Related Experiment Video
Updated: Aug 5, 2026

Plasma-assisted Molecular Beam Epitaxy of N-polar InAlN-barrier High-electron-mobility Transistors
Published on: November 24, 2016
Barrier-Assisted Plasma Doping for Spatially Selective Resistance Engineering in MoS2 Transistors
Inseong Lee1, Joonho Park1, Seungsun Yoo2
1School of Electrical Engineering, Korea Advanced Institute of Science and Technology (KAIST), Daejeon, Republic of Korea.
Abstract:
Atomically thin transition-metal dichalcogenides (TMDs) are promising channel materials for low-power logic. However, the absence of scalable and region-selective doping techniques leads to excessive local resistances that hinder the technological readiness of 2D transistors. Here, a barrier-assisted NH3 plasma process is demonstrated that enables degenerate n-type doping of monolayer MoS2 while preserving its crystallinity. The ultrathin pV3D3/Al2O3 dielectric stack not only blocks plasma-induced damage but also functions as a chemical filter that permits NHx radicals to diffuse through. Through this doping process, an electron density of 4.3 × 1013 cm-2 is achieved, yielding a contact resistance of 1.45 kΩ·µm. Density functional calculations show that NH2 radicals adsorbed on the pristine MoS2 surface are the main source of n-type doping while NH radicals can heal S-vacancy defects. Leveraging the spatial selectivity of this approach, mobility and on-current are enhanced by 5.8-fold with negligible threshold-voltage shift. Extension-region activation further suppresses series resistance, increasing the on-current by 260-fold (VDS = 0.05 V) while maintaining enhancement-mode operation. These findings establish barrier-assisted NH3 plasma doping as a promising approach for enabling high-performance n-type 2D transistors and advancing future energy-efficient 2D CMOS technology.
Related Concept Videos
MOSFET: Enhancement Mode
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no current...
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...
Characteristics of MOSFET
Various vital parameters influence their functionality, which is crucial for theory and electronics applications. First, channel dimensions, precisely length, and width, are pivotal. The size of these channels affects the transistor's ability to carry current and switching speeds; shorter channels typically enable quicker...
MOS Capacitor
The metal gate is typically made from highly conductive materials such as aluminum or polysilicon. Beneath the metal gate lies a thin layer of...
MOSFET: Depletion Mode
The primary characteristic of depletion-mode MOSFETs is their ability to conduct current between the drain and source terminals without gate bias. This inherent conductivity arises...
Schottky Barrier Diode

