A study of the crystallographic and magnetic structure of SrCoO 2.5 with a brownmillerite-type structure has been carried out from neutron powder-diffraction ͑NPD͒ measurements at temperatures ranging from 10 to 623 K, across the Néel temperature ͑T N = 537 K͒ of this antiferromagnetic oxide. The study has been complemented with differential scanning calorimeter ͑DSC͒, dc susceptibility and magnetization measurements. Although the refinement of the crystal structure from NPD data is possible in the orthorhombic Pnma and Ima2 space groups, the support of ab-initio band-structure calculations has allowed us to select, without ambiguity, the Ima2 space group as the ground state for SrCoO 2.5 brownmillerite. In Ima2 the crystallographic structure of SrCoO 2.5 is described as layers of corner-sharing Co1O 6 octahedra alternating along the a axis with layers of vertex-sharing Co2O 4 tetrahedra, conforming chains running along the ͓0 0 1͔ direction. The magnetic structure below T N = 537 K is G-type with the magnetic moments directed along the c axis. This magnetic arrangement is stable from T N down to 10 K. At T = 10 K, the magnetic moment values for Co1 and Co2 atoms are 3.12͑13͒ B and 2.88͑14͒ B , respectively, compatible with a Co 2+ L គ state, where L គ stands for a ligand hole. The magnetic susceptibility curves show, below 200 K, a divergence of zero-field cooling and field cooling curves, displaying broad maxima which are interpreted as due to the presence of ferromagnetic clusters embedded into an antiferromagnetic matrix. These inhomogeneities are inherent to the synthesis process, by quenching microcrystalline samples of SrCoO 3−x composition from high temperature, where cubic, ferromagnetic perovskites have been identified by diffraction methods.
We have synthesized Sr 6 Co 5 O 15 , a quasi-one-dimensional oxide, measured its magnetic properties, and calculated its electronic structure by ab initio techniques. We have found strong evidence for its electronic and magnetic behavior not to follow the trend of its structural series. The magnetic coupling inside the CoO 3 chains is not purely ferromagnetic, and the long-range coupling inside the chains is very weak. The Co moments are slightly canted due to their large orbital angular momenta being oriented along each particular quantization axis, which is different for each Co 4+ atom in the structure. Our thermopower calculations are in agreement with the experiment, supporting our model of the magnetic ground state of the compound.
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