Related Experiment Video
Updated: Mar 25, 2026

11:33
All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
Published on: January 19, 2018
10.4K
Probing dopants in wide semiconductor quantum point contacts.
1Department of Physics, Chemistry and Biology, Linköping University, SE-58183 Linköping, Sweden.
Journal of Physics. Condensed Matter : an Institute of Physics Journal
|February 18, 2016
Summary
Random impurities drastically alter electron behavior in semiconductor quantum point contacts (QPCs), causing electron localization and conductance fluctuations. Understanding impurity effects is key for designing high-mobility electronic devices.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Quantum Electronics
Background:
- Semiconductor quantum point contacts (QPCs) are crucial for understanding electron transport.
- The impact of random impurities on QPC properties is not fully understood.
- Realistic device designs require consideration of impurity effects.
Purpose of the Study:
- To simulate the effects of randomly distributed impurities on QPC conductance, spin polarization, and electron localization.
- To investigate how impurity proximity to the 2DEG influences transport phenomena.
- To guide the design of high-mobility semiconductor devices by evaluating impurity nature.
Main Methods:
- Numerical simulations using density functional theory (DFT) in the local spin-density approximation (LSDA).
- Modeling of gated semiconductor QPCs with realistic impurity distributions.
- Calculation of conductance as a function of gate voltage for various impurity scenarios.
Main Results:
- When impurities are far from the 2DEG, conventional ballistic transport occurs.
- Impurities near the 2DEG induce electron localization, conductance fluctuations, and resonances.
- Resonances shift and decrease in amplitude with asymmetrically charged gates, while interaction effects remain.
- Spin polarization can manifest as stripes in wide QPCs.
Conclusions:
- The position and ionization state of random impurities significantly impact QPC electronic properties.
- Electron localization and conductance anomalies are direct consequences of nearby impurities.
- Understanding these impurity effects is vital for optimizing high-mobility device performance.
Related Concept Videos
Semiconductors
1.8K
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...
1.8K
Metal-Semiconductor Junctions
1.3K
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...
1.3K
Biasing of Metal-Semiconductor Junctions
801
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...
801
Types of Semiconductors
1.8K
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...
1.8K
Fermi Level Dynamics
962
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...
962
P-N junction
1.6K
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...
1.6K

