The energetics of point defects in oxide materials plays a major role in determining their high-temperature properties, but experimental measurements are difficult, and calculations based on density functional theory ͑DFT͒ are not necessarily reliable. We report quantum Monte Carlo calculations of the formation energy E S of Schottky defects in MgO, which demonstrate the feasibility of using this approach to overcome the deficiencies of DFT. In order to investigate system-size errors, we also report DFT calculations of E S on repeating cells of up to ϳ1000 atoms, which indicate that QMC calculations on systems of only 54 atoms should yield high precision. The DFT calculations also provide the relaxed structures used in the variational and diffusion Monte Carlo calculations. For MgO, we find E S to be in close agreement with results from DFT and from model interaction potentials, and consistent with the scattered experimental values. The prospects for applying the same approach to transition metal oxides such as FeO are indicated.The quantum Monte Carlo ͑QMC͒ technique 1,2 is important in condensed matter science, because it is generally much more accurate than density functional theory ͑DFT͒ and allows one to make accurate predictions for problems where DFT fails. 3-7 It is usually competitive in accuracy with high-level quantum chemistry methods, but it has the advantage of being practicable for large systems containing hundreds of atoms. Recently, efforts have been made to apply QMC to oxide systems, including transition metal oxides, 8,9 for which DFT gives poor predictions for magnetic properties, phonon frequencies, and other properties. 10 We have recently reported 11 a QMC study of bulk MgO for which we find excellent agreement with experiments for the bulk lattice parameter and bulk modulus, provided appropriate corrections are made. We report here on a QMC calculation of an oxide lattice defect energy, namely the Schottky formation energy E S in MgO. Defect energies in oxide materials are technologically important for applications ranging from high-temperature superconductors to radioactive waste disposal, but are also very difficult to measure experimentally. We shall show that our results for E S in MgO are consistent with available experimental data, as well as supporting earlier DFT predictions. 12 The Schottky energy E S is the energy required to form a cation and anion vacancy pair, and governs the thermal equilibrium concentration of vacancies. 13 The calculation of E S in ionic materials has a very long history, going back to the very early work of Mott and Littleton. 14-16 DFT calculations on defect formation and migration energies in oxides first became possible in the early 1990s, and are now routinely performed. However, particularly in transition metal oxides, the reliability of DFT calculations is questionable.QMC calculations are usually performed in two stages. 1 In the first, known as variational Monte Carlo ͑VMC͒, a trial many-body wave function is constructed as a product of a Slater d...