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Modified Sierpinski Fractal Circular Antenna for
Wireless Automotive Applications
A.MADHUSUDANAN
M.TECH SENSOR
SYSTEM TECHNLOGY
VIT UNIVERSITY,
VELLORE -632014.
a.madhusudanan2016@vit
student.ac.in
ANUPAMA SARKAR
M.TECH SENSOR
SYSTEM TECHNLOGY
VIT UNIVERSITY,
VELLORE -632014.
anupamasarkar2012@
gmail.com
S.PRABHAKARAN
M.TECH SENSOR
SYSTEM TECHNLOGY
VIT UNIVERSITY,
VELLORE -632014
prabhakaran.s2016@vit
student.ac.in
GUIDE:
DR. ELIZABETH RUFUS
PROFESSOR, SENSE
VIT UNIVERSITY,
VELLORE -632014
elizabethrufus@vit.ac.in
Abstractโ€” In this paper, a novel structure of a planar monopole
antenna for wireless automotive applications is proposed. The
structure is based on the complementary Sierpinski triangle
surrounded by circular patch. The antenna has been modified
based on the iteration of triangles to improve the operating
bandwidth. The simulated results show good agreement with
the wideband characteristic. The proposed antenna was
designed to effectively support WLAN applications, at 2.4GHz.
The performance properties of the antenna such as return losses,
radiation patterns were verified by simulation
Key W0rdsโ€” SIERPINSKI, BANDWIDTH, WLAN.
I.)INTRODUCTION
In recent years, with widespread deployment of wireless
communications, especially in automotive vehicle to vehicle
communication, low cost, multiband antenna has increased
rapidly. WLAN are designed to operate in the 2.4GHz (2.4-
2.48GHz). The micro strip antenna has been widely analysed,
studied and developed. The micro strip antenna has the
characteristics of small size, light weight and low fabrication
cost. The fractals antennas are adopted for size reduction and
multiband/wideband characteristics. The size reduction is
mainly due to the self-similarity property of fractal geometry
and made of many copies of themselves with different scale
factors. The space filling characteristics of fractal antenna result
in increasing electrical length of the antenna. The
miniaturization effect of the fractal antenna is because of the
lengthening of the surface current line. The electrical length of
the antenna is increased and the structure can be miniaturized.
A lot of fractal geometries are available but only a limited
number are used in the design of micro strip antenna. One of
them is the Sierpinski Carpet geometry. The construction of
many ideal Fractal shapes is usually carried out by applying an
infinite number of times an iterative algorithm such as the
multiple reduction copy machine (MRCM) algorithm. In such
iterative procedure, an initial structure called generator is
replicated many times at different scales, positions and
directions, to grow the final Fractal structure. Fractal's antennas
are widely preferred for wireless communication systems as
they are of small size, light weight, low profile, low cost, and
are easy to fabricate and assemble.
The Sierpinski triangle geometry drew the attention of
researchers as it is smaller than other patch geometries .The
design of Sierpinski starts with a triangle with an operating
frequency in between 2.3GHz to 2.5 GHz at various iterations.
Two different iterations of triangular patch are compared in terms
of their return loss and bandwidths
.
II.)PROPOSED ANTENNA DESIGN
Classical Sierpinski triangle is having the scale factor of 2. This
is given by
ฮด =hn/hn+1 (1)
Where the n represent the iteration number and h represent the
height of the triangle. The antenna is fed by micro strip line, the
centre micro strip line (Lgร—Wg) is having 50ฮฉ impedance. It is
calculated using the equation (2) and (3).
