In this paper a novel band notch antenna in UWB
frequency range is designed using split rings. Split rings are
overlapped with designed monopole to give phi shape. The slit
gap gives band-notch operation from 5.1GHz to 6.29GHz and
from 4.94GHz to 5.91GHz for SPSSR and SPSCR antennas
respectively. Simulated and measured results are in good
agreement.
Phi shape uwb antenna with band notch characteristics
1. Engineering, Technology & Applied Science Research Vol. 8, No. 4, 2018, 3123-3127 3123
www.etasr.com Ajetrao & Dhande: Phi Shape UWB Antenna with Band Notch Characteristics
Phi Shape UWB Antenna with
Band Notch Characteristics
K. V. Ajetrao
Department of Electronics & Telecommunication Engineering
Dr. D. Y. Patil Institute of Technology
Pune, Maharashtra, India
kiran_ajetrao@rediffmail.com
A. P. Dhande
Department of Electronics & Telecommunication
Pune Institute of Computer Technology
Pune, Maharashtra, India
apdhande@pict.edu
Abstract—In this paper a novel band notch antenna in UWB
frequency range is designed using split rings. Split rings are
overlapped with designed monopole to give phi shape. The slit
gap gives band-notch operation from 5.1GHz to 6.29GHz and
from 4.94GHz to 5.91GHz for SPSSR and SPSCR antennas
respectively. Simulated and measured results are in good
agreement.
Keywords-monopole; split ring resonator; band-notch; UWB
antenna; VSWR
I. INTRODUCTION
For a wireless communication system, large bandwidth is
an important requirement. Although UWB antenna gives large
bandwidth of 7.7GHz (3.1GHz to 10.6GHz), it faces many
challenges of interference with existing systems in UWB range.
To avoid this interference with existing systems like WLAN,
HIPPERLAN, WiMAX, C-band satellite communication etc.,
band notch antennas are nowadays becoming popular and
necessary for communication. In this paper a novel band notch
antenna is designed by merging a monopole antenna with a
square or circular split ring resonator. This proposed antenna
shape looks like the Greek letter Phi (φ) hence is named as split
Phi shape square ring (SPSSR) antenna and split Phi shape
circular ring (SPSCR) antenna. Both antennas give single band
notch operation in UWB band. Monopole is designed at 3GHz.
The parameters for the SPSSR antenna are designed, optimized
and applied to the SPSCR antenna. It is found that both
antennas give the same response hence the same design can be
extended to any other shape as well. In proposed antennas, by
varying the split gap of rings, band notch frequency can be
tuned to the desired band. The length and width of split ring
resonator gives inductance, and the gap between two rings and
the slit gap of the rings gives the capacitance. The gap between
the rings and the slit gap is optimized to give UWB antenna
with notch band characteristics. At slit gap of 1.1mm the UWB
operation in with band notch at 5.87 and 5.47GHz is achieved
for SPSSR and SPSCR respectively.
Many antennas with band-notch characteristics are reported
in the literature. Band-notch characteristics are achieved by
inserting different slots in the radiating patch [1-3]. In [4, 5]
antennas with etching slots shapes such as H, M, W etc. slots in
the ground plane are reported. A band notch antenna by etching
a narrowband dual resonance fractal binary tree in the radiation
element of the conventional UWB antenna is reported in [6],
but the antenna manufacturing and structure are complex. The
band-notched characteristics are obtained by adding a stepped
impedance resonator (SIR) or a split ring resonator (SRR) on
the feed line or cutting slots in the ground plane [7, 8]. A band-
notch antenna is designed by etching a nested CSRR inside the
ground plane in [9]. Another technique to obtain band-notch
characteristics is by adding the parasitic elements in the form of
printed strips placed in the radiating aperture of the planar
antenna at the top and bottom layer. They are employed to
suppress the radiation at certain frequencies within an ultra-
wide frequency band [10, 11]. By inserting the U-shaped
parasitic element on the bottom plane of the basic planar
monopole antenna [12] or by using a pair of arc shaped
parasitic elements around the patch, an excellent notched
frequency band for rejecting the WLAN band (5-6GHz) can be
obtained [13]. The electromagnetic coupling of the SRR with
the CPW yields the frequency notch [14]. There are many more
techniques used to obtain band-notch operation in UWB range.
