2016
DOI: 10.1364/josab.33.000468
|View full text |Cite
|
Sign up to set email alerts
|

Defect modes in metamaterial photonic superlattices as tunneling resonances in trilayer structures

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
5
0

Year Published

2016
2016
2021
2021

Publication Types

Select...
7

Relationship

1
6

Authors

Journals

citations
Cited by 9 publications
(5 citation statements)
references
References 33 publications
0
5
0
Order By: Relevance
“…Comparative analysis between measured and calculated values of λ RB using eq reveals a residual deviation that oscillates between 0.1 and 5%, which demonstrates the suitability of our model to tune the position of the resonance band of NAA−μQVs by the input anodization period in the STPA profile. To further validate our model, a custom-built MATLAB application using the TMM approach was used to generate simulated optical spectra of NAA−μQVs, using experimentally quantified values of n eff–max , n eff–min , and λ RB as inputs. Details of the TMM implementation used to develop this application for NAA−μQVs considering resonance bands in photonic crystal structures in terms of bound states for a quarter quarter-wave-stack in air are provided in the Supporting Information. , Figure S4 (Supporting Information) shows the resulting simulated optical spectra of NAA−μQVs. At first glance, it is apparent that simulated optical spectra of NAA−μQVs feature resonance bands of higher quality than those of experimental NAA−μQVs, and more well-resolved photonic stopbands with reverberant, pronounced sidelobes.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Comparative analysis between measured and calculated values of λ RB using eq reveals a residual deviation that oscillates between 0.1 and 5%, which demonstrates the suitability of our model to tune the position of the resonance band of NAA−μQVs by the input anodization period in the STPA profile. To further validate our model, a custom-built MATLAB application using the TMM approach was used to generate simulated optical spectra of NAA−μQVs, using experimentally quantified values of n eff–max , n eff–min , and λ RB as inputs. Details of the TMM implementation used to develop this application for NAA−μQVs considering resonance bands in photonic crystal structures in terms of bound states for a quarter quarter-wave-stack in air are provided in the Supporting Information. , Figure S4 (Supporting Information) shows the resulting simulated optical spectra of NAA−μQVs. At first glance, it is apparent that simulated optical spectra of NAA−μQVs feature resonance bands of higher quality than those of experimental NAA−μQVs, and more well-resolved photonic stopbands with reverberant, pronounced sidelobes.…”
Section: Resultsmentioning
confidence: 99%
“…36−38 Details of the TMM implementation used to develop this application for NAA−μQVs considering resonance bands in photonic crystal structures in terms of bound states for a quarter quarter-wave-stack in air are provided in the Supporting Information. 42,43 Figure S4 (Supporting Information) shows the resulting simulated optical spectra of NAA−μQVs. At first glance, it is apparent that simulated optical spectra of NAA−μQVs feature resonance bands of higher quality than those of experimental NAA−μQVs, and more well-resolved photonic stopbands with reverberant, pronounced sidelobes.…”
Section: Introductionmentioning
confidence: 99%
“…In order to explain this behavior, we want to mention that it has been recently shown that defect modes behave in an analogous way to the bounded states in a quantum well. 43 Thus, in the region near ν T the dielectric permittivity of the polaritonic material reach very high values and the system behave as a very depth quantum well, which in the limit of n → ∞ will have infinite localized modes, of the form ϕ m = sin(ω m x), in the polaritonic layer, as it was previously shown from a tight-binding model. 23 With availability of metamaterials having unnaturally occurring high refractive indexes, 44 the present proposal is not limited to the inclusion of a polaritonic material as the defect layer.…”
Section: Accepted Manuscriptmentioning
confidence: 62%
“…Note that this approach is only valid for heterostructures with building layer thicknesses below λ/10 [34], where λ is the incident wavelength. Since all the thicknesses for ZnO and Al 2 O 3 layers in this work fulfill the condition < λ/10, the approach could be used to retrieve the corresponding refractive indexes.…”
Section: Resultsmentioning
confidence: 99%