# A Hybrid Method Based on the Iterative Fourier Transform and the Differential Evolution for Pattern Synthesis of Sparse Linear Arrays

Authors: Xin-Kuan Wang; Gui-Bao Wang
Journal: International Journal of Antennas and Propagation
 (2018)

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## Abstract

A hybrid method that combines the iterative Fourier transform (IFT) and the algorithm of differential evolution (DE) is proposed to address the synthesis of low sidelobe sparse linear array (SLA) including many elements. Firstly, a thinned linear array (TLA) with the lattices spaced at half wavelength is obtained by the IFT. Then, for the elements of the TLA whose left or right spacing are greater than half wavelength, their placements are selected as the candidates which will be further optimized by the DE, as long as the interelement spacing is not less than half wavelength. Consequently, the convergence pressure of DE is greatly alleviated for the reason that the selected elements only accounts for a small part of the total. Therefore, the SLA with improved sidelobe performance can be obtained at relative low hardware cost. Several numerical instances confirmed the effectiveness of the proposed method.


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## Body

## 1. Introduction

In some antenna applications, we focus the antenna array with narrow beamwidth to increase the resolution while allow sacrificing some antenna gain, so a certain percentage of the elements can be removed from a periodic, fully populated array. This is commonly known as thinned array (TA). For the advantages in reducing weight, power, and cost, TA had been used in satellite communications, ground-based radars, radio astronomy, and so on [1]. Over the past few decades, a number of tools, such as the genetic algorithm (GA) [2–4], the ant colony optimization (ACO) [5], the particle swarm optimization (PSO) [6], the biogeography-based optimization (BBO) [7], IFT [8–10], and the almost difference set- (ADS-) based approach [11], had been employed for TA synthesizing. In particular, the IFT [9] and ADS [11] had been confirmed very effective for thinning large planar arrays.Another kind of structure analogous to TA, which has the elements arbitrarily located within the antenna aperture and thereby provides more degree of freedom to achieve sidelobe suppression, is called sparse array (SA). Unfortunately, the synthesis for SA refers to a question of multiple constraints including the minimum element spacing, the antenna aperture, and the number of elements. Therefore, the use of stochastic optimization algorithms such as the simulated annealing [12], PSO [13], DE [14, 15], and GA [16] is not a computationally efficient way for the synthesis of the SA including many elements. During the past few years, the deterministic approaches, such as the IFT [8–10], the methodology by means of density taper [17], had been proposed. Most of this kind of methods require a priori estimate for the array performance as well as a predefined number of elements within a given aperture size; therefore, they cannot guarantee the array fitting desired power patterns with maximally reduced number of elements. Recently, a noniterative method for linear array based on the matrix pencil method (MPM) [18] is proposed and confirmed to be effective and computationally efficient in synthesizing the massively sparse arrays. More notably, the Bayesian compressive sensing (BCS) had been employed [19] to address the same issue. The reports in [19, 20] shown that the BCS-based approach allows the design of linear arrangement fitting desired power patterns with at least 35% elements reduced comparing to the regular array configuration. Furthermore, in order to synthesize the asymmetrical shaped beams, an advanced term of the BCS is applied in [21], which could deal with the SLA matching arbitrary reference patterns.In this manuscript, the synthesis of uniform-amplitude sparse linear array with many elements is considered. Naturally, the use of the stochastic method, typically as DE, always involves a large set of parameters and thereby requires high computational resources. To ease the impact, we propose a hybrid method that combines the IFT and DE (IFT-DE) to address the issue. The method is based on DE with the individual parameters constituted by the element locations. Differently, unlike the conventional DE in which all the individual parameters are randomly initialized, for the assumption that the element spacing is not less than0.5λ (λ denotes the wavelength), most element locations of this method are predetermined by a uniform excited TLA with the lattices spaced at 0.5λ that obtained by the IFT, the first step of the IFT-DE. Consequently, just a limited number of individual parameters that remain for DE are to be optimized. This will effectively narrow the solution space and thereby efficiently accelerate the convergence speed of DE.The manuscript is mainly organized as follows. Section2 describes the formulation of the proposed method. Section 3 provides a set of numerical examples to validate the effectiveness of the IFT-DE. Finally, the conclusion of this work is summarized in Section 4.