The proposed antenna is simple to design and implement. By
changing the slit gap of the antenna the desired band-notch
frequency can be tuned. Additional varactor diode can be
implemented with the antenna as a future scope to give variable
capacitance and the same antenna can be used to tune different
frequency bands. The proposed antenna was carefully
fabricated and measured. The return loss, VSWR, and
impedance are measured to certify the performance. Results
show acceptable discrepancy between simulation and
measurement due to the influence of the SMA connector for
testing and the indoor measurement environment.
II. PHI SHAPE UWB ANTENNA WITH BAND NOTCH
CHARACTERISTICS
Initially a monopole antenna at 3GHz frequency is
designed. The height of monopole antenna will be λ/4. Heights
of monopole antenna and ground plane dimensions are fixed by
optimization. Designed square and circular shape split ring
resonators are overlapped with monopole to form the proposed
phi shape antennas. The proposed SPSSR and SPSCR antennas
for band notch applications in UWB range are shown in Figure
2. 1.
1.1
ant
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The length of
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own in Table
ves the inducta
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anged by chan
pacitance by
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pacitance. Hen
rcular ring is g
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Fig.
Fig. 2
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to considerati
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f the outer rin
and inner ring
a split gap of
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ance and the sp
ives the capa
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changing the
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nce the resona
given as in (1)
are the equiva
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1. SPSSR ant
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C3 and C4 are
eft half and ri
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by (2) [16] as
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ng is 38mm an
gs are separate
1.1mm. Detai
th of rings w
pacing betwee
acitance. The
th and width o
e spacing and
a function o
ance frequency
[15]
alent inductan
split rings.
tenna and SPSCR
antenna equivalen
valent circuit
alent inductan
ause of the sli
capacitance b
ight half of a
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nd the ring wi
ed by 0.7mm.
iled dimension
with specified
en the two ring
inductance c
of rings where
d slit gap of
of inductance
y for the squar
(1)
nce and capac
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nt circuit.
diagram show
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it gap in oute
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ulated by takin
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Ajetrao & Dha
idth is
. Both
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width
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Vol. 8, No. 4, 20
ande: Phi Shap
Considering C
Metal thickne
ween rings is
itten as
for square
C 4a
for circula
,
Equivalent
tangular/circul
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SPSSR and S
WB range. The
0.0002
ere, ϒ is the co
8
The equivale
me as in (7) bu
cular geometry
2
Using (2)-(9)
ncept in [13, 1
d SPSCR ante
nge. Calculated
simulate the pr
Parameter
L1
L2
L
M
y1
W
Ring length
T
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g2
H
018, 3123-3127
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C1=C2= and
ess of copper
g1 and ε0=8.
e rings is given
g C
ar rings is give
and are
inductance
lar cross sect
ness of ring t
used to calcul
PSCR antenn
e equivalent in
2.303
onstant for wir
;
ent inductance
ut with differe
y and:
;
in (1) gives th
15-18] is used
ennas for ban
d dimensions w
roposed antenn
TABLE I.
SPSSR ant
dimensio
72mm
23mm
19.5mm
3mm
7.9mm
6.5mm
38mm (ringx=
1.1mm
0.7mm
1.1mm
1.6mm
na with Band N
d C3=C4= ,
is p=35µm, r
854187817×1
n by (5) [13, 1
en by (6) [15]
calculated as
Le c
ion of wire w
(mm) is prop
late the equiva
a for band no
nductance Le f
re loop of squa
; 2.
e Le for SPSC
ent (ϒ) consta
; 2.45
he ring resona
d to design the
nd notch app
with some opt
na.
