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International Journal of Electrical and Computer Engineering (IJECE)
Vol. 8, No. 4, August 2018, pp. 2531~2539
ISSN: 2088-8708, DOI: 10.11591/ijece.v8i4.pp2531-2539  2531
Journal homepage: http://iaescore.com/journals/index.php/IJECE
Dielectric Resonator Reflectarray Antenna Unit Cells
for 5G Applications
Nur Fazreen Sallehuddin1
, Mohd Haizal Jamaluddin2
, Muhammad Ramlee Kamarudin3
,
Muhammad Hashim Dahri4
, Siti Umairah Tajol Anuar5
1,2,4,5
Wireless Communication Centre, Universiti Teknologi Malaysia, Johor, Malaysia
3
Centre for Electronic Warfare, Information and Cyber, Cranfield University, UK
Article Info ABSTRACT
Article history:
Received Jan 27, 2018
Revised May 30, 2018
Accepted Jun 8, 2018
This paper presents an investigation for the performance comparison of three
different unit cell configurations operating at 26 GHz for 5G applications.
The unit cells are cross shape dielectric resonator, cross microstrip patch and
cross hybrid dielectric resonator. Verification of the comparison has been
done by simulations using commercial Computer Simulation Technology
Microwave Studio (CST MWS). The simulated results for reflection phase,
slope variation, reflection loss and 10% bandwidth were analyzed and
compared. The results indicate that the optimum configuration to be
deployed for the reflectarray’s unit element in order to fulfill the 5G
requirements of a wide bandwidth is the cross hybrid DRA. This
configuration is a combination of cross DRA with cross microstrip patch as
the parasitic element in order to tune the phase and provide a wide phase
range with smooth variation slope. Cross hybrid DRA provided a wide phase
range of 520° with 0.77 dB loss and 10% bandwidth of 160 MHz.
Keyword:
Cross microstrip patch
DRA reflectarray
Phase range
Reflection loss
Unit cell
Copyright © 2018 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Nur Fazreen Sallehuddin,
Wireless Communication Centre,
Universiti Teknologi Malaysia,
81310 Johor Bahru, Johor, Malaysia.
Email: nfazreen7@live.utm.my
1. INTRODUCTION
Wireless communication systems have been growing rapidly evolving from first generation (1G) to
fifth generation (5G). It is widely agreed that compare to fourth generation (4G) network, the 5G network
should achieve 1000 times the system capacity, 10 times the spectral efficiency and energy efficiency [1].
The fourth generation (4G) wireless communication systems have been deployed in many countries, and now
4G technology is reaching maturity [2]. Therefore, the wireless system designers and the researchers have
started research on the 5G wireless system that will provide very high speeds and efficient use of available
bandwidth with frequency spectrum from 3GHz to 300GHz. Wide bandwidth is the most effective and
straightforward method to provide the foreseen data demands for 5G services expected to be commercially
available in 2020 and beyond [3]. In conjunction with 5G systems, the most important components that have
to be taken into account in order to use a reflectarray antenna for high data rate application is its bandwidth
and gain [2].
Reflectarray antennas combine some of the best features and positive characteristic of reflector and
phased arrays antenna [4], [5]. It consists of an array of elementary antenna excited by a feed as shown in
Figure 1. The feed is positioned at the focal distance of the array and normally measured in f/D ratio where f
is the distance between the feed and the reflectarray whereas D is the maximum length of the reflectarray
[6]-[8]. As no feeding network is required in reflectarray, losses can be reduced. This antenna is able to
reradiate and scatter the incident waves coming from the feed with electrical phases that are required to form
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 8, No. 4, August 2018 : 2531 – 2539
2532
a planar phase front in the far-field distance into the desired direction. One of the essential parts of the
reflectarray is to design the precise characterization of the unit elements by depends on the unit element’s
geometry to predict the phase-shift accurately. An important aspect of reflectarray analysis which are the
radiation patterns only can be evaluated once the unit element has been fully characterize and the full
reflectarray antenna is designed [9].
Figure 1. Reflectarray antenna working principle
In the early development of reflectarray antenna, researchers contributed to develop a unit element
for reflectarrays by using microstrip due to their advantages such as easy deployment in space, reducing cost
production, low profile, low weight, flatness and beam steering capability. However, the efficiency of the
microstrip at millimeter wave frequencies may drop significantly and the conductor loss becomes severe. As
a solution, dielectric resonator antenna (DRA) reflectarray with low loss and high phase range
was proposed [10], [11].
Dielectric resonator (DR) have been widely used as antenna element started in early nineteen-
eighties, in which the DR is made of high dielectric constant material that are known as high Q-factor
elements [12]. Besides as energy storage devices, dielectric resonators can be efficient radiators [13]. DRA
has been explored for designing various reflectarray antennas to achieve large reflection phase range, as well
as low reflection loss. One common approach to introduce phase shifts to the radiating elements is by varying
one of its geometrical parameters such as the length of the DRA. Such change will be converted into a
reflection phase variation. However, DRAs with different sizes makes the fabrication process complex.
Therefore, DRA reflectarray unit element can also be incorporated with various microstrip elements such as
slots, patches and strip for designing broadband reflectarray [14]. Moreover, multi-resonants elements on a
single dielectric layer have been suggested in these recent years to improve bandwidth and at the same time
keep the simple fabrication process. Among them are coplanar parallel dipoles, concentric squared, a
combination of square patch and square ring slots and cross shape rings [15]. As a result, it is possible to
produce reflection phase range that more than 360⁰ , while achieving smooth variation slope. Another
approach that has a possibility to improve the bandwidth by attaining high phase range for the reflectarray’s
element is dual-polarized technique [16]. The selection of the polarization can be achieved by using
rectangular shapes for linear polarization and square shapes, circular shapes or crossed shapes for dual or
circular polarization [12], [17].
Motivated by the above previous researches on the unit cells, the purpose of this paper is to
investigate the performance of several different unit cell configurations in terms of the reflection
characteristics and phase range that will be the basic building block of the reflectarray in 5G applications at
operating frequency of 26 GHz. The specifications and criteria are focus on achieving wide phase range
which highly related to the large bandwidth of operation and low reflection loss. The goal is to determine the
best candidate to be deployed for the reflectarray’s unit element for the DRA-based reflectarray for 5G
applications in term of wide bandwidth, low reflection loss and easy fabrication.
