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Beilstein J. Nanotechnol. 2019, 10, 2163–2170, doi:10.3762/bjnano.10.209
Figure 1: COMSOL simulations of light propagation in a directional coupler and two MMIs, all having rectangul...
Figure 2: Power output in the input waveguide as a function of the effective refractive index of the LC cladd...
Figure 3: A directional coupler prototype showing power distribution between the output guides.
Figure 4: Power density distribution in the first three periods (3Lπ) of a 1 × 1 symmetric MMI and a 2 × 2 as...
Figure 5: The characteristic length of an MMI is nearly constant until the cladding index reaches values clos...
Figure 6: A number of SU8 PWG MMIs of different lengths prepared at the lab. The substrate is SiO2 on an Si w...
Figure 7: An MMI with inorganic Si3N4 core and high-birefringence LC cladding does not show variations in cha...
Figure 8: Two waveguides at short distance interacting through evanescent fields. The interaction is tuned by...
Beilstein J. Nanotechnol. 2016, 7, 1743–1748, doi:10.3762/bjnano.7.167
Figure 1: Incidence of the probe beam on the sample and the laboratory (x',y',z') and the sample (x,y,z) coor...
Figure 2: Porosity of SiO2 films vs angle of deposition (filled squares). Also shown are corrected data from [16]...
Figure 3: The anisotropic refractive index (nonfilled symbols) of porous SiO2 at λ = 532 nm vs angle of depos...
Figure 4: SiO2 column tilt vs the SiO2 deposition angle. The experimental data from [15] and the curves simulated...
Figure 5: LC pretilt vs the SiO2 deposition angle. The experimental data from [2] and [3] are shown for comparison.