ANTENNA DIMEN
tenna
ons
SP
m
m
m
m
m
=9.5mm) 38m
m
m
m
m
3124
Notch Character
(2) can be w
(3)
ring width is t
0−12
F/m. ca
(4)
6] as
(5)
as
(6)
in [13, 15-17]
calculation
with finite len
posed in [18].
alent inductanc
otch applicatio
for SPSSR ant
(7)
are geometry,
853 (8)
CR antenna i
ant for wire lo
1 (9)
ance. The prop
e proposed SP
plications in U
timization are
NSIONS
PSCR antenna
dimensions
72mm
23mm
19.5mm
3mm
7.9
6.5mm
mm(R1=6.05mm)
1.1mm
0.7mm
1.1mm
1.6mm
ristics
written
t, gap
an be
.
for
ngth l
. The
ce Le
ons in
tenna
is the
op of
posed
PSSR
UWB
used
3. by
by
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bot
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TABLE II.
I
The perform
parametric an
measuring t
tennas are fa
ickness, 4.4
ngent. The dim
e optimised a
own in Figure
ectromagnetic
mulated anten
th designs. Th
th antennas as
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ing the same
ay be a sligh
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better way S1
r both designs
Fig. 3. Sim
From Figure
ry close to eac
od agreement
ows the simu
PSCR antenna
tterns for the s
Band
UWB
range
F
Ba
Notched
Band
C
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SPSSR AND
III. RESULT
mance of the p
nalysis and th
the s-paramet
abricated usin
dielectric con
mensions of bo
as shown in T
e 1. Both ant
solver based
nnas give goo
he input impe
s reflected in T
R antenna and
optimised di
ht mismatch
SPSSR antenn
each other. To
11 verses frequ
in Figure 3.
mulated and measu
s 3 and 4 it is
ch other. Simu
t with each ot
ulated and me
as. Figure 5
specified band
Parameters
Frequency Range
(GHz)
S11 in dB
VSWR
and width in GHz
Impedance
Center frequency
(GHz)
VSWR
Freuency Band
otvh-Band BW in
MHz
Impedance
y & Applied Sci
SPSCR ANTENNA
TS AND DISCUS
proposed anten
he simulated r
ters and VSW
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nstant and 0
oth SPSSR an
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tenna designs
d on finite ele
od impedence
edance is quit
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imensions, be
in input im
na and result
understand th
uncy simulate
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clear that bot
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easured VSW
shows the s
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SPSSR
antenna
2.75-11.4
Less than -10
Less than
z 8.65
around 50Ω
said range
5.874
6.27
5.1-6.29
n
1190MHz
140 Ω
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SIMULATED RESU
SION
nnas is invest
results are val
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are simulated
ement method
characteristic
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al antenna des
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cause of this
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he antenna res
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and SPSCR antenn
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asured results
antennas. Fig
WR for SPSSR
simulated rad
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SPSCR
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4 2.63-11.4
0dB
Less than
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2 Less than
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e
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4.7
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Ajetrao & Dha
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tennas
are as
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a
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z
Vol. 8, No. 4, 20
ande: Phi Shap
3.4GHz and 8.
clear that both
pective band
enna and H-
tern gets dist
diation pattern
high frequenci
th antennas. Fr
d 5.87GHz for
clear that the
wing in opposi
4. Simulated
ng band-notch.
5. SPSSR a
GHz
Figure 7 sho
quency. As th
pacitance decr
quency is in
quency tuning
nnecting varac
timised to 1.1
LAN frequenc
ennas. The ga
quencies. Figu
018, 3123-3127
pe UWB Antenn
GHz respectiv
antennas are b
s. E-plane p
-plane pattern
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is caused by t
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rom the curren
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ite directions g
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and SPSCR ante
ows the effe
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reases and as
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g is possible
ctor diode in b
1mm which
cy band. Figu
ain for both sh
ure 9 shows the
na with Band N
vely. From the
behaving in si
pattern resem
n is omnidire
gh frequencies
the change in c
shows the curr
nt distribution
SPSCR in Figu
istributed only
giving band-no
VSWR for SPSSR
enna radiation p
ect of slit ga
increased the
an effect the
both antennas
by changing
between slit g
gives band n
ure 8 shows
hapes is consta
e fabricated an
3125
Notch Character
e radiation patt
imilar ways in
mbles with d
ectional. Radi
s. This chang
current distrib
rent distributio
pattern at 5.47
ure 6(b) and 6
y in one side
otch operation
R and SPSCR an
pattern at 3.0GH
ap on band n
overall equiv
notch-band c
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the slit gap o
gap. The slit g
notch operatio
the gain for
ant and equal
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ristics
tern it
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both
at all
4. Fig
rad
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g. 6. Current
diating patch at
quency 5.87GHz
Fig. 7.
