2021
DOI: 10.1038/s41928-021-00542-8
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A spin–orbit torque device for sensing three-dimensional magnetic fields

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Cited by 43 publications
(31 citation statements)
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“…The magnetization can be switched by an in-plane current I x with the assistance of a collinear magnetic field H x via SOT (Section S1, Supporting Information). Moreover, as found in our previous work, [23] the coercive field of the AHE loop (AHR R H vs H x ) decreases with I x increases. Here, at I x = 30 mA, R H varies linearly with applied H x within the range of −12 to +12 Oe (orange points in Figure 1b).…”
Section: In-memory Electrical Current Sensing Unitsupporting
confidence: 88%
“…The magnetization can be switched by an in-plane current I x with the assistance of a collinear magnetic field H x via SOT (Section S1, Supporting Information). Moreover, as found in our previous work, [23] the coercive field of the AHE loop (AHR R H vs H x ) decreases with I x increases. Here, at I x = 30 mA, R H varies linearly with applied H x within the range of −12 to +12 Oe (orange points in Figure 1b).…”
Section: In-memory Electrical Current Sensing Unitsupporting
confidence: 88%
“…Domain walls (DWs) in ferroic materials have attracted intensive interest over the past decades due to their physical phenomena and potential for applications in nanoelectronics 1 , 2 and spintronics 3 5 . Of particular interest are the designs of racetrack memory 6 , 7 and DW logic 8 , 9 based on moving magnetic DWs driven by a current or a magnetic field.…”
Section: Introductionmentioning
confidence: 99%
“…Spin–orbit torque (SOT)-driven magnetic switching has attracted a lot of attention because of its significant application potential in nonvolatile, low-power, high-speed, and high-density magnetic random access memories and emerging spin logic devices. The bilayer structure consisted of strong spin–orbit coupling (SOC) materials (e.g., topological insulator, two-dimensional electron gas, and Weyl semimetal and heavy metal) and ferromagnetic (FM) materials is widely accepted as the basic strategy of SOT switching. However, the thickness of the FM layer in the bilayer structure is subjected to the non-local spin injection and spin coherence length, and the critical current density ( J c ) is enlarged with the increasing thickness of the FM layer, that is, the interfacial nature of the SOT effect. This peculiarity results in incompatibility between low J c and a thick FM layer for high thermal stability, which hinders the application of SOT-based devices in low-power and high-density memory and computation systems. …”
Section: Introductionmentioning
confidence: 99%