2. RESEARCH METHOD
The unit cells of the reflectarray proposed in this paper for the investigation consist of DRA with
dielectric constant, ɛr = 10. For the cross shape DRA (CDRA) incorporate of two same sizes of rectangular
Int J Elec & Comp Eng ISSN: 2088-8708 
Dielectric Resonator Reflectarray Antenna Unit Cells for 5G Applications (Nur Fazreen Sallehuddin)
2533
DRA (RDRA) and the cross microstrip patch incorporate of two same sizes of the rectangular patch. The
resonant frequencies, f0 for the RDRA can be predicted by using equation derived from the Dielectric
Waveguide Model [12].
( ) √( )
Where kz is the wave propagation number in the z-direction, h is the width in the z-direction and k0
is the free space wave number. All types of the unit cell have been designed and simulated by using the
commercially Computer Simulation Technology Microwave Studio (CST MWS) software to analyze the
results and obtain the optimum parameter value. The dielectric substrate that used in these designs is Duroid
5880 with a thickness 0.381 mm, a permittivity of 2.2 with a loss tangent of 0.0009. Several different
frequency bands for communication 5G have been suggested by their ability to achieve the required
properties and features [18]. In this work, the resonant frequency of 26 GHz has been selected from the
frequency band of 24.25 GHz to 27.5 GHz for design considerations. The unit cell elements are simulated
using waveguide setup with periodic boundary condition with the E-wall (top and bottom surfaces) and H-
wall (left and right sides) to support an incident plane as depicting in Figure 2 for infinite array approach. The
incident wave is position at the top surface of the waveguide and the unit element is placed at the bottom
surface of the waveguide. In the next subsection, the designs of several different unit cells are presented.
Figure 2. Waveguide simulation setup for the unit cell
2.1. Rectangular DRA
Figure 3 shows the design configuration of the rectangular DRA. The design parameters after
simulation and optimization are shown in Table 1. The width of DRA, W is fixed at 2.4 mm while the length
of DRA, L is varying from 4.5 mm to 8.0 mm.
(a) 3D view (b) Top view
Figure 3. Rectangular DRA unit cell
Table 1. Rectangular DRA Unit Cell Design Parameters
Parameter Value (mm)
L Varies from 4.5 to 8.0
W 2.4
H 2.2
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 8, No. 4, August 2018 : 2531 – 2539
2534
2.2. Cross shape DRA
The design configuration of the cross shape DRA that have been combined from the two rectangular
DRA dimension is shown in Figure 4. Table 2 shows the optimized design parameters of the cross DRA. The
width of DRA, W is fixed at 2.4 mm while the length of DRA, L is varying from 4.5 mm to 8.0 mm
(to compare with rectangular DRA) and varying from 1.5 mm to 8.0 mm for the next section (to compare
with other cross shape unit cells).
(a) 3D view (b) Top view
Figure 4. Cross shape DRA unit cell
Table 2. Cross DRA Unit Cell Design Parameters
Parameter Value (mm)
L Varies from 1.5 to 8.0
W 2.4
H 2.2
2.3. Cross microstrip patch
The dimension of the microstrip patch with operating frequency of 26 GHz was determined by a
series of a mathematical equation. Then the two same sizes of the rectangular microstrip patch are designed
in cross shape. This unit cell design using cross microstrip patch as the phase variation technique. The
configuration of the unit cell is shown in Figure 5 and Table 3 shows the optimum parameters obtained. The
width of microstrip, WP is fixed at 1.5 mm while the length of microstrip, LP is varying from 1.5 mm
to 8.0 mm.
(a) 3D view (b) Top view
Figure 5. Cross microstrip unit cell
Table 3. Cross Microstrip Cell Design Parameters
Parameter Value (mm)
LP Varies from 1.5 to 8.0
WP 1.5
Int J Elec & Comp Eng ISSN: 2088-8708 
Dielectric Resonator Reflectarray Antenna Unit Cells for 5G Applications (Nur Fazreen Sallehuddin)
2535
2.4. Cross hybrid DRA
The configuration of the cross hybrid DRA is shown in Figure 6. Table 4 shows the unit cell design
parameters after simulation and optimization. This unit cell consists of a cross shape DRA combined with
cross shape microstrip patch below the cross DRA whereas the cross microstrip patch as the parasitic element
to tune the phase of the unit cell. Designing DRA with different size is always difficult to be implemented
[10]. Therefore, a design with fixed cross DRA size with the cross microstrip patch as the parasitic element to
tune the phase response by varying its length is designed. The width of DRA, W is fixed at 2.4 mm while the
length of DRA, L is fixed at 8.0 mm. On top of that, the width of microstrip, WP is fixed at 1.5 mm while the
length of microstrip, LP is varying from 1.5 mm to 8.0 mm.
(a) 3D view (b) Top view
Figure 6. Cross hybrid DRA unit cell
Table 4. Cross Hybrid DRA Unit Cell Design Parameters
Parameter Value (mm)
L 8.0
W 2.4
H 2.2
LP Varies from 1.5 to 8.0
WP 1.5
3. RESULTS AND ANALYSIS
The selected designs have been analyzed numerically by using CST MWS simulation tools. In this
section, the results for several types of the unit cell for the reflectarray’s unit cell are discussed in terms of
reflection phase range, reflection loss and 10% bandwidth.
3.1. Comparison of the simulated results between rectangular DRA and cross shape DRA
The two main parameters to show the performance of the reflectarray’s unit cells are the reflection
phase and the reflection loss. An important parameter that is availed to analyze the reflectivity and bandwidth
of reflectarray is reflection phase [19]. Figure 7 shows the reflection phase of S11 for rectangular DRA
(RDRA) and cross DRA. The graphs clearly indicate that cross DRA provides wider phase range than
rectangular DRA. This is because the cross DRA unit cell with two resonants element provide a dual-
polarization technique that could effectively attain higher phase range than rectangular DRA. The phase
range and slope variation of both types unit cells are summarized in Table 5. Based on the result, the slope
variation of both unit cells are smooth which indicate that DRA-based unit cells can provide wide bandwidth.
Therefore, the cross DRA is selected to combine with microstrip for further study on hybrid unit cell.
