# Multiobjective Synthesis of Steerable UWB Circular Antenna Array considering Energy Patterns

Authors: Leopoldo A. Garza; Marco A. Panduro; David H. Covarrubias; Alberto Reyna
Journal: International Journal of Antennas and Propagation
 (2015)

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## Abstract

True-time delay antenna arrays have gained a prominent attention in ultrawideband (UWB) applications such as directional communications and radar. This paper presents the design of steerable UWB circular array by using a multiobjective time-domain synthesis of energy pattern for circular antenna arrays. By this way we avoid individual beamforming for each frequency in UWB spectrum if the problem was addressed from the frequency domain. In order to obtain an energy pattern with low side lobe level and a desired main beam, the synthesis presented is performed by optimizing the true-time delays and amplitude coefficients for the antenna elements in a circular geometry. The method of Differential Evolution for Multiobjective Optimization (DEMO) is used as the optimization algorithm in this work. This design of steerable UWB circular arrays considers the optimization of the true-time exciting delays and the amplitude coefficients across the antenna elements to operate with optimal performance in the whole azimuth plane (360°). A comparative analysis of the performance of the optimized design with the case of conventional progressive delay excitations is achieved. The provided results show a good performance for energy patterns and for their respective power patterns in the UWB spectrum.


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## Body

## 1. Introduction

In recent times, ultrawideband (UWB) communications require antenna arrays for applications such as beamforming and directional communications with high rate data transmission and high sensitivity [1, 2]. In such applications, the UWB antenna arrays are required to establish a point-to-point communication with suppression of undesired interferences [3]. However, the power pattern changes significantly between the lower and upper edge of the UWB frequency band (3.1 GHz to 10.6 GHz) defined by the US Federal Communications Commission (FCC) [4]. This implies a complex design problem due to numerous radiation patterns if the analysis in the frequency domain is used [5]. An alternative approach is the analysis in the time domain to design UWB antenna arrays. The pattern in the time domain is defined as the energy pattern [6]. The energy pattern of the antenna array is the total response of the power patterns in the frequency domain [7]. Therefore, using the energy pattern in the time domain, we avoid the individual beamforming for the power patterns in the frequency domain.Time-domain (TD) or pulsed antenna arrays have recently been studied by pondering their advantages of low side lobe levels (SLL) and high resolution for applications such as communications, remote sensing, and radar [8]. The design of TD linear antenna array has been reported in [9–13], exploiting its features of fixed and scanning beam patterns. The synthesis of linear and circular antenna arrays has been reported in [14, 15] by modelling Hermite-Rodriguez waveforms functions to obtain arrays currents and the energy pattern by a generalized hypergeometric function. A TD UWB transverse electromagnetic horn antenna array optimized by a Micro Genetic Algorithm is presented in [16]. Furthermore, a nonuniform UWB linear antenna array optimized by the well-known Differential Evolution Method for low side lobe level during beam-scanning is presented in [17]. Moreover, two-dimensional TD arrays with scanning beam pattern by using the Sequential Quadratic Programming to find the optimum positions, amplitudes, and time delays are presented in [18–20].Now, our proposal presents the synthesis of TD circular antenna arrays for UWB spectrum. Particularly, our research considers the synthesis of a single-ring circular antenna array with low SLL and beamwidth and different requirements for a steerable main lobe. This design of steerable UWB circular arrays considers the optimization of the true-time exciting delays and the amplitude coefficients across the antenna elements to operate with optimal performance in the whole azimuth plane (360°). The performance of UWB circular array could be improved substantially (with respect to the UWB circular array with the conventional progressive delay excitation), if the amplitude and delay excitations are set or optimized in an adequate way. The synthesis process is carried out by Differential Evolution for Multiobjective Optimization (DEMO) [21] by finding out the optimal true-time exciting delays and amplitude coefficients of pulsed antenna elements. Hence, the novelty of this research is the synthesis of TD circular antenna array in order to obtain steerable energy patterns with low SLL; by this way we avoid the individual beamforming which would require an optimization process for each frequency in UWB spectrum.The remainder of the paper is organized as follows: Section2 presents the time-domain formulation for a steerable UWB circular antenna array model. Section 3 describes the synthesis algorithm, DEMO, to achieve a steerable energy pattern with low SLL. The optimization results are shown in Section 4. Finally, conclusions are presented in Section 5.