โˆˆ ๐‘’๐‘“๐‘“ =
โˆˆ๐‘Ÿ+1
2
+
โˆˆ๐‘Ÿ+1
2
[
1
โˆš1+12
โ„Ž
๐‘ค
] (2)
๐‘๐‘œ = ๐‘๐‘–๐‘› ๐‘๐‘œ๐‘ 2
(
๐œ‹๐‘‘
๐ฟ๐‘
) (3)
Where Zo = 50 ohms and Zin = 1/G1
๐บ1 = {1/90 (
๐‘ค
ฮปo
) 2
}
๐‘ค โ‰ช ฮปo
๐บ1 = {1/120 (
๐‘ค
ฮปo
)
1
}
๐‘ค โ‰ซ ฮปo
Where โˆˆ ๐‘’๐‘“๐‘“ = ๐‘’๐‘“๐‘“๐‘’๐‘๐‘ก๐‘–๐‘ฃ๐‘’ ๐‘‘๐‘–๐‘’๐‘™๐‘’๐‘๐‘ก๐‘Ÿ๐‘–๐‘ ๐‘๐‘œ๐‘›๐‘ ๐‘ก๐‘Ž๐‘›๐‘ก
โˆˆ ๐‘Ÿ = ๐‘‘๐‘–๐‘’๐‘™๐‘๐‘ก๐‘Ÿ๐‘–๐‘ ๐‘๐‘œ๐‘›๐‘ ๐‘ก๐‘Ž๐‘›๐‘ก ๐‘œ๐‘“ ๐‘ ๐‘ข๐‘๐‘ ๐‘ก๐‘Ž๐‘ก๐‘’
โ„Ž = โ„Ž๐‘’๐‘–๐‘”โ„Ž๐‘ก ๐‘œ๐‘“ ๐‘กโ„Ž๐‘’ ๐‘ ๐‘ข๐‘๐‘ ๐‘ก๐‘Ÿ๐‘Ž๐‘ก๐‘’
๐‘ค = ๐‘ค๐‘–๐‘‘๐‘กโ„Ž ๐‘œ๐‘“ ๐‘กโ„Ž๐‘’ ๐‘๐‘Ž๐‘ก๐‘โ„Ž
๐‘๐‘œ = ๐‘œ๐‘ข๐‘ก๐‘๐‘ข๐‘ก ๐‘–๐‘š๐‘๐‘’๐‘‘๐‘Ž๐‘›๐‘๐‘’
๐‘๐‘–๐‘› = ๐‘–๐‘›๐‘๐‘ข๐‘ก ๐‘–๐‘š๐‘๐‘’๐‘‘๐‘Ž๐‘›๐‘๐‘’
๐‘‘ = ๐‘“๐‘’๐‘’๐‘‘ ๐‘๐‘œ๐‘–๐‘›๐‘ก
๐ฟ๐‘ = ๐‘™๐‘’๐‘›๐‘”๐‘กโ„Ž ๐‘œ๐‘“ ๐‘กโ„Ž๐‘’ ๐‘๐‘Ž๐‘ก๐‘โ„Ž
๐บ1 = ๐‘’๐‘“๐‘“๐‘’๐‘๐‘ก๐‘–๐‘ฃ๐‘’ ๐‘๐‘œ๐‘›๐‘‘๐‘ข๐‘๐‘ก๐‘Ž๐‘›๐‘๐‘’
ฮปo = resonating wavelength
A circular microstrip patch can be designed by using following
equation with specified information including dielectric
constant of substrate (โˆˆ ๐‘Ÿ), resonant frequency (fr) & height of
the substrate (h).
The radius (a) of circular micro strip patch is
Where
Here circular patch antenna has been designed and simulated at
2.4GHZ resonant frequency. The original gasket is constructed
by removing a central triangle from circle with radius 28 mm.
The third iteration of fractal antenna has been constructed by
inscribing the Triangle makes three copies and positioned so
that each triangle touches the Midpoint of each side of large
triangle as shown in fig1. Fifth iteration are achieved in this
manner shown in the Fig.2. This antenna has been fed with the
micro strip feed with feed point d=24.456mm. Alumina (96%)
loss free is used as substrate with dielectric constant ฮตr = 9.4.
The length and width of the patch is taken to be 60mm & 48
mm respectively. The substrate height is selected to be 1.60
mm. The design specifications & physical dimensions are listed
in Table 1.
