The effects of B 2 O 3 vapor doping on the dielectric properties of barium titanate ceramics were studied. After the doping, the Curie point of BaTiO 3 ceramics was increased from 128°C to 130°C and the maximum dielectric constant was considerably increased. X-ray diffraction showed that both the grain lattice parameters and the tetragonality were increased by the boron oxide vapor doping. It was proposed that boron interstitial was introduced into the grain lattice of barium titanate ceramics by B 2 O 3 vapor doping and the dielectric properties were thus obviously changed. 9 However, B 2 O 3 has rarely caused attention as a dopant rather than flux addition. Because B 2 O 3 vaporizes easily at high temperatures, it can be adopted as a vapor dopant. In donor doped BaTiO 3 ceramics, the B 2 O 3 vapor dopant can improve the PTCR effect distinctly 11,12 and decrease the sintering temperature. 13 These effects were benefited from the introduction of boron interstitial in the perovskite lattice. In this paper, we focus our attention on the dielectric properties of barium titanate ceramics doped by B 2 O 3 vapor.High purity commercial BaTiO 3 (99.99%, Advanced Nano Products Co., Ltd., Chungcheongbuk-do, Korea), and B 2 O 3 (99.99%, Beijing Chemical Plant, Beijing, China) were adopted as starting materials. The barium titanate powders were pressed into small disks 1 mm thick and 10 mm in diameter with hydrostatic pressure of 98 MPa. The disks were placed in two bottom-up alumina crucibles marked as A , B, respectively. B 2 O 3 powders of 0.25 mol % (nominally) were placed beside the samples in crucible B. The samples were sintered at 1250°C for 2 h in air, then furnace cooled to room temperature. The samples in crucibles A and B were sintered in different runs to avoid cross contamination. The microstructure of the samples was studied by scanning electron microscopy (Leica Steroscan 440). The lattice parameters were measured by an x-ray diffractometer (Philips PW 3719) with Cu K a radiation. The ceramic samples were polished and silver paste electrodes were fired on both surfaces. The dielectric constant and the dielectric loss of the samples were measured through an impedance analyzer (Model HP 4192A LF, Hewlett-Packard Co., U.S.A.) from room temperature to 200°C.As temperature decreases, barium titanate undergoes three successive phase transitions: From paraelectric cubic phase to ferroelectric tetragonal phase and then to ferroelectric orthorhombic phase and finally to low-temperature rhombohedral phase. 14 The transition from cubic phase to tetragonal at 127°C is important because it is a transition from paraelectrics to ferroelectrics, and the transition temperature is called Curie point. The Curie point can be shifted by the doping of Pb ion to replace Ba to high temperature and by the doping of Sr to low temperature. It is found that the tetragonality, or c / a, of BaTiO 3 based materials at room temperature is related to their Curie point. A larger c / a corresponds to a higher Curie point. Figure 1 shows the ...