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Infrared avalanche photodiodes from bulk to 2D materials

Avalanche photodiodes (APDs) have drawn huge interest in recent years and have been extensively used in a range of fields including the most important one—optical communication systems due to their time responses and high sensitivities. This article shows the evolution and the recent development of...

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Autores principales: Martyniuk, Piotr, Wang, Peng, Rogalski, Antoni, Gu, Yue, Jiang, Ruiqi, Wang, Fang, Hu, Weida
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10471776/
https://www.ncbi.nlm.nih.gov/pubmed/37652900
http://dx.doi.org/10.1038/s41377-023-01259-3
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author Martyniuk, Piotr
Wang, Peng
Rogalski, Antoni
Gu, Yue
Jiang, Ruiqi
Wang, Fang
Hu, Weida
author_facet Martyniuk, Piotr
Wang, Peng
Rogalski, Antoni
Gu, Yue
Jiang, Ruiqi
Wang, Fang
Hu, Weida
author_sort Martyniuk, Piotr
collection PubMed
description Avalanche photodiodes (APDs) have drawn huge interest in recent years and have been extensively used in a range of fields including the most important one—optical communication systems due to their time responses and high sensitivities. This article shows the evolution and the recent development of A(III)B(V), A(II)B(VI), and potential alternatives to formerly mentioned—“third wave” superlattices (SL) and two-dimensional (2D) materials infrared (IR) APDs. In the beginning, the APDs fundamental operating principle is demonstrated together with progress in architecture. It is shown that the APDs evolution has moved the device’s performance towards higher bandwidths, lower noise, and higher gain-bandwidth products. The material properties to reach both high gain and low excess noise for devices operating in different wavelength ranges were also considered showing the future progress and the research direction. More attention was paid to advances in A(III)B(V) APDs, such as AlInAsSb, which may be used in future optical communications, type-II superlattice (T2SLs, “Ga-based” and “Ga-free”), and 2D materials-based IR APDs. The latter—atomically thin 2D materials exhibit huge potential in APDs and could be considered as an alternative material to the well-known, sophisticated, and developed A(III)B(V) APD technologies to include single-photon detection mode. That is related to the fact that conventional bulk materials APDs’ performance is restricted by reasonably high dark currents. One approach to resolve that problem seems to be implementing low-dimensional materials and structures as the APDs’ active regions. The Schottky barrier and atomic level thicknesses lead to the 2D APD dark current significant suppression. What is more, APDs can operate within visible (VIS), near-infrared (NIR)/mid-wavelength infrared range (MWIR), with a responsivity ~80 A/W, external quantum efficiency ~24.8%, gain ~10(5) for MWIR [wavelength, λ = 4 μm, temperature, T = 10–180 K, Black Phosphorous (BP)/InSe APD]. It is believed that the 2D APD could prove themselves to be an alternative providing a viable method for device fabrication with simultaneous high-performance—sensitivity and low excess noise.
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spelling pubmed-104717762023-09-02 Infrared avalanche photodiodes from bulk to 2D materials Martyniuk, Piotr Wang, Peng Rogalski, Antoni Gu, Yue Jiang, Ruiqi Wang, Fang Hu, Weida Light Sci Appl Review Article Avalanche photodiodes (APDs) have drawn huge interest in recent years and have been extensively used in a range of fields including the most important one—optical communication systems due to their time responses and high sensitivities. This article shows the evolution and the recent development of A(III)B(V), A(II)B(VI), and potential alternatives to formerly mentioned—“third wave” superlattices (SL) and two-dimensional (2D) materials infrared (IR) APDs. In the beginning, the APDs fundamental operating principle is demonstrated together with progress in architecture. It is shown that the APDs evolution has moved the device’s performance towards higher bandwidths, lower noise, and higher gain-bandwidth products. The material properties to reach both high gain and low excess noise for devices operating in different wavelength ranges were also considered showing the future progress and the research direction. More attention was paid to advances in A(III)B(V) APDs, such as AlInAsSb, which may be used in future optical communications, type-II superlattice (T2SLs, “Ga-based” and “Ga-free”), and 2D materials-based IR APDs. The latter—atomically thin 2D materials exhibit huge potential in APDs and could be considered as an alternative material to the well-known, sophisticated, and developed A(III)B(V) APD technologies to include single-photon detection mode. That is related to the fact that conventional bulk materials APDs’ performance is restricted by reasonably high dark currents. One approach to resolve that problem seems to be implementing low-dimensional materials and structures as the APDs’ active regions. The Schottky barrier and atomic level thicknesses lead to the 2D APD dark current significant suppression. What is more, APDs can operate within visible (VIS), near-infrared (NIR)/mid-wavelength infrared range (MWIR), with a responsivity ~80 A/W, external quantum efficiency ~24.8%, gain ~10(5) for MWIR [wavelength, λ = 4 μm, temperature, T = 10–180 K, Black Phosphorous (BP)/InSe APD]. It is believed that the 2D APD could prove themselves to be an alternative providing a viable method for device fabrication with simultaneous high-performance—sensitivity and low excess noise. Nature Publishing Group UK 2023-08-31 /pmc/articles/PMC10471776/ /pubmed/37652900 http://dx.doi.org/10.1038/s41377-023-01259-3 Text en © The Author(s) 2023 https://creativecommons.org/licenses/by/4.0/Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) .
spellingShingle Review Article
Martyniuk, Piotr
Wang, Peng
Rogalski, Antoni
Gu, Yue
Jiang, Ruiqi
Wang, Fang
Hu, Weida
Infrared avalanche photodiodes from bulk to 2D materials
title Infrared avalanche photodiodes from bulk to 2D materials
title_full Infrared avalanche photodiodes from bulk to 2D materials
title_fullStr Infrared avalanche photodiodes from bulk to 2D materials
title_full_unstemmed Infrared avalanche photodiodes from bulk to 2D materials
title_short Infrared avalanche photodiodes from bulk to 2D materials
title_sort infrared avalanche photodiodes from bulk to 2d materials
topic Review Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10471776/
https://www.ncbi.nlm.nih.gov/pubmed/37652900
http://dx.doi.org/10.1038/s41377-023-01259-3
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