Related Experiment Video
Updated: Jul 10, 2026

Ohmic Contact Fabrication Using a Focused-ion Beam Technique and Electrical Characterization for Layer Semiconductor Nanostructures
Published on: December 5, 2015
Charge transfer tunneling contacts for n-type monolayer semiconductor toward high performance electronics
Pan Chen1, Canfei Gao1, Wenjun Wu1
1Shanghai Key Laboratory of High Temperature Superconductors, Institute for Quantum Science and Technology, Department of Physics, Shanghai University, Shanghai 200444, China.
Abstract:
The emergence of two-dimensional (2D) semiconductors, particularly transition metal dichalcogenides (TMDs), shows great potential in revolution of the development of electronics. However, challenges in contact engineering, such as Fermi-level pinning and metal-induced gap states (MIGS) and disorders greatly hinder the high-performance devices based on 2D materials. Here, we propose a novel strategy to establish quasi-one-dimensional tunneling contacts through locally modulating the electronic properties of monolayer MoS2 beneath the metal electrode by high-electron-affinity transition metal oxides (TMOs). MoO3 is introduced to induce strong charge-transfer anti-doping in the contact region, effectively depleting free carriers and rendering the underlying MoS2 electrically insulating and behaving as the tunneling layer. The Au/MoO3-contacted monolayer-MoS2 field-effect transistors exhibit near-ideal ohmic characteristics with an exceptionally low Schottky barrier height (SBH) of 1.6 meV, nearing the theoretical limit. The field effect mobility reaches 559.5 cm2/V∙s at 10 K. Moreover, we demonstrate that substitution of MoO3 with V2O5 provides a means to tune the SBH, underscoring the versatility of this device fabrication strategy. This study presents a promising pathway for achieving efficient tunneling contacts in 2D electronics, paving the way for the advancement of next-generation high-performance devices.
More Related Videos
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 semiconductor's...
P-N junction
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...
Carrier Transport
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
Schottky Barrier Diode
Biasing of FET
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the gate...

