Issue 38, 2020, Issue in Progress

Highly spin-polarized electronic structure and magnetic properties of Mn2.25Co0.75Al1−xGex Heusler alloys: first-principles calculations

Abstract

Highly spin-polarized half-metals (HMs) and spin-gapless semiconductors (SGSs) are the promising candidates in spintronic devices. However, the HM and SGS Heusler materials are very sensitive to the stoichiometric defects and lattice distortion, which will be not beneficial to the practical applications. Here, the electronic structure and magnetic properties of Mn2.25Co0.75Al1−xGex (x = 0, 0.25, 0.50, 0.75 and 1.00) Heusler alloys were investigated by first-principles calculations. Large negative formation energy, cohesive energy and phonon spectra confirm that the Mn2.25Co0.75Al1−xGex alloys are stable. It is found that Mn2.25Co0.75Al1−xGex with x = 0, 0.25, 0.75 and 1.00 show robust ferrimagnetic HM characteristics, while Mn2.25Co0.75Al0.5Ge0.5 shows robust SGS characteristic. Under the hydrostatic and uniaxial strains, Mn2.25Co0.75Al1−xGex exhibit a series of rich electronic transitions. The magnetic anisotropy of Mn2.25Co0.75Al1−xGex turns from the in-plane [100] direction to the out-of-plane [001] one by applying the uniaxial strains. The results suggest that the complete spin polarizations of Mn2.25Co0.75Al1−xGex alloys are robust against the stoichiometric defects and lattice distortion, which have potential applications in spintronic devices.

Graphical abstract: Highly spin-polarized electronic structure and magnetic properties of Mn2.25Co0.75Al1−xGex Heusler alloys: first-principles calculations

Supplementary files

Article information

Article type
Paper
Submitted
16 Apr 2020
Accepted
04 Jun 2020
First published
12 Jun 2020
This article is Open Access
Creative Commons BY-NC license

RSC Adv., 2020,10, 22556-22569

Highly spin-polarized electronic structure and magnetic properties of Mn2.25Co0.75Al1−xGex Heusler alloys: first-principles calculations

Y. Wang, L. Wang and W. Mi, RSC Adv., 2020, 10, 22556 DOI: 10.1039/D0RA03413D

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