Figure 21
From: Full-wave electromagnetic modes and hybridization in nanoparticle dimers
Decomposition of the dimer-mode \({{\bf{d}}}_{e1,6}^{\perp }\) at x = 1.108, in terms of isolated-sphere modes Each isolated-sphere modes is multiplied by the expansion coefficients of Eq. 8. Below each isolated-sphere mode we show its hybridization weight \({H}_{e16nl}^{\perp |{\rm{TM}}}\) (\({H}_{o16nl}^{\perp |{\rm{TE}}}\)).
