We study the problem of non-integrability (integrability) of cosmological dynamical systems which are given in the Hamiltonian form with indefinite kinetic energy form T = 1 2 g (v, v), where g is a two-dimensional pseudo-Riemannian metric with a Lorentzian signature (+, −), and v ∈ T x M is a tangent vector at a point x ∈ M of the configuration space M.