Radiation pattern and frequency reconfigurable antenna using Padovan sequence

TP CHÍ KHOA HC VÀ CÔNG NGHNĂNG LƯỢNG - TRƯỜNG ĐẠI HỌC ĐIỆN LC  
(ISSN: 1859 - 4557)  
RADIATION PATTERN AND FREQUENCY RECONFIGURABLE ANTENNA  
USING PADOVAN SEQUENCE  
ANTEN TÁI CU HÌNH THEO GIẢN ĐỒ BC XVÀ TN SSDNG CHUI PADOVAN  
Duong Thi Thanh Tu1, Nguyen Tan Dung1, Hoang Thi Phuong Thao2  
1Posts and Telecommunications Institute of Technology; 2Electric Power University  
Ngày nhn bài: 05/01/2021, Ngày chp nhận đăng: 23/03/2021, Phn bin: TS. Nguyễn Đôn Nhân  
Abstract:  
This paper proposes a radiation pattern and frequency reconfigurable antenna using four PIN diodes.  
The antenna structure is based on the Padovan sequence of nine squares on the patch and four  
ones on the ground. In this way, the antenna's radiation pattern can be recognized at +52° and  
27°. Also, the reconfigurable frequency of the proposed antenna can change from 5 GHz to 18.74  
GHz. The total antenna size is rather small, which is 44.44 x 35 x 1.52 mm3. Besides, the antenna  
can achieve rather high efficiency and a quite good bandwidth at almost operating bands.  
Keywords:  
Reconfigurable antenna, radiation pattern reconfigurable, frequency reconfigurable, Padovan,  
PIN diode.  
Tóm tt:  
Nội dung bài báo đề xut mt cấu trúc anten đa tái cấu hình: va có thtái cu hình theo giản đồ  
bc xva có thtái cu hình theo tn sda trên các trng thái bt tt khác nhau ca bn diode  
PIN. Để làm được điều này, thiết kế anten được biến đổi theo hình vuông Padovan vi 9 phn tử  
trên mt bc xvà bn phn ttrên mt phẳng đất. Anten thu được có thtái cu hình theo gin  
đồ bc xtại hai phương +520 và 270, tái cu hình theo tn stừ 5Ghz đến 18.74GHz vi kích  
thước tng thkhá nhỏ, đạt 44.44 x 35 x 1.52 mm3. Bên cạnh đó, các tham số quan trng khác ca  
anten tái cấu hình như hiệu suất và băng thông thu được khá tt phn ln các tn scộng hưởng  
ca anten.  
Tkhóa:  
Anten tái cu hình, tái cu hình theo tn s, tái cấu hình theo đồ thbc x, Padovan; điôt PIN.  
1. INTRODUCTION  
adjust to achieve the desired characters  
like frequency band, radiation direction,  
or polarization. Reconfigurable antennas  
have many advantages over wideband  
antennas, such as smaller size,  
comparable radiation patterns among all  
The requirements for advanced antennas'  
multi-functional abilities are continuously  
increasing for wireless communications,  
radar  
systems,  
and  
satellite  
telecommunications. Their properties can  
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(ISSN: 1859 - 4557)  
multiple frequency bands, productive follows. In Part 2, the antenna design is  
utilization of electromagnetic range, and  
frequency discernment, decreasing the co-  
channel interference and jamming [1].  
Only in 2018-2019, a score of researches  
about reconfigurable antennas have been  
reported with different variations such  
as frequency reconfigurable [2]-[7],  
radiation pattern reconfigurable [8-15]. In  
[9], a wideband antenna was reconfigured  
radiation pattern by G. Jin et al. The  
antenna uses four diodes to change to four  
different directions but the average  
performance approximately 60%. Also,  
the antenna size is rather big, which is  
75×75×0.75 mm3, so it hard to apply to  
the user equipment. Scale problem is a  
challenge of the antenna in [11] because  
of numerous layers that significantly  
create large elevation. In [14], a design  
antenna with a ring structure can  
change radiation patterns by matching  
impedance, but performance only reaches  
50%.  
presented. The simulated and analysis are  
studied in Part 3. Finally, Part 4 concludes  
the study.  
