Related Experiment Video
Updated: Jan 8, 2026

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
The manipulation of exchange bias in van der Waal ferromagnetic/antiferromagnetic heterojunction by interfacial
Guangcheng Wang1, Lin Ma2, Zijing Zhao1
1School of Physics and Optoelectronic Engineering, Beijing University of Technology, Beijing 100124, China. xiaoleiwang@bjut.edu.cn.
Abstract:
Two-dimensional (2D) van der Waals (vdWs) heterostructures, with their atomically sharp interfaces and low defect densities, offer an ideal platform for studying interfacial spin phenomena and enabling low-power spintronic devices. However, achieving controllable and reversible exchange bias (EB) in 2D systems remains challenging. Here, we report a pronounced EB effect in a vdWs ferromagnetic/antiferromagnetic (FM/AFM) heterojunction composed of Fe3GaTe2/CrPS4, with the EB field reaching up to 850 Oe at 10 K. More importantly, we observe a temperature-driven reversal of the EB field direction from negative to positive, a rare phenomenon in 2D heterostructures. To explain this behavior, we propose a model in which spin-canted uncompensated moments in CrPS4 compete with asynchronous magnetization reversal between the surface and bulk regions of Fe3GaTe2, leading to a tunable EB response. Furthermore, the sign and magnitude of EB can be precisely controlled by adjusting temperature and ferromagnetic layer thickness under the same cooling field. This work reveals the fundamental role of interfacial exchange interactions and provides guidance for designing programmable magnetic states in next-generation spintronic devices.
Related Concept Videos
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...
Ferromagnetism
Biasing of FET
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the...
Biasing of P-N Junction
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
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...
NMR Spectroscopy: Spin–Spin Coupling

