2019 IEEE International Conference on Microwaves, Antennas, Communications and Electronic Systems (COMCAS) 2019
DOI: 10.1109/comcas44984.2019.8958421
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Retrieval of Polarizability Matrix for Metamaterials

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Cited by 4 publications
(2 citation statements)
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“…E pq (θ, φ)Γ t pq e j(kc((p−1)dx sin θ cos φ+(q−1)dy sin θ sin φ)) , (8) where θ and φ denote angles in spherical coordinates, E pq (θ, φ) is the pattern response, and k c = 2π λ c is the wavenumber. We scan the reflected beam by coding the RI-MTS with a progressively varying phase shift.…”
Section: Meta-atom Design For Im Transceiversmentioning
confidence: 99%
See 1 more Smart Citation
“…E pq (θ, φ)Γ t pq e j(kc((p−1)dx sin θ cos φ+(q−1)dy sin θ sin φ)) , (8) where θ and φ denote angles in spherical coordinates, E pq (θ, φ) is the pattern response, and k c = 2π λ c is the wavenumber. We scan the reflected beam by coding the RI-MTS with a progressively varying phase shift.…”
Section: Meta-atom Design For Im Transceiversmentioning
confidence: 99%
“…Lately, TMAA based on metasurfaces (MTSs) have drawn significant interest in the engineering community [5] because of their ability to control and manipulate electromagnetic (EM) waves in a sub-wavelength thickness through modified boundary conditions [6,7]. The MTS, viewed as a two-dimensional (2-D) equivalent of metamaterials (MTMs), is a synthetic electromagnetic (EM) surface composed of sub-wavelength patches, or meta-atoms, printed on one or more dielectric substrate layers [8]. Through careful engineering of each meta-atom, MTSs can transform an incident EM wave into an arbitrarily tailored transmitted or reflected wavefront [9][10][11][12].…”
Section: Introductionmentioning
confidence: 99%