Table 5. Phase Range and Slope Variation for different Configuration of DRA Unit Cells at 26 GHz
Type of Unit Cell
Phase range
(degrees)
Slope
Rectangular DRA 332° Slow
Cross DRA 497° Slow
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 8, No. 4, August 2018 : 2531 – 2539
2536
Figure 7. Phase of S11 for rectangular DRA and cross DRA unit cells
3.2. Comparison of the simulated results for three different cross-shape unit cell configurations for
bandwidth enhancement
The reflection phase of S11 for three different cross shape configurations obtained by varying the
length of the tunable parameter is presented in Figure 8. Based on the results, it can be seen that the cross
DRA unit cell exhibit highest reflected phase range which is 684°, followed by cross hybrid DRA phase
range equal to 520° and cross microstrip patch phase range is 298°. Limited reflection phase range that less
than 360 degrees causes phase errors and consequently reduces its directivity that will deteriorate the antenna
performance [9].
Figure 8. Phase of S11 for different unit cells Figure 9. Reflection loss curves for
different unit cells
For cross microstrip patch case, the gradient slope of the phase variation versus variable length is
steeper than the other two unit cells. This is expected to result in a reduced bandwidth [20]. Table 6 shows
the phase range and gradient slope for the structures that have been analyzed as the possible candidate for the
design of DRA-based reflectarray. In terms of gradient variation, the slope of cross DRA and cross hybrid
DRA unit cell is smoother than the slope of cross microstrip patch. The more gradual gradient variation of
the reflection phase curve corresponds to the wider bandwidth of the unit element [20], [21]. The phase range
of the cross DRA is wider than cross hybrid DRA, but in term of fabrication matter, the cross hybrid DRA
with fixed DRA is a better option than cross DRA to decrease the fabrication complexity during an array
arrangement.
Reflection loss or also known as insertion loss in reflectarray is another vital parameter in the
analysis of reflectarray. Normally a reflectarray antenna always exhibits some losses. Therefore, the
reflection coefficient or reflection loss is measured less than 1 dB for a reflectarray and the lower loss is the
better. Figure 9 illustrates the reflection loss for the three different unit cell configurations. It is demonstrated
in Figure 9 that cross DRA is observed to provide the lowest insertion loss value of 0.04 dB whereas the
cross hybrid DRA gives 0.77 dB insertion loss. Whilst the cross microstrip unit cell with 1.05 dB gives the
Int J Elec & Comp Eng ISSN: 2088-8708 
Dielectric Resonator Reflectarray Antenna Unit Cells for 5G Applications (Nur Fazreen Sallehuddin)
2537
highest insertion loss value. This is due to the dielectric resonator element gives low loss as compared to
microstrip element that gives higher conductor loss which produced by the microstrip patch.
The bandwidth of the unit cell of the reflectarray can be calculated by the reflection loss curves. The
bandwidth is determined by moving 10% above the maximum reflection loss value [22]. The 10% bandwidth
of the three unit cell configurations are shown in Table 7. From Table 7, it shows that the cross hybrid DRA
unit cell offers the wider bandwidth of 160 MHz whereas the cross microstrip unit cell gives a minimum
bandwidth of 136 MHz. The results indicate that the cross DRA unit cell gives the lowest reflection loss with
broader bandwidth due to the absence of conductor’s losses and surface wave losses.
Table 6. Phase Range and Slope Variation for different Configuration of Unit Cells at 26 GHz
Type of Unit Cell
Phase range
(degrees)
Slope
Cross Microstrip 298° Fast
Cross DRA 684° Slow
Cross hybrid DRA 520° Slow
Table 7. Reflection Loss and 10% Bandwidth for different Unit Cells at 26 GHz
Type of Unit Cell
Reflection Loss
(dB)
10 % Bandwidth
(MHz)
Cross Microstrip 1.05 136
Cross DRA 0.04 1617
Cross hybrid DRA 0.77 160
4. CONCLUSION
The design configurations with three potential cross shape unit cell designs for the reflectarray unit
cell at 26 GHz were investigated for the performance optimization of the reflectarray. The CST MWS
simulation showed that the best candidate to be deployed for the reflectarray’s unit element in order to fulfill
the 5G requirements of a wide bandwidth is the cross hybrid DRA which is the combined fixed cross DRA
with cross microstrip patch as the parasitic element. The parasitic element used to tune the phase to give a
wide phase range with smooth variation slope. Besides, it is shown that the cross hybrid DRA unit cell gives
low reflection loss with better bandwidth performance. Easy implementation and fabrication also emphasized
in a selection of the unit element. The simulation results for the unit cells will be validated experimentally in
next stage. The design for full reflectarray to predict the overall DRA reflectarray antenna performance and
further investigation into how a higher gain can be achieved are being conducted by the authors.
ACKNOWLEDGEMENTS
The authors would like to thank the Ministry of Education (MOE) for sponsoring the PhD study at
Universiti Teknologi Malaysia. Also, special thanks go to UTM GUP (votes 4J220, 05H62, 13H26, 03G59
and 4F733) and Ministry of Science Technology and Innovation (MOSTI) (vote 4S134) for sponsoring this
work.
REFERENCES
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[5] M. F. M. Yusoff, R. Sauleau, Z. Johari, M. K. A. Rahim, and H. A. Majid, “A Novel Right Handed Circular
Polarization Folded Reflectarray Antenna at 60 GHz,” Int. J. Electr. Comput. Eng., vol. 7, no. 3, p. 1580, 2017.
[6] M. M. Tahseen and A. A. Kishk, “Broadband Performance of Novel Closely Spaced Elements in Designing Ka-
Band Circularly Polarized Reflectarray Antennas,” vol. 1225, no. c, pp. 1-4, 2016.
[7] M. H. Dahri, M. R. Kamarudin, M. H. Jamaluddin, M. Inam, and R. Selvaraju, “Broadband Resonant Elements for
5G Reflectarray Antenna Design,” vol. 15, no. 2, pp. 793-798, 2017.
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[8] M. H. Dahri, M. R. Kamarudin, M. H. Jamaluddin, and R. R. Selvaraju, “Performance Investigation of Reflectarray
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[9] J. Huang and J. A. Encinar, Reflectarray Antenna. John Wiley and Sons, Inc, Publication, 2007.
