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TELKOMNIKA Telecommunication Computing Electronics and Control
Vol. 20, No. 6, December 2022, pp. 1200~1205
ISSN: 1693-6930, DOI: 10.12928/TELKOMNIKA.v20i6.24229  1200
Journal homepage: http://telkomnika.uad.ac.id
Semi-circular compact CPW-fed antenna for ultra-wideband
applications
Farhad E. Mahmood, Saad Wasmi Osman Luhaib
Electrical Engineering Department, College of Engineering, University of Mosul, Mosul, Iraq
Article Info ABSTRACT
Article history:
Received Mar 17, 2021
Revised Sep 02, 2022
Accepted Sep 12, 2022
This paper presents a simple structure and small size antenna design with
dimensions of 43×47 mm2
to perform an ultra-wideband (UWB) frequency
range using a semicircular co-planar waveguide (CPW). This antenna has
been designed and simulated by the computer simulation technology (CST)
microwave studio suit. In this work, we design an ultra-wideband antenna
(about 2 GHz to 10 GHz) by feeding a semi-circular compact antenna via a
co-planar waveguide for input impedance of 50 Ω. The CST simulation
results show that our designed antenna has a very good impedance and
radiation characteristic within the intended ultra-wideband. Because of the
small size and the suitable shape, this antenna can be used in many wireless
communication applications, such as a radio frequency identifier (RFID),
indoor wireless local area network or wireless fidelity (WiFi), internet of
things (IoT), millimeter waves communications (mmWave), global
positioning system (GPS), and many applications of 6G systems.
Keywords:
Antenna design
Coplanar waveguide
Semi-circular
Ultra-wideband
This is an open access article under the CC BY-SA license.
Corresponding Author:
Farhad E. Mahmood
Electrical engineering department, College of Engineering, University of Mosul
Mosul, Iraq
Email: farhad.m@uomosul.edu.iq
1. INTRODUCTION
Mobile communication becomes part of our daily life, as more data can be reached via a hand-size
device [1]–[25]. This motivates many research centers in the world to focus on this device to make it smaller
and perform better. This includes the design of antennas.
Since it was adopted by the United States, the federal communications commission (FCC) in 2002,
ultra wideband (UWB) communications, which allocated the 3.1 GHz to 10.6 GHz band, have attracted great
interest lately. The corresponding standards of IEEE 802.15.3a, which stand for the short rang high data rate,
and the IEEE 802.15.4a, the low power low data rate have been presented [3]. This help this technology is
one of the most promising technologies for short-range wireless communication systems.
UWB technology has increased in both academic and industry research laboratories as it is used in
high-speed communication data rate, wireless link connectivity, sufficient radiation pattern properties, and
sufficient impedance adaptation properties [1]. The system of UWB uses short-duration pulses for some
nanoseconds to send coded signals. Such short-duration spread the signal energy very widely on bandwidth
as we know from fourier transform formula.
The feature of short-duration pulses along with the low energy transmitted can ensure as low interference
as possible with current narrow-band systems. Range information can be extracted via either the frequency/phase
of continuous wave signal is modulated or via the short duration pulses are transmitted. In practice, the frequency
modulated continuous wave and phase modulated continuous wave radar are used [6].
TELKOMNIKA Telecommun Comput El Control 
Semi-circular compact CPW-fed antenna for ultra-wideband applications (Farhad E. Mahmood)
1201
The technology of UWB shows adequate performance for many wireless applications such as radars,
mobile wireless communication systems, vehicle-to-vehicle communications systems, behind-the-wall signal
penetration, medical image picturing radio, position location, and wideband game applications, navy and
defense applications [2]-[12]. Many articles have provided a similar design [8]-[12]. However, the design in
this paper provides a small antenna with high bandwidth that is allocated in the ultra-wideband.
