TY - JOUR
T1 - Strain-driven spin-state transition and superexchange interaction in LaCoO 3
T2 - Ab initio study
AU - Seo, Hosung
AU - Posadas, Agham
AU - Demkov, Alexander A.
PY - 2012/7/26
Y1 - 2012/7/26
N2 - Using spin density functional theory with the Hubbard correction, we investigate the magnetic structure of strained LaCoO 3. We show that beyond biaxial tensile strain of 2.5%, local magnetic moments originating from the high spin state of Co3 + emerge in a low spin Co3 + matrix. In contrast, we find that compressive strain is not able to stabilize a magnetic state due to geometric constraints. LaCoO 3 accommodates tensile strain via spin-state disproportionation, resulting in an unusual sublattice structure. In tensile-strained LaCoO 3, the first nearest-neighbor (n.n.) exchange coupling is ferromagnetic (FM), while the second n.n. interaction is stronger and antiferromagnetic (AFM). This unusual feature of the exchange parameters is qualitatively verified with a model superexchange calculation. Due to the competition between the FM and the AFM couplings in the system, we find that the most probable magnetic structure of tensile-strained LaCoO 3 is a canted-spin structure, which may explain the relatively small observed magnetic moment of 0.7μ B/Co3 +.
AB - Using spin density functional theory with the Hubbard correction, we investigate the magnetic structure of strained LaCoO 3. We show that beyond biaxial tensile strain of 2.5%, local magnetic moments originating from the high spin state of Co3 + emerge in a low spin Co3 + matrix. In contrast, we find that compressive strain is not able to stabilize a magnetic state due to geometric constraints. LaCoO 3 accommodates tensile strain via spin-state disproportionation, resulting in an unusual sublattice structure. In tensile-strained LaCoO 3, the first nearest-neighbor (n.n.) exchange coupling is ferromagnetic (FM), while the second n.n. interaction is stronger and antiferromagnetic (AFM). This unusual feature of the exchange parameters is qualitatively verified with a model superexchange calculation. Due to the competition between the FM and the AFM couplings in the system, we find that the most probable magnetic structure of tensile-strained LaCoO 3 is a canted-spin structure, which may explain the relatively small observed magnetic moment of 0.7μ B/Co3 +.
UR - https://www.scopus.com/pages/publications/84864472352
U2 - 10.1103/PhysRevB.86.014430
DO - 10.1103/PhysRevB.86.014430
M3 - Article
AN - SCOPUS:84864472352
SN - 1098-0121
VL - 86
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 1
M1 - 014430
ER -