Determination of spin Hall angle in the Weyl ferromagnet Co2MnGa by taking into account the thermoelectric contributions

被引:8
|
作者
Isshiki, Hironari [1 ,2 ]
Zhu, Zheng [1 ,2 ]
Mizuno, Hayato [1 ,2 ]
Uesugi, Ryota [1 ,2 ]
Higo, Tomoya [1 ,2 ,3 ]
Nakatsuji, Satoru [1 ,2 ,3 ,4 ]
Otani, YoshiChika [1 ,2 ,4 ,5 ]
机构
[1] Univ Tokyo, Inst Solid State Phys, Kashiwa, Chiba 2778581, Japan
[2] Japan Sci & Technol Agcy JST, Core Res Evolut Sci & Technol CREST, Saitama 3320012, Japan
[3] Univ Tokyo, Dept Phys, Tokyo 1130033, Japan
[4] Univ Tokyo, Transscale Quantum Sci Inst, Bunkyo ku, Tokyo 1130033, Japan
[5] RIKEN, Ctr Emergent Matter Sci, Wako, Saitama 510198, Japan
关键词
THERMAL-CONDUCTIVITY; SURFACE-STATES; OXIDE;
D O I
10.1103/PhysRevMaterials.6.084411
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The spin Hall effects of various materials, including Weyl semimetals, have been studied by the spin absorption method with the nonlocal spin valve structures. Here, we study Co2MnGa (CMG) by using the standard spin absorption method. A considerable amount of thermoelectric signal superimposes on the inverse spin Hall signal in the measurement configuration: the applied electric current between the spin injector (permalloy) and bridge (copper) wires produces heating or cooling at the interface via the Peltier effect, which causes an out-of-plane temperature gradient in CMG. As a result, a voltage signal induced by the anomalous Nernst effect (ANE) of CMG comes into the inverse spin Hall signal. We quantitatively separate these signals by combining the experiment and a numerical simulation. About 75% of the detected signal is found attributable to the thermoelectric effects. The superposing thermoelectric contribution is a general and unavoidable problem in this method when the spin Hall materials exhibit ANE. After eliminating the thermoelectric signal, the spin Hall angle of CMG turns out to be theta = -0.09 at room temperature.
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页数:8
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