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Charge Trapping and Emission Properties in CAAC-IGZO Transistor: A First-Principles Calculations

The c-axis aligned crystalline indium-gallium-zinc-oxide field-effect transistor (CAAC-IGZO FET), exhibiting an extremely low off-state leakage current (~10(−22) A/μm), has promised to be an ideal candidate for Dynamic Random Access Memory (DRAM) applications. However, the instabilities leaded by th...

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Autores principales: Wang, Ziqi, Lu, Nianduan, Wang, Jiawei, Geng, Di, Wang, Lingfei, Yang, Guanhua
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10058374/
https://www.ncbi.nlm.nih.gov/pubmed/36984162
http://dx.doi.org/10.3390/ma16062282
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author Wang, Ziqi
Lu, Nianduan
Wang, Jiawei
Geng, Di
Wang, Lingfei
Yang, Guanhua
author_facet Wang, Ziqi
Lu, Nianduan
Wang, Jiawei
Geng, Di
Wang, Lingfei
Yang, Guanhua
author_sort Wang, Ziqi
collection PubMed
description The c-axis aligned crystalline indium-gallium-zinc-oxide field-effect transistor (CAAC-IGZO FET), exhibiting an extremely low off-state leakage current (~10(−22) A/μm), has promised to be an ideal candidate for Dynamic Random Access Memory (DRAM) applications. However, the instabilities leaded by the drift of the threshold voltage in various stress seriously affect the device application. To better develop high performance CAAC-IGZO FET for DRAM applications, it’s essential to uncover the deep physical process of charge transport mechanism in CAAC-IGZO FET. In this work, by combining the first-principles calculations and nonradiative multiphonon theory, the charge trapping and emission properties in CAAC-IGZO FET have been systematically investigated. It is found that under positive bias stress, hydrogen interstitial in Al(2)O(3) gate dielectric is probable effective electron trap center, which has the transition level (ε (+1/−1) = 0.52 eV) above Fermi level. But it has a high capture barrier about 1.4 eV and low capture rate. Under negative bias stress, oxygen vacancy in Al(2)O(3) gate dielectric and CAAC-IGZO active layer are probable effective electron emission centers whose transition level ε (+2/0) distributed at −0.73~−0.98 eV and 0.69 eV below Fermi level. They have a relatively low emission barrier of about 0.5 eV and 0.25 eV and high emission rate. To overcome the instability in CAAC-IGZO FET, some approaches can be taken to control the hydrogen concentration in Al(2)O(3) dielectric layer and the concentration of the oxygen vacancy. This work can help to understand the mechanisms of instability of CAAC-IGZO transistor caused by the charge capture/emission process.
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spelling pubmed-100583742023-03-30 Charge Trapping and Emission Properties in CAAC-IGZO Transistor: A First-Principles Calculations Wang, Ziqi Lu, Nianduan Wang, Jiawei Geng, Di Wang, Lingfei Yang, Guanhua Materials (Basel) Article The c-axis aligned crystalline indium-gallium-zinc-oxide field-effect transistor (CAAC-IGZO FET), exhibiting an extremely low off-state leakage current (~10(−22) A/μm), has promised to be an ideal candidate for Dynamic Random Access Memory (DRAM) applications. However, the instabilities leaded by the drift of the threshold voltage in various stress seriously affect the device application. To better develop high performance CAAC-IGZO FET for DRAM applications, it’s essential to uncover the deep physical process of charge transport mechanism in CAAC-IGZO FET. In this work, by combining the first-principles calculations and nonradiative multiphonon theory, the charge trapping and emission properties in CAAC-IGZO FET have been systematically investigated. It is found that under positive bias stress, hydrogen interstitial in Al(2)O(3) gate dielectric is probable effective electron trap center, which has the transition level (ε (+1/−1) = 0.52 eV) above Fermi level. But it has a high capture barrier about 1.4 eV and low capture rate. Under negative bias stress, oxygen vacancy in Al(2)O(3) gate dielectric and CAAC-IGZO active layer are probable effective electron emission centers whose transition level ε (+2/0) distributed at −0.73~−0.98 eV and 0.69 eV below Fermi level. They have a relatively low emission barrier of about 0.5 eV and 0.25 eV and high emission rate. To overcome the instability in CAAC-IGZO FET, some approaches can be taken to control the hydrogen concentration in Al(2)O(3) dielectric layer and the concentration of the oxygen vacancy. This work can help to understand the mechanisms of instability of CAAC-IGZO transistor caused by the charge capture/emission process. MDPI 2023-03-12 /pmc/articles/PMC10058374/ /pubmed/36984162 http://dx.doi.org/10.3390/ma16062282 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Wang, Ziqi
Lu, Nianduan
Wang, Jiawei
Geng, Di
Wang, Lingfei
Yang, Guanhua
Charge Trapping and Emission Properties in CAAC-IGZO Transistor: A First-Principles Calculations
title Charge Trapping and Emission Properties in CAAC-IGZO Transistor: A First-Principles Calculations
title_full Charge Trapping and Emission Properties in CAAC-IGZO Transistor: A First-Principles Calculations
title_fullStr Charge Trapping and Emission Properties in CAAC-IGZO Transistor: A First-Principles Calculations
title_full_unstemmed Charge Trapping and Emission Properties in CAAC-IGZO Transistor: A First-Principles Calculations
title_short Charge Trapping and Emission Properties in CAAC-IGZO Transistor: A First-Principles Calculations
title_sort charge trapping and emission properties in caac-igzo transistor: a first-principles calculations
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10058374/
https://www.ncbi.nlm.nih.gov/pubmed/36984162
http://dx.doi.org/10.3390/ma16062282
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