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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...

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Detalles Bibliográficos
Autores principales: Labed, Madani, Sengouga, Nouredine, Rim, You Seung
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
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
Descripción
Sumario: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.