Related Experiment Video
Updated: Jan 8, 2026

A Fabrication and Measurement Method for a Flexible Ferroelectric Element Based on Van Der Waals Heteroepitaxy
Published on: April 8, 2018
Reconfigurable Symmetry-Broken van der Waals Ferroelectric Semiconductor Heterojunctions for All-in-One
Congmin Zhang1, Dabao Xie1, Zehao Liu1
1College of Optical and Electronic Technology, China Jiliang University, Hangzhou 310018, China.
None:
van der Waals heterojunctions (VHJs) consisting of distinct atomically thin semiconductors with weak interfacial interactions and complementary bandgaps provide a large degree of freedom to design their device structures for multifunctional applications. However, device multifunctionalities highly rely on heterojunctions with tunable band offsets and band alignment type. Herein, we theoretically explore a class of VHJs composed of two-dimensional low-symmetry semiconductors and ferroelectric (FE) semiconductors for achieving multifunctional device applications. Our results indicate that the switchable FE polarization and symmetry-breaking effect enable momentum-matching VHJs with tunable bandgap, band alignment type, and band offset values. Using an α-In2Se3/GeSe VHJ as a prototype example, we demonstrate a type-II-to-type-III band alignment transition driven by the FE polarization switching, resulting in a notable difference of carrier concentration and resistance state between the two FE states. The α-In2Se3/GeSe device presents a giant tunneling electroresistance ratio as high as 1015% that is at least 2 orders of magnitude larger than other VHJ devices. Benefiting from the momentum-matching band alignment and strong optical anisotropy, the device also exhibits FE-dependent photocurrent and broadband polarization sensitivity with a dichroic ratio up to 869, which provides it with huge potential for the realization of an all-in-one optoelectronic architecture with sensing, memory, and processing functions.
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...
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...
Types of Semiconductors
Schottky Barrier Diode
Fermi Level Dynamics
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...

