We present first principles charge-and spin-selfconsistent electronic structure computations on the Heusler-type disordered alloys Fe 3−x V x X for three different metalloids X= (Si, Ga and Al). In these calculations we use the methodology based on the Korringa-Kohn-Rostoker formalism and the coherent-potential approximation (KKR-CPA), generalized to treat disorder in multi-component complex alloys. Exchange correlation effects are incorporated within the local spin density (LSD) approximation. Total energy calculations for Fe 3−x V 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 3−x V x X alloys (with, x = 0.25, 0.50 and 0.75), together with the end compounds Fe 3 X and Fe 2 VX, and the limiting cases of a single V impurity in Fe 3 X and a single Fe(B) impurity in Fe 2 VX. We delineate clearly how the electronic states and magnetic moments at various sites in Fe 3−x V x X evolve as a function of the V content and the 1 metalloid valence. Notably, the spectrum of Fe 3−x V x X (X=Al and Ga) develops a pseudo-gap 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 3−x V x Si is found to decrease non-linearly, and the Fe(B) moment to increase with increasing x; this is in contrast to expectations of the 'local environment' 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.
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Spin-polarized measurements of the two-dimensional angular correlation of annihilation radiation in NiMnSb are presented. By making use of the inherent partial polarization of the positron beam and the alignment of the magnetic domains with the aid of an external magnetic field, the sum and difference of the spin-dependent contributions to the angular correlation have been obtained for integration directions (100), (110),and (111).The results are compared with calculated distributions. A least-squares analysis of the data yields a value of ( -8.4+0. 1)X 10 ' for the three-photon difference effect in NiMnSb and establishes the half-metallic character of the band structure with an accuracy of -+0 02 electrons per formula unit.
Nanosized inorganic particles are of great interest because their electronic properties can be easily tailored, providing a tremendous potential for applications in optoelectronic devices, light-emitting diodes, solar cells and hydrogen storage. Confinement of electrons and holes to dimensions comparable to their wavelength leads to quantum-well states with modified wavefunctions and density of states. Surface phenomena are crucial in determining nanoparticle properties in view of their large surface-to-volume ratio. Despite a wealth of information, many fundamental questions about the nature of the surface and its relationship with the electronic structure remain unsolved. Ab initio calculations on CdSe nanocrystals suggest that passivating the ligands does not produce the ideal wurtzite structure and that Se atoms relax outwards irrespective of passivation. Here we show that implanted positrons are trapped at the surface of CdSe nanocrystals. They annihilate mostly with the Se electrons, monitor changes in composition and structure of the surface while hardly sensing the ligand molecules, and we thus unambiguously confirm the predicted strong surface relaxation.
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