In this paper, we study the property of the proposed design of a semi-circular configuration with a
co-planar fading for ultra-wideband applications. The design, as shown in Figure 1, basically, consists of a
half-circle shape with a radius of 𝑟 that is fed by the co-planar way with a dimension of 𝐿𝑔 by 𝑊𝑔. The space
between the semi-circular shape and the co-planar is good enough to pass the ultra-wideband frequencies,
refer to it as 𝑡. There is a tiny space separation in the co-planar feed between the feeder and the wings called 𝑔.
We used the computer simulation technology (CST) Microwave Studio Suit TM 2018 to perform the
simulation and to run the optimization to obtain the ultra-wideband frequency and reduce the input
impedance. CST suit is based on the method of the three-dimensional finite time-domain integration (FTID).
the displayed simulation results provide and express the radiation pattern, the input impedance, gain, and the
electromagnetic characteristics of the surface current distribution.
Figure 1. The geometric shape of the proposed CPW-fed coplanar slot antenna configuration
2. ANTENNA GEOMETRY
Using the CST suite software, we design the co-planar waveguide (CPW-Fed) co-planar semicircle
antenna. The simulation results of CST for this design will show different parameters to show the
characteristic of the design, such as the input impedance, S11, the return loss, radiation pattern, and the
directivity and gain. The semicircle antenna is designed on a microstrip structure, where the wavelength 𝜆𝑔
that imports at the frequency designs can be calculated according to [5].
𝜆𝑔 =
𝜆𝑜
√𝜀𝑒𝑓𝑓
(1)
Where 𝜀𝑒𝑓𝑓 is an effective dielectric constant. 𝜆𝑜 is the wavelength in the air 𝜀𝑒𝑓𝑓 is usually computed via the (2).
𝜀𝑒𝑓𝑓 =
𝜀𝑟+1
2
(2)
Where 𝜀𝑟 is the circuit prints dielectric coefficients 𝜀𝑒𝑓𝑓 is the effective parameter of dielectric coefficient.
The design of antenna is implemented in this paper via considering the parameters in the following values:
dielectric constant 𝜀𝑟 = 4.3, FR4 epoxy substrate thickness ℎ = 1.54 mm, and loss tangent 𝑡𝑎𝑛𝛿 = 0.025.
The values of the rest of the parameters of the design are stated in Table 1.
Table 1. The proposed antenna parameters
Parameters value
𝑔 0.5 mm
𝑊𝑓 6.7 mm
𝑊𝑔 20 mm
𝐿𝑔 19 mm
𝑡 1 mm
𝑟 23 mm
ℎ 1.54 mm
 ISSN: 1693-6930
TELKOMNIKA Telecommun Comput El Control, Vol. 20, No. 6, December 2022: 1200-1205
1202
3. THE SIMULATION RESULTS
3.1. The implementation
In Figure 1, we see a rectangular shape of the radiator that has been fed by a 50 Ω co-planar
waveguide transmission line CPW. Along with the antenna the feeding structure layouts on the same plane,
leaving one substrate layer with a single sized metallization to be utilized. Such a structure yields a very easy
manufacturing antenna with an extremely low cost. Most of the design implementation and optimization have
been performed in the CST microwave studio, which is very well known in this field [3]. The design
parameters can be found in Table 1, which shows the details of the configuration.
3.2. The results
The bandwidth of the can be found either by the corresponding return loss (S11) parameter or by
voltage standing wave ratio (VSWR). Usually, the antenna bandwidth is determined as the return loss goes
beneath 10 dB. The things that are presented in the results are the s-parameters, the VSWR, the radiation pattern
of the proposed antenna, the gain and the bandwidth. All the results are presented in the associated figures.
