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Titlebook: Quantum Nano-Photonics; Baldassare Di Bartolo,Luciano Silvestri,John Colli Conference proceedings 2018 Springer Nature B.V. 2018 Bio Photo

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楼主: legerdemain
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Chapter 8 Casimir Forces: Fundamental Theory, Computation, and Nanodevice Applicationsd Polder, our understanding of such interactions in both the unretarded and retarded regimes has undergone a dramatic and intricate evolution. In this contribution, we explore the ultimate physical motivations leading to this fascinating trajectory rich in momentous implications for the goal of both
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Chapter 10 Fundamental Experiments and Quantum Technology Applications with Defect Centres in Diamon it is nowadays possible to observe such objects in the solid state with compact setups even at room temperature. In this contribution we introduce defect centres in diamond and discuss two recent experiments. One concerns the direct observation of the quantum nature of light with not more but a sin
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Chapter 13 Waveguide Integrated Superconducting Single Photon Detectorsted electrical circuits. Using materials with high refractive index allows for confining light into sub-wavelength dimensions as efficient optical wires. Interaction with the environment is possible through near-field coupling to the evanescent tail of propagating optical modes, given that the measu
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Chapter 14 Whispering Gallery Mode Resonators as Opto-Mechanical Probes to Nanoparticle-Microcavity than 200 nm. This range is ideal for observing the effect that double layers have on the motion of protein, virus, and artificial nanoparticles. In exploring the measurement possibilities we were immediately drawn to the opportunity for determining physical parameters that have not revealed themsel
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Chapter 15 Novel Aspects of the Fabry-Pérot Resonatorl resonance enhancement factor, and show that all related Airy distributions are obtained by simple scaling factors. We verify that the sum of the mode profiles of all longitudinal modes generates the Airy distribution. Consequently, the resonator losses are quantified by the linewidths of the under
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