## 2. Formulation of the Proposed Method

Consider a linear array withN isotropic elements. The array factor can be expressed as follows [8]:
(1)AFu=∑n=0N−1Anejkndu,where An represents the nth element excitation, and all the excitations are labeled as the collection An. k is the wavelength, and d is the element spacing. u=sinθ, where θ denotes the angle measured from the broadside of the array.The IFT in the proposed method is the same as that used in [10], which is a slight modification form to that presented in [8]. Therefore, the adaptively changed filling factor can be written as
(2)f=1−qΔf,q=1,2,…,Q,where Δf refers to the step size when f changes, q is the iteration number with Q representing its maxima. When f reaches its target value f0, Q can be written as
(3)Q=1−fΔf.Accordingly, a single trial of the IFT-DE can be divided into three steps, as are in turn described below.Step 1.
Perform the IFT to get a thinned linear array [8–10].
(1)
Randomly initialize the element excitationsAn over the N lattices with probability of 0.9 equal to one and the rest equal to zero.
(2)
Compute the array factorAFu from An through K points IFFT with K>2N.
(3)
Force the values in the sidelobe region ofAFu to match the predefined value that is obtained by trial and error.
(4)
ComputeAn from AFu through K points FFT.
(5)
Truncate theK samples of An to N samples that coincide with the total number of lattices.
(6)
ForAn, set the N⋅f samples which have higher amplitudes to be equal to 1, while others equal to 0.
(7)
Decreasef with step size of Δf so that in each iteration cycle, just one element is removed for asymmetrical array while in the opposite, two elements located in symmetrical positions are removed.
(8)
Repeat steps (2)–(7) untilf arrives at f0, then the iteration is terminated and a thinned array with filling factor of f0 is obtained.Step 2.
Select the element locations that need to be optimized.
For the above thinned array, select the elements whose left or right spacing are greater than0.5λ, and label their initial locations as the set zl,l=1,2,…,L, where L refers to the maximum number. Figure 1 illustrates a thinned array including six elements with the lattices spaced at 0.5λ. The symbols of solid circle indicate the activated elements, while the symbols “×” describe the other way (Figure 1). It can be seen that the elements numbered in 3rd, 4th, 5th, and 6th, whose initial locations are in turn recorded by z1, z2, z3, and z4, are deemed to meet the aforementioned selection rule.Step 3.
The optimization for the selected element locations using DE.(1)
Determine the lower and upper bounds for locations of the selected elements.
Assume that a total ofL element locations xl,l=1,…,L need to be optimized with zl,l=1,…,L the initial value, and the lower and upper bounds for xl are, respectively, indicated by xlmin and xlmax,l=1,…,L. For the constraint that the minimum element spacing is not less than 0.5λ, the values of xlmin and xlmax are set to be determined as follows:
(4)xlmax−zl=zl+1−xl+1min,xl+1min−xlmax=0.5λ,l=1,2,…,L−1.
It depicts that the maximum range of the adjacent elements moving in the opposite direction is set equal, and the minimum distance after the movement is0.5λ. To illustrate the above restriction, still in Figure 1 as an example, the location ranges (described by the double arrows) for the elements numbered in 3rd, 4th, 5th, and 6th are given by the following set of inequalities
(5)1.0λ≤x1≤1.25λ,1.75λ≤x2≤2.5λ,3.0λ≤x3≤3.75λ4.25λ≤x4≤4.5λ.
(2)
Perform DE.
A conventional DE similar to that presented in [22] is used to find the SLA with minimum peak sidelobe level (PSLL), where the mutation strategy of DE/rand/1, as well as the operator of binomial crossover, is adopted. Once the overall steps are finished, the best fitness value so far is retained, and the method will proceed to the next trial until it reaches the maxima.Figure 1
A thinned array to illustrate the way how to select the element locations that need to be optimized.


