Related Experiment Video
Updated: May 11, 2026

10:36
Electric-field Control of Electronic States in WS2 Nanodevices by Electrolyte Gating
Published on: April 12, 2018
Topological insulating states in laterally patterned ordinary semiconductors
1School of Physics, University of New South Wales, Sydney 2052, Australia.
Physical Review Letters
|May 21, 2013
Summary
We propose that ordinary semiconductors can host stable topological states. These states, featuring chiral spin edge states, are tunable and achievable with current technology, paving the way for room-temperature topological insulators.
Area of Science:
- Condensed matter physics
- Materials science
- Quantum mechanics
Background:
- Topological insulators are materials with unique electronic properties.
- Harnessing topological states in semiconductors is a key research area.
- Spin-orbit coupling is crucial for realizing topological phenomena.
Purpose of the Study:
- To propose a method for creating stable and tunable topological states in ordinary semiconductors.
- To investigate the potential for large electronic gaps supporting chiral spin edge states.
- To assess the feasibility of fabricating topological insulators using existing technology.
Main Methods:
- Theoretical modeling of semiconductor heterostructures.
- Incorporation of quantum confinement and hexagonal potentials.
- Analysis of electronic band structures and spin properties.
Main Results:
- Stable topological states can be hosted in semiconductors like GaAs with large spin-orbit coupling.
- Significant electronic gaps (up to bandwidth) supporting chiral spin edge states are achievable.
- Topological insulators operating at 10-100 K are producible with current lithography.
Conclusions:
- Ordinary semiconductors can be engineered into robust topological insulators.
- Existing lithographic techniques enable the creation of low-temperature topological insulators.
- Advancements in lithography promise tunable room-temperature topological insulators.
Related Concept Videos
Semiconductors
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Band Theory
When two or more atoms come together to form a molecule, their atomic orbitals combine and molecular orbitals of distinct energies result. In a solid, there are a large number of atoms, and therefore a large number of atomic orbitals that may be combined into molecular orbitals. These groups of molecular orbitals are so closely placed together to form continuous regions of energies, known as the bands.
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
Types of Semiconductors
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...
Metal-Semiconductor Junctions
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 semiconductor's...
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...
Fermi Level
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,...
Types Of Superconductors
A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...

