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Non-Markovian Hole Excess Noise in Avalanche Amorphous Selenium Thin Films

[Image: see text] Enhancing the signal-to-noise ratio in avalanche photodiodes by utilizing impact ionization gain requires materials exhibiting low excess noise factors. Amorphous selenium (a-Se) as a wide bandgap at ∼2.1 eV, a solid-state avalanche layer, demonstrates single-carrier hole impact io...

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Autores principales: Mukherjee, Atreyo, Han, Zhihang, Triet Ho, Le Thanh, Rumaiz, Abdul K., Vasileska, Dragica, Goldan, Amir H.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10324078/
https://www.ncbi.nlm.nih.gov/pubmed/37426242
http://dx.doi.org/10.1021/acsomega.3c01256
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author Mukherjee, Atreyo
Han, Zhihang
Triet Ho, Le Thanh
Rumaiz, Abdul K.
Vasileska, Dragica
Goldan, Amir H.
author_facet Mukherjee, Atreyo
Han, Zhihang
Triet Ho, Le Thanh
Rumaiz, Abdul K.
Vasileska, Dragica
Goldan, Amir H.
author_sort Mukherjee, Atreyo
collection PubMed
description [Image: see text] Enhancing the signal-to-noise ratio in avalanche photodiodes by utilizing impact ionization gain requires materials exhibiting low excess noise factors. Amorphous selenium (a-Se) as a wide bandgap at ∼2.1 eV, a solid-state avalanche layer, demonstrates single-carrier hole impact ionization gain and manifests ultralow thermal generation rates. A comprehensive study of the history dependent and non-Markovian nature of hot hole transport in a-Se was modeled using a Monte Carlo (MC) random walk of single hole free flights, interrupted by instantaneous phonon, disorder, hole–dipole, and impact-ionization scattering interactions. The hole excess noise factors were simulated for 0.1–15 μm a-Se thin-films as a function of mean avalanche gain. The hole excess noise factors in a-Se decreases with an increase in electric field, impact ionization gain, and device thickness. The history dependent nature of branching of holes is explained using a Gaussian avalanche threshold distance distribution and the dead space distance, which increases determinism in the stochastic impact ionization process. An ultralow non-Markovian excess noise factor of ∼1 was simulated for 100 nm a-Se thin films corresponding to avalanche gains of 1000. Future detector designs can utilize the nonlocal/non-Markovian nature of the hole avalanche in a-Se, to enable a true solid-state photomultiplier with noiseless gain.
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spelling pubmed-103240782023-07-07 Non-Markovian Hole Excess Noise in Avalanche Amorphous Selenium Thin Films Mukherjee, Atreyo Han, Zhihang Triet Ho, Le Thanh Rumaiz, Abdul K. Vasileska, Dragica Goldan, Amir H. ACS Omega [Image: see text] Enhancing the signal-to-noise ratio in avalanche photodiodes by utilizing impact ionization gain requires materials exhibiting low excess noise factors. Amorphous selenium (a-Se) as a wide bandgap at ∼2.1 eV, a solid-state avalanche layer, demonstrates single-carrier hole impact ionization gain and manifests ultralow thermal generation rates. A comprehensive study of the history dependent and non-Markovian nature of hot hole transport in a-Se was modeled using a Monte Carlo (MC) random walk of single hole free flights, interrupted by instantaneous phonon, disorder, hole–dipole, and impact-ionization scattering interactions. The hole excess noise factors were simulated for 0.1–15 μm a-Se thin-films as a function of mean avalanche gain. The hole excess noise factors in a-Se decreases with an increase in electric field, impact ionization gain, and device thickness. The history dependent nature of branching of holes is explained using a Gaussian avalanche threshold distance distribution and the dead space distance, which increases determinism in the stochastic impact ionization process. An ultralow non-Markovian excess noise factor of ∼1 was simulated for 100 nm a-Se thin films corresponding to avalanche gains of 1000. Future detector designs can utilize the nonlocal/non-Markovian nature of the hole avalanche in a-Se, to enable a true solid-state photomultiplier with noiseless gain. American Chemical Society 2023-06-16 /pmc/articles/PMC10324078/ /pubmed/37426242 http://dx.doi.org/10.1021/acsomega.3c01256 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by-nc-nd/4.0/Permits non-commercial access and re-use, provided that author attribution and integrity are maintained; but does not permit creation of adaptations or other derivative works (https://creativecommons.org/licenses/by-nc-nd/4.0/).
spellingShingle Mukherjee, Atreyo
Han, Zhihang
Triet Ho, Le Thanh
Rumaiz, Abdul K.
Vasileska, Dragica
Goldan, Amir H.
Non-Markovian Hole Excess Noise in Avalanche Amorphous Selenium Thin Films
title Non-Markovian Hole Excess Noise in Avalanche Amorphous Selenium Thin Films
title_full Non-Markovian Hole Excess Noise in Avalanche Amorphous Selenium Thin Films
title_fullStr Non-Markovian Hole Excess Noise in Avalanche Amorphous Selenium Thin Films
title_full_unstemmed Non-Markovian Hole Excess Noise in Avalanche Amorphous Selenium Thin Films
title_short Non-Markovian Hole Excess Noise in Avalanche Amorphous Selenium Thin Films
title_sort non-markovian hole excess noise in avalanche amorphous selenium thin films
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10324078/
https://www.ncbi.nlm.nih.gov/pubmed/37426242
http://dx.doi.org/10.1021/acsomega.3c01256
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