## 3. Numerical Examples

The proposed method is applied to the design cases similar to that taken from [3, 5, 8]. Therefore, the synthesis using the IFT-DE refers to firstly obtaining a TLA with different filling factors based on a total of 200 or 100 lattices spaced at 0.5λ. In each numerical instance, the IFT-DE is run for 100 independent trials. The sampling points of FFT are equal to 4096, and the initial parameters of DE, including the maxima of evolutionary generation, the population size, the scale factor, and the crossover probability, are equal to 20, 20, 0.7, and 0.9, respectively.


### 3.1. Comparing with the Reports Obtained by the IFT [8]

We consider synthesizing a symmetrical/asymmetrical SLA that is originally based on 200 lattices, symmetrical/asymmetrical TLA with different filling factors. The first case refers to synthesizing a symmetrical SLA through a symmetrical TLA with filling factor of 66%. The fitness convergence curve indicates that the optimal fitness value among 100 trials of IFT-DE is obtained at trial number 94 (Figure2(a). The far-field pattern, as is described in Figure 2(b), has the PSLL of −24.59 dB, about 1.73 dB sidelobe reduction compared with the report presented in [8], while the 3 dB beamwidth almost remained unchanged. To demonstrate the implementation process of the IFT-DE, Figure 3 gives the element distribution of the thinned linear array originally obtained by the IFT, the first step of this method at the same trial. The plane structure, started from the first row to the tenth, and each row from the left to right, describes in turn the TLA’s element locations, where the “solid squares” indicate the activated elements whose locations need to be optimized. As we can see, there are a total of 38 elements whose locations remain to be optimized among 132 candidates, and these locations are confined in some lattices. Furthermore, when the method is thoroughly performed, the element distribution of the SLA can be described by the plane structure in Figure 4. We can see that the positions of the selected elements are no longer confined in the lattices but randomly located around them. However, the unselected elements are still located in their initial lattices.Figure 2
The sparse linear array obtained by the IFT-DE based on a symmetrical TLA with a filling factor of 66%. (a) The convergence curve of the fitness value. (b) The optimal far-field pattern among 100 trials.
(a)
(b)Figure 3
The element locations of the symmetrical TLA with a filling factor of 66% obtained by the IFT.Figure 4
The element locations of the sparse linear array obtained by the IFT-DE based on the TLA described in Figure3.Similarly, as far as a symmetrical TLA with a filling factor of 77% is originally concerned, the far-field pattern of the best symmetrical SLA among 100 trials of IFT-DE shows 1 dB PSLL reduction compared with the report presented in [8], while the 3 dB beamwidth is almost unchanged. The third case considers an asymmetrical TLA with a filling factor equal to 39%. Figure 5(a) shows that the best sparse array is obtained at trial number 68 with the fitness value equal to −20.38 dB, about 3.0 dB lower than PSLL reported in [8]. However, the far-field pattern, as is depicted in Figure 5(b), only shows a beam-broaden about 0.254 degrees. The element locations of this SLA are described in Figure 6. It indicates that a total of 33 elements had their locations being readjusted among the 78 activated elements.Figure 5
The sparse linear array obtained by the IFT-DE based on an asymmetrical TLA with a filling factor of 39%. (a) The convergence curve of the fitness value. (b) The optimal far-field pattern among 100 trials.
(a)
(b)Figure 6
The element locations of the sparse linear array obtained by the IFT-DE based on an asymmetrical TLA with a filling factor of 39%.The fourth example assumes an asymmetrical TLA that is 69.5% filled. The obtained SLA shows about 1.16 dB PSLL decrement with no sacrifice of beamwidth, as is compared to the value presented in [8].