2. ANTENNA DESIGN  
2.1. Padovan sequence  
Unlike Fibonacci golden ratio on the 2D  
dimension, the Padovan sequence that is a  
golden ratio on the 3D dimensions is set  
through a cubic function. The Padovan  
sequence is defined by basic number  
value: 1, 1, 1, 2, 2, 3, 4, 5, 7, 9, … which  
is formed by formula (1).  
P(n)=P(n-2)+P(n3)  
(1)  
In this paper, a frequency and radiation  
pattern reconfigurable antenna using four  
PIN diodes is presented. The proposed  
antenna operates with four states of  
frequency reconfiguration and two states  
of radiation pattern one. Besides, using  
the variable squares based on the Padovan  
sequence, the antenna achieves a striking  
compact size. Thus, it can be easily  
integrated into modern compact devices  
while still being able to work with  
multiple technologies.  
Fig. 1. Padovan sequence variation  
Like Fibonacci’s spiral, the Padovan  
sequence varies to become Padovan’s  
spiral that is shown in (2).  
(푛)  
lim ((푛−1)) = 휌  
(2)  
푛→∞  
where the real value of is built through  
a cubic formula (3).  
3
3
9+ 69  
9− 69  
휌 =  
+
~ 1.324717957  
(3)  
18  
18  
The rest of this paper is organized as  
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(ISSN: 1859 - 4557)  
Table 1. Parameters and their dimensions (mm)  
2.2. Antenna structure  
Parameter Value  
Parameter  
Value  
2.2.1. Antenna using Padovan  
sequence  
35  
4
6
8
W
L
P2  
P3  
P4  
P5  
P7  
44.44  
5.16  
Figure 2 shows the proposed antenna's  
geometrical structure that consists of three  
parts: the radiation patch, the substrate,  
and the ground plane. The substrate layer  
is RO4350B with hs= 1.52 mm and  
ԑ=3.48, loss tangent 0.0037. The patch is  
constructed by the Padovan geometric  
sequence in the form of nine squares.  
These squares are arranged in ascending  
order in a counter-clockwise direction  
starting from 180° direction with  
incremental size 1, 1, 1, 2, 2, 3, 4, 5, 7.  
The ratio k = 2 is built according to the  
following formula (4) and (5).  
Ld  
0.2  
10  
14  
Wd  
k
2
2
P1  
(a)  
(b)  
Fig. 2. Antenna geometric. (a): Frontside;  
(b): Backside  
(
)
푃(푛) = 푃 푛 2 + 푃(푛 − 3)  
(4)  
(5)  
2.2.2. PIN diode  
( )  
푁 = 푃(푛) × 푘  
To switch the different antenna states,  
four PIN MA4AGBLP912 diodes are  
used due to low loss and high switching  
speed. The PIN diode can be turned on  
and off by using suitable polarity voltage.  
The ON state is made by a resistor in  
series with the inductor and the OFF state  
is made by a resistor connected in parallel  
with the capacitor then in series with the  
inductor. The values R, L, C of the diode  
PIN under both ON and OFF conditions  
are shown in Table 2.  
where P(n) is the value from the Padovan  
sequence, P(N) is the real value of the  
radiation patch.  
It is the same rule for the ground plane  
with the form of four DGS squares. The  
antenna is connected by coaxial cable  
through the ground plane to be exposed to  
the radiation patch. The position of  
coordinates (x,y) is (-3.5;6.5). Four diodes  
are connected to the feeding network  
by a microstrip line of 5.166 mm long  
and 0.2 mm width. The other antenna  
dimensions are detailed in Table 1.  
