2017
DOI: 10.1103/physrevb.95.094425
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First-principles calculation of the effects of partial alloy disorder on the static and dynamic magnetic properties ofCo2MnSi

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Cited by 40 publications
(39 citation statements)
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References 79 publications
(132 reference statements)
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“…Typical VNA-FMR measurements performed on Co 2 MnGe (left column) and Co 2 MnSi (right column) are shown in figure 3. [38] -0.68 [56] 0.66 [56] 0 [55] Ga 5.77 5.4 100 % 4.09 [57] -0.67 [56] 0.3 [56] 0 [55] Type IV [51] 6 10 -5 [22] 100 [56] [24] [54] 0.41 [24] 0.81 [54] ~ 0.2 [24] 0.33 [54] Ge 5.75 5 5. 3 10 -4 (290 K) 6.1 10 -4 (8 K) 100 % 4,94 [51] 1.9 10 -4 [21] 100 [53] [55] 0.58 [55] 0.54 [53] 0.07 [60] 0.03 [53] Sn 6.00 5.6 9.…”
Section: -Experimental Resultsmentioning
confidence: 99%
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“…Typical VNA-FMR measurements performed on Co 2 MnGe (left column) and Co 2 MnSi (right column) are shown in figure 3. [38] -0.68 [56] 0.66 [56] 0 [55] Ga 5.77 5.4 100 % 4.09 [57] -0.67 [56] 0.3 [56] 0 [55] Type IV [51] 6 10 -5 [22] 100 [56] [24] [54] 0.41 [24] 0.81 [54] ~ 0.2 [24] 0.33 [54] Ge 5.75 5 5. 3 10 -4 (290 K) 6.1 10 -4 (8 K) 100 % 4,94 [51] 1.9 10 -4 [21] 100 [53] [55] 0.58 [55] 0.54 [53] 0.07 [60] 0.03 [53] Sn 6.00 5.6 9.…”
Section: -Experimental Resultsmentioning
confidence: 99%
“…Looking first the PES results obtained on Co 2 MnZ IV compounds, the observed full spin polarization for Si and Ge is consistent with theoretical calculations regarding the calculated width of the spin gap and the position of the Fermi energy in the middle of the gap. For Co 2 MnSi band structure calculations, the Fermi energy is located right in the middle of the spin gap[24,54] and a large gap is obtained (0.8 eV[54], 0.41 eV[24,55]). Our results are consistent with these theoretical predictions since the measured (half-) gap between the minority spin valence band to E F is around 0.4 eV .06 eV below the top valence band (so not HMM).…”
mentioning
confidence: 97%
“…Both terms are important and the higher they are, the higher the GMR is. Most of the research efforts focused on improving the bulk parameter, searching for electrode materials with a spin polarization at the Fermi level as high as possible (ideally of 100%), and robust with respect to the unavoidable structural defects, like permutations between atoms of different chemical species, which can damage the physical properties in the case of full-Heusler alloys [5][6][7][8][9]. The interface spin-scattering asymmetry coefficient must, however, also be improved to further increase the GMR of SVs based on half-metallic electrodes.…”
Section: Introductionmentioning
confidence: 99%
“…Unfortunately, temperature, impurity, and other external factors can disrupt the completely spin-polarized band structures and further degrade the half-metallicity of ideal compounds [25][26][27][28][29][30][31][32][33][34]. For example, in the traditional full Heusler compound Co 2 MnSi, a remarkable gap with 0.4 eV in minority band at 985 K may disappear, and only a spin polarization of 61% can be observed at a barrier interface consisting of a single electrode made of a Co 2 MnSi film [35][36][37][38].…”
Section: Introductionmentioning
confidence: 99%