Figure 2, Figure 3, and Figure 4 show S11, VSWR, and the proposed antenna impedance, respectively. Figure 2
demonstrations that the bandwidth for the proposed antenna is taking place from 2.1 GHz to 9.8 GHz. It is clear
in Figure 2 that the ultra-wideband properties of the design from looking at the S11 values, which the under
-10 dB spans from 2 GHz until near the 10 GHz. We also study the case to change the parameter of the design
to increase the band to reach 12 GHz, but that led to an increase in the value of S11 near the two values 3.5 GHz
and 7 GHz. VSWR, which is shown in Figure 3, is calculated by:
𝑉𝑆𝑊𝑅 =
𝑉𝑀𝐴𝑋
𝑉𝑀𝐼𝑁
=
1+|𝛤|
1−|𝛤|
, (3)
Where the voltage reflection coefficient, 𝛤, is defined by:
𝛤 =
𝑉−
𝑉+ =
𝑍𝐿−𝑍𝑂
𝑍𝐿−𝑍𝑂
, (4)
Where the value of 𝑍𝐿 represents the amount of load impedance and 𝑍0 represents the transmission line
(which can be between the antenna and the feeding cable) characteristic impedance. The value of the
reflection coefficient is also displayed by showing the equivalent plot of the scattering parameters S11.
Figure 2. The simulated S11 for the antenna Figure 3. Simulated VSWR for the antenna proposed
Figure 4. The simulation result of gain for the proposed
antenna
Figure 5. Simulated real and imaginary
impedance
TELKOMNIKA Telecommun Comput El Control 
Semi-circular compact CPW-fed antenna for ultra-wideband applications (Farhad E. Mahmood)
1203
Figure 4 shows the relationship between antenna gain and the frequency in GHz. The proposed
antenna for a wideband operating frequency is shown. From the figure, we can notice that the lowest gain is 2 dB
at the frequency of 2.1 GHz and the maximum gain of 5.3 dB is achieved at 7.2 GHz. The average gain for
the proposed antenna is around 4 dB.
The input impedance in the shape of the real and imaginary plot of the proposed antenna is displayed
in Figure 5 over a range of frequencies that spans from 0.01 GHz to 12 GHz. Figure 5 shows the input
impedance of the proposed antenna near and around to desired impedance (50 Ω). In Figure 6, the far-field
radiated patterns in the frequencies of Figure 6(a) 2.5 GHz, Figure 6(b) 5 GHz, Figure 6(c) 7.5 GHz, and
Figure 6(d) 10 GHz. The obtained results in these figures clearly display the high gain of the proposed
antenna in the bandwidth within a range of 2.12 GHz to 9.8 GHz, at 55 Ω input impedance, which covers
many applications such as wireless fidelity (WiFi), internet-of-things (IoT), and long term evolution (LTE).
Figure 7 shows the 3D far-field radiation patterns for the four mentioned frequencies: Figure 7(a)
2.5 GHz, Figure 7(b) 5 GHz, Figure 7(c) 7.5 GHz, and Figure 7(d) 10 GHz. The color-coded power pattern
shows the red to be higher power concentrated (focused). For 2.5 GHz, the power is focused in only two
directions. After that, with increasing the frequency, the power start to distribute on multiple directions.
(a) (b)
(c) (d)
Figure 6. Far-field radiation pattern plot for (a) 2.5 GHz, (b) 5 GHz, (c) 7.5 GHz, and (d) 10 GHz
(a) (b) (c) (d)
Figure 7. 3D Far-field radiation pattern plot for (a) 2.5 GHz, (b) 5 GHz, (c) 7.5 GHz, and (d)10 GHz
 ISSN: 1693-6930
TELKOMNIKA Telecommun Comput El Control, Vol. 20, No. 6, December 2022: 1200-1205
1204
4. CONCLUSION
The wideband aperture antenna has been designed and simulated to work with many ultra-wideband
applications. The antenna is designed as a semi-circular compact fed by the CPW. The simulation is
performed by CST microwave studio software. The antenna footprint dimension is 4.3 cm × 4.72 cm with a
suitable impedance. The obtained results clearly show the high gain of the proposed antenna in the bandwidth
within a range of 2.12 GHz to 9.8 GHz, at 55 Ω input impedance, which covers many applications such as
WiFi, IoT, global positioning system (GPS), and LTE.
ACKNOWLEDGMENTS
Authors would like to show their gratitude to the University of Mosul for the help to the success of
this work.
