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Competing magnetic phases of Mn5Ge3compound

✍ Scribed by Stroppa, Alessandro ;Peressi, Maria


Publisher
John Wiley and Sons
Year
2007
Tongue
English
Weight
533 KB
Volume
204
Category
Article
ISSN
0031-8965

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✦ Synopsis


Abstract

Germanium‐based compounds have recently attracted considerable attention in Semiconductor Spintronics. The Mn~5~Ge~3~ compound have been grown on Ge(111) substrate so that epitaxial “spin valves” can be fabricated. Recent experiments suggest a spin structure that is likely non‐collinear. In order to gain deep insights into the magnetic structure of this compound, we have performed fully unconstrained ab‐initio pseudo‐potential calculations within spin density functional theory. We have considered several possible magnetic configurations: paramagnetic (PM), collinear (C) ferromagnetic (FM) and anti‐ferromagnetic (AFM), non‐collinear (NC) spin configurations. We first study the effect of the pressure. At equilibrium volume (V ~eq~ = 0.203 m^3^), the C‐FM and NC self‐consistent solutions (which have different magnetic states) are competing phases. For V ≃ 1.1__V__ ~eq~ there is a crossover of the C‐FM and C‐AFM curves, with the C‐AFM becoming favourite with respect to C‐FM for larger volumes. Finally, we have studied the effect of strain field. Interestingly, the degeneracy of the NC phase with the C‐spin configurations (FM and AFM) is definitely removed under the effect of uniaxial structural distortions (NC spin configuration is favoured under tensile uniaxial strain). (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)


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Magnetic Structure of the Mn5Ge3 Alloy
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## Abstract Neutron powder diffraction patterns are measured at 50°C and liquid nitrogen temperature. The crystal structure is defined as D8~8~ (space group P6~3~/mcm), in agreement with CASTELLIZ's data [2]. It is found that the atoms in the 4 (d) and 6 (g) positions have magnetic moments of (3 ±