Related Experiment Video
Updated: Jun 2, 2025

Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations
Published on: October 12, 2019
In-Plane Transition-Metal Dichalcogenide Junction with Nearly Zero Interfacial Band Offset
Jinfeng Zhang1, Genyu Hu1, Shihao Hu1
1Center for Interdisciplinary Science of Optical Quantum and NEMS Integration, School of Physics, Advanced Research Institute of Multidisciplinary Science, and School of Integrated Circuits and Electronics, Beijing Institute of Technology, Beijing 100081, China.
Abstract:
Two-dimensional in-plane transition-metal dichalcogenide (TMD) junctions have a range of potential applications in next-generation electronic devices. However, limited by the difficulties in ion implantation on 2D systems, the fabrication of the in-plane TMD junctions still relies on the lateral epitaxy of different materials, which always induces lattice mismatch and interfacial scattering. Here, we report the in-plane TMD junction formed with monolayer (ML) PtTe2 at the boundary of ML and bilayer graphene on SiC. As the scanning tunneling microscopy/spectroscopy results revealed, the substrate screen effect is weak on ML PtTe2, compared to the nonlayered materials. At the interface of the junction, the atomic lattice is continuous, and a smooth type-II band alignment is formed with a near-zero band offset. The reported technique can be readily extended to other 2D semiconductors with strong interlayer coupling and is feasible for fabricating TMD junctions with promising interfacial electronic structures, aimed at device applications based on low-dimensional electronic behaviors.
More Related Videos
08:50Preparation of Large-area Vertical 2D Crystal Hetero-structures Through the Sulfurization of Transition Metal Films for Device Fabrication
Published on: November 28, 2017
08:12Ohmic Contact Fabrication Using a Focused-ion Beam Technique and Electrical Characterization for Layer Semiconductor Nanostructures
Published on: December 5, 2015
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...
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...
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...
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...
Crystal Field Theory - Tetrahedral and Square Planar Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...