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distribution for
frequency of 3G
and 5.47GHz for
Effect of slit g
y & Applied Sci
(a)
(b)
(c)
SPSSR and SP
GHz and (b) (c
SPSCR and SPS
gap on notch-band
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PSCR antennas
c)for notch-band
SR respectively.
d frequency.
h V
Ajetrao & Dha
(a) for
center
inte
Ban
wir
SPS
SPS
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ban
can
des
not
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5.9
the
and
The
bot
agr
[1]
[2]
[3]
Vol. 8, No. 4, 20
ande: Phi Shap
Fig. 8
Applications
erference with
nd notch anten
reless commun
SSR antenna i
SCR antenna
ing similar r
tern and gain.
equivalent cap
nd-notch cente
n be connecte
sired frequency
tch at WLAN
nds are from 5
1GHz for SPS
WLAN and
d WiMAX wil
e theoretical d
th antennas. S
reement with e
S. Tu, Y. C. Jia
antenna with B
In Electromagn
K. Chung, J.
Antenna Havin
and Wireless co
M. Naghshvari
Transmission L
3, pp. 283–293,
018, 3123-3127
pe UWB Antenn
8. Gain of SPS
Fig. 9. Fab
IV. CO
of UWB anten
h existing syst
nnas are playi
nications in UW
is designed an
in UWB freq
response in te
. It is observe
apacitance incr
er frequency. A
ed between th
y. Both anten
and WiMAX
.1GHz to 6.28
SCR antenna.
WiMAX sys
ll be avoided
design results
Simulated and
each other.
REFER
ao, Y. Song, Z. Z
Band Notched fun
netics Research Le
Kim, J. Choi,
ng Frequency Ba
omponents Letters
ian-Jahromi ,“Co
Line fed”, Progres
, 2008
na with Band N
SSR and SPSCR
bricated antennas.
ONCLUSIONS
nnas find diffi
tems like WL
ing an import
WB range. In
nd the same d
quency range.
erms of S11,
ed that by incr
reases which in
As future wor
he slit gap in
nnas are capab
X system frequ
8GHz for SPSS
Both notch b
stems. Interfer
by using the p
s are verified
d measured re
RENCES.
Zhang, “A Novel M
nctions for UWB
etters, Vol. 10, pp
“Wideband Mic
and-Notch Functi
s, Vol. 15, No. 11
ompact UWB Ba
ss In Electromagn
3126
Notch Character
antenna
.
ficulties in avo
LAN and WiM
tant role in to
this paper, a n
design is appli
. Both design
VSWR, radi
reasing the sli
n turn increase
rk, a varactor d
order to tun
ble of giving
uencies. The n
SR and 4.94GH
bands are cov
rence with W
proposed ante
by simulatio
esults are in
Miniature strip-si
applications”, Pr
p. 29-38, 2009
crostrip-Fed Mon
ion”, IEEE Micr
1, pp. 766-768, 20
andnotch Antenna
netics Research B
ristics
oiding
MAX.
day’s
novel
ied to
ns are
iation
it gap
es the
diode
ne the
band
notch
Hz to
vering
WLAN
ennas.
n for
good
ine fed
rogress
nopole
rowave
005
a with
B, Vol.
