By Vladimir M. Shalaev

ISBN-10: 3540656154

ISBN-13: 9783540656159

Nonlinear Optics of Random Media studies fresh advances in in a single of the main famous fields of physics. It offers an overview of the elemental types of abnormal buildings of random inhomogeneous media and the ways used to explain their linear electromagnetic houses. Nonlinearities in random media also are mentioned. The chapters should be learn independently, so scientists and scholars drawn to a particular challenge can cross on to the suitable textual content.

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Additional resources for Nonlinear Optics of Random Media: Fractal Composites and Metal-Dielectric Films (Springer Tracts in Modern Physics)

Example text

65), with CRS obtained from the relation: GRS δ 3 ≈ 1 in the maxima occurring at X ≈ ± 4. 1 ≤ |X| ≤ 3. 70) is close to value 4. Note that for |X| < 4 the dependence associated with a pre-factor (in this case, X 4 ) dominates the relatively weak (in this interval) spectral dependence of Imα(X). GRS = CRS Fig. 11. Enhancement of Raman scattering in CCAs GRS (multiplied by lossparameter cubed δ 3 ) for negative X, corresponding to the visible and infrared parts of the spectrum (see Fig. 2a) As seen in Fig.

It is estimated as f ∼ δIm[α(X)], where δ characterizes the homogeneous width of individual resonances (in the X space) forming the inhomogeneous absorption spectrum Im[α(X)]. 46). Note also that |Ei | ∼ Ei,res × f ∼ |E (0) |. e. by the fraction of particles involved in the resonance excitation. (The sign ... 47) which is 1 for n > 1. Since this is only a rough estimation, an adjustable constant C should, in general, be added as a pre-factor. 46). The nonlinear dipole amplitude can be enhanced along with the linear local fields, provided that generated in a nonlinear process frequency lies within the spectral region of the fractal eigenmodes.

The SE rate in the cavity mode, referenced to the total SE rate in a homogeneous medium, is given by the Purcell figure of merit F ∼ Qλ3 /V , where V is the effective medium volume. By placing a fractal aggregate in a microcavity of volume ∼ λ3 , it is possible to achieve further enhancement of the zero-point fields (and thus the SE rate) because of high-quality factors of the fractal optical excitations and their localization in sub-wavelength areas. In Sect. 8 it will be shown that huge multiplicative enhancement can be obtained under the simultaneous, combined enhancement provided by microcavity resonators and fractal nanocomposites.

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Nonlinear Optics of Random Media: Fractal Composites and Metal-Dielectric Films (Springer Tracts in Modern Physics) by Vladimir M. Shalaev


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