Table 1
Fig 1: proposed antenna design-third iteration
Fig 2: proposed antenna design-fifth iteration
III.) RESULTS & ANALYSIS
The return loss of antenna at 3rd
and 5th
iteration is shown in the
figure 3 and 4.The third iteration of the antenna having
bandwidth of 0.01GHZ with return loss is less than -12dB . The
fifth iteration of the antenna having bandwidth of 0.03GHZ with
return loss is less than -15dB return loss is less than -15dB which
show good impedance matching. The operating frequencies of
the antenna suitable for many wireless communication
applications such WiMAX (2.11โ€“2.2), WLAN (2.4) GHz.
Fig 3: S parameter plot with return loss for antenna with 3rd
iteration
Fig 4: S parameter plot with return loss for antenna with 5th
iteration
The polar radiation patterns of antenna at third
iteration and fifth iteration is described in the Figure 5 and 6.
The main lobe direction and magnitude have been mention
under each plot. The polar radiation patterns of antenna at third
iteration show that at resonance frequency 2.4GHz, the main
lobe magnitude and direction have 0.561 dBi and 49 deg. The
3dB angular width which is also known as half power beam
width in the elevation plane has 61.6 deg. The half power beam
width is shown by two thin lines which show that when the
directivity increases the angle between the two lines decreases.
Antenna at fifth iteration with same resonance frequency shows
the main lobe magnitude and direction have 4.83 dBi and 22
respectively. The 3dB angular width which is also known as
half power beam width in the elevation plane has 116.5 deg.
Fig 5: polar plot for antenna with 3rd
iteration
Fig 6: polar plot for antenna with 5th
iteration
The 3-D radiation patterns of antenna at third iteration and fifth
iteration is shown in the Figure 7 and 8.The Directivity and Total
radiation efficiency have been mention under each plot. The 3-D
radiation patterns of antenna at third iteration show that at
resonance frequency 2.4GHz, the directivity and total radiation
efficiency have 4.833 dBi and-24.31 dB. Similarly radiation
patterns of antenna at fifth iteration show that at resonance
frequency 2.4GHz, the directivity and total radiation efficiency
have 6.309 dBi and -19.63 dB. Here the directivity of antenna
increases by increasing number of fractal structures in
iterations.so it can be used for high directional applications.
Fig 7: 3-D Radiation Pattern for antenna with 3rd
iteration
Fig 8: 3-D Radiation Pattern for antenna with 5th
Iteration
IV.) CONCLUSION
The present work has been carried out for the 3rd and 5th
iteration. From the above discussions it can be concluded that
on increasing the number of iterations the return loss and gain
of antenna are also increased. Also it can be concluded that the
self-similarity in the structure for the 3rd and 5th iteration to
possess shift in centre frequency, i.e., multiband. These
multiband antenna can cover the frequency bands of
WLAN/WIMAX applications. The designed antenna resonates
in (2.4- 2.6GHz) frequency band and can be used in Vehicle to
vehicle (V2V) and vehicle to infrastructure (V2I)
communications. With V2V communications, there are a large
number of signals being passed back and forth. The common
number is 1,000 to 1,500 received messages per second from
cars within a near proximity (roughly 100m). Table 2 shows the
comparative results of antenna for 3rd
and 5th
iterations.
S.NO Iteration Return
Loss
Gain VSWR Directivity
1.) Third
iteration
-11.63 - 3.550 1.723 4.833
2.) Fifth
iteration
-13.73 2.505 1.53 6.039
Table 2: Comparative Table of Modified Sierpinski Fractal
Circular Patch Antenna
V.) REFERENCES
1) Cruz Angel Figueroa-Torres, Jose Luis Medina-
Monroy, Humberto Lobato-Morales, Ricardo Arturo
Chavez-Perez, and Andres Calvillo-Tellez, โ€œA Novel
Fractal Antenna Based On The Sierpinski Structure
For Super Wide-Band Applications (2016)โ€.
2) Rowdra Ghatak, Anirban Karmakar, Balaka Biswas
and D R Poddar, โ€œInscribed Gasket Fractal Circular
Monopole Antenna for UWB Applicationโ€, 1st
International Conference on Emerging Technology
Trends in Electronics, Communication and
Networking (2012).