5. Engineering, Technology & Applied Science Research Vol. 8, No. 4, 2018, 3123-3127 3127
www.etasr.com Ajetrao & Dhande: Phi Shape UWB Antenna with Band Notch Characteristics
[4] J.-Q. Sun, X.-M. Zhang, Y.-B. Yang, R. Guan, L. Jin “Dual Band
Notched ultra-wideband planar Monopole antenna with M and W slots”,
Progress In Electromagnetics Research Letters, Vol. 19, pp. 1-8, 2010
[5] A. Falahati, M. Naghshvarian-Jahromi, R. M. Edwards ,“Dual Band-
Notch CPW-Ground-Fed UWB Antenna By Fractal Binary Tree Slot”,
Fifth International Conference on Wireless and Mobile
Communications, Cannes, France, August 23-29, 2009
[6] Z.-A. Zheng, Q.-X. Chu, “Compact CPW-fed UWB Antenna with dual
Band Notched Characteristics", Progress In Electromagnetics Research
Letters, Vol. 11, pp. 83-91, 2009
[7] Y. Zhang, W. Hong, Z.-Q. Kuai, J.-Y. Zhou, “A Compact Multiple
Bands Notched UWB Antenna by Loading SIR and SRR on the Feed
Line”, Proceedings of the 2008 International Conference on Microwave
and Millimeter Wave Technology, Nanjing, China, IEEE, 2008
[8] X. Li, L. Yang, S.-X. Gong, Y.-J. Yang, “Ultra-Wideband Monopole
Antenna with Four-Band-Notched Characteristics”, Progress In
Electromagnetics Research Letters, Vol. 6, pp. 27–34, 2009
[9] K.-H. Kim, Y.-J. Cho, S.-H. Hwang, S.-O. Park, “Band-notched UWB
planar monopole antenna withtwo parasitic patches”, Electronics Letters,
Vol. 41, No. 14, pp. 783-785, 2005
[10] A. M. Abbosh, M. E. Bialkowski, “Design of UWB Planar Band-
Notched Antenna Using Parasitic Elements”, IEEE Transactions on
Antennas and Propagation, Vol. 57, No. 3, pp. 796-799, 2009
[11] B. V. Kadam, L. J. Gudino, C. K. Ramesha, S. Nagaraju, “A Band-
notched Ultra-wideband Compact Planar Monopole Antenna With U-
shaped Parasitic Element”, Procedia Computer Science, Vol. 93, pp.
101–107, 2016
[12] M. Yazdi, N. Komjani, “A Compact Band-notched UWB Planr
Monopole Antenna with Parasitic Elements”, Progress In
Electromagnetics Research Letters, Vol. 24, pp. 129-138, 2011
[13] J. Y. Siddiqui, C. Saha, Y. M. M. Antar, “Compact SRR Loaded UWB
Circular Monopole Antenna With Frequency Notch Characteristics”,
IEEE Transactions on Antennas and Propagation, Vol. 62, No. 8, pp.
4015–4020, 2014
[14] J. Y. Siddiqui, C. Saha, Y. M. M. Antar, “Compact Dual-SRR-Loaded
UWB Monopole Antenna With Dual Frequency and Wideband Notch
Characteristics”, IEEE Antenna and Wireless Propagation letters Vol.
14, pp. 100-103, 2015
[15] C. Saha, J. Y. Siddiqui, “Versatile CAD Formulation for Estimation of
the Resonant Frequency and Magnetic Polarizability of Circular Split
Ring Resonators”, International Journal of RF and Microwave
Computer‐Aided Engineering, Vol. 21, No. 4, pp. 432-438, 2011
[16] C. Saha, J. Y. Siddiqui, Y. M. M. Antar, “Square split ring resonator
backed coplanar waveguide for filter applications”, 2011 XXXth URSI
General Assembly and Scientific Symposium, Istanbul, Turkey, August
13-20, IEEE, 2011
[17] I. Bahl, P. Bhartia, Microwave Solid State Circuit Design, 2nd Edition,
John Wiley & Sons, New York, 1998
[18] F. E. Terman, Radio Engineers’ Handbook, Mcgraw-Hill, New York,
1943