Bulletin of the American Physical Society
APS March Meeting 2020
Volume 65, Number 1
Monday–Friday, March 2–6, 2020; Denver, Colorado
Session R19: Magnetic interactions at complex oxide interfaces
8:00 AM–11:00 AM,
Thursday, March 5, 2020
Room: 207
Sponsoring
Unit:
GMAG
Chair: Alexander Grutter, National Institute of Standards and Technology
Abstract: R19.00004 : Spin to charge conversion in the topological insulator HgTe and in STO-based two-dimensional electron gas*
Presenter:
Jean-Phillippe Attane
(Univ. Grenoble Alpes, CEA, IRIG, 38000 Grenoble (France))
Author:
Jean-Phillippe Attane
(Univ. Grenoble Alpes, CEA, IRIG, 38000 Grenoble (France))
In this contribution, we first focus on strained mercury telluride, using spin pumping experiments at room temperature. We show that a HgCdTe barrier can be used to protect the HgTe topological surface states, leading to high conversion rates, with inverse Edelstein lengths up to 2.0±0.5 nm. These measurements, associated with the temperature dependence of the resistivity, suggest that these high conversion rates are due to the spin momentum locking property of HgTe surface states [1].
We then focus on the SrTiO3 (STO)-based 2D electron system, presenting experiments performed on NiFe/Al/STO heterostructures. We investigate the nature of the spin-to-charge conversion through a combination of spin pumping, magnetotransport, spectroscopy and gating experiments, finding a very highly efficient spin-to-charge conversion, with inverse Edelstein lengths beyond 20 nm. More importantly, we demonstrate that the conversion rate can be tuned in amplitude and rate by a gate voltage. We then discuss the amplitude of the effect and its gate dependence on the basis of the electronic structure of the 2DES and highlight the importance of a long scattering time to achieve efficient spin-to-charge interconversion.
[1] P. Noel et al., Phys. Rev. Lett. 120, 167201 (2018)
[2] D. C. Vaz et al., Nature Materials 1-7 (2019)
*Support from the ANR SOspin, ANR OISO, ANR Toprise and LANEF (ANR-10-LABX51-01) is acknowledged,
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