2020
DOI: 10.1364/oe.395223
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Reflectionless zero refractive index metasurface in the terahertz waveband

Abstract: Zero refractive index materials behave electromagnetically as single points despite the finite dimensions because a propagating electromagnetic wave passes with an infinite phase velocity. However, the composition of naturally occurring materials cannot produce a zero refractive index material because any effect of both of the dielectric and magnetic properties would have to vanish (be near zero). In this report, we demonstrate a zero refractive index metasurface with a refractive index of 0.16 + j0.09, the re… Show more

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Cited by 23 publications
(7 citation statements)
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“…We can see that at 0.225 THz, the effective permittivity is 0.12−0.002j, and the permeability is 0.11+0.001j, so the effective impedance is close to 1. In the range of 0.23 THz ∼ 0.24 THz, the effective permittivity and permeability are close to zero, as shown in the shaded part, and some scholars have found that near-zero refractive index materials have the characteristics of high transmittance [18]. There are zero refractive indexes near 0.225 THz, which is the representation for the maximum transmittance of metamaterials.…”
Section: Metamaterials and Designmentioning
confidence: 87%
“…We can see that at 0.225 THz, the effective permittivity is 0.12−0.002j, and the permeability is 0.11+0.001j, so the effective impedance is close to 1. In the range of 0.23 THz ∼ 0.24 THz, the effective permittivity and permeability are close to zero, as shown in the shaded part, and some scholars have found that near-zero refractive index materials have the characteristics of high transmittance [18]. There are zero refractive indexes near 0.225 THz, which is the representation for the maximum transmittance of metamaterials.…”
Section: Metamaterials and Designmentioning
confidence: 87%
“…Consequently, our initial attempt to achieve a via-less magnetic dipole response was to simply use the magnetic dipole antenna arising from the Huygens dipole antenna design in [15], remove the EAD NFRP element, and then remove all four vias of the CLL NFRP elements. It was anticipated that this would be successful because of the vaunted first magnetic optical metamaterial based on two parallel conducting strips [20], a concept that has been extended recently to attain a matched zero refractive index metasurface in the terahertz band [21]. However, it was unsuccessful for the following reasons.…”
Section: Operating Principlementioning
confidence: 99%
“…2(b) was assessed with a plane wave excitation of the equivalent two passive strip configuration, i.e., with them as scatterers. This model represents one unit cell of the infinite metasurface constructs considered in [20], [21]. Since the electric quadrupolar response was realized in the finite antenna design rather than a magnetic dipole one upon which those works were based, quadrupolar scattering results would also represent an additional contribution, i.e., one to the fundamental understanding of how finite electromagnetic metastructure designs actually work.…”
Section: Appendix a Two Passive Strips With Plane Wave Excitationmentioning
confidence: 99%
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“…Contrarily, metamaterials yield both negative permittivity and negative permeability or either trait can be negative by itself. An engineered structure indicating both negative permittivity and permeability is called a double negative (DNG) metamaterial, while a structure manifesting either negative value is called a single negative (SNG) metamaterial [ 1 , 2 ]. DNG and SNG metamaterials are extensively used in different technological developments.…”
Section: Introductionmentioning
confidence: 99%