Ferroelectric modulated giant valley polarization and half metallicity in 2D RuBrF/Sc2CO2 multiferroic heterostructure for non-volatile memory applications
Controlling two-dimensional (2D) valleytronics is challenging for information technology. This study shows that a ferroelectric-assisted layer can effectively enable non-volatile control of 2D valleytronics. Using first-principles simulations, we find that different polarization states in the Sc2CO2 layer cause the RuBrF monolayer to transition from a semiconductor to a half-metal, while also changing magnetic anisotropy from in-plane to out-of-plane. In the −P state, the system behaves as a ferromagnetic semiconductor with a spontaneous valley polarization of 329 meV. In the +P state, it becomes a ferromagnetic half-metal, blocking valleytronics. This enables electro-reversible control of valley electrons in the RuBrF/Sc2CO2 heterostructure. We explain the modulation of magnetic anisotropy and valley polarization using second-order perturbation theory and the k⋅p model. Our work offers a promising approach for non-volatile valleytronic control at the nanoscale, aiding the design of new devices.
Authors
- Qinfen Gu (ORCID: https://orcid.org/0000-0001-9209-4208)
- Minglei Jia (ORCID: https://orcid.org/0000-0002-6560-6244)
- Huimin Shen
- Fengzhu Ren (ORCID: https://orcid.org/0000-0002-9880-0158)
- Chang Liu (ORCID: https://orcid.org/0000-0002-5931-5475)
- Xiaoying Liu (ORCID: https://orcid.org/0009-0003-1821-5122)
- Bing Wang (ORCID: https://orcid.org/0009-0003-6884-8737)
- Cenhong Jin (ORCID: https://orcid.org/0000-0002-9704-3861)
Institutions
- Australian Nuclear Science and Technology Organisation (AU)
- Hainan Normal University (CN)
- Henan University (CN)
- Australian Synchrotron (AU)
- Yantai Nanshan University (CN)
Publication Details
- Journal
- Journal of Applied Physics
- Published
- 2025-08-12
- DOI
- https://doi.org/10.1063/5.0288245
- Citations
- 1
- Primary Topic
- 2D Materials and Applications
- Type
- article
- Field-Weighted Citation Impact
- 0.52