scholarly journals Granular Permittivity Representation in Extremely Near-Field Light–Matter Interaction Processes

ACS Photonics ◽  
2017 ◽  
Vol 4 (9) ◽  
pp. 2137-2143 ◽  
Author(s):  
Alexey S. Kadochkin ◽  
Alexander S. Shalin ◽  
Pavel Ginzburg
2020 ◽  
Vol 124 (51) ◽  
pp. 28178-28185
Author(s):  
Emanuele Poliani ◽  
Daniel Seidlitz ◽  
Maximilian Ries ◽  
Soo J. Choi ◽  
James S. Speck ◽  
...  

RSC Advances ◽  
2019 ◽  
Vol 9 (50) ◽  
pp. 29173-29181 ◽  
Author(s):  
Desalegn T. Debu ◽  
M. Hasan Doha ◽  
Hugh O. H. Churchill ◽  
Joseph B. Herzog

Plasmon coupling and hybridization in 2D materials plays a significant role for controlling light–matter interaction at the nanoscale.


APL Photonics ◽  
2018 ◽  
Vol 3 (9) ◽  
pp. 091101 ◽  
Author(s):  
Hervé Rigneault ◽  
Pascal Berto

Nanophotonics ◽  
2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Yu-Tsung Lin ◽  
Amir Hassanfiroozi ◽  
Wei-Rou Jiang ◽  
Mei-Yi Liao ◽  
Wen-Jen Lee ◽  
...  

Abstract Mie resonances have recently attracted much attention in research on dielectric metasurfaces, owning to their enriched multipole resonances, negligible optical loss, and efficient light emitter integration. Although there is a rapid advancement in this field, some fundamental developments are still required to provide a simpler and more versatile paradigm for photoluminescence (PL) control. In this work, we proposed that an all-dielectric coherent metasurface can engineer the PL response by tuning the array size. Such PL manipulation is attributed to the collective Mie resonances that mediate the inter-unit interactions between unit elements and alter the PL intensity. Metasurfaces with different chip sizes are utilized to explore the array size effect on the collective Mie resonances, field enhancement, and Q-factor in TiO2 metasurfaces. Incorporating the all-dielectric coherent metasurface with fluorescent photon emitters, we performed the dependence of PL enhancement on array size, which achieves an enhancement factor of ∼10 at the central area of a 90 × 90 μm2 TiO2 metasurface array. These findings provide an additional degree of freedom to engineer the near-field confinement and enhancement, allowing one to manipulate incoherent photon emission and tune light–matter interaction at the nanoscale.


2016 ◽  
Vol 18 (34) ◽  
pp. 23680-23685 ◽  
Author(s):  
A. K. Sivadasan ◽  
Kishore K. Madapu ◽  
Sandip Dhara

Near field scanning optical microscopy is used for imaging as well as understanding the intrinsic properties of semiconducting and noble-metal nanostructures of sub-diffraction size.


Author(s):  
Alexey V. Kavokin ◽  
Jeremy J. Baumberg ◽  
Guillaume Malpuech ◽  
Fabrice P. Laussy

In this chapter we study with the tools developed in Chapter 3 the basic models that are the foundations of light–matter interaction. We start with Rabi dynamics, then consider the optical Bloch equations that add phenomenologically the lifetime of the populations. As decay and pumping are often important, we cover the Lindblad form, a correct, simple and powerful way to describe various dissipation mechanisms. Then we go to a full quantum picture, quantizing also the optical field. We first investigate the simpler coupling of bosons and then culminate with the Jaynes–Cummings model and its solution to the quantum interaction of a two-level system with a cavity mode. Finally, we investigate a broader family of models where the material excitation operators differ from the ideal limits of a Bose and a Fermi field.


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