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Control of Ni/β-Ga(2)O(3) Vertical Schottky Diode Output Parameters at Forward Bias by Insertion of a Graphene Layer
Controlling the Schottky barrier height ([Formula: see text]) and other parameters of Schottky barrier diodes (SBD) is critical for many applications. In this work, the effect of inserting a graphene interfacial monolayer between a Ni Schottky metal and a β- [Formula: see text] semiconductor was inv...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8912321/ https://www.ncbi.nlm.nih.gov/pubmed/35269314 http://dx.doi.org/10.3390/nano12050827 |
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author | Labed, Madani Sengouga, Nouredine Rim, You Seung |
author_facet | Labed, Madani Sengouga, Nouredine Rim, You Seung |
author_sort | Labed, Madani |
collection | PubMed |
description | Controlling the Schottky barrier height ([Formula: see text]) and other parameters of Schottky barrier diodes (SBD) is critical for many applications. In this work, the effect of inserting a graphene interfacial monolayer between a Ni Schottky metal and a β- [Formula: see text] semiconductor was investigated using numerical simulation. We confirmed that the simulation-based on Ni workfunction, interfacial trap concentration, and surface electron affinity was well-matched with the actual device characterization. Insertion of the graphene layer achieved a remarkable decrease in the barrier height ([Formula: see text]), from 1.32 to 0.43 eV, and in the series resistance ([Formula: see text]), from 60.3 to 2.90 [Formula: see text]. However, the saturation current ([Formula: see text]) increased from [Formula: see text] to [Formula: see text] (A/cm(2)). The effects of a graphene bandgap and workfunction were studied. With an increase in the graphene workfunction and bandgap, the Schottky barrier height and series resistance increased and the saturation current decreased. This behavior was related to the tunneling rate variations in the graphene layer. Therefore, control of Schottky barrier diode output parameters was achieved by monitoring the tunneling rate in the graphene layer (through the control of the bandgap) and by controlling the Schottky barrier height according to the Schottky–Mott role (through the control of the workfunction). Furthermore, a zero-bandgap and low-workfunction graphene layer behaves as an ohmic contact, which is in agreement with published results. |
format | Online Article Text |
id | pubmed-8912321 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-89123212022-03-11 Control of Ni/β-Ga(2)O(3) Vertical Schottky Diode Output Parameters at Forward Bias by Insertion of a Graphene Layer Labed, Madani Sengouga, Nouredine Rim, You Seung Nanomaterials (Basel) Article Controlling the Schottky barrier height ([Formula: see text]) and other parameters of Schottky barrier diodes (SBD) is critical for many applications. In this work, the effect of inserting a graphene interfacial monolayer between a Ni Schottky metal and a β- [Formula: see text] semiconductor was investigated using numerical simulation. We confirmed that the simulation-based on Ni workfunction, interfacial trap concentration, and surface electron affinity was well-matched with the actual device characterization. Insertion of the graphene layer achieved a remarkable decrease in the barrier height ([Formula: see text]), from 1.32 to 0.43 eV, and in the series resistance ([Formula: see text]), from 60.3 to 2.90 [Formula: see text]. However, the saturation current ([Formula: see text]) increased from [Formula: see text] to [Formula: see text] (A/cm(2)). The effects of a graphene bandgap and workfunction were studied. With an increase in the graphene workfunction and bandgap, the Schottky barrier height and series resistance increased and the saturation current decreased. This behavior was related to the tunneling rate variations in the graphene layer. Therefore, control of Schottky barrier diode output parameters was achieved by monitoring the tunneling rate in the graphene layer (through the control of the bandgap) and by controlling the Schottky barrier height according to the Schottky–Mott role (through the control of the workfunction). Furthermore, a zero-bandgap and low-workfunction graphene layer behaves as an ohmic contact, which is in agreement with published results. MDPI 2022-03-01 /pmc/articles/PMC8912321/ /pubmed/35269314 http://dx.doi.org/10.3390/nano12050827 Text en © 2022 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 Labed, Madani Sengouga, Nouredine Rim, You Seung Control of Ni/β-Ga(2)O(3) Vertical Schottky Diode Output Parameters at Forward Bias by Insertion of a Graphene Layer |
title | Control of Ni/β-Ga(2)O(3) Vertical Schottky Diode Output Parameters at Forward Bias by Insertion of a Graphene Layer |
title_full | Control of Ni/β-Ga(2)O(3) Vertical Schottky Diode Output Parameters at Forward Bias by Insertion of a Graphene Layer |
title_fullStr | Control of Ni/β-Ga(2)O(3) Vertical Schottky Diode Output Parameters at Forward Bias by Insertion of a Graphene Layer |
title_full_unstemmed | Control of Ni/β-Ga(2)O(3) Vertical Schottky Diode Output Parameters at Forward Bias by Insertion of a Graphene Layer |
title_short | Control of Ni/β-Ga(2)O(3) Vertical Schottky Diode Output Parameters at Forward Bias by Insertion of a Graphene Layer |
title_sort | control of ni/β-ga(2)o(3) vertical schottky diode output parameters at forward bias by insertion of a graphene layer |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8912321/ https://www.ncbi.nlm.nih.gov/pubmed/35269314 http://dx.doi.org/10.3390/nano12050827 |
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