Fermi surface is at the heart of our understanding of metals and strongly correlated manybody systems 1 . An abrupt change in the Fermi surface topology, also called Lifshitz transition 2 , can lead to the emergence of fascinating phenomena like colossal magnetoresistance 3 and superconductivity 4, 5 . While Lifshitz transitions have been demonstrated for a broad range of materials and using different types of static external perturbations such as strain 6, 7 , doping 4, 5 , pressure 3, 8 and temperature 9, 10 , a non-equilibrium route toward ultrafast and transient modification of the Fermi surface topology has not been experimentally demonstrated. Combining time-resolved multidimensional photoemission spectroscopy 11 with state-of-the-art TDDFT+U simulations 12-14 , we introduce a scheme for driving an ultrafast Lifshitz transition