3) Yogesh Kumar Choukiker, S K Behera, โ€œCPW-Fed
Compact Multiband Sierpinski Triangle Antennaโ€,
IEEE INDICON,CALCUTTA, 17-19 DEC, 2010.
4) M. Naser-Moghadasi, R.A. Sadeghzadeh, T. Sedghi, T.
Aribi, and B.S. Virdee, UWB CPW-Fed Fractal Patch
Antenna With Band- Notched Function Employing
Folded T-Shaped Element, IEEE Antennas Wireless
Propagett 12 (2013), 504โ€“507.
5) S. Singhal, P. Singh, and A. Singh, Asymmetrically
CPW-FED Octagonal Sierpinski UWB fractal
Antenna, Microwave Opt Technol Lett 58 (2016),
1738โ€“1745.
6) M. Manohar, R. Kshetrimayum, and A. Gogoi, A
compact printed triangular monopole antenna for
ultrawideband applications, Microwave Opt Technol
Lett 56 (2014), 1155โ€“1159.
7) K.R. Chen, C.Y. Sim, and J.S. Row, A Compact
Monopole Antenna for Super Wideband Applications,
IEEE Antennas Wireless Propag Lett 10 (2011), 488โ€“
491.
8) M. Ding, R. Jin, J. Geng, Q. Wu, and W. Wang, Design
of a CPW fed Ultra Wideband Crown Circular Fractal
Antenna, Antennas Propag Soc Int Symp, Albuquerque,
NM (2006), 2049โ€“2052.
9) E. Lule, and T. Babij, Koch Island Fractal Ultra
Wideband Dipole Antenna, IEEE Antennas Propag Soc
Int Symp (2004), 2516โ€“2519.
10) M.G. Fekadu, and S.N. Sinha, UWB fractal slot antenna
designs, IEEE Int Conf Microwaves Commun Antennas
Electron Syst (2011),1โ€“4.
11) R. Liu and W. He, A Novel Sierpinski Fractal Antenna
for Wireless Application, Int Conf Comput Inf Sci
(2013), 1347โ€“1348.

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Sierpinski fractal circular antenna

  • 1. Modified Sierpinski Fractal Circular Antenna for Wireless Automotive Applications A.MADHUSUDANAN M.TECH SENSOR SYSTEM TECHNLOGY VIT UNIVERSITY, VELLORE -632014. a.madhusudanan2016@vit student.ac.in ANUPAMA SARKAR M.TECH SENSOR SYSTEM TECHNLOGY VIT UNIVERSITY, VELLORE -632014. anupamasarkar2012@ gmail.com S.PRABHAKARAN M.TECH SENSOR SYSTEM TECHNLOGY VIT UNIVERSITY, VELLORE -632014 prabhakaran.s2016@vit student.ac.in GUIDE: DR. ELIZABETH RUFUS PROFESSOR, SENSE VIT UNIVERSITY, VELLORE -632014 elizabethrufus@vit.ac.in Abstractโ€” In this paper, a novel structure of a planar monopole antenna for wireless automotive applications is proposed. The structure is based on the complementary Sierpinski triangle surrounded by circular patch. The antenna has been modified based on the iteration of triangles to improve the operating bandwidth. The simulated results show good agreement with the wideband characteristic. The proposed antenna was designed to effectively support WLAN applications, at 2.4GHz. The performance properties of the antenna such as return losses, radiation patterns were verified by simulation Key W0rdsโ€” SIERPINSKI, BANDWIDTH, WLAN. I.)INTRODUCTION In recent years, with widespread deployment of wireless communications, especially in automotive vehicle to vehicle communication, low cost, multiband antenna has increased rapidly. WLAN are designed to operate in the 2.4GHz (2.4- 2.48GHz). The micro strip antenna has been widely analysed, studied and developed. The micro strip antenna has the characteristics of small size, light weight and low fabrication cost. The fractals antennas are adopted