Related Experiment Video
Updated: Oct 10, 2025

05:39
Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
9.8K
Dark exciton anti-funneling in atomically thin semiconductors
Roberto Rosati1, Robert Schmidt2, Samuel Brem1
1Department of Physics, Philipps-Universität Marburg, 35032, Marburg, Germany.
Nature Communications
|December 11, 2021
Summary
Atomically thin semiconductors use excitons, not electric fields, for transport. New research reveals excitons move away from strain, enabling novel control strategies for nanoelectronic devices.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Nanoscience
Background:
- Charge carrier transport is fundamental to nanoelectronics.
- Atomically thin semiconductors rely on excitons (neutral electron-hole pairs) for transport, which are not electrically controllable.
- Strain engineering offers a method to manipulate exciton propagation.
Purpose of the Study:
- To investigate exciton transport dynamics in atomically thin semiconductors under strain.
- To understand the influence of strain gradients on exciton movement.
- To explore novel methods for controlling exciton behavior in these materials.
Main Methods:
- Combined spatiotemporal photoluminescence measurements.
- Microscopic theoretical modeling.
- Tracking exciton behavior in time, space, and energy.
Main Results:
- Excitons exhibit anti-funneling behavior, moving away from high-strain regions.
- This phenomenon is attributed to the influence of dark excitons with opposing strain-induced energy variations.
- Demonstrated control over exciton transport through strain engineering.
Conclusions:
- Strain engineering can be used to control exciton transport in atomically thin semiconductors.
- The interplay between bright and dark excitons dictates strain-induced exciton movement.
- Findings pave the way for advanced applications in exciton-dominated nanoelectronics.
Related Concept Videos
Fermi Level Dynamics
376
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
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...
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...
376
Types of Semiconductors
1000
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
1000
Metal-Semiconductor Junctions
558
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...
558
Fermi Level
921
The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
921
Biasing of Metal-Semiconductor Junctions
361
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
361
Energy Bands in Solids
1.4K
Isolated atoms have discrete energy levels that are well described by the Bohr model. And, it quantifies the energy of an electron in a hydrogen atom as En. Higher quantum numbers 'n' yield less negative, closer electron energy levels.
Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states...
Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states...
1.4K

