Related Experiment Video
Updated: Jun 4, 2025

15:58
Measurement of Coherence Decay in GaMnAs Using Femtosecond Four-wave Mixing
Published on: December 3, 2013
5.7K
Photo-Excited Carrier Dynamics in Ammonothermal Mn-Compensated GaN Semiconductor
Patrik Ščajev1, Paweł Prystawko2, Robert Kucharski2
1Institute of Photonics and Nanotechnology, Faculty of Physics, Vilnius University, Saulėtekio Ave. 3, 10257 Vilnius, Lithuania.
Materials (Basel, Switzerland)
|December 17, 2024
Summary
Investigating carrier dynamics in manganese-compensated gallium nitride (GaN:Mn) reveals how defects impact charge carrier relaxation. Understanding these dynamics is crucial for advanced electronic device applications.
Area of Science:
- Semiconductor Physics
- Materials Science
- Optoelectronics
Background:
- Ammonothermal gallium nitride (GaN:Mn) is a promising semiconductor material.
- Understanding carrier dynamics and defect impacts is crucial for device performance.
Purpose of the Study:
- To investigate carrier dynamics in ammonothermal GaN:Mn using photo-excitation.
- To determine the influence of Mn-induced states and Mg acceptors on charge carrier relaxation rates.
Main Methods:
- Photoluminescence analysis with sub-bandgap and above-bandgap photo-excitation.
- Pump-probe measurements for time-resolved carrier dynamics.
- Contactless probing techniques for defect analysis.
Main Results:
- Mn impurities exhibit photoconductivity and absorption bands around 700-800 nm.
- Electrons in conduction band tails drive photoconductivity and yellow luminescence decays.
- Mg acceptors dominate slower red luminescence and pump-probe decays.
- Yellow photoluminescence decay time increases with excitation intensity due to defect saturation.
Conclusions:
- Carrier relaxation in GaN:Mn is influenced by Mn states and Mg acceptors.
- Fast photo-carrier decay is vital for high-frequency and high-voltage device applications.
Related Concept Videos
Carrier Generation and Recombination
510
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...
510
Types of Semiconductors
525
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...
525
Metal-Semiconductor Junctions
292
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...
292
Atomic Nuclei: Nuclear Relaxation Processes
622
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
622