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BIOGRAPHIES OF AUTHORS
Nur Fazreen Sallehuddin received her Bachelor degree in Electrical Engineering (Hons.) (2006)
and Master degree in Technic and Vocational Education (2014) from Universiti Tun Hussein Onn
Malaysia (UTHM). Experienced as Integration Assistant Engineer and Quality Assurance Engineer
for solar industry and automotive industry respectively from 2007-2011. Currently she is pursuing
the Ph.D. degree in Electrical Engineering at Wireless Communication Centre, University
Technology of Malaysia (UTM). Her research interests and areas include dielectric resonators and
reflectarray antennas design in 5G applications and millimeter waves.
Mohd Haizal Jamaluddin received the bachelor's and master's degrees in electrical engineering
from Universiti Teknologi Malaysia, Malaysia, in 2003 and 2006, respectively, and the Ph.D. degree
in signal processing and telecommunications from the Université de Rennes 1, France, in 2009, with
a focus on microwavecommunication systems and specific antennas such as dielectric resonator and
reflect array and dielectric dome antennas. He joined the Department of Electronic Engineering,
Faculty of Electrical Engineering, Universiti Teknologi Malaysia, as a Tutor in 2003. He is currently
an Associate Professor with the Wireless Communication Centre, Universiti Teknologi Malaysia
(UTM). He was a Senior Lecturer at Wireless Communication Centre (WCC), Universiti Teknologi
Malaysia (UTM) until December 2017. He has published more than 40 ISI/Scopus papers in reputed
indexed journals and more than 40 conference proceedings.
Muhammad Ramlee Kamarudin (Senior Member IEEE 13', Member IEEE 08', Member IET 11')
obtained his first degree from Universiti Teknologi Malaysia (UTM), Johor Bahru, Malaysia, with
honours, majoring in electrical and telecommunication engineering and graduated in 2003. He
received the M.S. degree in communication engineering in 2004 from the University of Birmingham,
Birmingham, UK, and later he obtained his Ph.D. degree in 2007 from the same University under the
supervision of Professor Peter Hall. Dr Kamarudin is currently working as a Senior Lecturer at the
Centre for Electronic Warfare, Information and Cyber (EWIC), Cranfield Defence and Security,
Cranfield University, UK. Prior to this appointment, he was an Associate Professor at Wireless
Communication Centre (WCC), Universiti Teknologi Malaysia (UTM), Malaysia until May 2017.
He holds a H-Index of 19 (SCOPUS) and more than 1350 citations (SCOPUS). He is an author of a
book chapter of a book entitled Antennas and Propagation for Body-Centric Wireless
Communications and has published more than 200 technical papers in journals and proceedings
Int J Elec & Comp Eng ISSN: 2088-8708 
Dielectric Resonator Reflectarray Antenna Unit Cells for 5G Applications (Nur Fazreen Sallehuddin)
2539
including IEEE Transaction on Antenna and Propagation (TAP), IEEE Antennas and Wireless
Propagation Letter (AWPL), IEEE Antenna Magazine, IEEE Access, International Journal of
Antennas and Propagation (IJAP), Progress in Electromagnetics Research (PIER), Microwave and
Optical Technology Letters (MOTL), and Electronics Letters. His research interests include antenna
design for 5G, wireless on-body communications, in-body communications (implantable antenna),
RF and microwave communication systems, and antenna diversity. Dr Kamarudin is an IEEE Senior
Member (SMIEEE), a Member of IET (MIET), an Executive Member of Antenna and Propagation
(AP/MTT/EMC), Malaysia Chapter, and a Member of IEEE Antennas and Propagation Society,
IEEE Communication Society, IEEE Microwave Theory and Techniques Society and IEEE
Electromagnetic Compatibility Society.
Muhammad Hashim Dahri received the B.E degree in Telecommunications from the Mehran
University of Engineering and Technology (MUET), Pakistan, in 2010 and the Masters by Research
degree in Electrical Engineering from Universiti Tun Hussein Onn Malaysia (UTHM) in 2014. He is
currently pursuing the Ph.D. degree with the Wireless Communication Centre (WCC), Universiti
Teknologi Malaysia (UTM). He has authored over 20 research papers in various indexed journals
and conference proceedings. His research interests include reflectarray antennas, planar printed
antennas and tunable materials for antenna design.
Siti Umairah Tajol Anuar received her Bachelor degree in Electronic Telecomunication
Engineering (2015) in Universiti Malaysia Sarawak (UNIMAS) and Master in Electronic
Telecommunication (2017) from Universiti Teknologi Malaysia (UTM). She is currently pursuing
her Ph.D. at the Universiti Teknologi Malaysia (UTM). Her research interests and areas include
dielectric resonators antennas and wireless communication.

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Dielectric Resonator Reflectarray Unit Cells for 5G

  • 1. International Journal of Electrical and Computer Engineering (IJECE) Vol. 8, No. 4, August 2018, pp. 2531~2539 ISSN: 2088-8708, DOI: 10.11591/ijece.v8i4.pp2531-2539  2531 Journal homepage: http://iaescore.com/journals/index.php/IJECE Dielectric Resonator Reflectarray Antenna Unit Cells for 5G Applications Nur Fazreen Sallehuddin1 , Mohd Haizal Jamaluddin2 , Muhammad Ramlee Kamarudin3 , Muhammad Hashim Dahri4 , Siti Umairah Tajol Anuar5 1,2,4,5 Wireless Communication Centre, Universiti Teknologi Malaysia, Johor, Malaysia 3 Centre for Electronic Warfare, Information and Cyber, Cranfield University, UK Article Info ABSTRACT Article history: Received Jan 27, 2018 Revised May 30, 2018 Accepted Jun 8, 2018 This paper presents an investigation for the performance comparison of three different unit cell configurations operating at 26 GHz for 5G applications. The unit cells are cross shape dielectric resonator, cross microstrip patch and cross hybrid dielectric resonator. Verification of the comparison has been done by simulations using commercial Computer Simulation Technology Microwave Studio (CST MWS). The simulated results for reflection phase, slope variation, reflection loss and 10% bandwidth were analyzed and compared. The results indicate that the optimum configuration to be deployed for the reflectarray’s unit element in order to fulfill the 5G requirements of a wide bandwidth is the cross hybrid DRA. This configuration is a combination