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Title: Electronic structure and magnetism of Fe{sub 3{minus}x}V{sub x}X (X=Si, Ga, and Al) alloys by the KKR-CPA method

Journal Article · · Physical Review, B: Condensed Matter
 [1];  [1];  [2];  [3]
  1. Department of Physics, Northeastern University, Boston, Massachusetts 02115 (United States)
  2. Interfaculty Reactor Institute, Delft University of Technology, Mekelweg 15, 2629 JB Delft (The Netherlands)
  3. Faculty of Physics and Nuclear Techniques, Academy of Mining and Metallurgy, al. Mickiewicza 30, 30-073 Krakow (Poland)

We present first-principles charge- and spin-self-consistent electronic structure computations on the Heusler-type disordered alloys Fe{sub 3{minus}x}V{sub x}X for three different metalloids X=(Si,thinspGa, and Al). In these calculations we use the methodology based on the Korringa-Kohn-Rostoker formalism and the coherent-potential approximation generalized to treat disorder in multicomponent complex alloys. Exchange correlation effects are incorporated within the local spin density approximation. Total energy calculations for Fe{sub 3{minus}x}V{sub x}Si show that V substitutes preferentially on the Fe(B) site, not on the Fe(A,C) site, in agreement with experiment. Furthermore, calculations have been carried out for Fe{sub 3{minus}x}V{sub x}X alloys (with x=0.25, 0.50, and 0.75), together with the end compounds Fe{sub 3}X and Fe{sub 2}VX, and the limiting cases of a single V impurity in Fe{sub 3}X and a single Fe(B) impurity in Fe{sub 2}VX. We delineate clearly how the electronic states and magnetic moments at various sites in Fe{sub 3{minus}x}V{sub x}X evolve as a function of the V content and the metalloid valence. Notably, the spectrum of Fe{sub 3{minus}x}V{sub x}X (X=Al and Ga) develops a pseudogap for the majority as well as minority spin states around the Fermi energy in the V-rich regime, which, together with local moments of Fe(B) impurities, may play a role in the anomalous behavior of the transport properties. The total magnetic moment in Fe{sub 3{minus}x}V{sub x}Si is found to decrease {ital nonlinearly}, and the Fe(B) moment to {ital increase} with increasing {ital x}; this is in contrast to expectations of the {open_quotes}local environment{close_quotes} model, which holds that the total moment should vary linearly while the Fe(B) moment should remain constant. The common-band model, which describes the formation of bonding and antibonding states with different weights on the different atoms, however, provides insight into the electronic structure of this class of compounds. {copyright} {ital 1999} {ital The American Physical Society}

OSTI ID:
690743
Journal Information:
Physical Review, B: Condensed Matter, Vol. 60, Issue 19; Other Information: PBD: Nov 1999
Country of Publication:
United States
Language:
English