Related Experiment Video
Updated: Jun 26, 2025

In Situ Transmission Electron Microscopy with Biasing and Fabrication of Asymmetric Crossbars Based on Mixed-Phased a-VOx
Published on: May 13, 2020
Twist angle-dependent valley polarization switching in heterostructures.
Danjie Dai1,2, Bowen Fu3, Jingnan Yang3
1Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
We show how twisting van der Waals heterostructures controls valley polarization in interlayer excitons (IXs). This twist engineering enables electrical control for future valleytronic and twistronic devices.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Nanotechnology
Background:
- Moiré superlattices in transition metal dichalcogenide heterostructures offer control over valley physics.
- Interlayer excitons (IXs) exhibit valley properties crucial for valleytronics.
- Electrical control of valley polarization in these systems remains underexplored.
Purpose of the Study:
- Investigate the twist angle-dependent control of excitonic potential on valley polarization.
- Elucidate the physical mechanisms governing twist angle modulation of valley polarization.
- Demonstrate electrically controlled valley-addressable devices.
Main Methods:
- Fabrication of van der Waals heterostructures with controlled twist angles.
- Electrical gating to modulate carrier densities and exciton properties.
- Optical spectroscopy to probe valley polarization and exciton dynamics.
Main Results:
- Demonstrated dependence of polarization switching and degree of valley polarization on moiré period.
- Identified mechanisms for twist angle modulation of exciton potential and electron-hole exchange interaction.
- Achieved twist angle-dependent valley polarization of IXs.
Conclusions:
- Twist angle engineering effectively manipulates valley polarization of IXs in electrically controlled heterostructures.
- The findings provide a pathway for electrical control of valley degrees of freedom in twistronic devices.
- This work paves the way for next-generation valleytronic devices with tunable properties.
Related Concept Videos
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...
Biasing of P-N Junction
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
Dielectric Polarization in a Capacitor
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...
P-N junction
Induced Electric Dipoles
Since the absolute value of potential energy holds no physical meaning, its zero value can be chosen as per...

