2019
DOI: 10.1016/j.jqsrt.2018.11.028
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Engineering mode hybridization in regular arrays of plasmonic nanoparticles embedded in 1D photonic crystal

Abstract: We analytically and numerically study coupling mechanisms between 1D photonic crystal (PhC) and 2D array of plasmonic nanoparticles (NPs) embedded in its defect layer. We introduce general formalism to explain and predict the emergence of PhC-mediated Wood-Rayleigh anomalies, which spectral positions agree well with the results of exact simulations with Finite-Difference Time-Domain (FDTD) method. Electromagnetic coupling between localized surface plasmon resonance (LSPR) and PhC-mediated Wood-Rayleigh anomali… Show more

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Cited by 27 publications
(8 citation statements)
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“…All kinds of photonic crys- * Ilia.Fradkin@skoltech.ru tals and metasurfaces were studied intensively for the last several decades, and their optical properties are known in much detail. In recent years there was a growth of attention to stacks of metasurfaces [29][30][31][32][33][34][35][36][37][38] due to the new opportunities that they provide for the control and manipulation of light. Simultaneously, much fewer studies considered the interaction of crystals that do not have a mutual lattice either because of the periods discrepancy or even misalignment of crystallographic axes.…”
Section: Introductionmentioning
confidence: 99%
“…All kinds of photonic crys- * Ilia.Fradkin@skoltech.ru tals and metasurfaces were studied intensively for the last several decades, and their optical properties are known in much detail. In recent years there was a growth of attention to stacks of metasurfaces [29][30][31][32][33][34][35][36][37][38] due to the new opportunities that they provide for the control and manipulation of light. Simultaneously, much fewer studies considered the interaction of crystals that do not have a mutual lattice either because of the periods discrepancy or even misalignment of crystallographic axes.…”
Section: Introductionmentioning
confidence: 99%
“…In this case, a majority of NPs are excited with the same phase, which results in ultra-narrow high-Q spectral features. CLRs have been well studied for nanostructures from plasmonic NPs for a long time [44][45][46][47][48][49][50][51][52][53][54][55][56], while the all-dielectric analogues have gained attention only a decade ago [57]. In contrast to plasmonic NPs (in most of the cases characterized by weak magnetic and strong electric responses), all-dielectric NPs with pronounced electric and magnetic optical resonances [58] give rise to a rich variety of tunable CLRs that emerge even in regular rectangular-shaped arrays [32].…”
Section: Introductionmentioning
confidence: 99%
“…[1,2] Plasmonic materials are widely used in applications such as water splitting, [3] photovoltaic cells, [1,[4][5][6][7] plasmon lasers, [8] chemical synthesis, [9] high-resolution imaging, [10] and biomedical and telecom applications. [11][12][13][14] LSP resonance is also actively utilized for nanoscale chemical and biological sensing. [15][16][17][18] The sensor properties are conditioned here by the high sensitivity of the surface resonant frequency (SRF) to the permittivity of the surrounding chemical environment, which leads to the frequency shifting, for example, due to chemical adsorption.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore, there are a variety of different forms of plasmonic materials, such as individual NPs of different shapes and materials [20] and 2D lattices. [11][12][13]21] A presence of conductive material between two NPs leads to the emergence of a new mode, called the charge transfer plasmon (CTP), where the charge periodically moves between two NPs along a conductive bridge. For example, CTP was experimentally observed in a system consisting of two Au NPs linked by a thick gold bridge of radius %10 to 20 nm.…”
Section: Introductionmentioning
confidence: 99%