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Beilstein J. Nanotechnol. 2018, 9, 953–953, doi:10.3762/bjnano.9.88
Beilstein J. Nanotechnol. 2017, 8, 614–626, doi:10.3762/bjnano.8.66
Figure 1: Single sphere with multiple plane wave illuminations, depicted with their wave vectors in green.
Figure 2: Convergence of the T-matrix calculation with the increase of the number of plane wave illuminations...
Figure 3: Total scattering cross section (blue) of the dimer and the contributions of different multipoles. T...
Figure 4: The left picture shows the general form of the T-matrix, as described in the previous section. For ...
Figure 5: Convergence of the T-matrix calculation with the increase of the number of plane wave illuminations...
Figure 6: T-matrix entries of the dimer, calculated with the presented method at 600 THz. For the sake of cla...
Figure 7: Total scattering cross section (blue) of the sandwich particle and the contributions of different m...
Figure 8: T-matrix entries of the sandwich particle, calculated with the presented method at 336 THz with 50 ...
Figure 9: Right-handed metallic helix with two windings. Total scattering cross section for right-handed (sol...
Figure 10: T-matrix entries of the right handed helix, calculated with the presented method at 1.5 THz with 10...
Figure 11: T-matrix entries in the helicity basis (obtained by Equation 22) of a left-handed and a right-handed helix. We...
Figure 12: Duality breaking, electromagnetic chirality and cross section contrast of the left-handed helix.