for size reduction and multiband/wideband characteristics. The size reduction is mainly due to the self-similarity property of fractal geometry and made of many copies of themselves with different scale factors. The space filling characteristics of fractal antenna result in increasing electrical length of the antenna. The miniaturization effect of the fractal antenna is because of the lengthening of the surface current line. The electrical length of the antenna is increased and the structure can be miniaturized. A lot of fractal geometries are available but only a limited number are used in the design of micro strip antenna. One of them is the Sierpinski Carpet geometry. The construction of many ideal Fractal shapes is usually carried out by applying an infinite number of times an iterative algorithm such as the multiple reduction copy machine (MRCM) algorithm. In such iterative procedure, an initial structure called generator is replicated many times at different scales, positions and directions, to grow the final Fractal structure. Fractal's antennas are widely preferred for wireless communication systems as they are of small size, light weight, low profile, low cost, and are easy to fabricate and assemble. The Sierpinski triangle geometry drew the attention of researchers as it is smaller than other patch geometries .The design of Sierpinski starts with a triangle with an operating frequency in between 2.3GHz to 2.5 GHz at various iterations. Two different iterations of triangular patch are compared in terms of their return loss and bandwidths . II.)PROPOSED ANTENNA DESIGN Classical Sierpinski triangle is having the scale factor of 2. This is given by ฮด =hn/hn+1 (1) Where the n represent the iteration number and h represent the height of the triangle. The antenna is fed by micro strip line, the centre micro strip line (Lgร—Wg) is having 50ฮฉ impedance. It is calculated using the equation (2) and (3). โˆˆ ๐‘’๐‘“๐‘“ = โˆˆ๐‘Ÿ+1 2 + โˆˆ๐‘Ÿ+1 2 [ 1 โˆš1+12 โ„Ž ๐‘ค ] (2) ๐‘๐‘œ = ๐‘๐‘–๐‘› ๐‘๐‘œ๐‘ 2 ( ๐œ‹๐‘‘ ๐ฟ๐‘ ) (3) Where Zo = 50 ohms and Zin = 1/G1 ๐บ1 = {1/90 ( ๐‘ค ฮปo ) 2 } ๐‘ค โ‰ช ฮปo ๐บ1 = {1/120 ( ๐‘ค ฮปo ) 1 } ๐‘ค โ‰ซ ฮปo Where โˆˆ ๐‘’๐‘“๐‘“ = ๐‘’๐‘“๐‘“๐‘’๐‘๐‘ก๐‘–๐‘ฃ๐‘’ ๐‘‘๐‘–๐‘’๐‘™๐‘’๐‘๐‘ก๐‘Ÿ๐‘–๐‘ ๐‘๐‘œ๐‘›๐‘ ๐‘ก๐‘Ž๐‘›๐‘ก โˆˆ ๐‘Ÿ = ๐‘‘๐‘–๐‘’๐‘™๐‘๐‘ก๐‘Ÿ๐‘–๐‘ ๐‘๐‘œ๐‘›๐‘ ๐‘ก๐‘Ž๐‘›๐‘ก ๐‘œ๐‘“ ๐‘ ๐‘ข๐‘๐‘ ๐‘ก๐‘Ž๐‘ก๐‘’ โ„Ž = โ„Ž๐‘’๐‘–๐‘”โ„Ž๐‘ก ๐‘œ๐‘“ ๐‘กโ„Ž๐‘’ ๐‘ ๐‘ข๐‘๐‘ ๐‘ก๐‘Ÿ๐‘Ž๐‘ก๐‘’ ๐‘ค = ๐‘ค๐‘–๐‘‘๐‘กโ„Ž ๐‘œ๐‘“ ๐‘กโ„Ž๐‘’ ๐‘๐‘Ž๐‘ก๐‘โ„Ž ๐‘๐‘œ = ๐‘œ๐‘ข๐‘ก๐‘๐‘ข๐‘ก ๐‘–๐‘š๐‘๐‘’๐‘‘๐‘Ž๐‘›๐‘๐‘’ ๐‘๐‘–๐‘› = ๐‘–๐‘›๐‘๐‘ข๐‘ก ๐‘–๐‘š๐‘๐‘’๐‘‘๐‘Ž๐‘›๐‘๐‘’
  • 2. ๐‘‘ = ๐‘“๐‘’๐‘’๐‘‘ ๐‘๐‘œ๐‘–๐‘›๐‘ก ๐ฟ๐‘ = ๐‘™๐‘’๐‘›๐‘”๐‘กโ„Ž ๐‘œ๐‘“ ๐‘กโ„Ž๐‘’ ๐‘๐‘Ž๐‘ก๐‘โ„Ž ๐บ1 = ๐‘’๐‘“๐‘“๐‘’๐‘๐‘ก๐‘–๐‘ฃ๐‘’ ๐‘๐‘œ๐‘›๐‘‘๐‘ข๐‘๐‘ก๐‘Ž๐‘›๐‘๐‘’ ฮปo = resonating wavelength A circular microstrip patch can be designed by using following equation with specified information including dielectric constant of substrate (โˆˆ ๐‘Ÿ), resonant frequency (fr) & height of the substrate (h). The radius (a) of circular micro strip patch is Where Here circular patch antenna has been designed and simulated at 2.4GHZ resonant frequency. The original gasket is