Controlling the magnetic anisotropy in Cr2Ge2Te6 by electrostatic gating
By I. Verzhbitskiy, Hidekazu Kurebayashi, Hai-Xia Cheng, Jun Zhou, Safe-Ur-Rahman Khan, Y. Feng, G. Eda. Nature Electronics, 2020
232 citations recorded by the source corpus.
Electrical control of magnetism in van der Waals ferromagnetic semiconductors is an important step in creating novel spintronic devices, capable of processing and storing information, with these materials. For practical devices, electrical control at or near room temperature is sought, but most layered ferromagnetic semiconductors exhibit Curie temperatures below 100 K. Here, we show that electrostatic gating of thin chromium germanium telluride (Cr2Ge2Te6) crystals can be used to modulate the magnetic phase transition and magnetic anisotropy of this layered ferromagnetic semiconductor and increase its Curie temperature. Using an electric double-layer transistor device, we observe ferromagnetism in the material at temperatures up to 200 K and find that its magnetic easy axis is in the in-plane direction, in contrast to the out-of-plane easy axis of undoped Cr2Ge2Te6. Our analysis suggests that heavy doping promotes a double-exchange mechanism that is mediated by free carriers, which dominates over the superexchange mechanism of the original insulating state. Electrostatic gating can be used to modulate the magnetic anisotropy of chromium germanium telluride, a layered ferromagnetic semiconductor, and increase its Curie temperature to 200 K.
Subfields: Electronic, Optical and Magnetic Materials, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/ac041e6ae1297c7fcaa37159476cf0e15a9f58f3
Citations in the corpus
- Magnetism, symmetry and spin transport in van der Waals layered systems (2021, unknown): “As discussed later, Cr 2 Ge 2 Te 6 with chemical and electric doping 60,61 is one example where the exchange coupling strength is modified by the double-exchange mechanism, exhibiting large enhancements of the Curie temperature ( T C ) compared to undoped Cr 2 Ge 2 Te 6 .”