Fermi level tuning has been successfully demonstrated in Co-based full-Heusler alloy Co(2)FeAl(0.5)Si(0.5) (CFAS). The half-metallic band gap of CFAS was proved by the behavior of differential conductance of CFAS/(MgAl(2))O(x)/CoFe magnetic tunneling junctions with an unexplored crystalline (MgAl(2))O(x) barrier. CFAS exhibits the highest effective spin polarization (P_{eff}) at 300 K and the weakest temperature dependence of P_{eff} among all known half metals. Further study shows that P_{eff} of CFAS decays with increasing temperature (T) following T;{3/2} law perfectly, which indicates that the depolarization of CFAS is determined by spin wave excitation only.
We present experimental and theoretical studies of Pd/Cu(100) and Cu/Pd(100)
heterostructures in order to explore their structure and misfit strain
relaxation. Ultrathin Pd and Cu films are grown by pulsed laser deposition at
room temperature. For Pd/Cu, compressive strain is released by networks of
misfit dislocations running in the [100] and [010] directions, which appear
after a few monolayers already. In striking contrast, for Cu/Pd the tensile
overlayer remains coherent up to about 9 ML, after which multilayer growth
occurs. The strong asymmetry between tensile and compressive cases is in
contradiction with continuum elasticity theory, and is also evident in the
structural parameters of the strained films. Molecular Dynamics calculations
based on classical many-body potentials confirm the pronounced
tensile-compressive asymmetry and are in good agreement with the experimental
data.Comment: 4 pages, 5 figures, to appear in Phys. Rev. Let
We investigate the temperature dependence of the spin-resolved unoccupied density of states ͑DOS͒ in ferromagnetic Co 2 FeAl and ferrimagnetic Mn 2 VAl epitaxial films on MgO͑100͒ using x-ray magnetic circular dichroism. We observe an unexpected strong temperature dependence of the DOS beyond the change expected from the Fermi distribution function. An increase in spectral weight is observed for majority states below the Fermi energy in the case of Mn 2 VAl and for minority states above the Fermi energy in the case of Co 2 FeAl. Reduced atomic order near the interface suppresses the unexpected temperature dependence of the DOS for Mn 2 VAl.
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