We present the results of ab initio calculations on magnetic and electronic structures of La 1−x Sr x MnO 3 at low doping, x =1/8. Using the B3LYP hybrid exchange-correlation functional within the framework of densityfunctional theory, we predict a ferromagnetic ground state for La 0.875 Sr 0.125 MnO 3 in both the low-temperature orthorhombic and the high-temperature pseudocubic phases. This is in contrast to its parent compound LaMnO 3 , for which we find in agreement with experiment the layered antiferromagnetic state to be the most stable one. The calculated density of states and bond population analysis suggest a tendency of formation of half-metallic spin states in the band gap of both structures. Sr-doped LaMnO 3 ͑La 1−x Sr x MnO 3 , LSM͒ is one of many extensively studied perovskite-type oxides, attractive due to its colossal magnetoresistivity, a spin-glass behavior, a metal-to-insulator transition ͓at ϳ360 K for x = 0.3 ͑Ref. 1͔͒, charge ordering after doping with Sr, and a ferromagneticantiferromagnetic transitions observed. One of its important applications is also the use as a promising cathode material in high-temperature solid oxide fuel cells ͑SOFCs͒. 2 The high operating temperature of current SOFC technology is mandated by the necessity of high oxygen molecule reduction rate at the fuel cell cathode and high oxygen ion mobility in the solid electrolyte and in the cathode bulk or on surfaces and grain boundaries. Technologically, the first requirement ͑and partially the second one͒ can be met by reducing the thickness of electrolyte and cathode layers, as it is implemented in the Jülich planar substrate SOFC concept, where thin electrolyte ͑yttria stabilized zirconium oxide͒ and cathode layers ͑LSM or ͕Co, Fe͖-doped LaMnO 3 ͒ are supported by a millimeter thick nickel cermet anode. 3 Elucidating the mechanisms of oxygen reduction and mobility on LSM surfaces and in the bulk of LSM is thus beneficial for understanding the limitations of the currently used materials in SOFC technology and secondly aiding the development of higher-performance materials. LSM compounds exhibit a large variety of properties depending on the La/ Sr ratio, the degree of oxygen nonstoichiometry, temperature and/or pressure conditions, sample preparation, etc. Even at high SOFC working temperatures ͑T Ͼ 780 K͒, when cooperative Jahn-Teller distortion disappears, magnetic orbital ordering still can take place. Knowledge of proper spin redistribution in manganites is especially important because of the four unpaired electrons on Mn, which demand open-shell calculations. Thus, before one starts modeling the complex surface processes, it is indispensable to first investigate the magnetic and electronic structure of bulk LSM. In the current study, we chose to investigate the LSM with a 12.5% Sr doping, which is somewhat larger than typical experimental concentrations ͑ഛ10% Sr͒ in order to simplify the calculations ͑the larger the Sr content, the smaller the necessary system size͒.Recent series of local spin-density approximatio...