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  • Letter

Combining intrinsic and sliding-induced polarizations for multistates in two-dimensional ferroelectrics

Chuhan Tang1, Zhiqiang Tian1, Tao Ouyang2, Anlian Pan1,3, and Mingxing Chen1,4,*

  • 1Key Laboratory for Matter Microstructure and Function of Hunan Province, Key Laboratory of Low-Dimensional Quantum Structures and Quantum Control of Ministry of Education, School of Physics and Electronics, Hunan Normal University, Changsha 410081, China
  • 2Hunan Key Laboratory for Micro-Nano Energy Materials and Device and School of Physics and Optoelectronics, Xiangtan University, Hunan, Xiangtan 411105, China
  • 3Key Laboratory for Micro-Nano Physics and Technology of Hunan Province, College of Materials Science and Engineering, Hunan University, Changsha 410082, China
  • 4State Key Laboratory of Powder Metallurgy, Central South University, Changsha 410083, China

  • *Contact author: mxchen@hunnu.edu.cn

Phys. Rev. B 111, L081407 – Published 27 February, 2025

DOI: https://doi.org/10.1103/PhysRevB.111.L081407

Abstract

Going beyond the bistability paradigm of the charge polarization in ferroelectrics is highly desired for ferroelectric (FE) memory devices toward ultrahigh-density information storage. Here, we propose to build multistates by combining the intrinsic and sliding-induced polarizations. The physics is that there is at least one order of magnitude difference in the energy barriers between these two types of polarizations, which leads to a significant difference in the electric fields for reversing the polarization. This difference, along with the symmetry breaking, allows for a unique flipping mechanism involving layer-by-layer sliding followed by layer-by-layer flipping during the transformation of the multistates. As a result, six and ten switchable states can be achieved for the 1T″ bilayers and trilayers, respectively. We further illustrate the concept in H-stacking bilayers and trilayers of 1T″ transition-metal dichalcogenides by first-principles calculations. Our study provides a route to design polarization multistates for developing next-generation memory devices.

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