Related Experiment Video
Updated: Jan 13, 2026

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
Published on: April 12, 2018
Ferroelectric switchable valleytricity in 2D multiferroic semiconductors
Shuyan Chai1, Wei Wei1, Xinru Li1
1School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, China. lixr@sdu.edu.cn.
Abstract:
Efficient control of the valley index is of great importance for both fundamental research and device applications, yet it remains a challenging problem. Here, through symmetry analysis and an effective k·p model, we propose a novel mechanism for coupling valley index with ferroelectricity in a two-dimensional (2D) multiferroic lattice. The physics behind this is that inequivalent potential arising from ferroelectricity can reverse and annihilate nonsymmetric trigons. Owing to the intimate connection between nonsymmetric trigons and valley physics, the valley index is locked to ferroelectric polarization. This enables the efficient electrical reversal of valley index for carriers and the electrical creation/annihilation of valley polarization. Moreover, based on first-principles calculations, we validate this mechanism in the 2D multiferroic semiconductor TiCr2O4, which favors the paraelectric state as a metastable state. Our work establishes a new paradigm for the design and optimization of valleytronic devices.
Related Concept Videos
Types of Semiconductors
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...
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...
Semiconductors
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Field Effect Transistor
Dielectric Polarization in a Capacitor

