2016 10th European Conference on Antennas and Propagation (EuCAP) 2016
DOI: 10.1109/eucap.2016.7481401
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A new method for the design of slot antenna arrays: Theory and experiment

Abstract: Abstract-The present paper proposes and validates a new general design methodology that can be used to automatically find proper positions and orientations of waveguide-based radiating slots capable of realizing any given radiation beam profile. The new technique combines basic radiation theory and waveguide propagation theory in a novel analytical model that allows the prediction of the radiation characteristics of generic slots without the need to perform full-wave numerical solution. The analytical model is… Show more

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Cited by 7 publications
(5 citation statements)
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“…An array of IDs are located at ( x d , y d , z d ) and they are oriented along the angle ( θ d , ϕ d ). At an observation point ( x , y , z ), the $\vec{ E }$ and $\vec{ H }$ fields radiated by an array of N magnetic IDs can be expressed as [30–34], bold-italicE(bold-italicr)=falsefalsen=1Ncoko24π(bold-italicnbold-italicn×bold-italicpbold-italicn).enormaljkornrn bold-italicH(bold-italicr)=falsefalsen=1N14πϵo(ko2.(bold-italicnbold-italicn×bold-italicpbold-italicn)×bold-italicnbold-italicn).enormaljkornrn where c o is the speed of light in vacuum, k o is the free space wave‐number and n n represents the unit vector from the n th ID location to an observation point, and it can be expressed as bold-italicnbold-italicn=()xxd(n)rn,yyd(n)rn,zzd...…”
Section: Single Antenna Element Designmentioning
confidence: 99%
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“…An array of IDs are located at ( x d , y d , z d ) and they are oriented along the angle ( θ d , ϕ d ). At an observation point ( x , y , z ), the $\vec{ E }$ and $\vec{ H }$ fields radiated by an array of N magnetic IDs can be expressed as [30–34], bold-italicE(bold-italicr)=falsefalsen=1Ncoko24π(bold-italicnbold-italicn×bold-italicpbold-italicn).enormaljkornrn bold-italicH(bold-italicr)=falsefalsen=1N14πϵo(ko2.(bold-italicnbold-italicn×bold-italicpbold-italicn)×bold-italicnbold-italicn).enormaljkornrn where c o is the speed of light in vacuum, k o is the free space wave‐number and n n represents the unit vector from the n th ID location to an observation point, and it can be expressed as bold-italicnbold-italicn=()xxd(n)rn,yyd(n)rn,zzd...…”
Section: Single Antenna Element Designmentioning
confidence: 99%
“…An array of IDs are located at (x d , y d , z d ) and they are oriented along the angle (θ d , ϕ d ). At an observation point (x, y, z), the $\vec{ E }$ and $ \vec{ H }$ fields radiated by an array of N magnetic IDs can be expressed as [30][31][32][33][34],…”
Section: Introductionmentioning
confidence: 99%
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“…Finally, we add that the theory presented in this paper can be expanded to include larger antennas by aggregating the effects of individual infinitesimal dipoles using the Infinitesimal Dipole Model (IDM) technique, which is an electromagnetic machine learning capable of learning from NF or FF data the best small dipole model capable of representing radiation everywhere in the exterior domain [73][74][75][76][77][78][79][80][81]. The details of this expansion will be the subject of future work.…”
Section: Transmitter Receivermentioning
confidence: 99%
“…In this way, there is no need to find the slot impedance or to consider the total impedance matrix of the entire slot array as has been done so far in the literature. Preliminary results about the synthesis of a slotted waveguide using this new technique have been reported in Reference 16. In the present article, we first develop a general theoretical treatment of coupled radiating slots using the surface equivalence theorem and a new magnetic‐type current Green's function.…”
Section: Introductionmentioning
confidence: 99%