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Damage evaluation in graphene underlying atomic layer deposition dielectrics

Based on micro-Raman spectroscopy (μRS) and X-ray photoelectron spectroscopy (XPS), we study the structural damage incurred in monolayer (1L) and few-layer (FL) graphene subjected to atomic-layer deposition of HfO(2) and Al(2)O(3) upon different oxygen plasma power levels. We evaluate the damage lev...

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Autores principales: Tang, Xiaohui, Reckinger, Nicolas, Poncelet, Olivier, Louette, Pierre, Ureña, Ferran, Idrissi, Hosni, Turner, Stuart, Cabosart, Damien, Colomer, Jean-François, Raskin, Jean-Pierre, Hackens, Benoit, Francis, Laurent A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4550929/
https://www.ncbi.nlm.nih.gov/pubmed/26311131
http://dx.doi.org/10.1038/srep13523
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author Tang, Xiaohui
Reckinger, Nicolas
Poncelet, Olivier
Louette, Pierre
Ureña, Ferran
Idrissi, Hosni
Turner, Stuart
Cabosart, Damien
Colomer, Jean-François
Raskin, Jean-Pierre
Hackens, Benoit
Francis, Laurent A.
author_facet Tang, Xiaohui
Reckinger, Nicolas
Poncelet, Olivier
Louette, Pierre
Ureña, Ferran
Idrissi, Hosni
Turner, Stuart
Cabosart, Damien
Colomer, Jean-François
Raskin, Jean-Pierre
Hackens, Benoit
Francis, Laurent A.
author_sort Tang, Xiaohui
collection PubMed
description Based on micro-Raman spectroscopy (μRS) and X-ray photoelectron spectroscopy (XPS), we study the structural damage incurred in monolayer (1L) and few-layer (FL) graphene subjected to atomic-layer deposition of HfO(2) and Al(2)O(3) upon different oxygen plasma power levels. We evaluate the damage level and the influence of the HfO(2) thickness on graphene. The results indicate that in the case of Al(2)O(3)/graphene, whether 1L or FL graphene is strongly damaged under our process conditions. For the case of HfO(2)/graphene, μRS analysis clearly shows that FL graphene is less disordered than 1L graphene. In addition, the damage levels in FL graphene decrease with the number of layers. Moreover, the FL graphene damage is inversely proportional to the thickness of HfO(2) film. Particularly, the bottom layer of twisted bilayer (t-2L) has the salient features of 1L graphene. Therefore, FL graphene allows for controlling/limiting the degree of defect during the PE-ALD HfO(2) of dielectrics and could be a good starting material for building field effect transistors, sensors, touch screens and solar cells. Besides, the formation of Hf-C bonds may favor growing high-quality and uniform-coverage dielectric. HfO(2) could be a suitable high-K gate dielectric with a scaling capability down to sub-5-nm for graphene-based transistors.
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spelling pubmed-45509292015-09-04 Damage evaluation in graphene underlying atomic layer deposition dielectrics Tang, Xiaohui Reckinger, Nicolas Poncelet, Olivier Louette, Pierre Ureña, Ferran Idrissi, Hosni Turner, Stuart Cabosart, Damien Colomer, Jean-François Raskin, Jean-Pierre Hackens, Benoit Francis, Laurent A. Sci Rep Article Based on micro-Raman spectroscopy (μRS) and X-ray photoelectron spectroscopy (XPS), we study the structural damage incurred in monolayer (1L) and few-layer (FL) graphene subjected to atomic-layer deposition of HfO(2) and Al(2)O(3) upon different oxygen plasma power levels. We evaluate the damage level and the influence of the HfO(2) thickness on graphene. The results indicate that in the case of Al(2)O(3)/graphene, whether 1L or FL graphene is strongly damaged under our process conditions. For the case of HfO(2)/graphene, μRS analysis clearly shows that FL graphene is less disordered than 1L graphene. In addition, the damage levels in FL graphene decrease with the number of layers. Moreover, the FL graphene damage is inversely proportional to the thickness of HfO(2) film. Particularly, the bottom layer of twisted bilayer (t-2L) has the salient features of 1L graphene. Therefore, FL graphene allows for controlling/limiting the degree of defect during the PE-ALD HfO(2) of dielectrics and could be a good starting material for building field effect transistors, sensors, touch screens and solar cells. Besides, the formation of Hf-C bonds may favor growing high-quality and uniform-coverage dielectric. HfO(2) could be a suitable high-K gate dielectric with a scaling capability down to sub-5-nm for graphene-based transistors. Nature Publishing Group 2015-08-27 /pmc/articles/PMC4550929/ /pubmed/26311131 http://dx.doi.org/10.1038/srep13523 Text en Copyright © 2015, Macmillan Publishers Limited 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
Tang, Xiaohui
Reckinger, Nicolas
Poncelet, Olivier
Louette, Pierre
Ureña, Ferran
Idrissi, Hosni
Turner, Stuart
Cabosart, Damien
Colomer, Jean-François
Raskin, Jean-Pierre
Hackens, Benoit
Francis, Laurent A.
Damage evaluation in graphene underlying atomic layer deposition dielectrics
title Damage evaluation in graphene underlying atomic layer deposition dielectrics
title_full Damage evaluation in graphene underlying atomic layer deposition dielectrics
title_fullStr Damage evaluation in graphene underlying atomic layer deposition dielectrics
title_full_unstemmed Damage evaluation in graphene underlying atomic layer deposition dielectrics
title_short Damage evaluation in graphene underlying atomic layer deposition dielectrics
title_sort damage evaluation in graphene underlying atomic layer deposition dielectrics
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4550929/
https://www.ncbi.nlm.nih.gov/pubmed/26311131
http://dx.doi.org/10.1038/srep13523
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