1987
DOI: 10.1109/tap.1987.1144224
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An improved thinning method for density tapering of planar array antennas

Abstract: SEIJI MANO, TAKASHI KATAGI, AND MOT00 MIZUSAWA Abstruct-A thinning method is presented to realize the desired aperture distribution in a planar array antenna with elements fiied on an array lattice. In this method elements to be excited are determined by qnantizing cumulative weights which are calculated from the desired aperture distribution. At f i t , this method is applied to density tapering on orthogonal axes of a planar array. Radiation patterns of the planar array determined by this method are compared… Show more

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Cited by 22 publications
(8 citation statements)
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“…Consider a phased array in which an amplitude distribution is produced on the antenna aperture by the use of multiple excitation amplitude ratios or of a variable density arrangement of the elements such as a thinned array [8]. Figure 4 shows the amplitude of each element antenna at coordinate x m as well as the total amplitude on the right half of the phased array.…”
Section: Array With Amplitude Distributionmentioning
confidence: 99%
“…Consider a phased array in which an amplitude distribution is produced on the antenna aperture by the use of multiple excitation amplitude ratios or of a variable density arrangement of the elements such as a thinned array [8]. Figure 4 shows the amplitude of each element antenna at coordinate x m as well as the total amplitude on the right half of the phased array.…”
Section: Array With Amplitude Distributionmentioning
confidence: 99%
“…Till now, only a few studies have addressed this topic [ 17 , 19 , 20 , 21 , 22 , 23 ]. Even so, they are all implemented in a very similar statistical way.…”
Section: Introductionmentioning
confidence: 99%
“…However it is not optimum and in that it does not ensure that peak side lobes are maintained bellow a given level. In [9] a thinning method is presented to realize the desired aperture distribution in a planar array antenna with elements fixed on an array lattice. In this method elements to be excited are determined by quantizing cumulative weights which are calculated from the desired aperture distribution.…”
Section: Introductionmentioning
confidence: 99%
“…{x n det = ((−N/2) : 1 : (N/2))/N} (8) {x n rand = rn = −1/2 + rand(1, N)}(9) and each of the two workspaces operates over the interval[−1/2, 1/2]. Equation (8) means a uniform spacing with N elements in [−1/2, 1/2].…”
mentioning
confidence: 99%