image: Figure 1. Spin-orbit-torque-induced magnetization switching in MnSb2Te4. (a) Electronic band structures of MnSb2Te4 with SOC. (b) Spin Hall conductivity of MnSb2Te4 for different spin configurations. (c) The XRD spectrum of the MnSb2Te4 film. (d) Schematic representation of SOT-induced switching in MnSb2Te4. (e)-(f) Switching loops in MnSb2Te4.
Credit: ©Science China Press
Recently, a study on spin-orbit torque switching in the magnetic topological material MnSb₂Te₄ was published in National Science Review (NSR). The research has pioneered new pathways for applying intrinsic magnetic topological materials in spintronic devices. The paper features Dr. Zihan Li (Department of Physics, Fudan University) as the first author, with Sheng Pan (Ph.D. candidate from the School of Physical Science and Technology, Soochow University) serving as co-first author. The corresponding authors are Professor Faxian Xiu from Fudan University's Department of Physics and Professor Jiexiang Yu from Soochow University's School of Physical Science and Technology.
With the continuous advancement of storage technologies, there is growing demand for enhanced storage capacity and read/write speeds. Spin-orbit torques (SOTs), as an effective electric switching approach, have great potential for breakthroughs both in the spintronic theory and in device designs. SOT systems usually need to have large spin orbit coupling, such as ferromagnetic/heavy metal, inversion-symmetry-broken interface, etc. It seems that the high spin-to-charge conversion efficiency and simplified structures with good stability and repeatability cannot be satisfied simultaneously.
The intrinsic magnetic topological insulator MnSb2Te4 is a magnetic material with a special electronic band structure, which shows high spin-charge conversion efficiency due to the spin-momentum locking. The research team conducted first principles calculations to get the Hall conductivity. Notably, the magnitude of the spin Hall conductivity is invariant across different spin configurations. In contrast, the anomalous Hall conductivity, derived from Berry curvature, is zero for all configurations within the gap. This behavior originates from the weakly asymmetric topological surface states which generate persistent spin currents. In experiments, high-quality MnSb2Te4 thin films have been synthesized by molecular beam epitaxy (MBE). The ferromagnetism in MnSb2Te4 with an out-of-plane anisotropy has been confirmed by magnetization measurements and transport measurements. When the dc bias current changes under the external field of -0.2 T, the anomalous Hall measurement shows a clockwise loop with two distinct states that remain well-preserved at zero current. The hysteresis behavior confirms the current-induced magnetization switching in a single MnSb2Te4 layer. (Figure. 1)
To fully understand the characteristics of SOT in MnSb2Te4, the research team tried to test the samples at different temperatures and magnetic fields. In the comparison of switching behaviors under positive and negative fields at 10 K, the anomalous Hall resistances show the opposite polarities. With increasing temperature, the anomalous Hall resistances and switching currents decrease, attributable to the simultaneous decrease in magnetization. These observations indicate that in-plane fields and dc currents can independently modulate the different stable magnetization states in MnSb2Te4. (Figure. 2)
To quantify the efficiency, the harmonic Hall effect measurements were used to characterize the effective field of SOT. The ac current can generate an alternating effective field, driving the magnetization to oscillate around its equilibrium position, and then give rise to a second-harmonic resistance. The spin Hall angle, which characterizes the SOT efficiency, can be obtained quantitatively by analyzing the second-harmonic signal. The spin Hall angle of the sample at 6 K is about 41, which is much larger than that in the traditional systems. (Figure. 3)
Furthermore, the research team prepared MnSb2Te4/FeTe0.9 heterostructures, utilizing ferromagnetic/antiferromagnetic coupling to generate exchange bias. The exchange bias can generate an equivalent effective magnetic field, achieving the field-free switching. They successfully observed the exchange bias in the heterostructure and realized the SOT induced magnetization switching under zero magnetic field. (Figure. 4)
This study successfully predicted feasible magnetization switching in MnSb2Te4 utilizing SOT without the necessity of external spin generator layers through theoretical calculation and observed the switching in experiments. The spin Hall angle is about ~ 41 at 6 K, much larger than that in the traditional systems. The research team also achieved the field-free switching by constructing MnSb2Te4/FeTe0.9 heterostructures. These results reveal a new mechanism of magnetic modulation in a single MnSb2Te4 layer, and show its application potential in spintronic devices.