TY - JOUR
T1 - Half-metallic antiferromagnetic nature of La2 VTcO6 and La2 VCuO6 from ab initio calculations
AU - Wang, Y. K.
AU - Lee, P. H.
AU - Guo, G. Y.
PY - 2009/12/17
Y1 - 2009/12/17
N2 - Electronic structure calculations based on density-functional theory with the generalized gradient approximation for 406 double perovskites La 2BB′O6 have been performed using the accurate full-potential linearized augmented plane wave method. La2 VTcO 6 and La2 VCuO6 are found to be candidates of half-metallic (HM) antiferromagnets (AFM) among the 406 ordered double perovskites La2 B B′ O6 with all the possible B and B′ pairs from all the 3d, 4d, and 5d transition metals have been considered. Furthermore, the HM-AFM state in La2 VTcO6 and La2 VCuO6 survive the full lattice constant and atomic position optimizations which were carried out using the frozen-core full-potential projector-augmented wave method. In addition, the GGA+U electronic structure calculations have also been performed and the HM-AFM state still remains. Their AFM state is attributed to both the superexchange and generalized double exchange mechanisms via the B(t2g) -O (2pπ) - B′ (t2g) coupling, and the latter could also be the origin of their HM.
AB - Electronic structure calculations based on density-functional theory with the generalized gradient approximation for 406 double perovskites La 2BB′O6 have been performed using the accurate full-potential linearized augmented plane wave method. La2 VTcO 6 and La2 VCuO6 are found to be candidates of half-metallic (HM) antiferromagnets (AFM) among the 406 ordered double perovskites La2 B B′ O6 with all the possible B and B′ pairs from all the 3d, 4d, and 5d transition metals have been considered. Furthermore, the HM-AFM state in La2 VTcO6 and La2 VCuO6 survive the full lattice constant and atomic position optimizations which were carried out using the frozen-core full-potential projector-augmented wave method. In addition, the GGA+U electronic structure calculations have also been performed and the HM-AFM state still remains. Their AFM state is attributed to both the superexchange and generalized double exchange mechanisms via the B(t2g) -O (2pπ) - B′ (t2g) coupling, and the latter could also be the origin of their HM.
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U2 - 10.1103/PhysRevB.80.224418
DO - 10.1103/PhysRevB.80.224418
M3 - Article
AN - SCOPUS:77954704466
SN - 1098-0121
VL - 80
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 22
M1 - 224418
ER -