constructed by removing a central triangle from circle with radius 28 mm. The third iteration of fractal antenna has been constructed by inscribing the Triangle makes three copies and positioned so that each triangle touches the Midpoint of each side of large triangle as shown in fig1. Fifth iteration are achieved in this manner shown in the Fig.2. This antenna has been fed with the micro strip feed with feed point d=24.456mm. Alumina (96%) loss free is used as substrate with dielectric constant ฮตr = 9.4. The length and width of the patch is taken to be 60mm & 48 mm respectively. The substrate height is selected to be 1.60 mm. The design specifications & physical dimensions are listed in Table 1. Table 1 Fig 1: proposed antenna design-third iteration Fig 2: proposed antenna design-fifth iteration III.) RESULTS & ANALYSIS The return loss of antenna at 3rd and 5th iteration is shown in the figure 3 and 4.The third iteration of the antenna having bandwidth of 0.01GHZ with return loss is less than -12dB . The fifth iteration of the antenna having bandwidth of 0.03GHZ with return loss is less than -15dB return loss is less than -15dB which show good impedance matching. The operating frequencies of the antenna suitable for many wireless communication applications such WiMAX (2.11โ€“2.2), WLAN (2.4) GHz. Fig 3: S parameter plot with return loss for antenna with 3rd iteration
  • 3. Fig 4: S parameter plot with return loss for antenna with 5th iteration The polar radiation patterns of antenna at third iteration and fifth iteration is described in the Figure 5 and 6. The main lobe direction and magnitude have been mention under each plot. The polar radiation patterns of antenna at third iteration show that at resonance frequency 2.4GHz, the main lobe magnitude and direction have 0.561 dBi and 49 deg. The 3dB angular width which is also known as half power beam width in the elevation plane has 61.6 deg. The half power beam width is shown by two thin lines which show that when the directivity increases the angle between the two lines decreases. Antenna at fifth iteration with same resonance frequency shows the main lobe magnitude and direction have 4.83 dBi and 22 respectively. The 3dB angular width which is also known as half power beam width in the elevation plane has 116.5 deg. Fig 5: polar plot for antenna with 3rd iteration Fig 6: polar plot for antenna with 5th iteration The 3-D radiation patterns of antenna at third iteration and fifth iteration is shown in the Figure 7 and 8.The Directivity and Total radiation efficiency have been mention under each plot. The 3-D radiation patterns of antenna at third iteration show that at resonance frequency 2.4GHz, the directivity and total radiation efficiency have 4.833 dBi and-24.31 dB. Similarly radiation patterns of antenna at fifth iteration show that at resonance frequency 2.4GHz, the directivity and total radiation efficiency have 6.309 dBi and -19.63 dB. Here the directivity of antenna increases by increasing number of fractal structures in iterations.so it can be used for high directional applications. Fig 7: 3-D Radiation Pattern for antenna with 3rd iteration Fig 8: 3-D Radiation Pattern for antenna with 5th Iteration
