Killing tensor fields of third rank on a two-dimensional Riemannian torus

Abstract

A rank $m$ symmetric tensor field on a Riemannian manifold is called a Killing field if the symmetric part of its covariant derivative is equal to zero. Such a field determines the first integral of the geodesic flow which is a degree $m$ homogeneous polynomial in velocities. There exist global isothermal coordinates on a two-dimensional Riemannian torus such that the metric is of the form $d{s}^2=\lambda (z)|dz{|}^2$ in the coordinates. The torus admits a third rank Killing tensor field if and only if the function $\lambda$ satisfies the equation $\Re \left(\frac{\partial }{\partial z}\right(\lambda (c{\Delta }^{-1}{\lambda }_{zz}+a)\left)\right)=0$ with some complex constants $a$ and $c\ne 0$. The latter equation is equivalent to some system of quadratic equations relating Fourier coefficients of the function $\lambda$. If the functions $\lambda$ and $\lambda +{\lambda }_0$ satisfy the equation for a real constant ${\lambda }_0\ne 0$, then there exists a non-zero Killing vector field on the torus.