Design of a sub-terahertz sensor using the electro-optic effect in a semiconductor microcavity

We present design guidelines for a sub-terahertz (THz) sensor based on a semiconductor microcavity probed by transmission using 1.5 μm light. A 3λ cavity made of an InAs/GaAs quantum dot superlattice (QDSL) structure sandwiched between two GaAs/AlAs distributed Bragg reflectors is considered, and we predict a THz detection limit of ∼10 kV/m for a cavity quality factor of ∼1000 and an electro-optic coefficient of the cavity layer that is 20 times larger than that of GaAs. We show that such a sensor can provide relatively large phase-shift signals even when the QDSL structure does not extend over the entire cavity region; it is sufficient to form a relatively thin QDSL region at each antinode of the optical electric field inside the cavity.

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Publication Details

Journal
Journal of Applied Physics
Published
2026-04-15
DOI
https://doi.org/10.1063/5.0320028
Primary Topic
Terahertz technology and applications
Type
article
Field-Weighted Citation Impact
0.00

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article

Design of a sub-terahertz sensor using the electro-optic effect in a semiconductor microcavity

Yasuo Minami, Takahiro KITADA, Takashi Kita, Osamu Kojima et al.
Journal of Applied Physics
Terahertz technology and applications
article

Design of a sub-terahertz sensor using the electro-optic effect in a semiconductor microcavity

Yasuo Minami, Takahiro KITADA, Takashi Kita, Osamu Kojima, Yukihiro Harada, Toshiyuki Kaizu, Osamu Wada
article en

Abstract

We present design guidelines for a sub-terahertz (THz) sensor based on a semiconductor microcavity probed by transmission using 1.5 μm light. A 3λ cavity made of an InAs/GaAs quantum dot superlattice (QDSL) structure sandwiched between two GaAs/AlAs distributed Bragg reflectors is considered, and we predict a THz detection limit of ∼10 kV/m for a cavity quality factor of ∼1000 and an electro-optic coefficient of the cavity layer that is 20 times larger than that of GaAs. We show that such a sensor can provide relatively large phase-shift signals even when the QDSL structure does not extend over the entire cavity region; it is sufficient to form a relatively thin QDSL region at each antinode of the optical electric field inside the cavity.

Journal of Applied PhysicsVol. 139(15)
University of Electro-Communications (JP), National Institute of Technology, Matsue College (JP), College of Industrial Technology (JP), Kobe University (JP), Chiba Institute of Technology (JP)
Japan Society for the Promotion of Science
Affordable and clean energy
Openalex Percentile: Top 17%
Terahertz technology and applications
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