4.6 Article

Giant spin Hall angle in the Hensler alloy Weyl ferromagnet Co2MnGa

期刊

PHYSICAL REVIEW B
卷 103, 期 4, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.103.L041114

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资金

  1. Ministry of Education, Culture, Sports, Science and Technology (MEXT) of Japan (Innovative Area Nano Spin Conversion Science KAKENHI) [26103003, 16H06089, 16H06330]
  2. MEXT
  3. New Zealand Science for Technological Innovation National Science Challenge
  4. New Zealand Centres of Research Excellence Programme
  5. Grants-in-Aid for Scientific Research [16H06330, 16H06089] Funding Source: KAKEN

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The inverse spin Hall effect (ISHE) in the ferromagnetic Weyl semimetal Heusler alloy Co2MnGa was investigated, revealing a high spin Hall angle and the ability to control the intensity of the spin Hall effect through magnetization direction. Additionally, it was found that Onsager's reciprocity does not hold for this system, possibly due to different spin-dependent Hall conductivity for spin-up and spin-down carriers.
Weyl semimetals are playing a major role in condensed-matter physics due to exotic topological properties, and their coexistence with ferromagnetism may lead to enhanced spin-related phenomena. Here, the inverse spin Hall effect (ISHE) in the ferromagnetic Weyl semimetal Heusler alloy Co2MnGa was investigated at room temperature by means of electrical spin injection in lateral spin valve structures. Spin transport properties such as spin polarization and spin diffusion length in this material were precisely extracted in order to estimate the spin Hall angle theta(SH), which was found to be -0.19 +/- 0.04 and is among the highest reported for a ferromagnet. Although this value is on the same order of magnitude of known heavy metals, the significantly higher resistivity of Co2MnGa implies an improvement on the magnitude of detection voltages, while its ferromagnetic nature allows controlling the intensity of SHE through the magnetization direction. It was also shown that Onsager's reciprocity does not hold for this system, which is in part attributable to a different spin-dependent Hall conductivity for spin-up and spin-down carriers.

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