2011
DOI: 10.1109/tap.2011.2165691
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Spiral Leaky-Wave Antennas Based on Modulated Surface Impedance

Abstract: Different kinds of spiral planar circularly polarized (CP) antennas are presented. These antennas are based on an interaction between a cylindrical surface-wave excited by an omnidirectional probe and a inhomogeneous surface impedance with a spiral pattern. The surface impedance interaction transforms a bounded TM 0 surface wave into a circularly polarized leaky wave with almost broadside radiation. The problem is studied by adiabatically matching the local 2D solution of a modulated surface-impedance problem … Show more

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Cited by 262 publications
(137 citation statements)
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“…We finally note that the form of (6), whose coefficients in the TM/TE bases are functions of k ρ = |k t | only, exactly reflects the assumed rotational invariance of the homogenized metasurface. Furthermore, the non-local nature of the surface impedance dyadic is fully taken into account by its dependence with k ρ , in contrast to different approaches where the spatial dispersion is considered approximately by evaluating the impedance at a specific average wavenumber [34]. Let us now consider an omnidirectional (i.e., φ-independent) cylindrical wave with radial wavenumber k ρ propagating along the considered structure.…”
Section: Omnidirectional Homogenized Equivalent-network Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…We finally note that the form of (6), whose coefficients in the TM/TE bases are functions of k ρ = |k t | only, exactly reflects the assumed rotational invariance of the homogenized metasurface. Furthermore, the non-local nature of the surface impedance dyadic is fully taken into account by its dependence with k ρ , in contrast to different approaches where the spatial dispersion is considered approximately by evaluating the impedance at a specific average wavenumber [34]. Let us now consider an omnidirectional (i.e., φ-independent) cylindrical wave with radial wavenumber k ρ propagating along the considered structure.…”
Section: Omnidirectional Homogenized Equivalent-network Modelmentioning
confidence: 99%
“…Typical examples are Fabry-Pérot cavity antennas in which a simple source excites a parallel-plate waveguide whose upper plate is a partially-reflecting surface (PRS) [28][29][30][31]. The PRS may be a uniform dielectric medium or a periodic screen, e.g., a printed metasurface, which can be represented, in the low-frequency regime, as an equivalent uniform homogenized surface [32][33][34].…”
Section: Introductionmentioning
confidence: 99%
“…Since the elements are subwavelength in dimension, they can be used to approximate continuous hologram solutions, such as that considered early on by Oliner and Hessel [18]. The surface-wave metasurface antenna has proven to be an attractive platform for electrically large and conformal apertures [19], with many antenna variations now demonstrated [20][21][22][23][24][25]. The concept of slot arrays has also gained traction as a means of enabling beam synthesis for different applications [26,27].…”
Section: Introductionmentioning
confidence: 99%
“…The surface impedance is a continuous function in [18], so that there is no reduction to implementation in this work. That reduction to realizable structures occurred later [17,19,20] in the context of launching a surface mode that would then radiate as a collimated beam. This is an inherently different type of analysis and structure, and one that depending on a discrete surface impedance that would closely approximate a smooth, continuous function.…”
Section: Introductionmentioning
confidence: 99%
“…MTSs have also been successfully used to design and manufacture high-gain holographic antennas [6,7]. In [8], multi-layered MTSs with sub-wavelength profile were used as partial reflective surfaces to design a high-gain antenna with an enhanced bandwidth.…”
Section: Introductionmentioning
confidence: 99%