Electrical Characterizationon Commercially Available Chemical Vapor Deposition (CVD) Graphene

Field-effect transistors (FET) based on graphene as channel has extraordinaryproperties in terms of charge mobility, charge carrier density etc. However, there aremany challenges to graphene based FET due to the fact graphene is a monolayer ofatoms in 2-dimentional space that is strongly influenced...

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Main Author: Anttila-Eriksson, Mikael
Format: Others
Language:English
Published: Uppsala universitet, Tillämpad materialvetenskap 2016
Subjects:
Online Access:http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-298357
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spelling ndltd-UPSALLA1-oai-DiVA.org-uu-2983572016-07-06T05:08:59ZElectrical Characterizationon Commercially Available Chemical Vapor Deposition (CVD) GrapheneengAnttila-Eriksson, MikaelUppsala universitet, Tillämpad materialvetenskap2016GFETGrapheneDirac point shiftCharge carrier mobilityField-effect transistors (FET) based on graphene as channel has extraordinaryproperties in terms of charge mobility, charge carrier density etc. However, there aremany challenges to graphene based FET due to the fact graphene is a monolayer ofatoms in 2-dimentional space that is strongly influenced by the operating conditions.One issue is that the Dirac point, or K-point, shifts to higher gate voltage whengraphene is exposed to atmosphere. In this study graphene field-effect transistors(GFET) based on commercially available CVD graphene are electrically characterizedthrough field effect gated measurements. The Dirac point is initially unobservable andlocated at higher gate voltages (>+42 V), indicating high p-doping in graphene.Different treatments are tried to enhance the properties of GFET devices, such astransconductance, mobility and a decrease of the Dirac point to lower voltages, thatincludes current annealing, vacuum annealing, hot plate annealing, ionized water bathand UV-ozone cleaning. Vacuum annealing and annealing on a hot plate affect thegated response; they might have decreased the overall p-doping, but also introducedDirac points and non-linear features. These are thought to be explained by localp-doping of the graphene under the electrodes. Thus the Dirac point of CVDgraphene is still at higher gate voltages. Finally, the charge carrier mobility decreasedin all treatments except current – and hot plate annealing, and it is also observed that charge carrier mobilities after fabrication are lower than the manufacturer estimatesfor raw graphene on SiO2/Si substrate. Student thesisinfo:eu-repo/semantics/bachelorThesistexthttp://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-298357UPTEC Q, 1401-5773 ; 16008application/pdfinfo:eu-repo/semantics/openAccess
collection NDLTD
language English
format Others
sources NDLTD
topic GFET
Graphene
Dirac point shift
Charge carrier mobility
spellingShingle GFET
Graphene
Dirac point shift
Charge carrier mobility
Anttila-Eriksson, Mikael
Electrical Characterizationon Commercially Available Chemical Vapor Deposition (CVD) Graphene
description Field-effect transistors (FET) based on graphene as channel has extraordinaryproperties in terms of charge mobility, charge carrier density etc. However, there aremany challenges to graphene based FET due to the fact graphene is a monolayer ofatoms in 2-dimentional space that is strongly influenced by the operating conditions.One issue is that the Dirac point, or K-point, shifts to higher gate voltage whengraphene is exposed to atmosphere. In this study graphene field-effect transistors(GFET) based on commercially available CVD graphene are electrically characterizedthrough field effect gated measurements. The Dirac point is initially unobservable andlocated at higher gate voltages (>+42 V), indicating high p-doping in graphene.Different treatments are tried to enhance the properties of GFET devices, such astransconductance, mobility and a decrease of the Dirac point to lower voltages, thatincludes current annealing, vacuum annealing, hot plate annealing, ionized water bathand UV-ozone cleaning. Vacuum annealing and annealing on a hot plate affect thegated response; they might have decreased the overall p-doping, but also introducedDirac points and non-linear features. These are thought to be explained by localp-doping of the graphene under the electrodes. Thus the Dirac point of CVDgraphene is still at higher gate voltages. Finally, the charge carrier mobility decreasedin all treatments except current – and hot plate annealing, and it is also observed that charge carrier mobilities after fabrication are lower than the manufacturer estimatesfor raw graphene on SiO2/Si substrate.
author Anttila-Eriksson, Mikael
author_facet Anttila-Eriksson, Mikael
author_sort Anttila-Eriksson, Mikael
title Electrical Characterizationon Commercially Available Chemical Vapor Deposition (CVD) Graphene
title_short Electrical Characterizationon Commercially Available Chemical Vapor Deposition (CVD) Graphene
title_full Electrical Characterizationon Commercially Available Chemical Vapor Deposition (CVD) Graphene
title_fullStr Electrical Characterizationon Commercially Available Chemical Vapor Deposition (CVD) Graphene
title_full_unstemmed Electrical Characterizationon Commercially Available Chemical Vapor Deposition (CVD) Graphene
title_sort electrical characterizationon commercially available chemical vapor deposition (cvd) graphene
publisher Uppsala universitet, Tillämpad materialvetenskap
publishDate 2016
url http://urn.kb.se/resolve?urn=urn:nbn:se:uu:diva-298357
work_keys_str_mv AT anttilaerikssonmikael electricalcharacterizationoncommerciallyavailablechemicalvapordepositioncvdgraphene
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