of cross DRA with cross microstrip patch as the parasitic element in order to tune the phase and provide a wide phase range with smooth variation slope. Cross hybrid DRA provided a wide phase range of 520° with 0.77 dB loss and 10% bandwidth of 160 MHz. Keyword: Cross microstrip patch DRA reflectarray Phase range Reflection loss Unit cell Copyright © 2018 Institute of Advanced Engineering and Science. All rights reserved. Corresponding Author: Nur Fazreen Sallehuddin, Wireless Communication Centre, Universiti Teknologi Malaysia, 81310 Johor Bahru, Johor, Malaysia. Email: nfazreen7@live.utm.my 1. INTRODUCTION Wireless communication systems have been growing rapidly evolving from first generation (1G) to fifth generation (5G). It is widely agreed that compare to fourth generation (4G) network, the 5G network should achieve 1000 times the system capacity, 10 times the spectral efficiency and energy efficiency [1]. The fourth generation (4G) wireless communication systems have been deployed in many countries, and now 4G technology is reaching maturity [2]. Therefore, the wireless system designers and the researchers have started research on the 5G wireless system that will provide very high speeds and efficient use of available bandwidth with frequency spectrum from 3GHz to 300GHz. Wide bandwidth is the most effective and straightforward method to provide the foreseen data demands for 5G services expected to be commercially available in 2020 and beyond [3]. In conjunction with 5G systems, the most important components that have to be taken into account in order to use a reflectarray antenna for high data rate application is its bandwidth and gain [2]. Reflectarray antennas combine some of the best features and positive characteristic of reflector and phased arrays antenna [4], [5]. It consists of an array of elementary antenna excited by a feed as shown in Figure 1. The feed is positioned at the focal distance of the array and normally measured in f/D ratio where f is the distance between the feed and the reflectarray whereas D is the maximum length of the reflectarray [6]-[8]. As no feeding network is required in reflectarray, losses can be reduced. This antenna is able to reradiate and scatter the incident waves coming from the feed with electrical phases that are required to form
  • 2.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 8, No. 4, August 2018 : 2531 – 2539 2532 a planar phase front in the far-field distance into the desired direction. One of the essential parts of the reflectarray is to design the precise characterization of the unit elements by depends on the unit element’s geometry to predict the phase-shift accurately. An important aspect of reflectarray analysis which are the radiation patterns only can be evaluated once the unit element has been fully characterize and the full reflectarray antenna is designed [9]. Figure 1. Reflectarray antenna working principle In the early development of reflectarray antenna, researchers contributed to develop a unit element for reflectarrays by using microstrip due to their advantages such as easy deployment in space, reducing cost production, low profile, low weight, flatness and beam steering capability. However, the efficiency of the microstrip at millimeter wave frequencies may drop significantly and the conductor loss becomes severe. As a solution, dielectric resonator antenna (DRA) reflectarray with low loss and high phase range was proposed [10], [11]. Dielectric resonator (DR) have been widely used as antenna element started in early nineteen- eighties, in which the DR is made of high dielectric constant material that are known as high Q-factor elements [12]. Besides as energy storage devices, dielectric resonators can be efficient radiators [13]. DRA has been explored for designing various reflectarray antennas to achieve large reflection phase range, as well as low reflection loss. One common approach to introduce phase shifts to the radiating elements is by varying one of its geometrical parameters such as the length of the DRA. Such change will be converted into a reflection phase variation. However, DRAs with different sizes makes the fabrication process complex. Therefore, DRA reflectarray unit element can also be incorporated with various microstrip elements such as slots, patches and strip for designing broadband reflectarray [14]. Moreover, multi-resonants elements on a single dielectric layer have been suggested in these recent years to improve bandwidth and at the same time keep the simple fabrication process. Among them are coplanar parallel dipoles, concentric squared, a combination of square patch and square ring slots and cross shape rings [15]. As a result, it is possible to produce reflection phase range that more than 360⁰ , while achieving smooth variation slope. Another approach that has a possibility to improve the bandwidth by attaining high phase range for the reflectarray’s element is dual-polarized technique [16]. The selection of the polarization can be achieved by using rectangular shapes for linear polarization and square shapes, circular shapes or crossed shapes for dual or circular polarization [12], [17]. Motivated by the above previous researches on the unit cells, the purpose of this paper is to investigate the performance of several different unit cell configurations in terms of the reflection characteristics and phase range that will be the basic building block of the reflectarray in 5G applications at operating frequency of 26 GHz. The specifications and criteria are focus on achieving wide phase range which highly related to the large bandwidth of operation and low reflection loss. The goal is to determine the best candidate to be deployed for the reflectarray’s unit element for the DRA-based reflectarray for 5G applications in term of wide bandwidth, low reflection loss and easy fabrication. 2. RESEARCH METHOD The unit cells of the reflectarray proposed in this paper for the investigation consist of DRA with dielectric constant, ɛr = 10. For the cross shape DRA (CDRA) incorporate of two same sizes of rectangular