REFERENCES
[1] A. Hosseinzadeh, M. Mirmozafari, M. V. Varnoosfaderani, C. Ghobadi, and J. Nourinia, “A U-shaped UWB antenna with band-
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TELKOMNIKA Telecommun Comput El Control 
Semi-circular compact CPW-fed antenna for ultra-wideband applications (Farhad E. Mahmood)
1205
[23] R. Ullah et al., “High-gain vivaldi antenna with wide bandwidth characteristics for 5G mobile and Ku-Band radar applications, ”
Electronics, vol. 10, no. 6, 2021, doi: 10.3390/electronics10060667.
[24] F. Mahmood, E. Perrins, and L. liu, “Energy-Efficient Wireless Communications: From Energy Modeling to Performance
Evaluation,” IEEE Transactions on Vehicular Technology, vol. 68, no. 8, pp. 7643-7654, 2019, doi: 10.1109/TVT.2019.2921304.
[25] V. Kaim, B. K. Kanaujia, S. Kumar, H. C. Choi, K. W. Kim, and K. Rambabu, “Ultra-Miniature Circularly Polarized CPW-Fed
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doi: 10.1038/s41598-020-63780-4.
BIOGRAPHIES OF AUTHORS
Farhad E. Mahmood has received the bachelor and master degrees from the
University of Mosul. He received his Ph.D. from KU the University of Kansas in May 2019.
All the degrees are in electrical engineering. His research interests include wireless
communications, energy efficiency, Machine learning, and signal processing. Dr. Mahmood
is a reviewer in several IEEE transaction journals. He can be contacted at email:
farhad.m@uomosul.edu.iq.
Saad Wasmi Osman Luhaib has received the bachelor and master degrees
from the University of Mosul. He received his Ph.D. from the University of Leeds in 2018.
The common research are Microwave devices, DSP, and Multi-mode filters. Dr. Luhaib is a
reviewer in several Engineering journals. He can be contacted at email:
s.w.o.luhaib@uomosul.edu.iq.

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Semi-circular compact CPW-fed antenna for ultra-wideband applications

  • 1. TELKOMNIKA Telecommunication Computing Electronics and Control Vol. 20, No. 6, December 2022, pp. 1200~1205 ISSN: 1693-6930, DOI: 10.12928/TELKOMNIKA.v20i6.24229  1200 Journal homepage: http://telkomnika.uad.ac.id Semi-circular compact CPW-fed antenna for ultra-wideband applications Farhad E. Mahmood, Saad Wasmi Osman Luhaib Electrical Engineering Department, College of Engineering, University of Mosul, Mosul, Iraq Article Info ABSTRACT Article history: Received Mar 17, 2021 Revised Sep 02, 2022 Accepted Sep 12, 2022 This paper presents a simple structure and small size antenna design with dimensions of 43×47 mm2 to perform an ultra-wideband (UWB) frequency range using a semicircular co-planar waveguide (CPW). This antenna has been designed and simulated by the computer simulation technology (CST) microwave studio suit. In this work, we design an ultra-wideband antenna (about 2 GHz to 10 GHz) by feeding a semi-circular compact antenna via a co-planar waveguide for input impedance of 50 Ω. The CST simulation results show that our designed antenna has a very good impedance and radiation characteristic within the intended ultra-wideband. Because of the small size and the suitable shape, this antenna can be used in many wireless communication applications, such as a radio frequency identifier (RFID), indoor wireless local area network or wireless fidelity (WiFi), internet of things (IoT), millimeter waves communications (mmWave), global positioning system (GPS), and many applications of 6G systems. Keywords: Antenna design Coplanar waveguide Semi-circular Ultra-wideband This is an open access article under the CC BY-SA license. Corresponding Author: Farhad E. Mahmood Electrical engineering department, College of Engineering, University of Mosul Mosul, Iraq Email: farhad.m@uomosul.edu.iq 1. INTRODUCTION Mobile communication becomes part of our daily life, as more data can