Independent Ordering of Two Interpenetrating Magnetic Sublattices in the Double Perovskite SrCoOsO.

The insulating, fully ordered, double perovskite SrCoOsO undergoes two magnetic phase transitions. The Os(VI) ions order antiferromagnetically with a propagation vector k = (1/2, 1/2, 0) below T = 108 K, while the high-spin Co(II) ions order antiferromagnetically with a propagation vector k = (1/2,...

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Detalles Bibliográficos
Publicado en:Journal of the American Chemical Society Vol. 135; no. 50; pp. 18824 - 18831
Autores principales: Morrow, Ryan, Mishra, Rohan, Restrepo, Oscar D., Ball, Molly R., Windl, Wolfgang, Wurmehl, Sabine, Stockert, Ulrike, Büchner, Bernd, Woodward, Patrick M.
Formato: Artículo
Publicado: American Chemical Society 12/18/2013
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Acceso en línea:Ver este registro en EBSCOhost
Descripción
Sumario:The insulating, fully ordered, double perovskite SrCoOsO undergoes two magnetic phase transitions. The Os(VI) ions order antiferromagnetically with a propagation vector k = (1/2, 1/2, 0) below T = 108 K, while the high-spin Co(II) ions order antiferromagnetically with a propagation vector k = (1/2, 0, 1/2) below T = 70 K. Ordering of the Os(VI) spins is accompanied by a structural distortion from tetragonal I4/m symmetry to monoclinic I2/m symmetry, which reduces the frustration of the face centered cubic lattice of Os(VI) ions. Density functional theory calculations show that the long-range Os–O–Co–O–Os and Co–O–Os–O–Co superexchange interactions are considerably stronger than the shorter Os–O–Co interactions. The poor energetic overlap between the 3d orbitals of Co and the 5d orbitals of Os appears to be responsible for this unusual inversion in the strength of short and long-range superexchange interactions.