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Related Concept Videos

Types of Semiconductors01:20

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...
P-N junction01:11

P-N junction

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...
Energy Bands in Solids01:01

Energy Bands in Solids

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 that no two...
Valence Bond Theory02:42

Valence Bond Theory

Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
Biasing of P-N Junction01:16

Biasing of P-N Junction

The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

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...

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Related Experiment Video

Updated: Jun 15, 2026

Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots
15:47

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Published on: November 1, 2013

Zero-internal fields in nonpolar InGaN/GaN multi-quantum wells grown by the multi-buffer layer technique.

Hooyoung Song1, Jin Soak Kim, Eun Kyu Kim

  • 1Quantum-Function Spinics Laboratory, Department of Physics, Hanyang University, Seoul, Korea.

Nanotechnology
|March 9, 2010
PubMed
Summary

Nonpolar a-plane Indium Gallium Nitride/Gallium Nitride (InGaN/GaN) multi-quantum wells (MQWs) show potential for high-efficiency light-emitting diodes. These structures overcome efficiency droop issues common in traditional c-plane designs.

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Last Updated: Jun 15, 2026

Nanofabrication of Gate-defined GaAs/AlGaAs Lateral Quantum Dots
15:47

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Published on: November 1, 2013

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Plasma-assisted Molecular Beam Epitaxy of N-polar InAlN-barrier High-electron-mobility Transistors
10:31

Plasma-assisted Molecular Beam Epitaxy of N-polar InAlN-barrier High-electron-mobility Transistors

Published on: November 24, 2016

Area of Science:

  • Materials Science
  • Solid State Physics
  • Optoelectronics

Background:

  • Conventional c-plane Gallium Nitride (GaN) based light-emitting diodes (LEDs) suffer from efficiency limitations due to strong piezoelectric fields.
  • Nonpolar InGaN/GaN multi-quantum wells (MQWs) offer a promising alternative by minimizing these fields.

Purpose of the Study:

  • To demonstrate the potential of nonpolar a-plane InGaN/GaN MQWs for high-performance optoelectronic devices.
  • To investigate the structural quality, electron capture barriers, and optical properties of nonpolar InGaN/GaN MQWs.

Main Methods:

  • Growth of a-GaN template on r-plane sapphire using a multi-buffer layer technique.
  • High-resolution X-ray diffraction (HRXRD) for structural quality assessment.
  • Deep Level Transient Spectroscopy (DLTS) for barrier analysis.
  • Temperature-dependent photoluminescence (PL) spectroscopy.

Main Results:

  • Achieved high structural quality of the a-GaN template with a narrow omega full width at half maximum (FWHM) of 418 arcsec.
  • Identified lower electron capture barriers in a-plane InGaN/GaN MQWs compared to c-plane samples, suggesting a solution to efficiency droop.
  • Observed temperature-dependent PL peak shifts well-fitted by Varshni's equation, indicating minimal internal fields.
  • Demonstrated high photoluminescence efficiency (0.27) for the nonpolar MQWs.

Conclusions:

  • Nonpolar a-plane InGaN/GaN MQWs are free from strong piezoelectric fields, addressing a key limitation in GaN-based LEDs.
  • These nonpolar structures exhibit superior properties, including lower electron capture barriers and high optical efficiency, making them crucial for overcoming efficiency limitations in conventional LEDs.