micromachines
Review
2D Electronics Based on Graphene Field Effect Transistors:
Tutorial for Modelling and Simulation
Bassem Jmai
†
, Vitor Silva
†
and Paulo M. Mendes *
Citation: Jmai, B.; Silva, V.; Mendes,
P.M. 2D Electronics Based on
Graphene Field Effect Transistors:
Tutorial for Modelling and
Simulation. Micromachines 2021, 12,
979. https://doi.org/10.3390/
mi12080979
Academic Editor: Ha Duong Ngo
Received: 28 July 2021
Accepted: 16 August 2021
Published: 18 August 2021
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Attribution (CC BY) license (https://
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4.0/).
CMEMS-UMinho, University of Minho, 4800-058 Guimarães, Portugal; bassem.jmai@fst.utm.tn (B.J.);
vitor.silva@inl.int (V.S.)
* Correspondence: paulo.mendes@dei.uminho.pt
† These authors contributed equally to this work.
Abstract: This paper provides modeling and simulation insights into field-effect transistors based
on graphene (GFET), focusing on the devices’ architecture with regards to the position of the gate
(top-gated graphene transistors, back-gated graphene transistors, and top-/back-gated graphene
transistors), substrate (silicon, silicon carbide, and quartz/glass), and the graphene growth (CVD,
CVD on SiC, and mechanical exfoliation). These aspects are explored and discussed in order to
facilitate the selection of the appropriate topology for system-level design, based on the most
common topologies. Since most of the GFET models reported in the literature are complex and hard
to understand, a model of a GFET was implemented and made available in MATLAB, Verilog in
Cadence, and VHDL-AMS in Simplorer—useful tools for circuit designers with different backgrounds.
A tutorial is presented, enabling the researchers to easily implement the model to predict the
performance of their devices. In short, this paper aims to provide the initial knowledge and tools for
researchers willing to use GFETs in their designs at the system level, who are looking to implement
an initial setup that allows the inclusion of the performance of GFETs.
Keywords: graphene field-effect transistors (GFETs); MATLAB; Verilog; VHDL-AMS; modeling
1. Introduction
The development of CMOS (complementary metal-oxide semiconductor) transistors
is achieving its performance limit, due to the maximum downscaling according to Moore’s
law. Several new materials have appeared with the potential to overcome silicon devices’
performance; most of these rely on two-dimensional (2D) materials. Those families of
materials feature dangling-bond free surfaces exhibiting excellent electronic and optical
properties. Such materials range from graphene to other 2D materials, such as the transition
metal dichalcogenides (TMDCs). TMDCs have a finite bandgap, which is essential to
enable low-power digital electronics. The state of the art of the TMDC transistors and
silicon transistors is similar, as reported in [1], where MoS
2
was used as the channel of the
transistor, achieving an intrinsic maximum oscillation frequency (f
max
) of 50 GHz at low
temperatures. Despite the promising results at cryogenic temperatures, the FET mobility
at room temperature remains low for TMDCs. Because of that, graphene (a monolayer of
carbon atoms in a honeycomb lattice) is being widely pursued as an enabling material; it
has amazing properties at room temperature, such as high saturation velocity and high
carrier mobility, which make this material suitable for radiofrequency (RF) applications,
for example.
Since the discovery of graphene by Geim and Novoselov in 2004 [2], it continues to
attract the interest of the scientific community, both for the prospects it offers in fundamen-
tal research [3,4], and for applied physics [5,6]. Graphene is a 2D material, consisting of a
sheet of carbon atoms arranged in a honeycomb lattice, weakly bonded to a supporting
substrate [7]. The absence of a band gap in the band structure of graphene [8] is a serious
obstacle for the development of digital applications based on this material (in contrast with
Micromachines 2021, 12, 979. https://doi.org/10.3390/mi12080979 https://www.mdpi.com/journal/micromachines