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Quasi-ballistic carbon nanotube array transistors with current density exceeding Si and GaAs

Carbon nanotubes (CNTs) are tantalizing candidates for semiconductor electronics because of their exceptional charge transport properties and one-dimensional electrostatics. Ballistic transport approaching the quantum conductance limit of 2G(0) = 4e(2)/h has been achieved in field-effect transistors...

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Autores principales: Brady, Gerald J., Way, Austin J., Safron, Nathaniel S., Evensen, Harold T., Gopalan, Padma, Arnold, Michael S.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Association for the Advancement of Science 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5010372/
https://www.ncbi.nlm.nih.gov/pubmed/27617293
http://dx.doi.org/10.1126/sciadv.1601240
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author Brady, Gerald J.
Way, Austin J.
Safron, Nathaniel S.
Evensen, Harold T.
Gopalan, Padma
Arnold, Michael S.
author_facet Brady, Gerald J.
Way, Austin J.
Safron, Nathaniel S.
Evensen, Harold T.
Gopalan, Padma
Arnold, Michael S.
author_sort Brady, Gerald J.
collection PubMed
description Carbon nanotubes (CNTs) are tantalizing candidates for semiconductor electronics because of their exceptional charge transport properties and one-dimensional electrostatics. Ballistic transport approaching the quantum conductance limit of 2G(0) = 4e(2)/h has been achieved in field-effect transistors (FETs) containing one CNT. However, constraints in CNT sorting, processing, alignment, and contacts give rise to nonidealities when CNTs are implemented in densely packed parallel arrays such as those needed for technology, resulting in a conductance per CNT far from 2G(0). The consequence has been that, whereas CNTs are ultimately expected to yield FETs that are more conductive than conventional semiconductors, CNTs, instead, have underperformed channel materials, such as Si, by sixfold or more. We report quasi-ballistic CNT array FETs at a density of 47 CNTs μm(−1), fabricated through a combination of CNT purification, solution-based assembly, and CNT treatment. The conductance is as high as 0.46 G(0) per CNT. In parallel, the conductance of the arrays reaches 1.7 mS μm(−1), which is seven times higher than the previous state-of-the-art CNT array FETs made by other methods. The saturated on-state current density is as high as 900 μA μm(−1) and is similar to or exceeds that of Si FETs when compared at and equivalent gate oxide thickness and at the same off-state current density. The on-state current density exceeds that of GaAs FETs as well. This breakthrough in CNT array performance is a critical advance toward the exploitation of CNTs in logic, high-speed communications, and other semiconductor electronics technologies.
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spelling pubmed-50103722016-09-09 Quasi-ballistic carbon nanotube array transistors with current density exceeding Si and GaAs Brady, Gerald J. Way, Austin J. Safron, Nathaniel S. Evensen, Harold T. Gopalan, Padma Arnold, Michael S. Sci Adv Research Articles Carbon nanotubes (CNTs) are tantalizing candidates for semiconductor electronics because of their exceptional charge transport properties and one-dimensional electrostatics. Ballistic transport approaching the quantum conductance limit of 2G(0) = 4e(2)/h has been achieved in field-effect transistors (FETs) containing one CNT. However, constraints in CNT sorting, processing, alignment, and contacts give rise to nonidealities when CNTs are implemented in densely packed parallel arrays such as those needed for technology, resulting in a conductance per CNT far from 2G(0). The consequence has been that, whereas CNTs are ultimately expected to yield FETs that are more conductive than conventional semiconductors, CNTs, instead, have underperformed channel materials, such as Si, by sixfold or more. We report quasi-ballistic CNT array FETs at a density of 47 CNTs μm(−1), fabricated through a combination of CNT purification, solution-based assembly, and CNT treatment. The conductance is as high as 0.46 G(0) per CNT. In parallel, the conductance of the arrays reaches 1.7 mS μm(−1), which is seven times higher than the previous state-of-the-art CNT array FETs made by other methods. The saturated on-state current density is as high as 900 μA μm(−1) and is similar to or exceeds that of Si FETs when compared at and equivalent gate oxide thickness and at the same off-state current density. The on-state current density exceeds that of GaAs FETs as well. This breakthrough in CNT array performance is a critical advance toward the exploitation of CNTs in logic, high-speed communications, and other semiconductor electronics technologies. American Association for the Advancement of Science 2016-09-02 /pmc/articles/PMC5010372/ /pubmed/27617293 http://dx.doi.org/10.1126/sciadv.1601240 Text en Copyright © 2016, The Authors http://creativecommons.org/licenses/by-nc/4.0/ This is an open-access article distributed under the terms of the Creative Commons Attribution-NonCommercial license (http://creativecommons.org/licenses/by-nc/4.0/) , which permits use, distribution, and reproduction in any medium, so long as the resultant use is not for commercial advantage and provided the original work is properly cited.
spellingShingle Research Articles
Brady, Gerald J.
Way, Austin J.
Safron, Nathaniel S.
Evensen, Harold T.
Gopalan, Padma
Arnold, Michael S.
Quasi-ballistic carbon nanotube array transistors with current density exceeding Si and GaAs
title Quasi-ballistic carbon nanotube array transistors with current density exceeding Si and GaAs
title_full Quasi-ballistic carbon nanotube array transistors with current density exceeding Si and GaAs
title_fullStr Quasi-ballistic carbon nanotube array transistors with current density exceeding Si and GaAs
title_full_unstemmed Quasi-ballistic carbon nanotube array transistors with current density exceeding Si and GaAs
title_short Quasi-ballistic carbon nanotube array transistors with current density exceeding Si and GaAs
title_sort quasi-ballistic carbon nanotube array transistors with current density exceeding si and gaas
topic Research Articles
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5010372/
https://www.ncbi.nlm.nih.gov/pubmed/27617293
http://dx.doi.org/10.1126/sciadv.1601240
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