The different states of the antenna are  
shown in Table 3. Using four PIN diodes  
for the four radiating elements, the  
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TP CHÍ KHOA HC VÀ CÔNG NGHỆ NĂNG LƯNG - TRƯỜNG ĐẠI HỌC ĐIỆN LC  
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antenna can resonate at the respective S11 parameter in different states of  
the switch using the PIN diode  
corresponding to the 2D radiation  
patterns. Part 3.1 presents the frequencies  
of the reconfigured band while keeping  
the radiation intact. Section 3.2 analyzes  
the radiation pattern reconfiguration of  
the proposed antenna.  
frequencies while maintaining the same  
direction of the radiation plot. Besides, at  
a defined resonant frequency, the antenna  
will also have different radiation  
directions based on the state of the diode  
is activated.  
3.1. Frequency reconfiguration  
According to a state combination of four  
diodes from D1 to D4, the antenna can  
be reconfigured in four frequencies  
including 5 GHz, 6.81 GHz, 15.1 GHz,  
and 18.74 GHz as being shown in Table  
4. It is more clearly as seen in Figure 4  
and 5. At the first case of the frequency  
reconfiguration, the proposed antenna can  
operate at 5GHz or 6.8 GHz at the same  
direction angle of approximately -11°.  
The second frequency reconfigurable case  
is at the direction angle of +60°, the  
antenna can also operates at 15.1 GHz or  
18.7 GHz band.  
(a) ON state  
(b) OFF state  
Fig. 3. Equivalent of PIN diode  
Table 2. Diode’s parameters  
Parameter  
Value  
L
CT  
RS  
RP  
0.5nH 0.025pF 4Ω 10kΩ  
Table 3. States of antenna  
Active  
diodes  
States  
S1  
D1  
D2  
D3  
D4  
1/4  
ON  
OFF OFF OFF  
ON  
ON  
ON  
OFF OFF  
S2  
S3  
S4  
S5  
S6  
Table 4. The different states of the frequency  
reconfiguration  
OFF OFF  
ON  
OFF OFF  
ON  
ON  
2/4  
ON  
ON  
OFF  
ON  
Stat  
e
F
S11  
(dB)  
B
(%)  
G
(dBi)  
ƞ (%)  
(GHz)  
ON  
ON  
ON  
OFF  
OFF  
2.67  
37.0  
10.3  
6.81  
4.7  
64.78  
84.65  
86.09  
82  
S1  
S3  
S4  
S6  
5
17.17  
20.97  
32.16  
21.68  
OFF  
5.12  
6.43  
4.63  
15.3  
18.7  
6.8  
3/4  
ON  
ON  
ON  
ON  
ON  
ON  
ON  
OFF  
ON  
S7  
S8  
4/4  
ON  
3. SIMULATION RESULTS AND  
ANALYSIS  
The simulated results are performed on  
the CST MICROWAVE STUDIO  
commercial software that includes the  
(a) at S1 and S6 states  
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Freq.  
(GHz)  
S11  
(dB)  
Gain ƞ (%)  
(dBi)  
State  
D (°)  
B (%)  
S7  
S8  
6.7  
6.6  
2.56  
5.96  
4.89 81.06  
5.51 85.52  
19 13.6  
+6  
23.0  
The antenna operates at 14.2 GHz when  
two over four diodes turn ON. Fig 6(a)  
shows the main beam radiation direction  
between these two states in plan = 90°.  
At 6.7 GHz, the antenna can change its  
direction from +6° to 19° as shown in  
Fig 6(b).  
(b) at S3 and S4 states  
Fig 4. S11 parameters of frequency  
reconfiguration  
(a) at S1 and S6 states  
(b) at S3 and S4 states  
Fig 5. Radiation pattern of frequency  
reconfiguration  
(c) at 14.2 GHz band (b) at 6.7 GHz band  
Fig. 6. The direction pattern of radiation  
reconfiguration  
3.2. Radiation pattern reconfiguration  
The proposed antennas are structured for  
elemental radiation at different points on  
the rectangular platform. Thus, the  
directional radiation at the two and three  
diodes is activated for different radiations.  
Table 5 and Figure 6 and 7 display the  
changing of the radiation antenna by  
turning the diodes OFF or ON at different  
positions while maintaining the same  
frequency.  
(a) at 14.2 GHz band  
Table 5. The different states of the radiation  
pattern reconfiguration  
Freq.  
