Related Experiment Video
Updated: May 27, 2025

Ohmic Contact Fabrication Using a Focused-ion Beam Technique and Electrical Characterization for Layer Semiconductor Nanostructures
Published on: December 5, 2015
Twist-Dependent Semiconductor-to-Metal Transition in Epitaxial Bilayer α-Antimonene
Peiyao Xiao1,2, Ji Li1,2, Douxing Pan3
1Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement, Ministry of Education, School of Physics, Beijing Institute of Technology, Beijing 100081, China.
Abstract:
In spite of the observation of various exotic correlated physics in twisted graphene and transition metal dichalcogenides, it remains a great challenge to prepare twisted bilayers of puckered elemental layered crystals in the developing field of twistronics. Here, we report the first discovery and success in epitaxial growth of the 39°-twisted bilayer α-Sb. Molecular dynamics simulations verify that the 39°-twisted bilayer α-Sb is energetically stable, consistent with the experiments. Scanning tunneling spectroscopy in combination with first-principles calculations confirms that the 39°-twisted bilayer α-Sb is metallic, whereas the AB-stacked bilayer α-Sb appears semiconducting. Such a twist-dependent semiconductor-to-metal transition can be rationalized by the fact that the twist-induced reconstruction facilitates enhanced interlayer electron hopping between the p orbitals in the 39°-twisted bilayer α-Sb. Our work sheds light on the synthesis of twisted bilayers of puckered elemental layered crystals and paves the way for twistronics.
Related Concept Videos
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...
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...

