Collective spontaneous emission and strong coupling in semiconductor hyperbolic metamaterials

Author(s):  
Prashant Shekhar ◽  
Zubin Jacob
2020 ◽  
Vol 4 (1) ◽  
pp. 9
Author(s):  
Vasilios Karanikolas ◽  
Ioannis Thanopulos ◽  
Emmanuel Paspalakis

Two-dimensional materials allow for extreme light confinement, thus becoming important candidates for all optical application platforms.  [...]


2014 ◽  
Vol 9 (1) ◽  
pp. 48-53 ◽  
Author(s):  
Dylan Lu ◽  
Jimmy J. Kan ◽  
Eric E. Fullerton ◽  
Zhaowei Liu

Author(s):  
Harish N S Krishnamoorthy ◽  
Zubin Jacob ◽  
Evgenii Narimanov ◽  
Ilona Kretzschmar ◽  
Vinod M. Menon

2013 ◽  
Vol 114 (13) ◽  
pp. 134306 ◽  
Author(s):  
K. V. Sreekanth ◽  
T. Biaglow ◽  
G. Strangi

2021 ◽  
Vol 3 ◽  
Author(s):  
Manuel Rodrigues Gonçalves

Thin films of noble metals with thickness smaller than the wavelength of light constitute one of the most investigated structures in plasmonics. The fact that surface plasmon modes can be excited in these films by different ways and the simplicity of fabrication offer ideal conditions for applications in nanophotonics. The generation of optical modes in coupled Fabry-Pérot planar cavities and their migration to hyperbolic metamaterials is investigated. Coupled Fabry-Pérot cavities behave as simple coupled resonators. When the intra-cavity media have different refractive indices in two or more coupled cavities resonance anti-crossings arise. The application of this kind of strong coupling in sensing is foreseen. Beyond the cavity modes excited by propagating waves, also long range plasmonic guided modes can be excited using emitters or evanescent waves. A periodic structure made by multiple plasmonic films and dielectrica supports bulk plasmons, of large propagation constant and increasing field amplitude. The optical response of these structures approaches that of the hyperbolic metamaterial predicted by the effective medium theory. Light can propagate with full transmission in a structure made of a photonic crystal based on quarter wavelength layers and a second photonic crystal with an overlapping forbidden band, but presenting a non-trivial topological phase achieved by band inversion. This is due to excitation of optical Tamm states at the boundary between both crystals. The extension to multiple optical Tamm states using dielectric and plasmonic materials and the symmetries of the edge states is investigated.


2010 ◽  
Vol 82 (1) ◽  
Author(s):  
Zhen Fang ◽  
Rui Guo ◽  
Xiaoji Zhou ◽  
Xuzong Chen

2021 ◽  
Author(s):  
M. Channab ◽  
F. Ferrarese Lupi ◽  
I. Murataj ◽  
F. Pirri ◽  
A. Angelini

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