## 2. Time-Domain Antenna Array Model

Let us assume a TD circular antenna array ofN antenna elements grouped in a circular geometry located in the plane X
-
Y as shown in Figure 1. Each antenna is fed by a short pulse with different time delays and amplitude coefficients. The short pulses are added in space resulting in far-field waveform. Then, the far-field waveform will depend basically on four parameters referred to as the waveform of feeding short pulse, the antenna element positions, the time delays among the short pulses, and the amplitude coefficients [1].Figure 1
Time-domain circular antenna array model.It is known that the 5th derivative Gaussian pulse has the most effective pulse shape with power spectrum under FCC limitation floor, and this pulse can be transmitted without additional filtering [22]. For this reason, let us consider the 5th derivative Gaussian pulse as the waveform of the receiving short pulses to each antenna element as follows [22, 23]:(1)
f
n
t
=
A
-
t
5
2
π
σ
11
+
10
t
3
2
π
σ
9
-
15
t
2
π
σ
7
exp
⁡
-
t
2
2
σ
2
,where A is the amplitude of the pulse and σ is a time constant. In order to satisfy the FCC regulations, these parameters are chosen to be  A
=
1, σ
=
51 ps, and t
=
250 ps [22–24]. Now, the radiation properties of the TD circular antenna array can be modelled. Then, by using the pattern descriptors developed by [25], the energy pattern can be defined as(2)
P
e
n
e
r
g
y
θ
,
ϕ
=
∫
0
t
s
t
,
θ
,
ϕ
2
d
t
,where s
t
,
θ
,
ϕ is the far-field waveform of the antenna array and the direction θ
,
ϕ represents, respectively, the elevation and azimuth angles. The spectrum in frequency of s
t
,
θ
,
ϕ or power patterns can be obtained by a Fourier transform as follows [25]:(3)
P
f
,
θ
,
ϕ
=
∫
-
∞
∞
s
t
,
θ
,
ϕ
e
-
j
2
π
f
t
d
t
,where f is the frequency from 3.1 GHz to 10.6 GHz defined by the FCC regulations for UWB systems [22–24].Then, the far-field waveform for the TD circular antenna array shown in Figure1 is defined as follows [26]:(4)
s
t
,
θ
,
ϕ
=
∑
n
=
1
N
a
n
f
n
t
-
Δ
t
+
τ
p
-
τ
n
,
θ
,
ϕ
,where(5)
Δ
t
=
r
c
sin
⁡
θ
cos
⁡
ϕ
n
-
ϕ
,
r
=
∑
n
=
1
N
d
n
2
π
,
ϕ
n
=
∑
n
=
1
N
2
π
n
N
,
τ
p
=
r
c
sin
⁡
θ
0
cos
⁡
ϕ
n
-
ϕ
0
.The variableN is the number of antenna elements in the array; a
n is the amplitude coefficient of the antenna element n, d
n is the Euclidian space between antenna elements, r is the radius of the circle array, and c is the propagation speed. The direction θ
0
,
ϕ
0 is the desired maximum direction. The term ϕ
n is the angular position of the element n; τ
p is the progressive exciting time delay; and τ
n
∈
0
,
τ
m
a
x is the disturbed exciting time delay.The proposed synthesis problem is to obtain an optimum energy pattern by optimizing the amplitude excitations and the disturbing exciting time delay of a circular antenna array for a maximum performance in terms of the side lobe level and a desired main beamwidth in a scanning range of[
-
180
°
,
180
°
]. The design of a steerable UWB circular antenna array could be achieved by considering the rotation properties of monochromatic circular arrays; that is, the rotation properties of circular arrays (for just one frequency) could be extended to design steerable UWB circular arrays considering energy patterns.This design rule is very simple. Let us consider a circular array ofN elements to illustrate this point. In this case, the behavior of the array factor for the scanning range of -
180
≤
ϕ
n
≤
180
° is considered (with ϕ
0 as the beam direction in azimuth plane). If the number of antennas is N
=
8 and there is uniform angular separation of 45
° between different beam steering angles, the optimal excitation solution (amplitudes and time delays) for a particular beam steering angle should also apply to other beam steering angles by substituting a
n
,
τ
n into a
n
+
1
,
τ
n
+
1 when the beam steering is increased ϕ
0
+
45
° [27, 28].Through our proposal, only one optimization is required for beam steering in steps of45
° (in all azimuth plane) instead of one optimization for each beam steering direction. Then, the objective functions for this design case, o
f
1 and o
f
2, set to be minimized are defined as follows:(6)
o
f
1
n
=
P
e
n
e
r
g
y
θ
S
L
L
,
ϕ
S
L
L
,
o
f
2
n
=
B
W
P
e
n
e
r
g
y
.The proposedo
f
1 regards the maximum peak side lobe level represented by term P
e
n
e
r
g
y
θ
S
L
L
,
ϕ
S
L
L, and proposed o
f
2 regards the beamwidth of the obtained energy pattern and it is represented by term B
W
P
e
n
e
r
g
y.The present study will be focused on the behavior of the pattern descriptor (using the energy pattern in time domain) generated by the UWB circular antenna array. In particular, this design problem is not focused on any type of antenna element. In this case, the design problem is set at the array structure level, that is, the best design configuration (amplitude and time delays excitations), when a circular array structure with a steerable pattern is employed in UWB systems.Then, in order to solve this design problem, the method of Differential Evolution for Multiobjective Optimization (DEMO) is used in order to find the spread of solutions and the convergence to an optimum solution to minimize both objective functions. The procedure of the optimization process is described in the next subsection.


