Download Quantum Plasmonics by Sergey I. Bozhevolnyi, Luis Martin-Moreno, Francisco PDF

By Sergey I. Bozhevolnyi, Luis Martin-Moreno, Francisco Garcia-Vidal (eds.)

This ebook offers the most recent result of quantum houses of sunshine within the nanostructured surroundings helping floor plasmons, together with waveguide quantum electrodynamics, quantum emitters, strong-coupling phenomena and lasing in plasmonic buildings. assorted methods are defined for controlling the emission and propagation of sunshine with severe gentle confinement and box enhancement supplied by means of floor plasmons. contemporary development is reviewed in either experimental and theoretical investigations inside of quantum plasmonics, elucidating the basic actual phenomena concerned and discussing the conclusion of quantum-controlled units, together with single-photon resources, transistors and ultra-compact circuitry on the nanoscale.

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8) modifies the field distribution and needs to be considered [13]. As the radial field component along ????r in polar coordinates dominates in the near-field region, we restrict this analysis to the corresponding amplitude |gr |2 . For better intuition, we give in Fig. 6a the near-field squeezing pattern for a GNS of R = 200 nm. At the point opposite side from the emitter 10 nm below the GNS, the GNS provides enhancement by up to a factor of 2000 as compared to free space [13]. The pattern shows two lateral lobes, which stem from the excitation of higher-order plasmon-polariton resonances.

1 Macroscopic Quantum Electrodynamics We now outline the framework of macroscopic quantum electrodynamics [17, 29], which provides powerful tools to describe the TLE dynamics in arbitrary nanostructured environments. 3) with the first term describing the freely evolving driving field, and the second term arising from the response of scatterers. 4) a classical dipole ????, placed in an inhomogeneous dielectric ????(????, ????) at position ????E , and oscillating at a frequency ???? generates the (classical) source field [2] ????(+) (????, ????) = ????2 ????(????, ????E , ????)????.

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