(GHz)  
S11  
(dB)  
Gain ƞ (%)  
(dBi)  
State  
D (°)  
B (%)  
S2  
S5  
14.24 +52  
20.75 4.8 77.19  
26.7  
(b) at 6.7 GHz band  
Fig. 7. S11 parameters of radiation  
reconfiguration  
14.2  
6.11  
6.1 78.44  
27 22.8  
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In Table 6, the proposed antenna is while their lower resonant frequencies  
compared with some other recently are the same. Though the operation  
reported reconfigurable antennas. It can frequencies in [9], [13], and [14] are  
be noted that the total size of antennas [8], lower four times. However, the volume of  
[12] is larger than the proposed antenna these publics is much larger.  
Table 6. Comparison of the proposed antenna and recent public antennas  
References Volume Radiation  
Switching  
elements/  
Frequency  
(GHz)  
Gain  
(dBi)  
B (%)  
ƞ (%)  
(mm3)  
patterns  
reconfigurations  
[8]  
[9]  
10,268.8  
4,275  
6
4
6
6/12  
4/4  
5.1 - 5.9;  
10  
14.5  
33.6  
10  
80.5  
60  
2.25 - 3.16;  
4.11  
[11]  
32,357.5  
6/6  
3.5 - 3.9; 5.2 - 6.0  
5.2; 10.5  
1.02 - 1.8; 5.2 - 6.2  
72 - 86  
changing feed  
network 1 over 4  
channels  
−80° ≤ 휃  
+80°  
[12]  
79,849  
5.8  
74  
[13]  
[14]  
1,600,000  
136,687.5  
3
2
3/30  
2/2  
58  
80 - 85  
50  
1.74;  
3 - 3.9  
14.1  
2.67; 5.96;  
14.97;  
37.02;  
7.82  
5; 6.6;  
14.2;  
15.3;18.7  
64.78-  
86.09  
This  
article  
2,473.086  
2
4/4  
4.7 - 6  
14.2 GHz to 18.7 GHz in the Ku band, the  
antenna is suitable for communication  
application in satellite protection. At  
5 GHz, antenna operation can access in  
standard Wi-Fi at 5th generation is  
802.11ac. All antenna performance  
4. CONCLUSION  
In this paper, the proposed Padovan  
antenna which can reconfigure with  
frequency and radiation using PIN diode  
switching is presented. The output of the  
antenna provides high efficiency and  
overall small size compared to the  
reconfigurable antennas studied recently.  
With reconfiguration in frequency from  
characters are  
analysed by CST  
simulation. The measurement results as  
well as the power effect on PIN diode will  
be done in the future research.  
REFERENCES  
[1] Naser Ojaroudi Parchin, Haleh Jahanbakhsh Basherlou, Yasir I.A. AlYasir, Raed A. Abd-Alhameed,  
Ahmed M. Abdulkhaleq and James M. Noras, “Recent Developments of Reconfigurable Antennas  
for Current and Future Wireless Communication Systems,” Electronics 2019, 26 January 2019.  
14  
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[2] Tayyaba Khan, MuhibUr Rahman, Adeel Akram, Yasar Amin and Hannu Tenhunen, “A Low-Cost  
CPW-Fed Multiband Frequency Reconfigurable Antenna for Wireless Applications,” Electronics  
2019, 14 August 2019.  
[3] Jayendra Kumar, Banani Basu, Fazal Ahmed Talukdar, Arnab Nandi, “Stable-multiband frequency  
reconfigurable antenna with improved radiation efficiency and increased number of multiband  
operations,” IET Microwave, Antennas & Propagation, vol. 13, Iss.5, pp. 642-648, 28th February  
2019.  
[4] Ajay Yadav, Minakshi Tewari, and Rajendra P. Yadav, Pixed Shap Ground Inspired Frequency  
Reconfigurable Antenna,” Progress In Electromagnetics Research C, Vol. 89, 75-85, 2019.  