  • 3. Int J Elec & Comp Eng ISSN: 2088-8708  Dielectric Resonator Reflectarray Antenna Unit Cells for 5G Applications (Nur Fazreen Sallehuddin) 2533 DRA (RDRA) and the cross microstrip patch incorporate of two same sizes of the rectangular patch. The resonant frequencies, f0 for the RDRA can be predicted by using equation derived from the Dielectric Waveguide Model [12]. ( ) √( ) Where kz is the wave propagation number in the z-direction, h is the width in the z-direction and k0 is the free space wave number. All types of the unit cell have been designed and simulated by using the commercially Computer Simulation Technology Microwave Studio (CST MWS) software to analyze the results and obtain the optimum parameter value. The dielectric substrate that used in these designs is Duroid 5880 with a thickness 0.381 mm, a permittivity of 2.2 with a loss tangent of 0.0009. Several different frequency bands for communication 5G have been suggested by their ability to achieve the required properties and features [18]. In this work, the resonant frequency of 26 GHz has been selected from the frequency band of 24.25 GHz to 27.5 GHz for design considerations. The unit cell elements are simulated using waveguide setup with periodic boundary condition with the E-wall (top and bottom surfaces) and H- wall (left and right sides) to support an incident plane as depicting in Figure 2 for infinite array approach. The incident wave is position at the top surface of the waveguide and the unit element is placed at the bottom surface of the waveguide. In the next subsection, the designs of several different unit cells are presented. Figure 2. Waveguide simulation setup for the unit cell 2.1. Rectangular DRA Figure 3 shows the design configuration of the rectangular DRA. The design parameters after simulation and optimization are shown in Table 1. The width of DRA, W is fixed at 2.4 mm while the length of DRA, L is varying from 4.5 mm to 8.0 mm. (a) 3D view (b) Top view Figure 3. Rectangular DRA unit cell Table 1. Rectangular DRA Unit Cell Design Parameters Parameter Value (mm) L Varies from 4.5 to 8.0 W 2.4 H 2.2
  • 4.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 8, No. 4, August 2018 : 2531 – 2539 2534 2.2. Cross shape DRA The design configuration of the cross shape DRA that have been combined from the two rectangular DRA dimension is shown in Figure 4. Table 2 shows the optimized design parameters of the cross DRA. The width of DRA, W is fixed at 2.4 mm while the length of DRA, L is varying from 4.5 mm to 8.0 mm (to compare with rectangular DRA) and varying from 1.5 mm to 8.0 mm for the next section (to compare with other cross shape unit cells). (a) 3D view (b) Top view Figure 4. Cross shape DRA unit cell Table 2. Cross DRA Unit Cell Design Parameters Parameter Value (mm) L Varies from 1.5 to 8.0 W 2.4 H 2.2 2.3. Cross microstrip patch The dimension of the microstrip patch with operating frequency of 26 GHz was determined by a series of a mathematical equation. Then the two same sizes of the rectangular microstrip patch are designed in cross shape. This unit cell design using cross microstrip patch as the phase variation technique. The configuration of the unit cell is shown in Figure 5 and Table 3 shows the optimum parameters obtained. The width of microstrip, WP is fixed at 1.5 mm while the length of microstrip, LP is varying from 1.5 mm to 8.0 mm. (a) 3D view (b) Top view Figure 5. Cross microstrip unit cell Table 3. Cross Microstrip Cell Design Parameters Parameter Value (mm) LP Varies from 1.5 to 8.0 WP 1.5
  • 5. Int J Elec & Comp Eng ISSN: 2088-8708  Dielectric Resonator Reflectarray Antenna Unit Cells for 5G Applications (Nur Fazreen Sallehuddin) 2535 2.4. Cross hybrid DRA The configuration of the cross hybrid DRA is shown in Figure 6. Table 4 shows the unit cell design parameters after simulation and optimization. This unit cell consists of a cross shape DRA combined with cross shape microstrip patch below the cross DRA whereas the cross microstrip patch as the parasitic element to tune the phase of the unit cell. Designing DRA with different size is always difficult to be implemented [10]. Therefore, a design with fixed cross DRA size with the cross microstrip patch as the parasitic element to tune the phase response by varying its length is designed. The width of DRA, W is fixed at 2.4 mm while the length of DRA, L is fixed at 8.0 mm. On top of that, the width of microstrip, WP is fixed at 1.5 mm while the length of microstrip, LP is varying from 1.5 mm to 8.0 mm. (a) 3D view (b) Top view Figure 6. Cross hybrid DRA unit cell Table 4. Cross Hybrid DRA Unit Cell Design Parameters Parameter Value (mm) L 8.0 W 2.4 H 2.2 LP Varies from 1.5 to 8.0 WP 1.5 3. RESULTS AND ANALYSIS The selected designs have been analyzed numerically by using CST MWS simulation tools. In this section, the results for several types of the unit cell for the reflectarray’s unit cell are discussed in terms of reflection phase range, reflection loss and 10% bandwidth. 3.1. Comparison of the simulated results between rectangular DRA and cross shape DRA The two main parameters to show the performance of the reflectarray’s unit cells are the reflection phase and the reflection loss. An important parameter that is availed to analyze the reflectivity and bandwidth of reflectarray is reflection phase [19]. Figure 7 shows the reflection phase of S11 for rectangular DRA (RDRA) and cross DRA. The graphs clearly indicate that cross DRA provides wider phase range than rectangular DRA. This is because the cross DRA unit cell with two resonants element provide a dual- polarization technique that could effectively attain higher phase range than rectangular DRA. The phase range and slope variation of both types unit cells are summarized in Table 5. Based on the result, the slope variation of both unit cells are smooth which indicate that DRA-based unit cells can provide wide bandwidth. Therefore, the cross DRA is selected to combine with microstrip for further study on hybrid unit cell. Table 5. Phase Range and Slope Variation for different Configuration of DRA Unit Cells at 26 GHz Type of Unit Cell Phase range (degrees) Slope Rectangular DRA 332° Slow Cross DRA 497° Slow
