Figure 19
From: Full-wave electromagnetic modes and hybridization in nanoparticle dimers
Decomposition of the dimer-mode \({{\bf{d}}}_{e1,3}^{\perp }\) at x = 0.967, in terms of isolated-sphere modes (real part of the projection on the y = 0 plane). Each isolated-sphere modes is multiplied by the expansion coefficients of Eq. 8. Below each isolated-sphere mode we show its hybridization weight \({H}_{e13nl}^{\perp |{\rm{TM}}}\) (\({H}_{o13nl}^{\perp |{\rm{TE}}}\)).
