Titlebook: Optical Properties of Metallic Nanoparticles; Basic Principles and Andreas Trügler Book 2016 Springer International Publishing Switzerland

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金盤(pán)是高原

The World of Plasmons we ignore the lattice, in a first approximation, we end up with a different approach where the free electrons of a metal can be treated as an electron liquid of high density [1, 2]. From this plasma model it follows that longitudinal density fluctuations, so-called plasma oscillations or ., with an

immunity

Theoryentury [1–3] and brought us a very successful part of theoretical physics: classical field theory. A detailed overview about the historical evolution from René Descartes up to Maxwell and Lorentz can be found in Whittaker [4]. After the revolution of our understanding of the basic forces and constit

BRINK

Modeling the Optical Response of Metallic Nanoparticlesutions for light scattering problems if we expand the electromagnetic potentials and fields to spherical harmonics and limit ourselves to spherical or spheroidal particle shapes. In reality, however, we want to work with arbitrary shaped nanostructures and take advantage of certain structure depende

思考而得

拒絕

Influence of Surface Roughnesstical properties of MNPs [1, 34]. Especially if e-beam lithography (see Sect. 2.10.2) is used to produce the particles, the resulting metal structures are polycrystalline and the surfaces are quite rough [2, 3]. Contrary to what one might anticipate, initial indications are that a moderate amount of

Countermand

Nonlinear Optical Effects of Plasmonic Nanoparticlesn Sect. 2.7, already after a few femtoseconds the plasmonic excitations start to vanish again. The temporal evolution and this ultrafast relaxation of surface plasmon polaritons is of central importance for many kinds of plasmonic applications. It is amazing that we can explore such rapid dynamic pr

glomeruli

Nonlocal Responsee microscopic dynamic of the electrons has been lumped into the macroscopic dielectric function. We have discussed the classical concept of this function and in Sect. 3.3 we have seen that a simple frequency dependence of ε has far-reaching consequences like temporal nonlocal equations and the manda

腐敗

Metamaterialsm rather than in vacuum. Hence it describes a ratio and is therefore a dimensionless number. A value of .??=?1.?5, for example, states that a light wave travels 1.5 times faster in vacuum than it does in the corresponding medium (glass in this case). Since we also know the laws of relativity and its

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