TY - JOUR
T1 - New ferromagnetic semiconductor double perovskites
T2 - La2FeMO6 (M = Co, Rh, and Ir)
AU - Fuh, Huei Ru
AU - Weng, Ke Chuan
AU - Liu, Yun Ping
AU - Wang, Yin Kuo
N1 - Funding Information:
The authors gratefully acknowledge the resource support from the Computational Materials Research Focus Group, the National Science Council, and the National Center for High-Performance Computing of Taiwan for their computer time and facilities. Finally, Y.K. Wang would also like to thank Chun-Yen Chang for the financial support received from the Science Education Center .
Publisher Copyright:
© 2014 Elsevier B.V. All rights reserved.
PY - 2015/2/15
Y1 - 2015/2/15
N2 - Density functional theory with generalized gradient approximation (GGA) plus onsite Coulomb interaction (GGA + U) was used to calculate physical proprieties of new ferromagnetic semiconductor materials of the La2FeMO6 (M = Co, Rh, and Ir). We calculate the 406 (C229) La2MM′O6 compounds which MM′ can be any pair taken from the 29 transition metal elements except La. La2FeCoO6 is a potential candidate for ferromagnetic semiconductor. For the GGA + U scheme, La2FeCo6 remains a stable FM semiconductor, whereas La2FeRhO6 and La2FeIrO6 are shown the FM and AFM states of which are degenerate with each other. The FM semiconductor gap remains in existence under tensile or compressive strain in La2FeRhO6 and La2FeIrO6. The superexchange interaction in ferromagnetic La2FeMO6 (M = Co, Rh, and Ir) is high spin (HS) Fe completely empty eg orbital hopping to the half-filled (LS) Co (Rh and Ir) empty eg orbital.
AB - Density functional theory with generalized gradient approximation (GGA) plus onsite Coulomb interaction (GGA + U) was used to calculate physical proprieties of new ferromagnetic semiconductor materials of the La2FeMO6 (M = Co, Rh, and Ir). We calculate the 406 (C229) La2MM′O6 compounds which MM′ can be any pair taken from the 29 transition metal elements except La. La2FeCoO6 is a potential candidate for ferromagnetic semiconductor. For the GGA + U scheme, La2FeCo6 remains a stable FM semiconductor, whereas La2FeRhO6 and La2FeIrO6 are shown the FM and AFM states of which are degenerate with each other. The FM semiconductor gap remains in existence under tensile or compressive strain in La2FeRhO6 and La2FeIrO6. The superexchange interaction in ferromagnetic La2FeMO6 (M = Co, Rh, and Ir) is high spin (HS) Fe completely empty eg orbital hopping to the half-filled (LS) Co (Rh and Ir) empty eg orbital.
KW - Density functional theory
KW - Double perovskite
KW - Ferromagnetic semiconductor
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U2 - 10.1016/j.jallcom.2014.10.010
DO - 10.1016/j.jallcom.2014.10.010
M3 - Article
AN - SCOPUS:84910604106
SN - 0925-8388
VL - 622
SP - 657
EP - 661
JO - Journal of Alloys and Compounds
JF - Journal of Alloys and Compounds
ER -