  • 6.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 8, No. 4, August 2018 : 2531 – 2539 2536 Figure 7. Phase of S11 for rectangular DRA and cross DRA unit cells 3.2. Comparison of the simulated results for three different cross-shape unit cell configurations for bandwidth enhancement The reflection phase of S11 for three different cross shape configurations obtained by varying the length of the tunable parameter is presented in Figure 8. Based on the results, it can be seen that the cross DRA unit cell exhibit highest reflected phase range which is 684°, followed by cross hybrid DRA phase range equal to 520° and cross microstrip patch phase range is 298°. Limited reflection phase range that less than 360 degrees causes phase errors and consequently reduces its directivity that will deteriorate the antenna performance [9]. Figure 8. Phase of S11 for different unit cells Figure 9. Reflection loss curves for different unit cells For cross microstrip patch case, the gradient slope of the phase variation versus variable length is steeper than the other two unit cells. This is expected to result in a reduced bandwidth [20]. Table 6 shows the phase range and gradient slope for the structures that have been analyzed as the possible candidate for the design of DRA-based reflectarray. In terms of gradient variation, the slope of cross DRA and cross hybrid DRA unit cell is smoother than the slope of cross microstrip patch. The more gradual gradient variation of the reflection phase curve corresponds to the wider bandwidth of the unit element [20], [21]. The phase range of the cross DRA is wider than cross hybrid DRA, but in term of fabrication matter, the cross hybrid DRA with fixed DRA is a better option than cross DRA to decrease the fabrication complexity during an array arrangement. Reflection loss or also known as insertion loss in reflectarray is another vital parameter in the analysis of reflectarray. Normally a reflectarray antenna always exhibits some losses. Therefore, the reflection coefficient or reflection loss is measured less than 1 dB for a reflectarray and the lower loss is the better. Figure 9 illustrates the reflection loss for the three different unit cell configurations. It is demonstrated in Figure 9 that cross DRA is observed to provide the lowest insertion loss value of 0.04 dB whereas the cross hybrid DRA gives 0.77 dB insertion loss. Whilst the cross microstrip unit cell with 1.05 dB gives the
  • 7. Int J Elec & Comp Eng ISSN: 2088-8708  Dielectric Resonator Reflectarray Antenna Unit Cells for 5G Applications (Nur Fazreen Sallehuddin) 2537 highest insertion loss value. This is due to the dielectric resonator element gives low loss as compared to microstrip element that gives higher conductor loss which produced by the microstrip patch. The bandwidth of the unit cell of the reflectarray can be calculated by the reflection loss curves. The bandwidth is determined by moving 10% above the maximum reflection loss value [22]. The 10% bandwidth of the three unit cell configurations are shown in Table 7. From Table 7, it shows that the cross hybrid DRA unit cell offers the wider bandwidth of 160 MHz whereas the cross microstrip unit cell gives a minimum bandwidth of 136 MHz. The results indicate that the cross DRA unit cell gives the lowest reflection loss with broader bandwidth due to the absence of conductor’s losses and surface wave losses. Table 6. Phase Range and Slope Variation for different Configuration of Unit Cells at 26 GHz Type of Unit Cell Phase range (degrees) Slope Cross Microstrip 298° Fast Cross DRA 684° Slow Cross hybrid DRA 520° Slow Table 7. Reflection Loss and 10% Bandwidth for different Unit Cells at 26 GHz Type of Unit Cell Reflection Loss (dB) 10 % Bandwidth (MHz) Cross Microstrip 1.05 136 Cross DRA 0.04 1617 Cross hybrid DRA 0.77 160 4. CONCLUSION The design configurations with three potential cross shape unit cell designs for the reflectarray unit cell at 26 GHz were investigated for the performance optimization of the reflectarray. The CST MWS simulation showed that the best candidate to be deployed for the reflectarray’s unit element in order to fulfill the 5G requirements of a wide bandwidth is the cross hybrid DRA which is the combined fixed cross DRA with cross microstrip patch as the parasitic element. The parasitic element used to tune the phase to give a wide phase range with smooth variation slope. Besides, it is shown that the cross hybrid DRA unit cell gives low reflection loss with better bandwidth performance. Easy implementation and fabrication also emphasized in a selection of the unit element. The simulation results for the unit cells will be validated experimentally in next stage. The design for full reflectarray to predict the overall DRA reflectarray antenna performance and further investigation into how a higher gain can be achieved are being conducted by the authors. ACKNOWLEDGEMENTS The authors would like to thank the Ministry of Education (MOE) for sponsoring the PhD study at Universiti Teknologi Malaysia. Also, special thanks go to UTM GUP (votes 4J220, 05H62, 13H26, 03G59 and 4F733) and Ministry of Science Technology and Innovation (MOSTI) (vote 4S134) for sponsoring this work. REFERENCES [1] C.-X. Wang, F. Haider, X. Gao, X.-H. You, Y. Yang, D. Yuan, H. Aggoune, H. Haas, S. Fletcher, and E. Hepsaydir, “Cellular architecture and key technologies for 5G wireless communication networks,” IEEE Commun. Mag., vol. 52, no. 2, pp. 122-130, 2014. [2] J. G. Andrews, S. Buzzi, W. Choi, S. V. Hanly, A. Lozano, A. C. K. Soong, and J. C. Zhang, “What will 5G be?,” IEEE J. Sel. Areas Commun., vol. 32, no. 6, pp. 1065-1082, 2014. [3] Z. Pi and F. Khan, “An introduction to millimeter-wave mobile broadband systems,” IEEE Commun. Mag., vol. 49, no. 6, pp. 101-107, 2011. [4] S. Mener, R. Gillard, R. Sauleau, C. Cheymol, and P. Potier, “Design and Characterization of a CPSS-Based Unit- Cell for Circularly Polarized Re fl ectarray Applications,” IEEE Trans. Antennas Propag., vol. 61, no. 4, pp. 2313-2318, 2013. [5] M. F. M. Yusoff, R. Sauleau, Z. Johari, M. K. A. Rahim, and H. A. Majid, “A Novel Right Handed Circular Polarization Folded Reflectarray Antenna at 60 GHz,” Int. J. Electr. Comput. Eng., vol. 7, no. 3, p. 1580, 2017. [6] M. M. Tahseen and A. A. Kishk, “Broadband Performance of Novel Closely Spaced Elements in Designing Ka- Band Circularly Polarized Reflectarray Antennas,” vol. 1225, no. c, pp. 1-4, 2016. [7] M. H. Dahri, M. R. Kamarudin, M. H. Jamaluddin, M. Inam, and R. Selvaraju, “Broadband Resonant Elements for 5G Reflectarray Antenna Design,” vol. 15, no. 2, pp. 793-798, 2017.
