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Metal-Semiconductor Junctions01:24

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...
558
Carrier Generation and Recombination01:22

Carrier Generation and Recombination

866
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...
866
Fermi Level Dynamics01:12

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...
376
Energy Bands in Solids01:01

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...
1.4K
Biasing of Metal-Semiconductor Junctions01:27

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...
361
Types of Semiconductors01:20

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

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Related Experiment Video

Updated: Oct 11, 2025

Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations
13:56

Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations

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Indirect to Direct Band Gap Transformation by Surface Engineering in Semiconductor Nanostructures.

Marco Califano1,2, Ruiyan Lu3, Yeke Zhou3

  • 1Pollard Institute, School of Electronic and Electrical Engineering, University of Leeds, Leeds LS2 9JT, United Kingdom.

ACS Nano
|December 7, 2021
PubMed
Summary

Researchers transformed indirect semiconductors like GaP into direct gap materials using nanostructuring and surface engineering. This method enhances optical properties without altering the material

Keywords:
AlAsGaPindirect materialsindirect-to-direct transitionsk-vector analysisnanocrystalspseudopotential method

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Area of Science:

  • Materials Science
  • Solid State Physics
  • Optoelectronics

Background:

  • Indirect band gap semiconductors have limited optical conversion efficiency due to poor optical properties.
  • Current strategies like doping or alloying to improve efficiency often alter material properties and band gap energy.
  • A significant challenge is enhancing optical transitions without changing the intrinsic nature of these materials.

Purpose of the Study:

  • To develop a strategy for enhancing optical transitions in indirect band gap semiconductors.
  • To demonstrate that nanostructuring and surface engineering can convert indirect semiconductors into direct gap materials.
  • To establish a generalizable method for improving the optical properties of indirect materials.

Main Methods:

  • Nanostructuring and surface engineering of Gallium Phosphide (GaP).
  • Distillation of key procedure elements into a generalizable recipe.
  • Application of the recipe to Aluminum Arsenide (AlAs) for validation.

Main Results:

  • Gallium Phosphide (GaP) was successfully transformed into a direct gap material.
  • The nanostructuring and surface engineering approach preserved the intrinsic properties of GaP.
  • A significant increase of over 4 orders of magnitude in emission intensity and radiative rates was observed for AlAs.

Conclusions:

  • Nanostructuring and surface engineering offer an effective route to enhance optical transitions in indirect band gap materials.
  • This approach allows for the conversion to direct gap properties while maintaining the material's original identity.
  • The developed method is broadly applicable to other indirect band gap semiconductors, as demonstrated with AlAs.