be reached via a hand-size device [1]–[25]. This motivates many research centers in the world to focus on this device to make it smaller and perform better. This includes the design of antennas. Since it was adopted by the United States, the federal communications commission (FCC) in 2002, ultra wideband (UWB) communications, which allocated the 3.1 GHz to 10.6 GHz band, have attracted great interest lately. The corresponding standards of IEEE 802.15.3a, which stand for the short rang high data rate, and the IEEE 802.15.4a, the low power low data rate have been presented [3]. This help this technology is one of the most promising technologies for short-range wireless communication systems. UWB technology has increased in both academic and industry research laboratories as it is used in high-speed communication data rate, wireless link connectivity, sufficient radiation pattern properties, and sufficient impedance adaptation properties [1]. The system of UWB uses short-duration pulses for some nanoseconds to send coded signals. Such short-duration spread the signal energy very widely on bandwidth as we know from fourier transform formula. The feature of short-duration pulses along with the low energy transmitted can ensure as low interference as possible with current narrow-band systems. Range information can be extracted via either the frequency/phase of continuous wave signal is modulated or via the short duration pulses are transmitted. In practice, the frequency modulated continuous wave and phase modulated continuous wave radar are used [6].
  • 2. TELKOMNIKA Telecommun Comput El Control  Semi-circular compact CPW-fed antenna for ultra-wideband applications (Farhad E. Mahmood) 1201 The technology of UWB shows adequate performance for many wireless applications such as radars, mobile wireless communication systems, vehicle-to-vehicle communications systems, behind-the-wall signal penetration, medical image picturing radio, position location, and wideband game applications, navy and defense applications [2]-[12]. Many articles have provided a similar design [8]-[12]. However, the design in this paper provides a small antenna with high bandwidth that is allocated in the ultra-wideband. In this paper, we study the property of the proposed design of a semi-circular configuration with a co-planar fading for ultra-wideband applications. The design, as shown in Figure 1, basically, consists of a half-circle shape with a radius of 𝑟 that is fed by the co-planar way with a dimension of 𝐿𝑔 by 𝑊𝑔. The space between the semi-circular shape and the co-planar is good enough to pass the ultra-wideband frequencies, refer to it as 𝑡. There is a tiny space separation in the co-planar feed between the feeder and the wings called 𝑔. We used the computer simulation technology (CST) Microwave Studio Suit TM 2018 to perform the simulation and to run the optimization to obtain the ultra-wideband frequency and reduce the input impedance. CST suit is based on the method of the three-dimensional finite time-domain integration (FTID). the displayed simulation results provide and express the radiation pattern, the input impedance, gain, and the electromagnetic characteristics of the surface current distribution. Figure 1. The geometric shape of the proposed CPW-fed coplanar slot antenna configuration 2. ANTENNA GEOMETRY Using the CST suite software, we design the co-planar waveguide (CPW-Fed) co-planar semicircle antenna. The simulation results of CST for this design will show different parameters to show the characteristic of the design, such as the input impedance, S11, the return loss, radiation pattern, and the directivity and gain. The semicircle antenna is designed on a microstrip structure, where the wavelength 𝜆𝑔 that imports at the frequency designs can be calculated according to [5]. 𝜆𝑔 = 𝜆𝑜 √𝜀𝑒𝑓𝑓 (1) Where 𝜀𝑒𝑓𝑓 is an effective dielectric constant. 𝜆𝑜 is the wavelength in the air 𝜀𝑒𝑓𝑓 is usually computed via the (2). 𝜀𝑒𝑓𝑓 = 𝜀𝑟+1 2 (2) Where 𝜀𝑟 is the circuit prints dielectric coefficients 𝜀𝑒𝑓𝑓 is the effective parameter of dielectric coefficient. The design of antenna is implemented in this paper via considering the parameters in the following values: dielectric constant 𝜀𝑟 = 4.3, FR4 epoxy substrate thickness ℎ = 1.54 mm, and loss tangent 𝑡𝑎𝑛𝛿 = 0.025. The values of the rest of the parameters of the design are stated in Table 1. Table 1. The proposed antenna parameters Parameters value 𝑔 0.5 mm 𝑊𝑓 6.7 mm 𝑊𝑔 20 mm 𝐿𝑔 19 mm 𝑡 1 mm 𝑟 23 mm ℎ 1.54 mm
  • 3.  ISSN: 1693-6930 TELKOMNIKA Telecommun Comput El Control, Vol. 20, No. 6, December 2022: 1200-1205 1202 3. THE SIMULATION RESULTS 3.1. The implementation In Figure 1, we see a rectangular shape of the radiator that has been fed by a 50 Ω co-planar waveguide transmission line CPW. Along with the antenna the feeding structure layouts on the same plane, leaving one substrate layer with a single sized metallization to be utilized. Such a structure yields a very easy manufacturing antenna with an extremely low cost. Most of the design implementation and optimization have been performed in the CST microwave studio, which is very well known in this field [3]. The design parameters can be found in Table 1, which shows the details of the configuration. 3.2. The results The bandwidth of the can be found either by the corresponding return loss (S11) parameter or by voltage standing wave ratio (VSWR). Usually, the antenna bandwidth is determined as the return loss goes beneath 10 dB. The things that are presented in the results are the s-parameters, the VSWR, the radiation pattern of the proposed antenna, the gain and the bandwidth. All the results are presented in the associated figures. Figure 2, Figure 3, and Figure 4 show S11, VSWR, and the proposed antenna impedance, respectively. Figure 2 demonstrations that the bandwidth for the proposed antenna is taking place from 2.1 GHz to 9.8 GHz. It is clear in Figure 2 that the ultra-wideband properties of the design from looking at the S11 values, which the under -10 dB spans from 2 GHz until near the 10 GHz. We also study the case to change the parameter of the design to increase the band to reach 12 GHz, but that led to an increase in the value of S11 near the two values 3.5 GHz and 7 GHz. VSWR, which is shown in Figure 3, is calculated by: 𝑉𝑆𝑊𝑅 = 𝑉𝑀𝐴𝑋 𝑉𝑀𝐼𝑁 = 1+|𝛤| 1−|𝛤| , (3) Where the voltage reflection coefficient, 𝛤, is defined by: 𝛤 = 𝑉− 𝑉+ = 𝑍𝐿−𝑍𝑂 𝑍𝐿−𝑍𝑂 , (4) Where the value of 𝑍𝐿 represents the amount of load impedance and 𝑍0 represents the transmission line (which can be between the antenna and the feeding cable) characteristic impedance. The value of the reflection coefficient is also displayed by showing the equivalent plot of the scattering parameters S11. Figure 2. The simulated S11 for the antenna Figure 3. Simulated VSWR for the antenna proposed Figure 4. The simulation result of gain for the proposed antenna Figure 5. Simulated real and imaginary impedance
  • 4. TELKOMNIKA Telecommun Comput El Control  Semi-circular compact CPW-fed antenna for ultra-wideband applications (Farhad E. Mahmood) 1203 Figure 4 shows the relationship between antenna gain and the frequency in GHz. The proposed antenna for a wideband operating frequency is shown. From the figure, we can notice that the lowest gain is 2 dB at the frequency of 2.1 GHz and the maximum gain of 5.3 dB is achieved at 7.2 GHz. The average gain for the proposed antenna is around 4 dB. The input impedance in the shape of the real and imaginary plot of the proposed antenna is displayed in Figure 5 over a range of frequencies that spans from 0.01 GHz to 12 GHz. Figure 5 shows the input impedance of the proposed antenna near and around to desired impedance (50 Ω). In Figure 6, the far-field radiated patterns in the frequencies of Figure 6(a) 2.5 GHz, Figure 6(b) 5 GHz, Figure 6(c) 7.5 GHz, and Figure 6(d) 10 GHz. The obtained results in these figures clearly display the high gain of the proposed antenna in the bandwidth within a range of 2.12 GHz to 9.8 GHz, at 55 Ω input impedance, which covers many applications such as wireless fidelity (WiFi), internet-of-things (IoT), and long term evolution (LTE). Figure 7 shows the 3D far-field radiation patterns for the four mentioned frequencies: Figure 7(a) 2.5 GHz, Figure 7(b) 5 GHz, Figure 7(c) 7.5 GHz, and Figure 7(d) 10 GHz. The color-coded power pattern shows the red to be higher power concentrated (focused). For 2.5 GHz, the power is focused in only two directions. After that, with increasing the frequency, the power start to distribute on multiple directions. (a) (b) (c) (d) Figure 6. Far-field radiation pattern plot for (a) 2.5 GHz, (b) 5 GHz, (c) 7.5 GHz, and (d) 10 GHz (a) (b) (c) (d) Figure 7. 3D Far-field radiation pattern plot for (a) 2.5 GHz, (b) 5 GHz, (c) 7.5 GHz, and (d)10 GHz
  • 5.  ISSN: 1693-6930 TELKOMNIKA Telecommun Comput El Control, Vol. 20, No. 6, December 2022: 1200-1205 1204 4. CONCLUSION The wideband aperture antenna has been designed and simulated to work with many ultra-wideband applications. The antenna is designed as a semi-circular compact fed by the CPW. The simulation is performed by CST microwave studio software. The antenna footprint dimension is 4.3 cm × 4.72 cm with a suitable impedance. The obtained results clearly show the high gain of the proposed antenna in the bandwidth within a range of 2.12 GHz to 9.8 GHz, at 55 Ω input impedance, which covers many applications such as WiFi, IoT, global positioning system (GPS), and LTE. ACKNOWLEDGMENTS Authors would like to show their gratitude to the University of Mosul for the help to the success of this work. REFERENCES [1] A. Hosseinzadeh, M. Mirmozafari, M. V. Varnoosfaderani, C. Ghobadi, and J. 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  • 6. TELKOMNIKA Telecommun Comput El Control  Semi-circular compact CPW-fed antenna for ultra-wideband applications (Farhad E. Mahmood) 1205 [23] R. Ullah et al., “High-gain vivaldi antenna with wide bandwidth characteristics for 5G mobile and Ku-Band radar applications, ” Electronics, vol. 10, no. 6, 2021, doi: 10.3390/electronics10060667. [24] F. Mahmood, E. Perrins, and L. liu, “Energy-Efficient Wireless Communications: From Energy Modeling to Performance Evaluation,” IEEE Transactions on Vehicular Technology, vol. 68, no. 8, pp. 7643-7654, 2019, doi: 10.1109/TVT.2019.2921304. [25] V. Kaim, B. K. Kanaujia, S. Kumar, H. C. Choi, K. W. Kim, and K. Rambabu, “Ultra-Miniature Circularly Polarized CPW-Fed Implantable Antenna Design and its Validation for Biotelemetry Applications,” Scientific Reports, vol. 10, no. 6975, 2020, doi: 10.1038/s41598-020-63780-4. BIOGRAPHIES OF AUTHORS Farhad E. Mahmood has received the bachelor and master degrees from the University of Mosul. He received his Ph.D. from KU the University of Kansas in May 2019. All the degrees are in electrical engineering. His research interests include wireless communications, energy efficiency, Machine learning, and signal processing. Dr. Mahmood is a reviewer in several IEEE transaction journals. He can be contacted at email: farhad.m@uomosul.edu.iq. Saad Wasmi Osman Luhaib has received the bachelor and master degrees from the University of Mosul. He received his Ph.D. from the University of Leeds in 2018. The common research are Microwave devices, DSP, and Multi-mode filters. Dr. Luhaib is a reviewer in several Engineering journals. He can be contacted at email: s.w.o.luhaib@uomosul.edu.iq.