4 research outputs found
Magnetic exchange coupling and Curie temperature of Ni(1+x)MnSb (x=0, 0.25, 0.5, 0.75, 1) from first principles
We study the dependence of magnetic interactions and Curie temperature in
Ni(1+x)MnSb system on the Ni concentration within the framework of the
density-functional theory. The calculation of the exchange parameters is based
on the super-cell and frozen-magnon approaches. The Curie temperatures, Tc, are
calculated within the random-phase approximation. In agreement with experiment
we obtain decrease of the Curie temperature with increasing Ni content.Comment: 3 pages, 2 figure
Role of defects on the electronic and magnetic properties of CrAs/InAs and CrAs/CdSe half-metallic interfaces
We present an extended study of single impurity atoms at the interface
between the half-metallic ferromagnetic zinc-blende CrAs compound and the
zinc-blende binary InAs and CdSe semiconductors in the form of very thin
multilayers. Contrary to the case of impurities in the perfect bulk CrAs
studied in [I. Galanakis and S.G. Pouliasis, J. Magn. Magn. Mat. 321 (2009)
1084] defects at the interfaces do not alter in general the half-metallic
character of the perfect systems. The only exception are Void impurities at Cr
or In(Cd) sites which lead, due to the lower-dimensionality of the interfaces
with respect to the bulk CrAs, to a shift of the bands of the nearest
neighboring As(Se) atom to higher energies and thus to the loss of the
half-metallicity. But Void impurities are Schottky-type and should exhibit high
formation energies and thus we expect the interfaces in the case of thin
multilayers to exhibit a robust half-metallic character
Half-metallic ferrimagnetism in the [ScV]C and [ScV]Si alloys adopting the zinc-blende and wurtzite structures from first-principles
Employing first-principles calculations we study the structural, electronic
and magnetic properties of the [ScV]C and [ScV]Si
alloys. In their equilibrium rocksalt structure all alloys are non-magnetic.
The zincblende and wurtzite structures are degenerated with respect to the
total energy. For all concentrations the alloys in these lattice structures are
half-metallic with the gap located in the spin-down band. The total spin moment
follows the Slater-Pauling behavior varying linearly between the -1 of
the perfect ScC and ScSi alloys and the +1 of the perfect VC and VSi
alloys. For the intermediate concentrations V and Sc atoms have antiparallel
spin magnetic moments and the compounds are half-metallic ferrimagnets. At the
critical concentration, both [ScV]C and [ScV]Si
alloys present zero total spin-magnetic moment but the C-based alloy shows a
semiconducting behavior contrary to the Si-based alloys which is a
half-metallic antiferromagnet