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ALD-grown two-dimensional TiS(x) metal contacts for MoS(2) field-effect transistors

Metal contacts to MoS(2) field-effect transistors (FETs) play a determinant role in the device electrical characteristics and need to be chosen carefully. Because of the Schottky barrier (SB) and the Fermi level pinning (FLP) effects that occur at the contact/MoS(2) interface, MoS(2) FETs often suff...

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Detalles Bibliográficos
Autores principales: Mahlouji, Reyhaneh, Kessels, Wilhelmus M. M. (Erwin), Sagade, Abhay A., Bol, Ageeth A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: RSC 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10496909/
https://www.ncbi.nlm.nih.gov/pubmed/37705798
http://dx.doi.org/10.1039/d3na00387f
Descripción
Sumario:Metal contacts to MoS(2) field-effect transistors (FETs) play a determinant role in the device electrical characteristics and need to be chosen carefully. Because of the Schottky barrier (SB) and the Fermi level pinning (FLP) effects that occur at the contact/MoS(2) interface, MoS(2) FETs often suffer from high contact resistance (R(c)). One way to overcome this issue is to replace the conventional 3D bulk metal contacts with 2D counterparts. Herein, we investigate 2D metallic TiS(x) (x ∼ 1.8) as top contacts for MoS(2) FETs. We employ atomic layer deposition (ALD) for the synthesis of both the MoS(2) channels as well as the TiS(x) contacts and assess the electrical performance of the fabricated devices. Various thicknesses of TiS(x) are grown on MoS(2), and the resultant devices are electrically compared to the ones with the conventional Ti metal contacts. Our findings show that the replacement of 5 nm Ti bulk contacts with only ∼1.2 nm of 2D TiS(x) is beneficial in improving the overall device metrics. With such ultrathin TiS(x) contacts, the ON-state current (I(ON)) triples and increases to ∼35 μA μm(−1). R(c) also reduces by a factor of four and reaches ∼5 MΩ μm. Such performance enhancements were observed despite the SB formed at the TiS(x)/MoS(2) interface is believed to be higher than the SB formed at the Ti/MoS(2) interface. These device metric improvements could therefore be mainly associated with an increased level of electrostatic doping in MoS(2), as a result of using 2D TiS(x) for contacting the 2D MoS(2). Our findings are also well supported by TCAD device simulations.