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Gate Tunable Transport in Graphene/MoS(2)/(Cr/Au) Vertical Field-Effect Transistors

Two-dimensional materials based vertical field-effect transistors have been widely studied due to their useful applications in industry. In the present study, we fabricate graphene/MoS(2)/(Cr/Au) vertical transistor based on the mechanical exfoliation and dry transfer method. Since the bottom electr...

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Autores principales: Nazir, Ghazanfar, Khan, Muhammad Farooq, Aftab, Sikandar, Afzal, Amir Muhammad, Dastgeer, Ghulam, Rehman, Malik Abdul, Seo, Yongho, Eom, Jonghwa
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5791101/
https://www.ncbi.nlm.nih.gov/pubmed/29283377
http://dx.doi.org/10.3390/nano8010014
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author Nazir, Ghazanfar
Khan, Muhammad Farooq
Aftab, Sikandar
Afzal, Amir Muhammad
Dastgeer, Ghulam
Rehman, Malik Abdul
Seo, Yongho
Eom, Jonghwa
author_facet Nazir, Ghazanfar
Khan, Muhammad Farooq
Aftab, Sikandar
Afzal, Amir Muhammad
Dastgeer, Ghulam
Rehman, Malik Abdul
Seo, Yongho
Eom, Jonghwa
author_sort Nazir, Ghazanfar
collection PubMed
description Two-dimensional materials based vertical field-effect transistors have been widely studied due to their useful applications in industry. In the present study, we fabricate graphene/MoS(2)/(Cr/Au) vertical transistor based on the mechanical exfoliation and dry transfer method. Since the bottom electrode was made of monolayer graphene (Gr), the electrical transport in our Gr/MoS(2)/(Cr/Au) vertical transistors can be significantly modified by using back-gate voltage. Schottky barrier height at the interface between Gr and MoS(2) can be modified by back-gate voltage and the current bias. Vertical resistance (R(vert)) of a Gr/MoS(2)/(Cr/Au) transistor is compared with planar resistance (R(planar)) of a conventional lateral MoS(2) field-effect transistor. We have also studied electrical properties for various thicknesses of MoS(2) channels in both vertical and lateral transistors. As the thickness of MoS(2) increases, R(vert) increases, but R(planar) decreases. The increase of R(vert) in the thicker MoS(2) film is attributed to the interlayer resistance in the vertical direction. However, R(planar) shows a lower value for a thicker MoS(2) film because of an excess of charge carriers available in upper layers connected directly to source/drain contacts that limits the conduction through layers closed to source/drain electrodes. Hence, interlayer resistance associated with these layers contributes to planer resistance in contrast to vertical devices in which all layers contribute interlayer resistance.
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spelling pubmed-57911012018-02-05 Gate Tunable Transport in Graphene/MoS(2)/(Cr/Au) Vertical Field-Effect Transistors Nazir, Ghazanfar Khan, Muhammad Farooq Aftab, Sikandar Afzal, Amir Muhammad Dastgeer, Ghulam Rehman, Malik Abdul Seo, Yongho Eom, Jonghwa Nanomaterials (Basel) Article Two-dimensional materials based vertical field-effect transistors have been widely studied due to their useful applications in industry. In the present study, we fabricate graphene/MoS(2)/(Cr/Au) vertical transistor based on the mechanical exfoliation and dry transfer method. Since the bottom electrode was made of monolayer graphene (Gr), the electrical transport in our Gr/MoS(2)/(Cr/Au) vertical transistors can be significantly modified by using back-gate voltage. Schottky barrier height at the interface between Gr and MoS(2) can be modified by back-gate voltage and the current bias. Vertical resistance (R(vert)) of a Gr/MoS(2)/(Cr/Au) transistor is compared with planar resistance (R(planar)) of a conventional lateral MoS(2) field-effect transistor. We have also studied electrical properties for various thicknesses of MoS(2) channels in both vertical and lateral transistors. As the thickness of MoS(2) increases, R(vert) increases, but R(planar) decreases. The increase of R(vert) in the thicker MoS(2) film is attributed to the interlayer resistance in the vertical direction. However, R(planar) shows a lower value for a thicker MoS(2) film because of an excess of charge carriers available in upper layers connected directly to source/drain contacts that limits the conduction through layers closed to source/drain electrodes. Hence, interlayer resistance associated with these layers contributes to planer resistance in contrast to vertical devices in which all layers contribute interlayer resistance. MDPI 2017-12-28 /pmc/articles/PMC5791101/ /pubmed/29283377 http://dx.doi.org/10.3390/nano8010014 Text en © 2017 by the authors. 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 (http://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Nazir, Ghazanfar
Khan, Muhammad Farooq
Aftab, Sikandar
Afzal, Amir Muhammad
Dastgeer, Ghulam
Rehman, Malik Abdul
Seo, Yongho
Eom, Jonghwa
Gate Tunable Transport in Graphene/MoS(2)/(Cr/Au) Vertical Field-Effect Transistors
title Gate Tunable Transport in Graphene/MoS(2)/(Cr/Au) Vertical Field-Effect Transistors
title_full Gate Tunable Transport in Graphene/MoS(2)/(Cr/Au) Vertical Field-Effect Transistors
title_fullStr Gate Tunable Transport in Graphene/MoS(2)/(Cr/Au) Vertical Field-Effect Transistors
title_full_unstemmed Gate Tunable Transport in Graphene/MoS(2)/(Cr/Au) Vertical Field-Effect Transistors
title_short Gate Tunable Transport in Graphene/MoS(2)/(Cr/Au) Vertical Field-Effect Transistors
title_sort gate tunable transport in graphene/mos(2)/(cr/au) vertical field-effect transistors
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5791101/
https://www.ncbi.nlm.nih.gov/pubmed/29283377
http://dx.doi.org/10.3390/nano8010014
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