Crystal structure and thermoelectric properties of Nb 5+ -and Ln 3+ -͑rare earth: La 3+ , Nd 3+ , Sm 3+ , and Gd 3+ ͒ doped SrO͑SrTiO 3 ͒ n ͑n =1,2͒ ceramics, which were fabricated by conventional hot-pressing, were measured to clarify the effects of Ti 4+ -and Sr 2+ -site substitution on the thermoelectric properties. The thermal conductivities are very close between the n = 1 and 2 phases either doped with Nb 5+ or Ln 3+ and decreased by ϳ60% at room temperature and ϳ30% at 1000 K as compared to that of SrTiO 3 , which is likely due to an enhanced phonon scattering at the SrO/ ͑SrTiO 3 ͒ n ͑n =1,2͒ interfaces. The density of states effective mass m d ء ͑1.8-2.4 m 0 ͒ and consequently the Seebeck coefficient ͉S͉ in Nb 5+ -doped samples are fairly smaller than those reported for SrTiO 3 , which probably resulted from a deterioration of DOS due to the formation of the singly degenerate a 1g ͑Ti 3d xy ͒ orbital as the conduction band bottom, which should be induced by the distortion of TiO 6 octahedra in ͑SrTiO 3 ͒ n layers. However, in the Ln 3+ -doped SrO͑SrTiO 3 ͒ 2 , the TiO 6 octahedra were found to be restored, in contrast to the Nb 5+ -doped, with a gradually increasing O-Ti-O bond angle in the ͑100͒ plane at high temperatures, which would lead to the formation of triply degenerate Ti 3d-t 2g ͑d xy , d yz , and d xz ͒ orbitals to cause a significant enhancement in m d ء ͑ϳ7.5 m 0 at 1000 K͒ and consequently in ͉S͉. Accordingly, the maximum dimensionless figure of merit ZT ϳ 0.24 obtained in 5%-Gd 3+ -doped SrO͑SrTiO 3 ͒ 2 at 1000 K is about 70% larger than that of Nb-doped SrO͑SrTiO 3 ͒ 2 ͑ZT 1000 K ϳ 0.14͒.