Total energies, electronic structure, surface energies, polarization, potentials and charge densities were studied for slabs of BaTiO 3 using the Linearized Augmented Plane Wave (LAPW) method. The depolarization field inhibits ferroelectricity in the slabs, and the macroscopic field set up across a ferroelectric slab is sufficient to cause electronic states to span the gap and give a metallic band structure, but the band shifts are not rigid and O p states tend to pile up at the Fermi level. There are electronic surface states, especially evident on TiO 2 surfaces. The dangling bonds bond back to the surface Ti's and make the surface stable and reactive. The BaO surfaces are more ionic than the bulk.
I. INTRODUCTIONSurfaces of ferroelectrics can strongly effect their properties. In general this is a much stronger effect than in paraelectric materials, because the termination of a ferroelectric gives rise to a depolarization field, which is huge in an ideal, ionic ferroelectric. The depolarization field, E d, is opposite in sign to the bulk polarization, and gives a contribution to the energy of −E d ·P large enough to completely destabilize the bulk ferroelectric state 1,2 . The ferroelectric 1 distortion in thin films varies with thickness so that the structures become cubic at thin edges 3 . Huge particle size effects are observed 4,5 , orders of magnitude greater than observed for non-ferroelectrics. Surfaces are important also during crystal growth, and their properties are key to catalysis and use as a epitaxial substrate. Here we study thin slabs of BaTiO 3 to better understand the electronic structure of the surface, surface energetics and relaxation, and intrinsic screening of the depolarization field.Experimental studies of BaTiO 3 surfaces are few and many more studies have focused on SrTiO 3 which lacks the complications of ferroelectricity. Photoemission studies of sputtered and annealed BaTiO 3 show evidence of significant surface defects 6 , and a number of papers have addressed the defect properties of the surface 7-9 . Studies of SrTiO 3 surfaces show evidence for minor relaxations by motions of atoms perpendicular to the surfaces 10,11 and show no evidence for states in the gap. 12 Some recent studies of BaTiO 3 show evidence for gap states 8 , and others do not 13 , probably indicating sensitivity to the surface defect state. Photoemission spectroscopy on BaTiO 3 shows excellent agreement with bulk LAPW computations of the LDA band structure 13 .First-principles electronic structure approaches have been very successful for bulk ferroelectrics 14-21 but the application of first-principles band structure methods to surface properties is daunting due to the giant computational burden. Here the first set of accurate electronic structure calculations for periodic BaTiO 3 slabs are presented. These results can be considered benchmark results for faster, more approximate methods, and also give some insights into the electronic structure of ferroelectric BaTiO 3 surfaces.
II. METHODWe studied six to sev...