## 3. Differential Evolution for Multiobjective Optimization

The optimization process is carried out by the algorithm of DEMO for the effectiveness in antenna arrays design [29]. DEMO is an optimization approach based on the classical method of Differential Evolution (DE) [30] combined with the mechanisms of Pareto-based ranking and crowding distance sorting, employed in the literature of evolutionary algorithms for multiobjective optimization.In order to resolve the proposed synthesis design problem, the DEMO algorithm was selected based on the performance comparison of NSGA-II [31], EM-MOPSO [32], and DEMO variants [21] made by Panduro et al. [29] for the design of circular concentric rings antenna arrays. The results of that performance comparison showed that the variants of DEMO/parent and DEMO/closest/dec found better nondominated solutions as an approximation to the Pareto solution. Moreover, the performance comparison also evaluates the metric of the binary epsilon indicator [33] to calculate how much the nondominated front of each optimization algorithm is separated from the Pareto front. DEMO/parent outperforms totally the other algorithms by having a better behavior on this metric and a better approximation to the Pareto front. Based on these comparisons for the design of antenna arrays over a circular geometry, DEMO/parent is implemented in this synthesis of steerable UWB circular antenna arrays.The procedure for used DEMO/parent is described as follows [21]:(1) Evaluate the initial populationP of random individuals.
(2) While stopping criterion not met, do the following:
(a) For each individualP
i
i
=
1
,
…
,
p
o
p
S
i
z
e from P repeat:
(i) Create candidateC from P
i.
(ii) Evaluate candidate.
(iii) If the candidate dominates the parent, the candidate replaces the parent.
If the parent dominates the candidate, the candidate is discarded.
Otherwise, the candidate is added in the population.
(b) If the population has more thanp
o
p
S
i
z
e individuals, truncate it sorting the individuals with nondominated sorting and then evaluating the individuals of the same front with the crowding distance metric.
(c) Randomly enumerate the individuals inP.For the candidate creation, the DE scheme DE/rand/1/bin [21, 30] is used, and the procedure for this scheme is described as follows:(1)
Randomly select three individualsP
i
1, P
i
2, and P
i
3 from P, where i, i
1, i
2, and i
3 are pairwise different.
(2)
Calculate candidateC as C
=
P
i
1
+
F
×
P
i
2
-
P
i
3, where F is a scaling factor.
(3)
Modify the candidate by binary crossover with the parent using crossover probabilityp
c.The immediate replacement of the parent individual with the candidate that dominates it emphasizes elitism within reproduction, helping achieve the convergence to the true Pareto front. And the use of nondominated sorting and crowding distance metric in truncation of the extended population stimulates the uniform spread of solutions, finding as many nondominated solutions as possible [21].Therefore, the procedure of the DEMO/parent process for our synthesis problem is described in Figure2. The individuals are encoded in a vector of real numbers that represents the amplitudes excitations on the range 0
,
a
m
a
x, and a vector of real numbers restrained on the range 0
,
τ
m
a
x that represents the disturbing exciting time delay. And the stopping criterion to meet is the total number of iterations.Figure 2
Flow chart for the implemented DEMO/parent procedure.In the next section, the results of using this optimization process in the synthesis of TD circular antenna arrays are presented.


