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The Effect of C60 and Pentacene Adsorbates on the Electrical Properties of CVD Graphene on SiO(2)
Graphene is an excellent 2D material for vertical organic transistors electrodes due to its weak electrostatic screening and field-tunable work function, in addition to its high conductivity, flexibility and optical transparency. Nevertheless, the interaction between graphene and other carbon-based...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2023
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10052095/ https://www.ncbi.nlm.nih.gov/pubmed/36986028 http://dx.doi.org/10.3390/nano13061134 |
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author | Oswald, Jacopo Beretta, Davide Stiefel, Michael Furrer, Roman Vuillaume, Dominique Calame, Michel |
author_facet | Oswald, Jacopo Beretta, Davide Stiefel, Michael Furrer, Roman Vuillaume, Dominique Calame, Michel |
author_sort | Oswald, Jacopo |
collection | PubMed |
description | Graphene is an excellent 2D material for vertical organic transistors electrodes due to its weak electrostatic screening and field-tunable work function, in addition to its high conductivity, flexibility and optical transparency. Nevertheless, the interaction between graphene and other carbon-based materials, including small organic molecules, can affect the graphene electrical properties and therefore, the device performances. This work investigates the effects of thermally evaporated C60 (n-type) and Pentacene (p-type) thin films on the in-plane charge transport properties of large area CVD graphene under vacuum. This study was performed on a population of 300 graphene field effect transistors. The output characteristic of the transistors revealed that a C60 thin film adsorbate increased the graphene hole density by (1.65 ± 0.36) × 10(12) cm(−2), whereas a Pentacene thin film increased the graphene electron density by (0.55 ± 0.54) × 10(12) cm(−2). Hence, C60 induced a graphene Fermi energy downshift of about 100 meV, while Pentacene induced a Fermi energy upshift of about 120 meV. In both cases, the increase in charge carriers was accompanied by a reduced charge mobility, which resulted in a larger graphene sheet resistance of about 3 kΩ at the Dirac point. Interestingly, the contact resistance, which varied in the range 200 Ω–1 kΩ, was not significantly affected by the deposition of the organic molecules. |
format | Online Article Text |
id | pubmed-10052095 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-100520952023-03-30 The Effect of C60 and Pentacene Adsorbates on the Electrical Properties of CVD Graphene on SiO(2) Oswald, Jacopo Beretta, Davide Stiefel, Michael Furrer, Roman Vuillaume, Dominique Calame, Michel Nanomaterials (Basel) Article Graphene is an excellent 2D material for vertical organic transistors electrodes due to its weak electrostatic screening and field-tunable work function, in addition to its high conductivity, flexibility and optical transparency. Nevertheless, the interaction between graphene and other carbon-based materials, including small organic molecules, can affect the graphene electrical properties and therefore, the device performances. This work investigates the effects of thermally evaporated C60 (n-type) and Pentacene (p-type) thin films on the in-plane charge transport properties of large area CVD graphene under vacuum. This study was performed on a population of 300 graphene field effect transistors. The output characteristic of the transistors revealed that a C60 thin film adsorbate increased the graphene hole density by (1.65 ± 0.36) × 10(12) cm(−2), whereas a Pentacene thin film increased the graphene electron density by (0.55 ± 0.54) × 10(12) cm(−2). Hence, C60 induced a graphene Fermi energy downshift of about 100 meV, while Pentacene induced a Fermi energy upshift of about 120 meV. In both cases, the increase in charge carriers was accompanied by a reduced charge mobility, which resulted in a larger graphene sheet resistance of about 3 kΩ at the Dirac point. Interestingly, the contact resistance, which varied in the range 200 Ω–1 kΩ, was not significantly affected by the deposition of the organic molecules. MDPI 2023-03-22 /pmc/articles/PMC10052095/ /pubmed/36986028 http://dx.doi.org/10.3390/nano13061134 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 Oswald, Jacopo Beretta, Davide Stiefel, Michael Furrer, Roman Vuillaume, Dominique Calame, Michel The Effect of C60 and Pentacene Adsorbates on the Electrical Properties of CVD Graphene on SiO(2) |
title | The Effect of C60 and Pentacene Adsorbates on the Electrical Properties of CVD Graphene on SiO(2) |
title_full | The Effect of C60 and Pentacene Adsorbates on the Electrical Properties of CVD Graphene on SiO(2) |
title_fullStr | The Effect of C60 and Pentacene Adsorbates on the Electrical Properties of CVD Graphene on SiO(2) |
title_full_unstemmed | The Effect of C60 and Pentacene Adsorbates on the Electrical Properties of CVD Graphene on SiO(2) |
title_short | The Effect of C60 and Pentacene Adsorbates on the Electrical Properties of CVD Graphene on SiO(2) |
title_sort | effect of c60 and pentacene adsorbates on the electrical properties of cvd graphene on sio(2) |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10052095/ https://www.ncbi.nlm.nih.gov/pubmed/36986028 http://dx.doi.org/10.3390/nano13061134 |
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