| Literature DB >> 28032768 |
Alexander Generalov1, Mikhail M Otrokov2,3, Alla Chikina4, Kristin Kliemt5, Kurt Kummer6, Marc Höppner7, Monika Güttler4, Silvia Seiro8, Alexander Fedorov9, Susanne Schulz4, Steffen Danzenbächer4, Evgueni V Chulkov2,3,10, Christoph Geibel8, Clemens Laubschat4, Pavel Dudin11, Moritz Hoesch11, Timur Kim11, Milan Radovic, Ming Shi, Nicholas C Plumb, Cornelius Krellner5, Denis V Vyalikh2,4,10,12.
Abstract
Finding ways to create and control the spin-dependent properties of two-dimensional electron states (2DESs) is a major challenge for the elaboration of novel spin-based devices. Spin-orbit and exchange-magnetic interactions (SOI and EMI) are two fundamental mechanisms that enable access to the tunability of spin-dependent properties of carriers. The silicon surface of HoRh2Si2 appears to be a unique model system, where concurrent SOI and EMI can be visualized and controlled by varying the temperature. The beauty and simplicity of this system lie in the 4f moments, which act as a multiple tuning instrument on the 2DESs, as the 4f projections parallel and perpendicular to the surface order at essentially different temperatures. Here we show that the SOI locks the spins of the 2DESs exclusively in the surface plane when the 4f moments are disordered: the Rashba-Bychkov effect. When the temperature is gradually lowered and the system experiences magnetic order, the rising EMI progressively competes with the SOI leading to a fundamental change in the spin-dependent properties of the 2DESs. The spins rotate and reorient toward the out-of-plane Ho 4f moments. Our findings show that the direction of the spins and the spin-splitting of the two-dimensional electrons at the surface can be manipulated in a controlled way by using only one parameter: the temperature.Entities:
Keywords: ARPES; Spin−orbit coupling; antiferromagnetism; exchange−magnetic interaction; rare-earth intermetallics
Year: 2017 PMID: 28032768 DOI: 10.1021/acs.nanolett.6b04036
Source DB: PubMed Journal: Nano Lett ISSN: 1530-6984 Impact factor: 11.189