Related Experiment Video
Updated: Aug 1, 2025

07:12
A Standard and Reliable Method to Fabricate Two-Dimensional Nanoelectronics
Published on: August 28, 2018
9.7K
Interface engineering of charge-transfer excitons in 2D lateral heterostructures
Roberto Rosati1, Ioannis Paradisanos2, Libai Huang3
1Department of Physics, Philipps-Universität Marburg, Renthof 7, D-35032, Marburg, Germany. rosatir@staff.uni-marburg.de.
Nature Communications
|April 28, 2023
Summary
Bound charge transfer (CT) excitons in 2D lateral heterostructures were investigated. This study confirms their existence and explores tuning their properties for optoelectronic applications.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Nanotechnology
Background:
- The existence of bound charge transfer (CT) excitons in monolayer lateral heterostructures remains debated.
- Observation of these CT excitons is less confirmed compared to interlayer excitons in vertical heterostructures.
Purpose of the Study:
- To investigate signatures of bound CT excitons in photoluminescence spectra of MoSe2-WSe2 lateral heterostructures.
- To reveal the underlying many-particle processes for CT exciton formation and their tunability.
- To provide a microscopic understanding of optical properties in 2D lateral heterostructures.
Main Methods:
- Microscopic theoretical study based on material-specific theory.
- Photoluminescence (PL) spectroscopy at low temperatures.
- Interface and dielectric engineering for tuning CT exciton properties.
Main Results:
- Predicted the appearance of a low-energy CT exciton for junction widths smaller than the Coulomb-induced Bohr radius.
- Experimental PL measurements confirmed emission in the predicted energy range for bound CT excitons.
- Demonstrated that hBN-encapsulated heterostructures exhibit CT excitons with small binding energies and large dipole moments.
Conclusions:
- This joint theory-experiment study confirms the existence of bound CT excitons in 2D lateral heterostructures.
- CT excitons with small binding energies and large dipole moments are promising for optoelectronics due to efficient exciton dissociation and propagation.
- The findings represent a significant step towards understanding the optical properties of technologically relevant 2D lateral heterostructures.
Related Concept Videos
Metal-Semiconductor Junctions
400
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
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...
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...
400
P-N junction
591
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
591
Carrier Generation and Recombination
648
Carrier generation is the process by which electron-hole pairs (EHPs) are created within the semiconductor. In direct-bandgap semiconductors, such as gallium arsenide (GaAs), this occurs efficiently when energy absorption prompts valence electrons to leap into the conduction band, leaving behind holes.
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
648

