TY - JOUR
T1 - Electronic properties of double perovskite compounds
AU - Carvajal, E.
AU - Navarro, O.
AU - Allub, R.
AU - Avignon, M.
AU - Alascio, B.
PY - 2005/7
Y1 - 2005/7
N2 - The double perovskites family A2MM'O6 (A being an alkaline-earth and M, M' two different transitionmetal elements) is considered as a serious candidate for magnetoelectronic applications. It appears to be fundamental to understand the role of electronic parameters controlling the half-metallic ground state and high Curie temperature Tc. In this respect it is very interesting that different members of the family present a variety of electronic and magnetic properties. Among them, Sr 2FeMoO6 and Sr2FeReO6 are halfmetallic ferromagnets with fairly large Tc(≈450 K) while Sr2FeWO6 is known as an antiferromagnetic insulator with Tn*ap;37 K. As expected, a metal-insulator and magnetic transition has been reported in the substituted compounds Sr2FeMo^W,_XO6. To elucidate the origin of such different behavior in these Sr2FeMO 6 double perovskites we consider a correlated electron picture with localized Fe-spins (d5 configuration) and conduction electrons originating from M (M = Mo, Re or W) together with the doubleexchange type interaction taking place in the hybridized Fe-M t2g band and competing with the antiferromagnetic superexchange interactions between the Fe-spins. We consider here only the ordered stucture in which Fe and M constitute two interpenetrating sublattices. Using a tight-binding model and the renormalized perturbation expansion technique, we calculate the density of states and determine the behaviour of the critical temperature as a function of the band filling and the Fe-M charge transfer energy. This allows us to discuss the stability of the half-metallic ferromagnetic state with increasing charge transfer energy. We will also discuss the electronic properties and the ferro-antiferromagnetic transition hi the substituted compounds like Sr 2FeMoxW1-xO6, when disorder among Mo/W takes place in the M- sublattice.
AB - The double perovskites family A2MM'O6 (A being an alkaline-earth and M, M' two different transitionmetal elements) is considered as a serious candidate for magnetoelectronic applications. It appears to be fundamental to understand the role of electronic parameters controlling the half-metallic ground state and high Curie temperature Tc. In this respect it is very interesting that different members of the family present a variety of electronic and magnetic properties. Among them, Sr 2FeMoO6 and Sr2FeReO6 are halfmetallic ferromagnets with fairly large Tc(≈450 K) while Sr2FeWO6 is known as an antiferromagnetic insulator with Tn*ap;37 K. As expected, a metal-insulator and magnetic transition has been reported in the substituted compounds Sr2FeMo^W,_XO6. To elucidate the origin of such different behavior in these Sr2FeMO 6 double perovskites we consider a correlated electron picture with localized Fe-spins (d5 configuration) and conduction electrons originating from M (M = Mo, Re or W) together with the doubleexchange type interaction taking place in the hybridized Fe-M t2g band and competing with the antiferromagnetic superexchange interactions between the Fe-spins. We consider here only the ordered stucture in which Fe and M constitute two interpenetrating sublattices. Using a tight-binding model and the renormalized perturbation expansion technique, we calculate the density of states and determine the behaviour of the critical temperature as a function of the band filling and the Fe-M charge transfer energy. This allows us to discuss the stability of the half-metallic ferromagnetic state with increasing charge transfer energy. We will also discuss the electronic properties and the ferro-antiferromagnetic transition hi the substituted compounds like Sr 2FeMoxW1-xO6, when disorder among Mo/W takes place in the M- sublattice.
UR - http://www.scopus.com/inward/record.url?scp=23044509192&partnerID=8YFLogxK
U2 - 10.1002/pssb.200461726
DO - 10.1002/pssb.200461726
M3 - Artículo
AN - SCOPUS:23044509192
SN - 0370-1972
VL - 242
SP - 1942
EP - 1945
JO - physica status solidi (b)
JF - physica status solidi (b)
IS - 9
ER -