  The Eisenhart lift provides an elegant geometric description of a dynamical
system of second order in terms of null geodesics of the Brinkmann-type metric.
In this work, we attempt to generalize the Eisenhart method so as to encompass
higher derivative models. The analysis relies upon Ostrogradsky's Hamiltonian.
A consistent geometric description seems feasible only for a particular class
of potentials. The scheme is exemplified by the Pais-Uhlenbeck oscillator.
