2016
DOI: 10.1109/tap.2016.2608934
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Design Formulas for Planar Fabry–Pérot Cavity Antennas Formed by Thick Partially Reflective Surfaces

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Cited by 16 publications
(11 citation statements)
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“…The use of lens antennas allows to efficiently achieve larger gains >30 dBs, over larger bandwidths (>20%) in comparison with other more resonant antenna solutions, such as Fabry-Perot [3], metasurfaces [4], or transmitarrays [5]. Moreover, the lens-steering capability enables the generation of simultaneous multiple beams pointing in different directions with planar Fly's eye lens array panels, as displayed in Fig.…”
Section: Introductionmentioning
confidence: 99%
“…The use of lens antennas allows to efficiently achieve larger gains >30 dBs, over larger bandwidths (>20%) in comparison with other more resonant antenna solutions, such as Fabry-Perot [3], metasurfaces [4], or transmitarrays [5]. Moreover, the lens-steering capability enables the generation of simultaneous multiple beams pointing in different directions with planar Fly's eye lens array panels, as displayed in Fig.…”
Section: Introductionmentioning
confidence: 99%
“…As the grid can be considered as a partially reflecting surface (PRS) for poor polarization waves, Then, a certain height h a is required to compensate the phases of the reflecting surfaces. [39][40][41] However, as the xand y-polarizations radiated from the MZR-MA have different phases, the equation should be modified as the following: where Δφ x-y is the phase difference between the X-and Ypolarizations radiated from the MZR-MA, φ PF is the reflection phase of the X-polarization of the PF, φ MZR-MA is the reflection phase of X-to-Y polarization at the MZR-MA. Moreover, as the PCR is medium (not large), multiple reflection would be occurred resonant cavity between the PF and the MZR-MA, which forms a resonant cavity.…”
Section: Operational Process and Discussionmentioning
confidence: 99%
“…As the grid can be considered as a partially reflecting surface (PRS) for poor polarization waves, Then, a certain height h a is required to compensate the phases of the reflecting surfaces 39‐41 . However, as the x ‐ and y ‐polarizations radiated from the MZR‐MA have different phases, the equation should be modified as the following: normalΔφ=normalΔφxy+φPF+φitalicMZRitalicMA4πhafc=2italicNπ,normalN=0,1,2, where Δφ x‐y is the phase difference between the X ‐ and Y ‐polarizations radiated from the MZR‐MA, φ PF is the reflection phase of the X ‐polarization of the PF, φ MZR‐MA is the reflection phase of X ‐to‐ Y polarization at the MZR‐MA.…”
Section: Mechanisms and Approachmentioning
confidence: 99%
“…The associate editor coordinating the review of this manuscript and approving it for publication was Santi C. Pavone . performance in different aspects, including the optimization analysis [2]- [4], theoretical interpretation [5]- [8], and optimization design [9]- [12]. Many properties can be achieved with FP antennas, such as low profile [9], multi-band [10], circular polarization [11], RCS reduction [12], reconfigurable [13]- [15] and wideband [16] operation.…”
Section: Introductionmentioning
confidence: 99%