Sub-THz Antenna for High-Speed Wireless Communication Systems
Hindawi
International Journal of Antennas and Propagation
Volume 2019, Article ID 9573647, 9 pages
https://doi.org/10.1155/2019/9573647
Research Article
Sub-THz Antenna for High-Speed Wireless
Communication Systems
Hamsakutty Vettikalladi ,1 Waleed Tariq Sethi,2 Ahmad Fauzi Bin Abas ,1 Wonsuk Ko,1
Majeed A. Alkanhal,1 and Mohamed Himdi 2
1
2
Department of Electrical Engineering, College of Engineering, King Saud University, 11421 Riyadh, Saudi Arabia
IETR University of Rennes 1, France
Correspondence should be addressed to Hamsakutty Vettikalladi;
Received 9 October 2018; Revised 27 December 2018; Accepted 1 January 2019; Published 27 March 2019
Academic Editor: Ikmo Park
Copyright © 2019 Hamsakutty Vettikalladi et al. This is an open access article distributed under the Creative Commons Attribution
License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is
properly cited.
Terahertz (THz) links will play a major role in high data rate communication over a distance of few meters. In order to achieve this
task, antenna designs with high gain and wideband characteristics will spearhead these links. In this contribution, we present
different antenna designs that offer characteristics better suited to THz communication over short distances. Firstly, a
single-element antenna having a dipole and reflector is designed to operate at 300 GHz, which is considered as a sub-terahertz
band. That antenna achieves a wide impedance bandwidth of 38.6% from 294 GHz to 410 GHz with a gain of 5.14 dBi. Secondly,
two designs based on the same dipole structure but with added directors are introduced to increase the gain while maintaining
almost the same bandwidth. The gains achieved are 8.01 dBi and 9.6 dBi, respectively. Finally, an array of 1 × 4 elements is used
to achieve the highest possible gain of 13.6 dBi with good efficiency about 89% and with limited director elements for a planar
compact structure to state-of-the-art literature. All the results achieved make the proposed designs viable candidates for
high-speed and short-distance wireless communication systems.
1. Introduction
Over the last few years, wireless data traffic has been drastically increasing due to a change in the way today’s society
creates, shares, and consumes information. This change has
been accompanied by an increasing demand for much
higher speed wireless communication anywhere at any
time. In particular, wireless data rates have doubled every
eighteen months over the last three decades and are quickly
approaching the capacity of wired communication systems.
Following this trend, wireless terabit-per-second (Tbps) links
are expected to become a reality within the next five to ten
years [1]. Advanced physical layer solutions and, more
importantly, new spectral bands will be required to support
these extremely high data rates [2].
Terahertz (THz) and sub-THz communication refers
to the use of the band that coves region from (0.1–10) THz
and sub-THz region is covered from (0.1–0.3) THz [1].
THz communication links will play a major role in which
very high data rates are required over short distances. Terahertz band can be used for high-speed data transmission
within a range of 10 m. This coverage area consists of small
cells of cellular networks. Terahertz communication is applicable in the indoor as well as outdoor environments with stationary and mobile users. Terabit wireless local area networks
(T-WLAN) can provide flawless communication between
high-speed fiber optical links and personal laptops and tablets. Wired and wireless links enjoy the same speed in terahertz communication [2]. Very high path loss is imposed as
one of the main challenges at THz band frequencies, which
poses a major constraint on communication distances. Additional challenges range from the implementation of compact
high-power THz band transceivers, the development of
efficient ultra-broadband antennas at THz Band frequencies, and characterization of the frequency-selective path
loss of the THz band channel to the development of novel
2
International Journal of Antennas and Propagation
d1
Ld
Gold
Wf
h3
Wff
W
Feed
Lf
Ls
Driven dipole
g
Reflector
d2
h2
BCB
InP
h1
Lr
d3
Ws
(a)
(b)
Figure 1: Geometric design of single-element dipole antenna: (a) perspective view and (b) front view.
Table 1: Optimized dimensions of single-element dipole antenna.
Dimensions
y
dBi
5.74
Value (μm)
d1
78
d2
116
d3
82
h1
50
h2
6
h3
2
g
4
Lf
35
Lr
280
Ld
115
Wf
10
modulations, transmission schemes, and communication
protocols tailored to the peculiarities of this paradigm.
Many of these challenges are common to mm-wave communication systems, and as a result, the THz band is not
yet regulated [3].
One of the major advantages of THz and sub-THz frequencies is the antenna size, which reduces to about submillimeter [4]. The implementation of these systems is
now possible due to the advancements in the realization
of the photonic and semiconductor devices with an operating frequency in the terahertz band. A common approach is
to design the antenna in a low loss substrate and then integrate it to the active devices. On-chip antennas are easily
integrated to the rest of the system but they have lower efficiencies due to the lossy substrate [5–7]. The substrate integration technology, one of the technologies used in THz,
converts nonplanar antenna structures into their planar
forms. Advanced microfabrication techniques are adopted
for the design of terahertz antennas. Some of the substrate-
Phi
x
z
Theta
y
z
y
z
Theta
x
3.94
2.87
1.79
0.717
−2.14
−8.57
−15
−21.4
−27.8
−34.3
dB
5.14
3.54
2.57
1.61
0.643
Phi −2.18
x −8.71
−15.2
−21.8
y
−28.3
x −34.9
z
Figure 2: Reflection coefficient (S11 ) and gain (dB) of singleelement dipole antenna.
integrated antenna structures used in THz technology are
slot array, dipole, reflector, horn, and leaky wave antennas
[8]. For the sub-THz designs, high gain with compact size
and wide bandwidth is preferred. Some antennas have been
presented in literature such as in [9] where authors presented three antenna designs (rectangular horn, Cassegrain,
International Journal of Antennas and Propagation
3
dBi
dBi
5.74
y
5.14
y
3.94
3.54
2.87
2.57
1.79
1.61
0.717
phi
-8.57
x
z
0.643
phi
-2.14
-15
Theta
x
z
-8.71
-15.2
Theta
-21.4
-21.8
-27.8
-28.3
-34.3
-34.9
(a) 3D directivity of single-element dipole
(b) 3D gain of single-element dipole
0
0
330
6
4
2
0
300
–2
–4
–6
–8
–10
–12 270
–12
–10
–8
–6
–4
240
–2
0
2
4
6
-2.18
30
60
90
120
150
210
180
6
4
2
0
300
–2
–4
–6
–8
–10
–12 270
–12
–10
–8
–6
–4
240
–2
0
2
4
6
330
30
60
90
120
150
210
180
CST_gain
HSFF_gain
CST_gain
HSFF_gain
°
(c) E-plane versus ϕ: Eϕ at θ=90
(d) H-plane versus θ: Eϕ at ϕ=0
°
Figure 3: Radiation pattern of the single-element dipole antenna at 300 GHz: (a) 3D directivity, (b) 3D gain, (c) E-plane, and (d) H-plane.
Ld1
d1´
d1´
(...truncated)