  • 4. IV.) CONCLUSION The present work has been carried out for the 3rd and 5th iteration. From the above discussions it can be concluded that on increasing the number of iterations the return loss and gain of antenna are also increased. Also it can be concluded that the self-similarity in the structure for the 3rd and 5th iteration to possess shift in centre frequency, i.e., multiband. These multiband antenna can cover the frequency bands of WLAN/WIMAX applications. The designed antenna resonates in (2.4- 2.6GHz) frequency band and can be used in Vehicle to vehicle (V2V) and vehicle to infrastructure (V2I) communications. With V2V communications, there are a large number of signals being passed back and forth. The common number is 1,000 to 1,500 received messages per second from cars within a near proximity (roughly 100m). Table 2 shows the comparative results of antenna for 3rd and 5th iterations. S.NO Iteration Return Loss Gain VSWR Directivity 1.) Third iteration -11.63 - 3.550 1.723 4.833 2.) Fifth iteration -13.73 2.505 1.53 6.039 Table 2: Comparative Table of Modified Sierpinski Fractal Circular Patch Antenna V.) REFERENCES 1) Cruz Angel Figueroa-Torres, Jose Luis Medina- Monroy, Humberto Lobato-Morales, Ricardo Arturo Chavez-Perez, and Andres Calvillo-Tellez, โ€œA Novel Fractal Antenna Based On The Sierpinski Structure For Super Wide-Band Applications (2016)โ€. 2) Rowdra Ghatak, Anirban Karmakar, Balaka Biswas and D R Poddar, โ€œInscribed Gasket Fractal Circular Monopole Antenna for UWB Applicationโ€, 1st International Conference on Emerging Technology Trends in Electronics, Communication and Networking (2012). 3) Yogesh Kumar Choukiker, S K Behera, โ€œCPW-Fed Compact Multiband Sierpinski Triangle Antennaโ€, IEEE INDICON,CALCUTTA, 17-19 DEC, 2010. 4) M. Naser-Moghadasi, R.A. Sadeghzadeh, T. Sedghi, T. Aribi, and B.S. Virdee, UWB CPW-Fed Fractal Patch Antenna With Band- Notched Function Employing Folded T-Shaped Element, IEEE Antennas Wireless Propagett 12 (2013), 504โ€“507. 5) S. Singhal, P. Singh, and A. Singh, Asymmetrically CPW-FED Octagonal Sierpinski UWB fractal Antenna, Microwave Opt Technol Lett 58 (2016), 1738โ€“1745. 6) M. Manohar, R. Kshetrimayum, and A. Gogoi, A compact printed triangular monopole antenna for ultrawideband applications, Microwave Opt Technol Lett 56 (2014), 1155โ€“1159. 7) K.R. Chen, C.Y. Sim, and J.S. Row, A Compact Monopole Antenna for Super Wideband Applications, IEEE Antennas Wireless Propag Lett 10 (2011), 488โ€“ 491. 8) M. Ding, R. Jin, J. Geng, Q. Wu, and W. Wang, Design of a CPW fed Ultra Wideband Crown Circular Fractal Antenna, Antennas Propag Soc Int Symp, Albuquerque, NM (2006), 2049โ€“2052. 9) E. Lule, and T. Babij, Koch Island Fractal Ultra Wideband Dipole Antenna, IEEE Antennas Propag Soc Int Symp (2004), 2516โ€“2519. 10) M.G. Fekadu, and S.N. Sinha, UWB fractal slot antenna designs, IEEE Int Conf Microwaves Commun Antennas Electron Syst (2011),1โ€“4. 11) R. Liu and W. He, A Novel Sierpinski Fractal Antenna for Wireless Application, Int Conf Comput Inf Sci (2013), 1347โ€“1348.