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Deep-submicron Graphene Field-Effect Transistors with State-of-Art f(max)
In order to conquer the short-channel effects that limit conventional ultra-scale semiconductor devices, two-dimensional materials, as an option of ultimate thin channels, receive wide attention. Graphene, in particular, bears great expectations because of its supreme carrier mobility and saturation...
Autores principales: | , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group
2016
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5075922/ https://www.ncbi.nlm.nih.gov/pubmed/27775009 http://dx.doi.org/10.1038/srep35717 |
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author | Lyu, Hongming Lu, Qi Liu, Jinbiao Wu, Xiaoming Zhang, Jinyu Li, Junfeng Niu, Jiebin Yu, Zhiping Wu, Huaqiang Qian, He |
author_facet | Lyu, Hongming Lu, Qi Liu, Jinbiao Wu, Xiaoming Zhang, Jinyu Li, Junfeng Niu, Jiebin Yu, Zhiping Wu, Huaqiang Qian, He |
author_sort | Lyu, Hongming |
collection | PubMed |
description | In order to conquer the short-channel effects that limit conventional ultra-scale semiconductor devices, two-dimensional materials, as an option of ultimate thin channels, receive wide attention. Graphene, in particular, bears great expectations because of its supreme carrier mobility and saturation velocity. However, its main disadvantage, the lack of bandgap, has not been satisfactorily solved. As a result, maximum oscillation frequency (f(max)) which indicates transistors’ power amplification ability has been disappointing. Here, we present submicron field-effect transistors with specially designed low-resistance gate and excellent source/drain contact, and therefore significantly improved f(max). The fabrication was assisted by the advanced 8-inch CMOS back-end-of-line technology. A 200-nm-gate-length GFET achieves f(T)/f(max) = 35.4/50 GHz. All GFET samples with gate lengths ranging from 200 nm to 400 nm possess f(max) 31–41% higher than f(T), closely resembling Si n-channel MOSFETs at comparable technology nodes. These results re-strengthen the promise of graphene field-effect transistors in next generation semiconductor electronics. |
format | Online Article Text |
id | pubmed-5075922 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2016 |
publisher | Nature Publishing Group |
record_format | MEDLINE/PubMed |
spelling | pubmed-50759222016-10-28 Deep-submicron Graphene Field-Effect Transistors with State-of-Art f(max) Lyu, Hongming Lu, Qi Liu, Jinbiao Wu, Xiaoming Zhang, Jinyu Li, Junfeng Niu, Jiebin Yu, Zhiping Wu, Huaqiang Qian, He Sci Rep Article In order to conquer the short-channel effects that limit conventional ultra-scale semiconductor devices, two-dimensional materials, as an option of ultimate thin channels, receive wide attention. Graphene, in particular, bears great expectations because of its supreme carrier mobility and saturation velocity. However, its main disadvantage, the lack of bandgap, has not been satisfactorily solved. As a result, maximum oscillation frequency (f(max)) which indicates transistors’ power amplification ability has been disappointing. Here, we present submicron field-effect transistors with specially designed low-resistance gate and excellent source/drain contact, and therefore significantly improved f(max). The fabrication was assisted by the advanced 8-inch CMOS back-end-of-line technology. A 200-nm-gate-length GFET achieves f(T)/f(max) = 35.4/50 GHz. All GFET samples with gate lengths ranging from 200 nm to 400 nm possess f(max) 31–41% higher than f(T), closely resembling Si n-channel MOSFETs at comparable technology nodes. These results re-strengthen the promise of graphene field-effect transistors in next generation semiconductor electronics. Nature Publishing Group 2016-10-24 /pmc/articles/PMC5075922/ /pubmed/27775009 http://dx.doi.org/10.1038/srep35717 Text en Copyright © 2016, The Author(s) http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ |
spellingShingle | Article Lyu, Hongming Lu, Qi Liu, Jinbiao Wu, Xiaoming Zhang, Jinyu Li, Junfeng Niu, Jiebin Yu, Zhiping Wu, Huaqiang Qian, He Deep-submicron Graphene Field-Effect Transistors with State-of-Art f(max) |
title | Deep-submicron Graphene Field-Effect Transistors with State-of-Art f(max) |
title_full | Deep-submicron Graphene Field-Effect Transistors with State-of-Art f(max) |
title_fullStr | Deep-submicron Graphene Field-Effect Transistors with State-of-Art f(max) |
title_full_unstemmed | Deep-submicron Graphene Field-Effect Transistors with State-of-Art f(max) |
title_short | Deep-submicron Graphene Field-Effect Transistors with State-of-Art f(max) |
title_sort | deep-submicron graphene field-effect transistors with state-of-art f(max) |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5075922/ https://www.ncbi.nlm.nih.gov/pubmed/27775009 http://dx.doi.org/10.1038/srep35717 |
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