2019
DOI: 10.1109/tap.2019.2922730
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Higher-Order Cylindrical Leaky Waves—Part I: Canonical Sources and Radiation Formulas

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Cited by 18 publications
(10 citation statements)
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“…It is worth to recall here that a simple source, such as a vertical electric dipole (VED), in a partially-open 2-D uniform planar waveguide made of ordinary materials can excite a forward, fast (i.e., 0 < β ρ < k 0 ) cylindrical leaky wave [45,46], thus giving rise to an outward cylindrical aperture distribution (which cannot focus radiation around the axis of symmetry), instead of the required inward one. However, if a radially periodic grating is placed on top of the structure, the period can be selected in order to have the n = −1 Floquet harmonic (note that the radially periodic nature of the grating allows for describing the electromagnetic field in terms of a complete infinite set of Floquet harmonics) radiating with a specific angle at a given frequency.…”
Section: Bessel Beams Leaky-wave Bessel Beams Bessel-gauss Beamsmentioning
confidence: 99%
“…It is worth to recall here that a simple source, such as a vertical electric dipole (VED), in a partially-open 2-D uniform planar waveguide made of ordinary materials can excite a forward, fast (i.e., 0 < β ρ < k 0 ) cylindrical leaky wave [45,46], thus giving rise to an outward cylindrical aperture distribution (which cannot focus radiation around the axis of symmetry), instead of the required inward one. However, if a radially periodic grating is placed on top of the structure, the period can be selected in order to have the n = −1 Floquet harmonic (note that the radially periodic nature of the grating allows for describing the electromagnetic field in terms of a complete infinite set of Floquet harmonics) radiating with a specific angle at a given frequency.…”
Section: Bessel Beams Leaky-wave Bessel Beams Bessel-gauss Beamsmentioning
confidence: 99%
“…1(b)], the vertical z-component of the magnetic vector potential A has a sin φ variation along the azimuthal plane. Although in principle, cylindrical waves with higher order φ variation could be treated (see, e.g., [36], [37], [38]), the n = 0 (for the cases with azimuthal symmetry) and n = 1 modes are the most important since elementary electric and magnetic dipoles within layered media will excite only these wave types [35]. An HMD excites both TE and TM waves that can initially be studied separately and then added together.…”
Section: Theoretical Approachmentioning
confidence: 99%
“…In a 2D-LWA excited by a finite three-dimensional (3D) source, the field distribution is mainly described by cylindrical leaky waves that propagate in the transverse plane with a complex radial wavenumber k ρ = β ρ − jα ρ , where β ρ and α ρ are the phase and the leakage constant, respectively [25]. It is worthwhile recalling here that β ρ is intimately related to the axicon angle θ 0 (which entirely defines the focusing properties of Bessel beams [21]) through the well-known ray-optics formula β ρ /k 0 = sin θ 0 [26].…”
Section: The Leaky-wave Approachmentioning
confidence: 99%