Formulas and results for optimizing Fabry–Perot cavity antennas (FPCAs) are examined, for structures excited by either an HMD or VED source. The HMD source can produce a narrow pencil beam at broadside, while the VED source can produce a narrow null pattern at broadside. The effects of the aperture truncation on the nullwidth and beamwidth properties are also taken into account.
Optimization of Fabry–Perot Cavity Antennas having Horizontal or Vertical Dipole Sources
Fuscaldo W.
Primo
;
2024
Abstract
Formulas and results for optimizing Fabry–Perot cavity antennas (FPCAs) are examined, for structures excited by either an HMD or VED source. The HMD source can produce a narrow pencil beam at broadside, while the VED source can produce a narrow null pattern at broadside. The effects of the aperture truncation on the nullwidth and beamwidth properties are also taken into account.File in questo prodotto:
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Fuscaldo_NRSM2024_opt2DLWAs.pdf
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