Related Experiment Video
Updated: Mar 16, 2026

11:14
Comprehensive Characterization of Extended Defects in Semiconductor Materials by a Scanning Electron Microscope
Published on: May 28, 2016
14.5K
Laser damage mechanisms in conductive widegap semiconductor films
Optics Express
|August 10, 2016
Summary
Researchers investigated laser damage in indium tin oxide (ITO) and silicon-doped gallium nitride (Si:GaN) films. ITO showed thermal degradation, while Si:GaN exhibited interface-driven eruptions, revealing distinct laser interaction mechanisms.
Area of Science:
- Materials Science
- Semiconductor Physics
- Laser-Material Interactions
Background:
- Conductive wide-bandgap semiconductors like Indium Tin Oxide (ITO) and Silicon-doped Gallium Nitride (Si:GaN) are crucial for optoelectronic applications.
- Understanding their laser damage mechanisms is vital for device reliability and performance.
- Previous studies often focused on laser photon energies exceeding the bandgap, limiting insights into sub-bandgap interactions.
Purpose of the Study:
- To investigate and compare the laser damage mechanisms of ITO and Si:GaN films under nanosecond pulsed laser irradiation.
- To elucidate the distinct damage morphologies and underlying physical processes in these two conductive semiconductor films.
- To explore the role of free carrier absorption and potential defect markers in laser-induced damage.
Main Methods:
- Microscopy (e.g., optical, electron microscopy) for morphological analysis.
- Spectroscopy (e.g., optical, Raman) for chemical and electronic state characterization.
- Photoluminescence (PL) spectroscopy to probe electronic transitions and defect states.
- Elemental analysis (e.g., EDX) to determine film composition.
- Controlled nanosecond laser pulse exposure with photon energy below the film bandgaps (1.03 eV, 1064 nm).
Main Results:
- Indium Tin Oxide (ITO) films displayed deterministic features indicative of thermal degradation.
- Silicon-doped Gallium Nitride (Si:GaN) films exhibited highly localized damage, manifesting as eruptions originating at internal interfaces.
- Thermally driven damage in ITO was correlated with free carrier absorption.
- Carbon complexes were identified as potential precursors or markers for laser damage in Si:GaN.
Conclusions:
- Laser-induced damage mechanisms in ITO and Si:GaN differ significantly, even under sub-bandgap irradiation.
- Thermal degradation via free carrier absorption dominates ITO laser damage.
- Interface-related phenomena and potential defect markers like carbon complexes are critical in Si:GaN laser damage.
- These findings provide crucial insights for the design and application of wide-bandgap semiconductor devices subjected to laser exposure.
More Related Videos
Related Concept Videos
Metal-Semiconductor Junctions
1.2K
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...
1.2K
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
Fermi Level Dynamics
919
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...
919
Carrier Generation and Recombination
1.5K
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...
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...
1.5K