## 4. Simulation Results

The method DEMO/parent was implemented to optimize the disturbed exciting time delays and amplitude excitations of TD circular antenna array. For the case of a steerable energy pattern, the main beam is steered in the azimuth plane-
180
°
≤
ϕ
0
≤
180
° with an angular step of 45
° in the cut of θ
=
θ
0
=
90
°. Since the principal advantage of the circular array is steering the beam without significant changes over the pattern, we evaluate the rotation properties in all azimuth plane, but this property could be extended to consider the elevation plane. Therefore, the number of elements for the circular antenna array is given by N
=
360
°
/
45
°
=
8, with Euclidean spacing of 150 mm among the antenna elements. According to [10] this spacing value can be enough to avoid important coupling effects. For generation of individuals, the maximum value of amplitudes excitation a
m
a
x was set to 10, and the maximum value of disturbing exciting time delay τ
m
a
x we have considered is 100 ps. For the parameters of the DEMO/parent algorithm, we have set the population size to 600. We consider a scaling factor F
=
0.5 and a two-point crossover with a crossover probability of p
c
=
0.15. And the stopping criterion is 600 iterations.The algorithm was executed 10 times and the consolidated front for each run is considered as the nondominated front. Figure3 shows the nondominated front of both objective functions obtained by the DEMO/parent algorithm for the circular antenna array proposed. The result shown in Figure 3 illustrates that the DEMO/parent algorithm found nondominated solutions for the two objective functions. Furthermore, this figure shows the selected design solution from the nondominated front. As shown in Figure 3, this design solution represents the best compromise between the side lobe level and beamwidth for a steerable energy pattern. As additional information, the nondominated front was obtained after the 600 iterations in an average time of 13415 seconds, for a population of 600.Figure 3
Nondominated front obtained by DEMO/parent algorithm and the selected solution for steerable energy pattern of a circular antenna array.Figure4 illustrates the selected solution from the nondominated front for the steerable energy patterns considering the circular antenna array with amplitude excitations and disturbing exciting time delay optimized by DEMO/parent algorithm. The sets of amplitudes and time delays provide the normalized energy pattern with a maximum S
L
L
≤
-
12.7014
d
B and a maximum B
W
≤
11.52
° for the beam steering directions of (a) ϕ
0
=
-
135
°, (b) ϕ
0
=
-
90
°, (c) ϕ
0
=
-
45
°, (d)ϕ
0
=
0
°, (e) ϕ
0
=
45
°, (f) ϕ
0
=
90
°, (g) ϕ
0
=
135
°, and (h) ϕ
0
=
180
°. Each energy pattern is compared against a conventional case of circular antenna array with uniform amplitude excitations and progressive delay excitation. From Figure 4, we can conclude that the DEMO algorithm obtained a reduction of the SLL and kept a beamwidth narrow for all beam steering directions. It is essential to mention that the obtained values of SLL and beamwidth for the optimized energy pattern are the same when the main beam is steered in the proposed directions, by rotating the optimized set of amplitude excitations and the disturbing exciting time delays in the circular antenna array.Figure 4
Comparison of the energy patterns between conventional case and optimized solution by DEMO/parent algorithm for (a)ϕ
0
=
-
135
°, (b) ϕ
0
=
-
90
°, (c) ϕ
0
=
-
45
°, (d) ϕ
0
=
0
°, (e) ϕ
0
=
45
°, (f) ϕ
0
=
90
°, (g) ϕ
0
=
135
°, and (h) ϕ
0
=
180
°.
(a)
ϕ
0
=
-
135
°
(b)
ϕ
0
=
-
90
°
(c)
ϕ
0
=
-
45
°
(d)
ϕ
0
=
0
°
(e)
ϕ
0
=
45
°
(f)
ϕ
0
=
90
°
(g)
ϕ
0
=
135
°
(h)
ϕ
0
=
180
°The numerical values of the side lobe level and beamwidth for the optimized steerable energy pattern and its sets of amplitudes and time delays are presented in Table1.Table 1
Comparison of numerical values between the conventional case and the optimized solution by DEMO/parent for the steerable energy pattern shown in Figure4 (amplitude and time delays values are for the case ϕ
0
=
0
°).
Design case
Max SLL (dB)
BW (degrees)
Amplitude excitations
Time delays (ps)
Conventional case
−6.8731
9.6
1
1
0
0
1
1
0
0
1
1
0
0
1
1
0
0
Optimized solution
−12.7014
11.52
7.1734
4.9271
77.1268
87.0812
4.1092
8.5237
84.9614
87.8917
3.8870
6.4498
72.6069
75.0366
6.9596
9.0309
73.3821
69.7864It is observed in Table1 that the DEMO algorithm could minimize the SLL and maintain a narrow beamwidth with respect to the conventional case. Moreover, this table shows the amplitude excitations and disturbing exciting time delays required to generate the energy pattern for the direction of ϕ
0
=
0
°. Please note that, to generate the energy pattern in other directions, the rotation properties (mentioned previously for the circular array proposed) are applied.Now, in order to observe the effect of the time-domain synthesis over the response in the frequency domain, we calculated the spectrum in frequency of the far-field waveform in time domain by using (3). Figure 5 shows the spectrum in frequency for all UWB frequency band of (a) optimized solution and (b) conventional case, for ϕ
0
=
0. Because there are no variations when the main beam is steered to the proposed directions, one case is enough to observe the effect of the time-domain synthesis over the response in the frequency domain.Figure 5
Spectrum in frequency of (a) optimized solution and (b) conventional case, forϕ
0
=
0.
(a)
Optimized solution
(b)
Conventional caseFigure5 illustrates that the different power patterns show variations in the SLL, with a maximum SLL of -
8.5134
d
B for the optimized solution and -
5.9157
d
B for the conventional case; and the maximum beamwidth for the optimized solution was 15.6
° and 12
° for the conventional case. These variations are due to many frequencies in the UWB frequency band. Figure 6 presents the variations of the maximum SLL in the spectrum frequency of each case, as it can be observed that the optimization solution has lower SLL over the most part of the UWB frequency band. The variations of SLL are due to wavelength changes in each frequency, and the uniform spacing of the antenna elements in the array caused an increase in the SLL, especially near the boundaries of the spectrum frequency for the optimized solution. Furthermore Figure 7 illustrates the variations of the beamwidth along the frequency spectrum for each case; it is worth mentioning that the value of beamwidth decreases at higher frequency, with a difference (between its boundaries) of 7.2
° for the optimized solution and 2.6
° for the conventional case. This difference is due to the nonuniform set of amplitude excitations and disturbing exciting time delays of the optimized solution.Figure 6
Comparison of the maximum SLL of the power pattern in each frequency in the UWB spectrum for the optimized solution and the conventional case.Figure 7
Comparison of the beamwidth of the power pattern in each frequency in the UWB spectrum for the optimized solution and the conventional case.


## 5. Conclusions

This paper presented the synthesis of energy patterns for a TD circular antenna array by using the DEMO/parent algorithm to optimize the amplitude excitations and the disturbing exciting time delays. The study presented the synthesis process in the time domain for a steerable energy pattern and its effect in the UWB spectrum frequency. The results show a good performance in both proposed cases. For the case of the steerable energy pattern low values of SLL and beamwidth were achieved. The optimized solution presents a reduction of SLL of5.82
d
B with respect to the conventional case. All patterns in the UWB spectrum resulted in a good performance of SLL and beamwidth. Furthermore, the presented synthesis in time domain is an alternative to avoid individual beamforming for each frequency in the UWB spectrum. The proposed time-domain synthesis for the design of circular antenna array along with the application of the rotation properties allowed optimized beam pattern for different steering direction and for the whole UWB spectrum by just one optimization process. Future works can be addressed to include mutual coupling effects of different antenna elements for UWB antenna arrays.



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*Source: 789094-2015-10-28.xml*