2011
DOI: 10.1103/physrevlett.107.133901
|View full text |Cite
|
Sign up to set email alerts
|

Funneling Light through a Subwavelength Aperture with Epsilon-Near-Zero Materials

Abstract: We present a comprehensive study of enhanced light funneling through a subwavelength aperture with realistic (lossy) epsilon-near-zero (ENZ) materials. We realize experimentally an inclusion-free ENZ material layer operating at optical frequencies and characterize its performance. An analytical expression describing light funneling through several structures involving ENZ coupling layers is developed, validated with numerical solutions of Maxwell equations, and utilized to relate the performance of the ENZ cou… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

2
97
1
2

Year Published

2012
2012
2020
2020

Publication Types

Select...
10

Relationship

0
10

Authors

Journals

citations
Cited by 155 publications
(102 citation statements)
references
References 28 publications
2
97
1
2
Order By: Relevance
“…For noblemetal plasmonic structures, the electrostatic resonances tend to occur in the visible and near-IR, with Q in the 20-40 range, depending on the particular data set and material, corresponding to modal lifetimes on the order of 10 fs. In doped III-V semiconductors such as GaAs, InAs, and various alloys, the modal lifetime can be as long as 100 fs, but the typical operating wavelengths are near 10 μm [29,118,119]. As a result, no improvement in the Q over the metallic case is expected.…”
Section: The Promise Of Phonon Polaritons: a Comparison With Plasmonicsmentioning
confidence: 99%
“…For noblemetal plasmonic structures, the electrostatic resonances tend to occur in the visible and near-IR, with Q in the 20-40 range, depending on the particular data set and material, corresponding to modal lifetimes on the order of 10 fs. In doped III-V semiconductors such as GaAs, InAs, and various alloys, the modal lifetime can be as long as 100 fs, but the typical operating wavelengths are near 10 μm [29,118,119]. As a result, no improvement in the Q over the metallic case is expected.…”
Section: The Promise Of Phonon Polaritons: a Comparison With Plasmonicsmentioning
confidence: 99%
“…As one such example, the use of heavily doped semiconductors as ENZ materials was demonstrated to enhance the transmission of light through subwavelength apertures. 50,51 For any bulk ENZ material, we can describe wave propagation with a complex wavevector, k ¼ ω ffiffiffiffiffi εμ p , which effectively determines the propagation length and local wavelength of light at ENZ frequencies. Assuming μ ¼ μ o (as we will throughout this paper), we can gain an effective measure of the quality of any bulk ENZ material by determining the imaginary component (κ) of the complex refractive index (n ∼ ¼ n þ iκ) at the wavelength λ ENZ , where the real part of the refractive index is minimum ½nð∼λ ENZ Þ.…”
Section: Enz Materialsmentioning
confidence: 99%
“…The refractive index of a metamaterial can be tailored to be negative, 13 close to zero, [14][15][16][17][18][19] 12,21,22 Among various metamaterials, zero-index-metamaterial (ZIM, n = 0), was first presented by Enoch et al 23 in 2002, and has received consistent attention in the microwave, 24,25 THz, 26,27 optics, 14,28 and even acoustics. 29 According to Snell's Law of refraction between two media (n 1 sin θ 1 = n 2 sin θ 2 ), if one medium is a ZIM with n 1 = 0 and the other one has n 2 = 0, then whatever the incident angle θ 1 is, the refraction angle θ 2 will trend to zero.…”
Section: Introductionmentioning
confidence: 99%