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The Effect of Cobalt-Sublattice Disorder on Spin Polarisation in Co(2)Fe(x)Mn(1−x)Si Heusler Alloys

In this work we present a theoretical study of the effect of disorder on spin polarisation at the Fermi level, and the disorder formation energies for Co(2)Fe(x)Mn(1−)(x)Si (CFMS) alloys. The electronic calculations are based on density functional theory with a Hubbard U term. Chemical disorders stu...

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Detalles Bibliográficos
Autores principales: Hasnip, Philip J., Loach, Christian H., Smith, Joseph H., Probert, Matthew I. J., Gilks, Daniel, Sizeland, James, Lari, Leonardo, Sagar, James, Yoshida, Kenta, Oogane, Mikihiko, Hirohata, Atsufumi, Lazarov, Vlado K.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2014
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5453278/
https://www.ncbi.nlm.nih.gov/pubmed/28788526
http://dx.doi.org/10.3390/ma7031473
Descripción
Sumario:In this work we present a theoretical study of the effect of disorder on spin polarisation at the Fermi level, and the disorder formation energies for Co(2)Fe(x)Mn(1−)(x)Si (CFMS) alloys. The electronic calculations are based on density functional theory with a Hubbard U term. Chemical disorders studied consist of swapping Co with Fe/Mn and Co with Si; in all cases we found these are detrimental for spin polarisation, i.e., the spin polarisation not only decreases in magnitude, but also can change sign depending on the particular disorder. Formation energy calculation shows that Co–Si disorder has higher energies of formation in CFMS compared to Co(2)MnSi and Co(2)FeSi, with maximum values occurring for x in the range 0.5–0.75. Cross-sectional structural studies of reference Co(2)MnSi, Co(2)Fe(0.5)Mn(0.5)Si, and Co(2)FeSi by Z-contrast scanning transmission electron microscopy are in qualitative agreement with total energy calculations of the disordered structures.