Figure 13
From: Full-wave electromagnetic modes and hybridization in nanoparticle dimers
Decomposition of the dimer-mode \({{\bf{d}}}_{e1,8}^{\perp }\) at \(x=1.366\) in terms of hybridizing 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 also show its hybridization weight \({H}_{e18\,nl}^{\perp \,|\text{TM}}\) (\({H}_{o18\,nl}^{\perp \,|\text{TE}}\)).