### 3.2. Comparing with the Reports Obtained by GA and ACO [3, 5]

We first consider synthesizing a low sidelobe symmetrical SLA based on 100 lattices, symmetrical TLA with a filling factor of 80%. The PSLL of the sparse array obtained by IFT-DE is equal to −20.52 dB, which is 1.7 dB lower than the reports using ACO [5]. More notably, when the filling factor decreased to 78% and 76%, the SLA obtained by the IFT-DE, respectively, shows PSLL decrement about 2.4 dB and 3.0 dB, as is compared to the value given by GA [3]. Furthermore, for the purpose of comparison, all the above synthesis results using the IFT-DE and that obtained by other tools are tabulated in Table 1. It indicates that through performing the proposed method, the SLA shows about 1~3 dB PSLL suppression without a notable tradeoff at the beamwidth. Therefore, the effectiveness of the IFT-DE is confirmed.Table 1
Comparative synthesizing results by using the IFT-DE and some published tools.
The structure of the SLA
Filling factor of the TLA originally obtained by the IFT (%)
PSLL (dB)
3 dB beamwidth (degree)
IFT-DE
IFT [8]
IFT-DE
IFT [8]
Symmetrical
77 (N = 200), symmetrical
−24.04
−22.92
0.58
0.588
66 (N = 200), symmetrical
−24.59
−22.86
0.68
0.685
Asymmetrical
69.5 (N = 200), asymmetrical
−25.46
−24.3
0.64
0.643
39 (N = 200), asymmetrical
−20.38
−17.33
0.8
0.546
Symmetrical
76 (N = 100), symmetrical
−23.56
−20.53 (by GA in [3])
—
78 (N = 100), symmetrical
−22.97
−20.56 (by GA in [3])
—
80 (N = 100), symmetrical
−22.2
−20.52 (by ACO in [5])
—All the aforementioned results are obtained by using a PC equipped with an 8 GB RAM as well as an Intel I7-6700 Processor that operates at 3.4 GHz, and the hardware cost is about an hour for each numerical instance.


## 3.1. Comparing with the Reports Obtained by the IFT [8]

We consider synthesizing a symmetrical/asymmetrical SLA that is originally based on 200 lattices, symmetrical/asymmetrical TLA with different filling factors. The first case refers to synthesizing a symmetrical SLA through a symmetrical TLA with filling factor of 66%. The fitness convergence curve indicates that the optimal fitness value among 100 trials of IFT-DE is obtained at trial number 94 (Figure2(a). The far-field pattern, as is described in Figure 2(b), has the PSLL of −24.59 dB, about 1.73 dB sidelobe reduction compared with the report presented in [8], while the 3 dB beamwidth almost remained unchanged. To demonstrate the implementation process of the IFT-DE, Figure 3 gives the element distribution of the thinned linear array originally obtained by the IFT, the first step of this method at the same trial. The plane structure, started from the first row to the tenth, and each row from the left to right, describes in turn the TLA’s element locations, where the “solid squares” indicate the activated elements whose locations need to be optimized. As we can see, there are a total of 38 elements whose locations remain to be optimized among 132 candidates, and these locations are confined in some lattices. Furthermore, when the method is thoroughly performed, the element distribution of the SLA can be described by the plane structure in Figure 4. We can see that the positions of the selected elements are no longer confined in the lattices but randomly located around them. However, the unselected elements are still located in their initial lattices.Figure 2
The sparse linear array obtained by the IFT-DE based on a symmetrical TLA with a filling factor of 66%. (a) The convergence curve of the fitness value. (b) The optimal far-field pattern among 100 trials.
(a)
(b)Figure 3
The element locations of the symmetrical TLA with a filling factor of 66% obtained by the IFT.Figure 4
The element locations of the sparse linear array obtained by the IFT-DE based on the TLA described in Figure3.Similarly, as far as a symmetrical TLA with a filling factor of 77% is originally concerned, the far-field pattern of the best symmetrical SLA among 100 trials of IFT-DE shows 1 dB PSLL reduction compared with the report presented in [8], while the 3 dB beamwidth is almost unchanged. The third case considers an asymmetrical TLA with a filling factor equal to 39%. Figure 5(a) shows that the best sparse array is obtained at trial number 68 with the fitness value equal to −20.38 dB, about 3.0 dB lower than PSLL reported in [8]. However, the far-field pattern, as is depicted in Figure 5(b), only shows a beam-broaden about 0.254 degrees. The element locations of this SLA are described in Figure 6. It indicates that a total of 33 elements had their locations being readjusted among the 78 activated elements.Figure 5
The sparse linear array obtained by the IFT-DE based on an asymmetrical TLA with a filling factor of 39%. (a) The convergence curve of the fitness value. (b) The optimal far-field pattern among 100 trials.
(a)
(b)Figure 6
The element locations of the sparse linear array obtained by the IFT-DE based on an asymmetrical TLA with a filling factor of 39%.The fourth example assumes an asymmetrical TLA that is 69.5% filled. The obtained SLA shows about 1.16 dB PSLL decrement with no sacrifice of beamwidth, as is compared to the value presented in [8].


## 3.2. Comparing with the Reports Obtained by GA and ACO [3, 5]

We first consider synthesizing a low sidelobe symmetrical SLA based on 100 lattices, symmetrical TLA with a filling factor of 80%. The PSLL of the sparse array obtained by IFT-DE is equal to −20.52 dB, which is 1.7 dB lower than the reports using ACO [5]. More notably, when the filling factor decreased to 78% and 76%, the SLA obtained by the IFT-DE, respectively, shows PSLL decrement about 2.4 dB and 3.0 dB, as is compared to the value given by GA [3]. Furthermore, for the purpose of comparison, all the above synthesis results using the IFT-DE and that obtained by other tools are tabulated in Table 1. It indicates that through performing the proposed method, the SLA shows about 1~3 dB PSLL suppression without a notable tradeoff at the beamwidth. Therefore, the effectiveness of the IFT-DE is confirmed.Table 1
Comparative synthesizing results by using the IFT-DE and some published tools.
The structure of the SLA
Filling factor of the TLA originally obtained by the IFT (%)
PSLL (dB)
3 dB beamwidth (degree)
IFT-DE
IFT [8]
IFT-DE
IFT [8]
Symmetrical
77 (N = 200), symmetrical
−24.04
−22.92
0.58
0.588
66 (N = 200), symmetrical
−24.59
−22.86
0.68
0.685
Asymmetrical
69.5 (N = 200), asymmetrical
−25.46
−24.3
0.64
0.643
39 (N = 200), asymmetrical
−20.38
−17.33
0.8
0.546
Symmetrical
76 (N = 100), symmetrical
−23.56
−20.53 (by GA in [3])
—
78 (N = 100), symmetrical
−22.97
−20.56 (by GA in [3])
—
80 (N = 100), symmetrical
−22.2
−20.52 (by ACO in [5])
—All the aforementioned results are obtained by using a PC equipped with an 8 GB RAM as well as an Intel I7-6700 Processor that operates at 3.4 GHz, and the hardware cost is about an hour for each numerical instance.


## 4. Conclusion

The use of IFT could efficiently provide a thinned linear array with improved sidelobe performance. For the assumption that the element spacing is not less than half wavelength, most element locations of the thinned array are predetermined after performing the IFT. Therefore, the number of element locations needing to be optimized is largely reduced, which makes the solution space of DE greatly narrowed. Consequently, the low sidelobe SLA with many elements could be synthesized at relative low hardware cost. Some numerical results confirmed the effectiveness of the IFT-DE in synthesizing large SLA at a faster convergence speed. Furthermore, by simple modification, the proposed method can also be extended to 2D arrays and thereby provides a candidate way for pattern synthesis of planar sparse arrays.



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*Source: 6309192-2018-07-05.xml*