Related Experiment Video
Updated: Jul 9, 2026

Analysis of Contact Interfaces for Single GaN Nanowire Devices
Published on: November 15, 2013
Growth Mode-Dependent Bi Incorporation and Carrier Localization in GaAsBi Wires
Chalermchai Himwas1, Aritath Thammathikul1, Nathachon Tachapisitpong1
1Semiconductor Device Research Laboratory, Department of Electrical Engineering, Faculty of Engineering, Chulalongkorn University, 254 Phayathai Road, Bangkok 10330, Thailand.
Abstract:
Dilute bismide III-V semiconductors are attractive for infrared optoelectronics because of their large band gap bowing and suppressed Auger recombination; however, achieving controlled Bi incorporation with uniform optical quality remains challenging. Here, we systematically investigate the relationship between growth mode, Bi incorporation, and carrier dynamics in GaAsBi wires grown by molecular beam epitaxy. By varying the substrate temperature and V/III beam-equivalent pressure ratio, growth transitions from planar deposition to vapor-liquid-solid (VLS) wire growth and subsequently to vapor-solid (VS) growth, defining a process window for homogeneous axial Bi incorporation of up to 2.4%. STEM-EDS analysis confirms uniform axial composition under stable VLS conditions, whereas VS growth results in radial overgrowth and compositional averaging. Temperature-dependent photoluminescence reveals growth-dependent alloy fluctuations and carrier localization, which are quantitatively analyzed using a two-activation Arrhenius model to distinguish carrier delocalization from nonradiative recombination pathways. Homogeneous GaAsBi wires exhibit an internal quantum efficiency of ∼0.2% at 260 K and a temperature-dependent band gap shift slightly larger than those of GaAs nanowires and GaAsBi bulk alloys. Furthermore, droplet-mediated growth enables axial GaAsBi/GaAs heterostructures, demonstrating controlled band-structure engineering in dilute bismide wires. This work establishes a quantitative growth-mode stability window for homogeneous axial Bi incorporation in GaAsBi wires and reveals how VLS-to-VS transitions fundamentally alter carrier localization and thermal quenching behavior.
Related Concept Videos
Carrier Generation and Recombination
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...
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Biasing of P-N Junction
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...
Metal-Semiconductor Junctions
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 semiconductor's...
Semiconductors
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...
Biasing of FET
In an N-channel JFET, the structure consists of N-type material forming the channel on a P-type substrate, with the gate...

