g}*$ and $\beta \in \mathfrak{g}$ are fixed elements. In the case of a semisimple Lie algebra $\mathfrak{g}$ , the above identity takes the form ?x, a] = β, x] and naturally arises in the theory of integrable systems and differential geometry (namely, in the dynamics of n-dimensional rigid bodies, the argument shift method, and the classification of projectively equivalent Riemannian metrics). This paper studies general properties of sectional operators, in particular, integrability and the bi-Hamiltonian property for the corresponding Euler equation $\dot x = ad_{\varphi x}^* x$ .