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Beilstein J. Nanotechnol. 2013, 4, 974–987, doi:10.3762/bjnano.4.110
Figure 1: Geometry of the sphere and the illuminating plane wave. The k-vector of the plane wave is defined b...
Figure 2: Cross sections of the (a) extinction, (b) scattering and (c) absorption of a PS sphere of diameter d...
Figure 3: Mode characteristics of the two absorption maxima in Figure 2d ((0,0), i.e., sphere side illumination, h = 2...
Figure 4: Dependence of the cross sections of the semi-shell structure with a core diameter d = 390 nm and a ...
Figure 5: Fine-tuning of the Ag semi-shell resonances to the emission band of the dye. Parameters and the org...
Figure 6: Approach to lasing for a semi-shell thickness of h = 16 nm. Parameters and order of panels a,b,c ar...
Figure 7: Differential scattering cross section σsc, linear scale, for resonant semi-shells with thickness h ...
Figure 8: (a,c) Field enhancement |E|/E0 for two modes with gain close to the lasing threshold. The z-polariz...
Figure 9: (a) Cross sections in case of a semi-shell of thickness h = 20 nm near the lasing threshold of ΔεDye...
Figure 10: Differential cross sections for semi-shell thicknesses h = 20 nm (solid curves) and h = 16 nm (dash...