Related Experiment Video
Updated: May 29, 2025

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
Electrical mutual switching in a noncollinear-antiferromagnetic-ferromagnetic heterostructure
Ju-Young Yoon1,2, Yutaro Takeuchi1,3,4, Ryota Takechi1,2
1Laboratory for Nanoelectronics and Spintronics, Research Institute of Electrical Communication, Tohoku University, Sendai, Japan.
This study introduces a novel current-programmed spin-orbit torque (SOT) device. It demonstrates active control over SOT polarity for programmable magnetic data encoding, paving the way for advanced computing.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Spintronics
Background:
- Spin-orbit torque (SOT) is crucial for electrical control of magnetic states.
- Current SOT devices lack active manipulation of SOT polarity.
- Programmable SOT devices require electrical control of spin polarization.
Purpose of the Study:
- To demonstrate a proof-of-concept current-programmed SOT device.
- To achieve active manipulation of intrinsic SOT polarity.
- To explore applications in unconventional computing.
Main Methods:
- Fabrication of a Mn3Sn/Mo/CoFeB heterostructure.
- Utilizing noncollinear antiferromagnetic/ferromagnetic coupling.
- Applying current to induce mutual magnetic switching.
Main Results:
- Demonstrated current-induced switching in CoFeB layer.
- Showcased reversal of Mn3Sn magnetic orientation by CoFeB spin current.
- Established a spin-valve-like protocol for reversible spin source and electrode functionality.
Conclusions:
- Developed a novel current-programmed SOT device with tunable polarity.
- The device enables flexible programming of magnetic states for data encoding.
- Potential applications in unconventional logic and neuromorphic computing architectures.
More Related Videos
Related Concept Videos
Ferromagnetism
Mutual Inductance
When two circuits carrying time-varying currents are close to one another, the magnetic flux through each circuit varies because of the changing current in the other circuit. Consequently, an emf is induced in each circuit by the changing current in the other. Therefore, this type of emf is called...
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Paramagnetism
Magnetostatic Boundary Conditions

