Terahertz emission mechanisms in low-temperature-grown and semi-insulating gallium arsenide photoconductive antenna devices excited at above- and below-bandgap photon energies

Abstract In this work, the terahertz (THz) time-domain spectroscopy was employed in studying the carrier dynamics in low-temperature grown (LT-) and semi-insulating (SI-) gallium arsenide (GaAs) photoconductive antenna (PCA) at above- ( λ = 780 nm, E g = 1.59 eV) and below- ( λ = 1.55 µ m, E g 0.80...

Full description

Saved in:
Bibliographic Details
Published inSemiconductor science and technology Vol. 39; no. 7; pp. 75010 - 75019
Main Authors F Dela Rosa, L N, Publico, J B, F Cabello, N I, R Ferrolino, J P, P Juguilon, V P, M Verona, I C, Salvador, A A, Somintac, A S, De Los Reyes, A E, Bardolaza, H R, Estacio, E S
Format Journal Article
LanguageEnglish
Published IOP Publishing 01.07.2024
Subjects
Online AccessGet full text

Cover

Loading…
More Information
Summary:Abstract In this work, the terahertz (THz) time-domain spectroscopy was employed in studying the carrier dynamics in low-temperature grown (LT-) and semi-insulating (SI-) gallium arsenide (GaAs) photoconductive antenna (PCA) at above- ( λ = 780 nm, E g = 1.59 eV) and below- ( λ = 1.55 µ m, E g 0.80 eV) bandgap excitation. We measured the excitation power dependence of the LT-GaAs (SI-GaAs) THz emission. Then, the equivalent circuit model which considers the (i) photogeneration, (ii) screening effects, and (iii) transport of carriers was utilized in analyzing the THz radiation mechanisms in the above- and below-bandgap excitation of the two substrates. In simulating the above-bandgap THz emission of both PCAs, we employed the direct bandgap excitation model which takes into account the band-to-band transitions of photoexcited carriers. Meanwhile, to simulate the LT-GaAs (SI-GaAs) THz emission at below-bandgap excitation we utilized the two-step photoabsorption facilitated by the mid-gap states. In this model the photoexcited carriers jump from the valence band to the mid-gap states and then to the conduction band. Results suggest that the THz emission from LT-GaAs and SI-GaAs at above- and below-bandgap excitation occur due to band-to-band transitions, and two-step photoabsorption process via midgap states, respectively.
Bibliography:SST-109876.R4
ISSN:0268-1242
1361-6641
DOI:10.1088/1361-6641/ad4322