2019
DOI: 10.1134/s1063776119060049
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Kinetic Properties and Half-Metallic Magnetism in Mn2YAl Heusler Alloys

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Cited by 25 publications
(20 citation statements)
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“…For other compounds of this system there are regions with negative TCR. Contrary to the electronic structure calculations [21], magnetic measurements for the Mn 2 CrAl, Mn 3 Al and Mn 2 FeAl systems give zero total magnetization and may indicate compensated ferrimagnetism [22,23].…”
Section: Results On Magnetic and Transport Propertiesmentioning
confidence: 61%
“…For other compounds of this system there are regions with negative TCR. Contrary to the electronic structure calculations [21], magnetic measurements for the Mn 2 CrAl, Mn 3 Al and Mn 2 FeAl systems give zero total magnetization and may indicate compensated ferrimagnetism [22,23].…”
Section: Results On Magnetic and Transport Propertiesmentioning
confidence: 61%
“…According to many ab initio calculations, alloys with the L2 1 structure are of interest as materials such as half-metallic ferromagnets, [15][16][17][18] and inverse alloys are interesting as gapless semiconductors with ferrimagnetic properties or spin gapless semiconductors (SGS). 14,19 Calculations show that the X a structure is characteristic of the Mn 2 CoAl alloy. 20 According to Ref.…”
Section: Introductionmentioning
confidence: 97%
“…The Heusler compounds family has more than 1500 alloys which exhibit various functional properties, i.e., magnetocaloric effect, 3,4 unusual thermal, 5,6 thermoelectric 7 and semiconductor [8][9][10] characteristics, properties of half-metallic ferromagnets 11,12,18 and spin gapless semiconductors. 13,14,19 The so-called full and inverse Heusler alloys are studied the most. These alloys have the same general formula X 2 YZ, where X and Y are 3d metals, and Z are s, p element, but a different crystal structure: L2 1 of the Cu 2 MnAl-type (full) and X a of the Hg 2 CuTi-type (inverse).…”
Section: Introductionmentioning
confidence: 99%
“…A special place in this series is occupied by Heusler alloys, which are in the state of a half-metal ferromagnet (HMF) [12][13][14][15] and a spin gapless semiconductor (SGS). [16][17][18][19] In the HMF state, an interesting feature is observed in the electronic energy spectrum near the Fermi level E F : for one spin direction (usually for the spin oriented against the direction of magnetization, i.e., spin "down"), there is a wide energy gap (∼ 1 eV) at E F , while for the opposite direction of spin (spin "up") the band gap is absent at E F . In SGS materials, there is a wide gap at E F for spin-down electrons and a zero gap for spin-up electrons (the valence and conduction bands are in a contact).…”
Section: Introductionmentioning
confidence: 99%