Fig. 5: Elimination of the ordinary and -1st-order reflections at θWA = 5° and 45°.
The scattered field distribution contributed (a) by the channel n = 0 correspondings to an isotropic mode and (b) by the channels n = − 1 and 1 corresponding to a standard dipole mode at θWA = 5°. The scattered field distribution contributed (c) by the channels n = −2 and −1 and (d) by the channels n = 0 and 1 at θWA = 45°. The calculation is performed for the same QD with the inter-QD interaction considered as in Fig. 4. Ki and R0 denote the incident and ordinary reflection directions, respectively.