[5] A. Vamseekrishna, B.T.P Madhav, T. Anilkumar, L.S.S. Reddy, “An IoT controlled octahedron  
frequency reconfigurable multiband antenna for microwave sensing applications,” IEEE Sensors  
Letters, vol. 2(3), 2019.  
[6] V. Arun and L.R. Karl Marx, “Internet of Things Controlled Reconfigurable Antenna for RF  
Harvesting,” Defense Science Journal, vol. 68, pp. 566-571, No. 6, November 2018.  
[7] M. Jenath Sathikbasha and V.Nagarajan, “DGS based Multiband Frequency Reconfigurable  
Antenna for Wireless Applications,” International Conference on Communication and Signal  
Processing, April 4-6, 2019, India.  
[8] Y. Yang and X. Zhu, "A Wideband Reconfigurable Antenna With 360° Beam Steering for 802.11ac  
WLAN Applications," in IEEE Transactions on Antennas and Propagation, vol. 66, no. 2, pp. 600-  
608, Feb. 2018.  
[9] G. Jin, M. Li, D. Liu and G. Zeng, "A Simple Planar Pattern Reconfigurable Antenna Based on Arc  
Dipoles," in IEEE Antennas and Wireless Propagation Letters, vol. 17, no. 9, pp. 1664-1668, Sept.  
2018.  
[10] Z. Gan, Z. Tu and Z. Xie, "Pattern-Reconfigurable Unidirectional Dipole Antenna Array Fed by  
SIW Coupler for Millimeter Wave Application," in IEEE Access, vol. 6, pp. 22401-22407, 2018.  
[11] G. Yang, J. Li, D. Wei, S. Zhou and R. Xu, "Pattern Reconfigurable Microstrip Antenna With  
Multidirectional Beam for Wireless Communication," in IEEE Transactions on Antennas and  
Propagation, vol. 67, no. 3, pp. 1910-1915, March 2019.  
[12] H. Zhou et al., "Reconfigurable Phased Array Antenna Consisting of High-Gain High-Tilt Circularly  
Polarized Four-Arm Curl Elements for Near Horizon Scanning Satellite Applications," in IEEE  
Antennas and Wireless Propagation Letters, vol. 17, no. 12, pp. 2324-2328, Dec. 2018.  
[13] S. Ahdi Rezaeieh and A.M. Abbosh, "Pattern-Reconfigurable Magneto electric Antenna Utilizing  
Asymmetrical Dipole Arms," in IEEE Antennas and Wireless Propagation Letters, vol. 18, no. 4,  
pp. 688-692, April 2019.  
[14] Mingyu Sun, Zhe Zhang, Kang An, Xianghui Wang, Yuezhi Jiang, Aixin Chen, "Dual-Sense Circular  
Polarization Antenna Based on Reconfigurable Orthogonal Network", International Journal of  
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[15] X. Yi, L. Huitema and H. Wong, "Polarization and Pattern Reconfigurable Cuboid Quadrifilar  
Helical Antenna," in IEEE Transactions on Antennas and Propagation, vol. 66, no. 6, pp. 2707-  
2715, June 2018.  
Biography:  
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Duong Thi Thanh Tu, received B.E, M.E and PhD degrees in Electronics and  
Telecommunications from Hanoi University of Science in 1999 and 2005, and  
2019, respectively. She is current senior lecturer at Faculty of Telecommunications  
1, Posts and Telecommunications Institute of Technology.  
Research interests include antenna design for new generation wireless networks  
as well as the special structure of material such as metamaterial, electromagnetic  
band gap structure.  
Nguyen Tan Dung: His is current student at Faculty of Telecommunications 1,  
Posts and Telecommunications Institute of Technology.  
His current research interest is antenna design for new generation wireless  
networks.  
Hoang Thi Phuong Thao, Received B.E, M.E and PhD degrees in Electronics and  
Telecommunications from Hanoi University of Science in 2004 and 2007, and  
2019, respectively. She is current senior Lecturer at Electronics and  
Telecommunications Faculty, Electric Power University.  
Her current research interests are designing antenna, metamaterial, and  
localization systems.  
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