  • 8.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 8, No. 4, August 2018 : 2531 – 2539 2538 [8] M. H. Dahri, M. R. Kamarudin, M. H. Jamaluddin, and R. R. Selvaraju, “Performance Investigation of Reflectarray Resonant Elements for 5G Communications,” IEEE Asia-Pacific Conf. Appl. Electromagn., no. December, pp. 11-13, 2016. [9] J. Huang and J. A. Encinar, Reflectarray Antenna. John Wiley and Sons, Inc, Publication, 2007. [10] M. H. Jamaluddin, R. Gillard, R. Sauleau, L. Le Coq, X. Castel, R. Benzerga, and T. Koleck, “A dielectric resonator antenna (DRA) reflectarray,” Eur. Microw. Week 2009, EuMW 2009 Sci. Prog. Qual. Radiofreq. Conf. Proc. - 39th Eur. Microw. Conf. EuMC 2009, vol. 6164, no. October, pp. 25-28, 2009. [11] M. H. Jamaluddin, G. C. Eu, S. K. Abdul Rahim, and N. I. Dzulkipli, “Wideband Aperture-Coupled Dielectric Resonator Antenna at 5.8 GHz,” J. Teknol. (Sciences Eng., vol. 69, no. 1, pp. 25-30, 2014. [12] K.-M. Luk and K.-W. Leung, Dielectric Resonator Antennas, no. c. England: Research Studies Press, 2003. [13] Z. Rahimian, “Circularly Polarized Cylindrical Dielectric Resonator Antenna with Different Shapes Cross Slot,” vol. 4, no. 6, pp. 974-978, 2014. [14] E. Lim, H. Y. Wong, and F. L. Lo, “Rectangular DRA Reflectarray with an Inclined Top-loading Micostrip Patch,” pp. 878-881, 2014. [15] R. Florencio, J. Encinar, R. R. Boix, and G. Perez-palomino, “Dual-polarisation reflectarray made of cells with two orthogonal sets of parallel dipoles for bandwidth and cross-polarisation improvement,” IET Microwaves, Antennas Propag., vol. 8, no. 15, pp. 1389-1397, 2014. [16] F. Ahmadi, K. Forooraghi, Z. Atlasbaf, and B. Virdee, “Dual linear-polarized dielectric resonator reflectarray antenna,” IEEE Antennas Wirel. Propag. Lett., vol. 12, pp. 635-638, 2013. [17] A. Petosa, Dielectric resonator antenna handbook. Artech House Publishers, 2007. [18] Final Acts WRC, “In World Radiocommunication Conference Geneva: International Telecommunication Union,” World Radiocommun. Conf., vol. 238, pp. 25-27, 2015. [19] J. Shaker, M. R. Chaharmir, and J. Ethier, Reflectarray Antennas: Analysis, design, fabrication, and measurement. Artech House Publishers, 2013. [20] M. Y. Ismail and M. Inam, “Resonant Elements for Tunable Reflectarray Antenna Design,” Int. J. Antennas Propag., vol. 2012, pp. 1-6, 2012. [21] R. K. Mongia and A. Ittipiboon, “Theoretical and experimental investigations on rectangular dielectric resonator antennas,” IEEE Trans. Antennas Propag., vol. 45, no. 9, pp. 1348-1356, 1997. [22] A. Kiyani and M. Y. Ismail, “Design and analysis of high performance reflectarray resonant elements,” Procedia Eng., vol. 53, pp. 248-254, 2013. BIOGRAPHIES OF AUTHORS Nur Fazreen Sallehuddin received her Bachelor degree in Electrical Engineering (Hons.) (2006) and Master degree in Technic and Vocational Education (2014) from Universiti Tun Hussein Onn Malaysia (UTHM). Experienced as Integration Assistant Engineer and Quality Assurance Engineer for solar industry and automotive industry respectively from 2007-2011. Currently she is pursuing the Ph.D. degree in Electrical Engineering at Wireless Communication Centre, University Technology of Malaysia (UTM). Her research interests and areas include dielectric resonators and reflectarray antennas design in 5G applications and millimeter waves. Mohd Haizal Jamaluddin received the bachelor's and master's degrees in electrical engineering from Universiti Teknologi Malaysia, Malaysia, in 2003 and 2006, respectively, and the Ph.D. degree in signal processing and telecommunications from the Université de Rennes 1, France, in 2009, with a focus on microwavecommunication systems and specific antennas such as dielectric resonator and reflect array and dielectric dome antennas. He joined the Department of Electronic Engineering, Faculty of Electrical Engineering, Universiti Teknologi Malaysia, as a Tutor in 2003. He is currently an Associate Professor with the Wireless Communication Centre, Universiti Teknologi Malaysia (UTM). He was a Senior Lecturer at Wireless Communication Centre (WCC), Universiti Teknologi Malaysia (UTM) until December 2017. He has published more than 40 ISI/Scopus papers in reputed indexed journals and more than 40 conference proceedings. Muhammad Ramlee Kamarudin (Senior Member IEEE 13', Member IEEE 08', Member IET 11') obtained his first degree from Universiti Teknologi Malaysia (UTM), Johor Bahru, Malaysia, with honours, majoring in electrical and telecommunication engineering and graduated in 2003. He received the M.S. degree in communication engineering in 2004 from the University of Birmingham, Birmingham, UK, and later he obtained his Ph.D. degree in 2007 from the same University under the supervision of Professor Peter Hall. Dr Kamarudin is currently working as a Senior Lecturer at the Centre for Electronic Warfare, Information and Cyber (EWIC), Cranfield Defence and Security, Cranfield University, UK. Prior to this appointment, he was an Associate Professor at Wireless Communication Centre (WCC), Universiti Teknologi Malaysia (UTM), Malaysia until May 2017. He holds a H-Index of 19 (SCOPUS) and more than 1350 citations (SCOPUS). He is an author of a book chapter of a book entitled Antennas and Propagation for Body-Centric Wireless Communications and has published more than 200 technical papers in journals and proceedings
  • 9. Int J Elec & Comp Eng ISSN: 2088-8708  Dielectric Resonator Reflectarray Antenna Unit Cells for 5G Applications (Nur Fazreen Sallehuddin) 2539 including IEEE Transaction on Antenna and Propagation (TAP), IEEE Antennas and Wireless Propagation Letter (AWPL), IEEE Antenna Magazine, IEEE Access, International Journal of Antennas and Propagation (IJAP), Progress in Electromagnetics Research (PIER), Microwave and Optical Technology Letters (MOTL), and Electronics Letters. His research interests include antenna design for 5G, wireless on-body communications, in-body communications (implantable antenna), RF and microwave communication systems, and antenna diversity. Dr Kamarudin is an IEEE Senior Member (SMIEEE), a Member of IET (MIET), an Executive Member of Antenna and Propagation (AP/MTT/EMC), Malaysia Chapter, and a Member of IEEE Antennas and Propagation Society, IEEE Communication Society, IEEE Microwave Theory and Techniques Society and IEEE Electromagnetic Compatibility Society. Muhammad Hashim Dahri received the B.E degree in Telecommunications from the Mehran University of Engineering and Technology (MUET), Pakistan, in 2010 and the Masters by Research degree in Electrical Engineering from Universiti Tun Hussein Onn Malaysia (UTHM) in 2014. He is currently pursuing the Ph.D. degree with the Wireless Communication Centre (WCC), Universiti Teknologi Malaysia (UTM). He has authored over 20 research papers in various indexed journals and conference proceedings. His research interests include reflectarray antennas, planar printed antennas and tunable materials for antenna design. Siti Umairah Tajol Anuar received her Bachelor degree in Electronic Telecomunication Engineering (2015) in Universiti Malaysia Sarawak (UNIMAS) and Master in Electronic Telecommunication (2017) from Universiti Teknologi Malaysia (UTM). She is currently pursuing her Ph.D. at the Universiti Teknologi Malaysia (UTM). Her research interests and areas include dielectric resonators antennas and wireless communication.