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Coexistence of large conventional and planar spin Hall effect with long spin diffusion length in a low-symmetry semimetal at room temperature
The spin Hall effect (SHE) is usually observed as a bulk effect in high-symmetry crystals with substantial spin–orbit coupling (SOC), where the symmetric spin–orbit field imposes a widely encountered trade-off between spin Hall angle ( θ SH ) and spin diffusion length ( L sf ), and spin polarization...
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Published in: | Nature materials 2020-03, Vol.19 (3), p.292-298 |
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Main Authors: | , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | The spin Hall effect (SHE) is usually observed as a bulk effect in high-symmetry crystals with substantial spin–orbit coupling (SOC), where the symmetric spin–orbit field imposes a widely encountered trade-off between spin Hall angle (
θ
SH
) and spin diffusion length (
L
sf
), and spin polarization, spin current and charge current are constrained to be mutually orthogonal. Here, we report a large
θ
SH
of 0.32 accompanied by a long
L
sf
of 2.2 μm at room temperature in a low-symmetry few-layered semimetal MoTe
2
, thus identifying it as an excellent candidate for simultaneous spin generation, transport and detection. In addition, we report that longitudinal spin current with out-of-plane polarization can be generated by both transverse and vertical charge current, due to the conventional and a newly observed planar SHE, respectively. Our study suggests that manipulation of crystalline symmetries and strong SOC opens access to new charge-spin interconversion configurations and spin–orbit torques for spintronic applications.
A large spin Hall angle and long spin diffusion length are found in the low-symmetry, few-layer semimetal MoTe
2
at room temperature, thus identifying this material as an excellent candidate for simultaneous spin generation, transport and detection. |
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ISSN: | 1476-1122 1476-4660 |
DOI: | 10.1038/s41563-019-0600-4 |