2018
DOI: 10.1103/physrevb.97.115447
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Near-perfect conversion of a propagating plane wave into a surface wave using metasurfaces

Abstract: In this paper theoretical and numerical studies of perfect/nearly perfect conversion of a plane wave into a surface wave are presented. The problem of determining the electromagnetic properties of an inhomogeneous lossless boundary which would fully transform an incident plane wave into a surface wave propagating along the boundary is considered. An approximate field solution which produces a slowly growing surface wave and satisfies the energy conservation law is discussed and numerically demonstrated. The re… Show more

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Cited by 45 publications
(37 citation statements)
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“…the unit cells, and inherit the unique properties of their 3D counterparts while minimizing bulkiness, losses, and cost. Functionalities such as beam steering, focusing, vorticity control, or RCS reduction have been demonstrated across the spectrum, from microwaves [6]- [8] to terahertz [9]- [13], or optical frequencies [14], [15].…”
Section: Introductionmentioning
confidence: 99%
“…the unit cells, and inherit the unique properties of their 3D counterparts while minimizing bulkiness, losses, and cost. Functionalities such as beam steering, focusing, vorticity control, or RCS reduction have been demonstrated across the spectrum, from microwaves [6]- [8] to terahertz [9]- [13], or optical frequencies [14], [15].…”
Section: Introductionmentioning
confidence: 99%
“…Since X 12 = X 21 , the impedance matrix (3) corresponds to a nonreciprocal and locally active or lossy metasurface. Equation (2) has other thenZ = iX forms of solutions, as it was shown in [37] for an anisotropic metasurface. However, for any exact solution, one arrives at the same conclusion: The impedance matrix corresponds to either reciprocal or nonreciprocal but always locally active or lossy metasurface.…”
Section: A Impedance Matrix Of An Ideal Convertermentioning
confidence: 74%
“…Recently, Tcvetkova et al have for the first time rigorously studied the problem of conversion of an incident plane wave into a surface wave with a growing amplitude [37] by means of a reflecting anisotropic metasurface (described by tensor surface parameters). The incident plane wave and the surface wave had orthogonal polarizations in order to avoid interference resulting in the requirement of "loss-gain" power flow into the metasurface [35,36].…”
Section: Introductionmentioning
confidence: 99%
“…Assuming first that r ∈ Ω + and letting r = |r|(cos θ, sin θ), θ ∈ (−π, 0) ∪ (0, π), we have that the resulting reflected and transmitted fields in (42) can be expressed as…”
Section: Generalized Laws Of Reflection and Transmissionmentioning
confidence: 99%