2021
DOI: 10.1038/s41565-020-00841-9
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Fano-resonant ultrathin film optical coatings

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Cited by 63 publications
(61 citation statements)
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“…Introduction of loss in the film modifies the phases as shown by solid lines in Figure 4a. The plot demonstrates that in the ITER regime, the reflection phase at the top interface plays a dominant role in determining resonant interferences, which require ϕ 12 ¼ ϕ d , in contrast to those in Fabry-Perot resonances (which is determined by propagation phase in the film) and the previously investigated ultrathin film interferences [11][12][13][14][15][16][17][18][19][20] dominated by reflection phase at the bottom interface. Figure 4b plots the variation in magnitudes of r 12 and e 2iδ for real and lossless ENZ.…”
Section: Spectral and Angular Characteristics Of Infrared Absorptionmentioning
confidence: 90%
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“…Introduction of loss in the film modifies the phases as shown by solid lines in Figure 4a. The plot demonstrates that in the ITER regime, the reflection phase at the top interface plays a dominant role in determining resonant interferences, which require ϕ 12 ¼ ϕ d , in contrast to those in Fabry-Perot resonances (which is determined by propagation phase in the film) and the previously investigated ultrathin film interferences [11][12][13][14][15][16][17][18][19][20] dominated by reflection phase at the bottom interface. Figure 4b plots the variation in magnitudes of r 12 and e 2iδ for real and lossless ENZ.…”
Section: Spectral and Angular Characteristics Of Infrared Absorptionmentioning
confidence: 90%
“…Such homogeneous ultrathin films are attractive for applications in coloring, filtering, absorption enhancement in photovoltaic applications, infrared absorbers and emitters, and in reconfigurable flat optics. [11][12][13][14][15][16][17][18][19][20] Epsilon-near-zero (ENZ) materials are one such class of thin film materials that have gained much interest in recent times. [21,22] The real part of permittivity (ε 0 ) of ENZ materials becomes zero at the zero-epsilon wavelength (λ ZE ), such that ε 0 is positive (negative) at shorter (longer) wavelengths.…”
Section: Introductionmentioning
confidence: 99%
“…[1][2][3] In particular thin-film metamaterials, metamaterials with varied material composition restricted to a single axis, have garnered widespread attention in the photonics community and are commonly utilized in applications such as optical coatings and sensors. 4,5 The engineered design of metamaterials sustaining a desired optical response in a given spectral range, termed inverse design (ID), is the basis for most optical applications. Successful metamaterial design requires the exploration of the global materials parameter space to engineer an optimized response.…”
Section: Introductionmentioning
confidence: 99%
“…As a parallel research direction in nanophotonics, flat optics, including planar multilayer thin-film coatings, have also been extensively studied to exhibit various functionalities in spectral engineering, with large-area fabrication and simpler flat architecture. [6,[17][18][19] For example, typical metal-insulator-metal (MIM) nanocavity has been widely used to design color filters or perfect absorbers in the visible frequencies for transmission/reflection mode. [20][21][22][23] Based on the spectral characteristics of MIM patterns and grayscale exposure, [24] numerous studies have shown the micro-image nanoprinting functionality and the great potential in information storage/encryption at the nanoscale.…”
mentioning
confidence: 99%