1981
DOI: 10.1109/tap.1981.1142602
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Determination of phase functions for a desired one-dimensional pattern

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Cited by 44 publications
(10 citation statements)
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“…In particular, we selected two types of array factors forφ DES (u): the sector and the cosecant patterns. These are more complex than the relatively simple multi-beams addressed in [4] and are often employed in literature as reference for the introduction of continuous source and uniformly-spaced unequally-excited arrays synthesis methods [13,14]. Let us start by the sector-pattern case.…”
Section: Numerical Analysismentioning
confidence: 99%
“…In particular, we selected two types of array factors forφ DES (u): the sector and the cosecant patterns. These are more complex than the relatively simple multi-beams addressed in [4] and are often employed in literature as reference for the introduction of continuous source and uniformly-spaced unequally-excited arrays synthesis methods [13,14]. Let us start by the sector-pattern case.…”
Section: Numerical Analysismentioning
confidence: 99%
“…In [11], the stationary-phase method was used to derive 1D phase functions for phase-only synthesis of the principleplane radiation pattern from a circular phased array aperture of radius R. That work focused on two specific one-dimensional pattern shapes: a sector beam and a cosecant beam. For a sector beam having uniform pattern amplitude for − …”
Section: B Initializationmentioning
confidence: 99%
“…1. Approximation of the desired cosecant pattern obtained using Chakraborty's [11] derived phase-functions for a circular array with radius R = 10λ. Here, we approximate the pattern using the product of a horizontal sector beam (shown on left) and a vertical cosecant amplitude distribution (shown in the center).…”
Section: Examplementioning
confidence: 99%
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“…Also, is the number of displaced nulls in the right hand side and is the number of displaced nulls in the left hand side. If nulls can be calculated, the Fourier expansion method as applied in [11] can be used to write and as (11) and then substituting (11) in (8) gives (12) where, the integral in (12) for is zero and for reduces to (13) Since is zero for or , then applying (13) to (11) leads to a truncated Fourier series as (14) and…”
Section: B Desired Pattern Synthesis With Pattern's Null Manipulationmentioning
confidence: 99%