Related Experiment Video
Updated: Dec 26, 2025

Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
Published on: April 12, 2018
Charge transfers and charged defects in WSe2/graphene-SiC interfaces
Y J Dappe1, Y Almadori2, M T Dau3
1SPEC, CEA, CNRS, Université Paris Saclay, CEA Saclay, 91191 Gif-sur-Yvette Cedex France.
Kelvin probe force microscopy and DFT reveal electron transfer in tungsten diselenide/graphene heterojunctions. This charge transfer neutralizes graphene doping, consistent with the Schottky-Mott model, with minimal impact from additional layers.
Area of Science:
- Materials Science
- Condensed Matter Physics
- Surface Science
Background:
- Vertical heterojunctions are crucial for advanced electronic devices.
- Understanding charge transfer at interfaces is key to optimizing device performance.
- Tungsten diselenide (WSe2) and graphene are promising 2D materials for such applications.
Purpose of the Study:
- To investigate charge transfer mechanisms in WSe2/graphene vertical heterojunctions.
- To determine the origin of interface dipoles.
- To validate the applicability of the Schottky-Mott model.
Main Methods:
- Kelvin probe force microscopy (KPFM) for experimental surface potential measurements.
- Density functional theory (DFT) for atomic-level simulations of electronic structure and charge distribution.
- Fabrication of WSe2/graphene heterojunctions on silicon carbide substrates.
Main Results:
- Experimental evidence of an interface dipole was observed.
- DFT confirmed electron transfer from n-doped graphene to the WSe2 layer, neutralizing the doping.
- KPFM showed a constant vacuum level shift with varying graphene layers, supporting the Schottky-Mott model.
- DFT indicated that the first WSe2 layer captures most excess charge, with minimal influence from subsequent layers.
- Charged defects at WSe2 edges impact the electrostatic landscape.
Conclusions:
- Charge transfer is the dominant mechanism governing the electronic properties of WSe2/graphene heterojunctions.
- The Schottky-Mott model accurately describes these interfaces when considering charge transfer.
- Interface dipole formation is primarily driven by the initial WSe2 layer and graphene doping levels.
More Related Videos
11:42Fabrication of Gate-tunable Graphene Devices for Scanning Tunneling Microscopy Studies with Coulomb Impurities
Published on: July 24, 2015
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...
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: