2010
DOI: 10.2528/pierb10070607
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Synthesis of Optimal Narrow Beam Low Sidelobe Linear Array With Constrained Length

Abstract: Abstract-The synthesis of optimal narrow beam low sidelobe linear array is addressed. Only the length of the array is constrained. The number, the positions and the weightings of the elements are left free. It is proven, that the optimal design is always an array with a small number of elements. One first demonstrates that among equally spaced linear arrays of given length, the sparsest Dolph-Chebyshev design, i.e., the one with the largest admissible inter-element distance, is the optimal one. Then, the restr… Show more

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Cited by 2 publications
(3 citation statements)
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“…A n e jkx n sin(θ) (2) where θ is the observation angle, k the free space propagation constant, A n and x n are respectively the complex amplitude and the position of the nth element, with x 1 = −a for simplicity (see Figure 1). So, x N + a can be considered as the total size of the aperture array.…”
Section: Aperiodic Array Studymentioning
confidence: 99%
See 1 more Smart Citation
“…A n e jkx n sin(θ) (2) where θ is the observation angle, k the free space propagation constant, A n and x n are respectively the complex amplitude and the position of the nth element, with x 1 = −a for simplicity (see Figure 1). So, x N + a can be considered as the total size of the aperture array.…”
Section: Aperiodic Array Studymentioning
confidence: 99%
“…In particular, works on array synthesis methods, based on deterministic procedures [1,2] or on heuristic search methods [3,4], are addressed. Usually, these techniques are focused on the array factor synthesis, assuming ideal isotropic radiators separated a distance close to half of a wavelength.…”
Section: Introductionmentioning
confidence: 99%
“…This synthesis problem can be solved by means of the classical solution from Dolph-Chebyshev [14] to achieve the minimum beamwidth for the chosen SLL; this kind of excitation, together with equal spacing among elements, has previously shown to provide almost optimal patterns [18]. For a Dolph-Chebyshev excitation, in the case of d E = λ/2, the value of u 1 can be calculated as:…”
Section: Equispaced Arrays As Referencementioning
confidence: 99%