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International Journal on Recent and Innovation Trends in Computing and Communication ISSN: 2321-8169
Volume: 5 Issue: 12 235 - 238
______________________________________________________________________________________
235
IJRITCC | December 2017, Available @ http://www.ijritcc.org
_______________________________________________________________________________________
Mathematical Analysis of Half Volume DRA with Performance Evaluation for
High Speed System Applications
Dr. S. V. A. V. Prasad#
and Anshu Thakur*
#
Dean (Research, Development & Industrial Consultancy), Lingaya's University, Faridabad, Haryana, India
*
Research Scholar, Dept. Of ECE, Lingaya’s University, Faridabad, Haryana, India
Abstract:- A novel efficient design analysis has been proposed for a reduced-size dielectric resonator antenna (DRA). This has been done by
using half-volume resonator with short-circuited plane of symmetry. The design serves as a new configuration of planar antenna, thus making
integration of active devices easier. The antenna shows remarkable performance, having low cross-polarization levels and reasonably well
radiation patterns. The antenna design has been simulated using a new analytical framework created in MATLAB giving accurate measurement
details.
Keywords: Dielectric Resonator Antenna, Half-volume, High Speed Systems, Simulation Framework.
__________________________________________________*****_________________________________________________
1. Introduction
The ever increasing demand for high speed and reliable
communication systems have pushed the development of
microwave and mm-wave systems which requires new and
improved antennas with outstanding performance
characteristics. Moreover, many base stations and new
communication systems require compact and cost-effective
components. Since about 1970’s, dielectric resonators have
helped achieve the miniaturization of active and passive
microwave components, such as oscillators and filters [1, 2]
and have proved to be one of the driving forces behind
advancement of communication systems such as Spatial
Division Multiple Access.
A lot of extensive work has been done on microstrip-fed
DRAs [1]-[8] and probe-fed DRAs [9]-[12], but only limited
attempts have been made at designing DRAs using a common
analytical approach. New feed mechanisms like CPW has
been shown to be used to excite cylindrical resonator antenna
[13]. There have been some recent developments also which
shows that the CPW is quite effective as a mechanism for
excitation for the rectangular type DRA [14]-[15]. There are
also research on half-volume DRA which is fed by microstrip
line. [16]-[17].
It is the intent of this paper to propose a reduced size
dielectric resonator antenna which is excited by coplanar
waveguide through an aperture in the ground plane. The
antenna design is optimized, using a new analytical
framework created by authors of this paper in [18], to improve
the coupling and performance parameters of the antenna. The
design proposed in this paper has the clear advantage of
fabrication ease owing to its single process of metallization
and dielectric layers.
Detailed theoretical analysis is carried out for performance
evaluation using the new analytical framework created in
MATLAB. The gain, return loss, and radiation pattern of the
proposed antenna are shown and analyzed. The choice of
MATLAB as the design of analytical framework is primarily
governed by the fact that it is highly capable in solving partial
differential equations derived from the original Maxwell
equations using which we have created this simulation
framework.
2. Mathematical Equations of Analysis
As emphasized earlier, a new simulation framework has been
developed to assess the performance of the DRA derived from
the Maxwell's equations. Based on the different modes
expected to be present in the CPW feed and antenna
characteristics, equations for different resonant frequencies as
a function of height has been derived. This gives an important
insight regarding the geometric parameters of the antenna that
can be suitably chosen according to the equation for optimal
performance.
The resonant frequency as a function of height for
different permittivities for TE01 mode is :-
... (1)
Corresponding to this equation, the results have been plotted
and shown in figure below :-
Figure 1: Graph of resonant frequencies for TE01 mode
International Journal on Recent and Innovation Trends in Computing and Communication ISSN: 2321-8169
Volume: 5 Issue: 12 235 - 238
______________________________________________________________________________________
236
IJRITCC | December 2017, Available @ http://www.ijritcc.org
_______________________________________________________________________________________
Similarly, the equation for resonant frequency as a
function of height for different permittivities for TM01 mode
is :-
... (2)
Corresponding to this equation, the results have been
plotted and has been shown in figure below :-
Figure 2: Graph of resonant frequencies for TM01 mode
The equation for resonant frequency as a function of height
for different permittivities for HE11 mode is :-
(3...)
The graph of this equation happens to be the one shown
below :-
Figure 3: Graph of resonant frequencies for HE11 mode
Using the above equations and selection of optimal resonant
frequency leads to direct selection of dielectric material with
certain permittivity for creating the DRA with required
characteristics.
3. Design and Geometry of the Antenna
The design and the geometry of the antenna has been decided
in a manner that leads to maximum performance
characteristics specifically for real-time high speed
communication systems.
The top view and the corresponding side view of the
dielectric resonator antenna is shown in the figure below for
greater understanding :-
Figure 4: Top view and side view of the DRA
The DRA has a radius of R = 15 mm, height h = 10.5 mm
and a permittivity of εdra = 31.5. The coaxial line connecting
the CPW feed is at a distance of 9 mm from the center. The
DRA is printed on a substrate of permittivity 2.2 and
thickness 3.2 mm. The metallic via have a radius a=2mm, and
they are disposed with the same transversal period and the
same radial period Pr2=23.6mm. In this structure, no back
conductor for the substrate was used in order to reduce the
adverse effects of the leaky waves that might otherwise
degrade the performance of the antenna. However, the
dimensions are chosen such that the radiation under the
substrate is insignificant.
The entire design of the antenna was created in HFSS
software and accordingly a sample simulation was performed
to verify the design. During simulation the practical
performance characteristics of the antenna is inferred which is
later used to simulate within the analytical framework created
in MATLAB. The result obtained is then correlated with the
HFSS software for accurate validation of the analytical
method.
International Journal on Recent and Innovation Trends in Computing and Communication ISSN: 2321-8169
Volume: 5 Issue: 12 235 - 238
______________________________________________________________________________________
237
IJRITCC | December 2017, Available @ http://www.ijritcc.org
_______________________________________________________________________________________
4. Simulation Results
The simulation was performed using MATLAB. A
combination of PDE toolbox and scratch coding was used to
come up with graphs of various performance metrics.
In figure 5 below, the return loss of the proposed antenna is
shown.
Figure 5: Simulated return loss of the proposed antenna
Note that the return loss is around –35 dB at resonance.
This indicates that most of the input power at the feedline is
absorbed by the resonator which is then radiated into the
surrounding space. The graph shows two scenarios that is
with etched background plane (EBG) and without EBG to
provide greater insight into the working characteristics of the
antenna.
The graph for the gain of the antenna is shown in the figure
below :-
Figure 6: Simulated gain of the proposed antenna
As can be seen that the maximum gain of the antenna
remains constant across a range of operational frequency
which is highly desired characteristic in any antenna.
The simulated radiation pattern observed by plotting the
graph is shown in the figure below :-
Figure 7: Simulated radiation pattern of the proposed antenna
The simulated radiation patterns in both the E- and H-
planes are shown. It was also noted that the cross polarization
levels were low. The radiation is mostly in the resonator
direction and negligible radiation is directed below the
substrate.
The interference between the antenna radiation pattern and
the far-field pattern of the diffracted waves results in the
measured co-polarized component ripples around the
simulated component. The E-plane suffers from greater
diffraction than the H-plane, due to the fact that the space
wave in the vicinity of the truncated ground plane is stronger
in the E-plane. In consequence, the diffracted fields are also
stronger in the E-plane.
All of these simulation results show and validate the efficacy
of the analytical framework developed to simulate and verify
the performance characteristics of any DRA using relevant
mathematical modeling.
5. Conclusions
In this paper, a new analytical framework using mathematical
modeling has been proposed that led to accurate design of
DRA fed via CPW. Detailed performance evaluation of the
proposed antenna was carried out and it was conclusively
shown how the new analytical framework leads to design
criteria which allows one to select appropriate dielectric
material for the DRA giving better results. The antenna shows
good performance in terms of low cross-polarization levels,
matching to the feeding structure, and low back radiation.
References
[1] R. A. Kranenburg and S. A. Long, “Microstrip
transmission line excitation of dielectric resonator
antennas,” Electronics Letters, Vol. 24, pp. 1156-1157,
1988.
[2] J. T. St. Martin, Y. M. M. Antar, A. A. Kishk, A.
Ittipiboon, and M. Cuhaci, “Dielectric resonator antenna
using aperture coupling,“ Electronics Letters, Vol. 26, No.
24, pp. 2015-2016, Nov. 1990.
International Journal on Recent and Innovation Trends in Computing and Communication ISSN: 2321-8169
Volume: 5 Issue: 12 235 - 238
______________________________________________________________________________________
238
IJRITCC | December 2017, Available @ http://www.ijritcc.org
_______________________________________________________________________________________
[3] A. Ittipiboon, R. K. Mongia, Y. M. M. Antar, P. Bhartia,
and M. Cuhaci, “Aperture fed rectangular and triangular
dielectric resonators for use as magnetic dipole antennas,”
Electronics Letters, Vol. 29, No. 23, pp. 2001-2002, Nov.
1993.
[4] G. D. Loos and Y. M. M. Antar, “A new aperture-coupled
rectangular dielectric resonator antenna array,” Microwave
and Optical Technology Letters, Vol. 7, No. 14, pp. 642-
644, Oct. 1994.
[5] A. A. Kishk, A. Ittipiboon, Y. M. M. Antar, and M.
Cuhaci, “Slot excitation of the dielectric disk radiator,”
IEEE Transactions on Antennas and Propagation, Vol. 43,
No. 2, pp. 198-201, Feb. 1995.
[6] M. G. Keller, D. J. Roscoe, M. B. Oliver, R. K. Mongia, Y.
M. M. Antar, and A. Ittipiboon, “Active aperture-coupled
rectangular dielectric resonator antenna,” IEEE Microwave
and Guided Wave Letters, Vol. 5, No. 11, pp. 376-378,
Nov. 1995.
[7] Y. M. M. Antar and Z. Fan, “Theoretical investigation of
aperture-coupled rectangular dielectric resonator antenna,”
IEE Proc.-Microw. Antennas Propag., Vol. 143, No. 2, pp.
113-118, Apr. 1996.
[8] C.-Y. Huang, J.-Y. Wu, and K.-L. Wong, “Cross-slot-
coupled microstrip antenna and dielectric resonator
antenna for circular polarization,” IEEE Transactions on
Antennas and Propagation, Vol. 47, No. 4, pp. 605-609,
Apr. 1999.
[9] S. A. Long, M. W. McAllister, and L. C. Shen, “The
resonant cylindrical dielectric cavity antenna,” IEEE
Transactions on Antennas and Propagation, Vol. 31, pp.
406-412, 1983.
[10] K. W. Leung, K. M. Luk, and K. Y. A. Lai, “Theory and
experiment of a coaxial probe fed hemispherical dielectric
resonator antenna,” IEEE Transactions on Antennas and
Propagation, Vol. 41, No. 6, pp. 1390-1398, 1993.
[11] R. K. Mongia, A. Ittipiboon, M. Cuhaci, and D. Roscoe,
“Circularly polarized dielectric resonator antenna,”
Electronics Letters, Vol. 30, No. 17, pp. 1361-1362, Aug.
1994.
[12] M. T. K. Tam and R. D. Murch, “Circularly polarized
circular sector dielectric resonator antenna,” IEEE
Transactions on Antennas and Propagation, Vol. 48, No.
1, pp. 126-128, Jan. 2000.
[13] R. A. Kranenburg, S. A. Long, and J. T. Williams,
“Coplanar waveguide excitation of dielectric resonator
antennas,” IEEE Transactions on Antennas and
Propagation, Vol. 39, No. 1, pp. 119-122, Jan. 1991.
[14] Y. M. M. Antar, M. S. Al Salameh, and G. Seguin,
“Coplanar waveguide fed dielectric resonator antenna,”
Proceedings of Progress in Electromagnetics Research
Symposium PIERS2000, Cambridge, Massachusetts, USA,
5-14 July 2000.
[15] M. S. Al Salameh, Y. M. M. Antar, and G. Seguin,
“Coplanar-waveguide-fed slot-coupled rectangular
dielectric resonator antenna,” IEEE Transactions on
Antennas and Propagation, Vol. 50, No. 10, pp. 1415-
1419, Oct. 2002.
[16] A. Petosa, A. Ittipiboon, Y. M. M. Antar, D. Roscoe, and
M. Cuhaci, “Recent advances in dielectric resonator
antenna technology,” Antennas and Propagation
Magazine, pp. 35-48, June 1998.
[17] O. Lehmus, J. Ollikainen, and P. Vainikainen,
“Characteristics of half-volume DRAs with different
permittivities,” Proceedings of IEEE Antennas and
Propagation Society International Symposium, Vol. 1, pp.
22-25, Orlando, FL, USA, 11-16 July 1999.
[18] Dr. S. V. A. V. Prasad and Anshu Thakur, "Mathematical
Modeling of Circular Dielectric Resonator Antenna for
Applications in High Speed Real-time Communication
Systems", International Journal of Engineering Research
and Applications, Vol. 5, Issue 2 (Part 3), pp. 33-37, Feb.
2015
[19] R. Mongia and A. Ittipiboon, “Theoretical and
experimental investigations on rectangular dielectric
resonator antennas,” IEEE Transactions on Antennas and
Propagation, Vol. 45, No. 9, pp. 1348-1356, Sept. 1997.

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Mathematical Analysis of Half Volume DRA with Performance Evaluation for High Speed System Applications

  • 1. International Journal on Recent and Innovation Trends in Computing and Communication ISSN: 2321-8169 Volume: 5 Issue: 12 235 - 238 ______________________________________________________________________________________ 235 IJRITCC | December 2017, Available @ http://www.ijritcc.org _______________________________________________________________________________________ Mathematical Analysis of Half Volume DRA with Performance Evaluation for High Speed System Applications Dr. S. V. A. V. Prasad# and Anshu Thakur* # Dean (Research, Development & Industrial Consultancy), Lingaya's University, Faridabad, Haryana, India * Research Scholar, Dept. Of ECE, Lingaya’s University, Faridabad, Haryana, India Abstract:- A novel efficient design analysis has been proposed for a reduced-size dielectric resonator antenna (DRA). This has been done by using half-volume resonator with short-circuited plane of symmetry. The design serves as a new configuration of planar antenna, thus making integration of active devices easier. The antenna shows remarkable performance, having low cross-polarization levels and reasonably well radiation patterns. The antenna design has been simulated using a new analytical framework created in MATLAB giving accurate measurement details. Keywords: Dielectric Resonator Antenna, Half-volume, High Speed Systems, Simulation Framework. __________________________________________________*****_________________________________________________ 1. Introduction The ever increasing demand for high speed and reliable communication systems have pushed the development of microwave and mm-wave systems which requires new and improved antennas with outstanding performance characteristics. Moreover, many base stations and new communication systems require compact and cost-effective components. Since about 1970’s, dielectric resonators have helped achieve the miniaturization of active and passive microwave components, such as oscillators and filters [1, 2] and have proved to be one of the driving forces behind advancement of communication systems such as Spatial Division Multiple Access. A lot of extensive work has been done on microstrip-fed DRAs [1]-[8] and probe-fed DRAs [9]-[12], but only limited attempts have been made at designing DRAs using a common analytical approach. New feed mechanisms like CPW has been shown to be used to excite cylindrical resonator antenna [13]. There have been some recent developments also which shows that the CPW is quite effective as a mechanism for excitation for the rectangular type DRA [14]-[15]. There are also research on half-volume DRA which is fed by microstrip line. [16]-[17]. It is the intent of this paper to propose a reduced size dielectric resonator antenna which is excited by coplanar waveguide through an aperture in the ground plane. The antenna design is optimized, using a new analytical framework created by authors of this paper in [18], to improve the coupling and performance parameters of the antenna. The design proposed in this paper has the clear advantage of fabrication ease owing to its single process of metallization and dielectric layers. Detailed theoretical analysis is carried out for performance evaluation using the new analytical framework created in MATLAB. The gain, return loss, and radiation pattern of the proposed antenna are shown and analyzed. The choice of MATLAB as the design of analytical framework is primarily governed by the fact that it is highly capable in solving partial differential equations derived from the original Maxwell equations using which we have created this simulation framework. 2. Mathematical Equations of Analysis As emphasized earlier, a new simulation framework has been developed to assess the performance of the DRA derived from the Maxwell's equations. Based on the different modes expected to be present in the CPW feed and antenna characteristics, equations for different resonant frequencies as a function of height has been derived. This gives an important insight regarding the geometric parameters of the antenna that can be suitably chosen according to the equation for optimal performance. The resonant frequency as a function of height for different permittivities for TE01 mode is :- ... (1) Corresponding to this equation, the results have been plotted and shown in figure below :- Figure 1: Graph of resonant frequencies for TE01 mode
  • 2. International Journal on Recent and Innovation Trends in Computing and Communication ISSN: 2321-8169 Volume: 5 Issue: 12 235 - 238 ______________________________________________________________________________________ 236 IJRITCC | December 2017, Available @ http://www.ijritcc.org _______________________________________________________________________________________ Similarly, the equation for resonant frequency as a function of height for different permittivities for TM01 mode is :- ... (2) Corresponding to this equation, the results have been plotted and has been shown in figure below :- Figure 2: Graph of resonant frequencies for TM01 mode The equation for resonant frequency as a function of height for different permittivities for HE11 mode is :- (3...) The graph of this equation happens to be the one shown below :- Figure 3: Graph of resonant frequencies for HE11 mode Using the above equations and selection of optimal resonant frequency leads to direct selection of dielectric material with certain permittivity for creating the DRA with required characteristics. 3. Design and Geometry of the Antenna The design and the geometry of the antenna has been decided in a manner that leads to maximum performance characteristics specifically for real-time high speed communication systems. The top view and the corresponding side view of the dielectric resonator antenna is shown in the figure below for greater understanding :- Figure 4: Top view and side view of the DRA The DRA has a radius of R = 15 mm, height h = 10.5 mm and a permittivity of εdra = 31.5. The coaxial line connecting the CPW feed is at a distance of 9 mm from the center. The DRA is printed on a substrate of permittivity 2.2 and thickness 3.2 mm. The metallic via have a radius a=2mm, and they are disposed with the same transversal period and the same radial period Pr2=23.6mm. In this structure, no back conductor for the substrate was used in order to reduce the adverse effects of the leaky waves that might otherwise degrade the performance of the antenna. However, the dimensions are chosen such that the radiation under the substrate is insignificant. The entire design of the antenna was created in HFSS software and accordingly a sample simulation was performed to verify the design. During simulation the practical performance characteristics of the antenna is inferred which is later used to simulate within the analytical framework created in MATLAB. The result obtained is then correlated with the HFSS software for accurate validation of the analytical method.
  • 3. International Journal on Recent and Innovation Trends in Computing and Communication ISSN: 2321-8169 Volume: 5 Issue: 12 235 - 238 ______________________________________________________________________________________ 237 IJRITCC | December 2017, Available @ http://www.ijritcc.org _______________________________________________________________________________________ 4. Simulation Results The simulation was performed using MATLAB. A combination of PDE toolbox and scratch coding was used to come up with graphs of various performance metrics. In figure 5 below, the return loss of the proposed antenna is shown. Figure 5: Simulated return loss of the proposed antenna Note that the return loss is around –35 dB at resonance. This indicates that most of the input power at the feedline is absorbed by the resonator which is then radiated into the surrounding space. The graph shows two scenarios that is with etched background plane (EBG) and without EBG to provide greater insight into the working characteristics of the antenna. The graph for the gain of the antenna is shown in the figure below :- Figure 6: Simulated gain of the proposed antenna As can be seen that the maximum gain of the antenna remains constant across a range of operational frequency which is highly desired characteristic in any antenna. The simulated radiation pattern observed by plotting the graph is shown in the figure below :- Figure 7: Simulated radiation pattern of the proposed antenna The simulated radiation patterns in both the E- and H- planes are shown. It was also noted that the cross polarization levels were low. The radiation is mostly in the resonator direction and negligible radiation is directed below the substrate. The interference between the antenna radiation pattern and the far-field pattern of the diffracted waves results in the measured co-polarized component ripples around the simulated component. The E-plane suffers from greater diffraction than the H-plane, due to the fact that the space wave in the vicinity of the truncated ground plane is stronger in the E-plane. In consequence, the diffracted fields are also stronger in the E-plane. All of these simulation results show and validate the efficacy of the analytical framework developed to simulate and verify the performance characteristics of any DRA using relevant mathematical modeling. 5. Conclusions In this paper, a new analytical framework using mathematical modeling has been proposed that led to accurate design of DRA fed via CPW. Detailed performance evaluation of the proposed antenna was carried out and it was conclusively shown how the new analytical framework leads to design criteria which allows one to select appropriate dielectric material for the DRA giving better results. The antenna shows good performance in terms of low cross-polarization levels, matching to the feeding structure, and low back radiation. References [1] R. A. Kranenburg and S. A. Long, “Microstrip transmission line excitation of dielectric resonator antennas,” Electronics Letters, Vol. 24, pp. 1156-1157, 1988. [2] J. T. St. Martin, Y. M. M. Antar, A. A. Kishk, A. Ittipiboon, and M. Cuhaci, “Dielectric resonator antenna using aperture coupling,“ Electronics Letters, Vol. 26, No. 24, pp. 2015-2016, Nov. 1990.
  • 4. International Journal on Recent and Innovation Trends in Computing and Communication ISSN: 2321-8169 Volume: 5 Issue: 12 235 - 238 ______________________________________________________________________________________ 238 IJRITCC | December 2017, Available @ http://www.ijritcc.org _______________________________________________________________________________________ [3] A. Ittipiboon, R. K. Mongia, Y. M. M. Antar, P. Bhartia, and M. Cuhaci, “Aperture fed rectangular and triangular dielectric resonators for use as magnetic dipole antennas,” Electronics Letters, Vol. 29, No. 23, pp. 2001-2002, Nov. 1993. [4] G. D. Loos and Y. M. M. Antar, “A new aperture-coupled rectangular dielectric resonator antenna array,” Microwave and Optical Technology Letters, Vol. 7, No. 14, pp. 642- 644, Oct. 1994. [5] A. A. Kishk, A. Ittipiboon, Y. M. M. Antar, and M. Cuhaci, “Slot excitation of the dielectric disk radiator,” IEEE Transactions on Antennas and Propagation, Vol. 43, No. 2, pp. 198-201, Feb. 1995. [6] M. G. Keller, D. J. Roscoe, M. B. Oliver, R. K. Mongia, Y. M. M. Antar, and A. Ittipiboon, “Active aperture-coupled rectangular dielectric resonator antenna,” IEEE Microwave and Guided Wave Letters, Vol. 5, No. 11, pp. 376-378, Nov. 1995. [7] Y. M. M. Antar and Z. Fan, “Theoretical investigation of aperture-coupled rectangular dielectric resonator antenna,” IEE Proc.-Microw. Antennas Propag., Vol. 143, No. 2, pp. 113-118, Apr. 1996. [8] C.-Y. Huang, J.-Y. Wu, and K.-L. Wong, “Cross-slot- coupled microstrip antenna and dielectric resonator antenna for circular polarization,” IEEE Transactions on Antennas and Propagation, Vol. 47, No. 4, pp. 605-609, Apr. 1999. [9] S. A. Long, M. W. McAllister, and L. C. Shen, “The resonant cylindrical dielectric cavity antenna,” IEEE Transactions on Antennas and Propagation, Vol. 31, pp. 406-412, 1983. [10] K. W. Leung, K. M. Luk, and K. Y. A. Lai, “Theory and experiment of a coaxial probe fed hemispherical dielectric resonator antenna,” IEEE Transactions on Antennas and Propagation, Vol. 41, No. 6, pp. 1390-1398, 1993. [11] R. K. Mongia, A. Ittipiboon, M. Cuhaci, and D. Roscoe, “Circularly polarized dielectric resonator antenna,” Electronics Letters, Vol. 30, No. 17, pp. 1361-1362, Aug. 1994. [12] M. T. K. Tam and R. D. Murch, “Circularly polarized circular sector dielectric resonator antenna,” IEEE Transactions on Antennas and Propagation, Vol. 48, No. 1, pp. 126-128, Jan. 2000. [13] R. A. Kranenburg, S. A. Long, and J. T. Williams, “Coplanar waveguide excitation of dielectric resonator antennas,” IEEE Transactions on Antennas and Propagation, Vol. 39, No. 1, pp. 119-122, Jan. 1991. [14] Y. M. M. Antar, M. S. Al Salameh, and G. Seguin, “Coplanar waveguide fed dielectric resonator antenna,” Proceedings of Progress in Electromagnetics Research Symposium PIERS2000, Cambridge, Massachusetts, USA, 5-14 July 2000. [15] M. S. Al Salameh, Y. M. M. Antar, and G. Seguin, “Coplanar-waveguide-fed slot-coupled rectangular dielectric resonator antenna,” IEEE Transactions on Antennas and Propagation, Vol. 50, No. 10, pp. 1415- 1419, Oct. 2002. [16] A. Petosa, A. Ittipiboon, Y. M. M. Antar, D. Roscoe, and M. Cuhaci, “Recent advances in dielectric resonator antenna technology,” Antennas and Propagation Magazine, pp. 35-48, June 1998. [17] O. Lehmus, J. Ollikainen, and P. Vainikainen, “Characteristics of half-volume DRAs with different permittivities,” Proceedings of IEEE Antennas and Propagation Society International Symposium, Vol. 1, pp. 22-25, Orlando, FL, USA, 11-16 July 1999. [18] Dr. S. V. A. V. Prasad and Anshu Thakur, "Mathematical Modeling of Circular Dielectric Resonator Antenna for Applications in High Speed Real-time Communication Systems", International Journal of Engineering Research and Applications, Vol. 5, Issue 2 (Part 3), pp. 33-37, Feb. 2015 [19] R. Mongia and A. Ittipiboon, “Theoretical and experimental investigations on rectangular dielectric resonator antennas,” IEEE Transactions on Antennas and Propagation, Vol. 45, No. 9, pp. 1348-1356, Sept. 1997.