Titlebook: Collective Plasmon-Modes in Gain Media; Quantum Emitters and V.A.G. Rivera,O.B. Silva,E. Marega Jr. Book 2015 V.A.G. Rivera, O.B. Silva, Y.

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Plasmonic Nanostructure Arrays Coupled with a Quantum Emitter,m give rise to strong EM fields inside the feedgap of the antenna. When the antenna is resonant at optical frequencies, it can be called a resonant nanoantenna. In this case, with sufficiently close spacing with respect to a quantum emitter (QE) and nanoantenna, they can interact forming an electric

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,Quantum Aspects of Light–Matter Interaction,tieth century. By now, the phenomena of light propagation in matter, such as absorption, nonlinear absorption, refraction, reflection, dispersion, etc., are considered to be perfectly well understood and described from macro- and micro-scale points of view. For a comprehensive description of the phe

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,Plasmonic Nanoparticles Coupled with an |n〉-State Quantum System,ical properties of metals and rare-earth ions (REI), and the surface plasmon polariton (SPP) in a gain medium, thus laying the foundation for a good understanding of the field and easier reading of this book. In this chapter, we will describe the behaviors resulting from coupling between plasmonic n

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Plasmonic Nanostructure Arrays Coupled with a Quantum Emitter,f free electrons on a curved surface. We also mentioned the main difference between surface plasmon polaritons (SPP) and LSPR, namely that SPPs are propagating waves, while LSPR is a nonpropagating excitation of free electrons in a metallic nanostructure coupled to an EM field. In this chapter, we w

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