Figure 5
From: Full-wave electromagnetic modes and hybridization in nanoparticle dimers
Decomposition of the dimer-mode \({{\bf{d}}}_{e0,1}^{\parallel }\) at x = 0.747, in terms of hybridizing isolated-sphere modes (real part of the projection on the y = 0 plane). Each isolated-sphere mode is multiplied by the corresponding expansion coefficient of Eq. 8. Below each isolated-sphere mode its hybridization weight \({H}_{e01\,nl}^{\parallel \,|{\rm{T}}{\rm{M}}}\) is shown.
