Table 3 Values of x minimizing the residua, corresponding value of the resonant frequency (when R = 100 nm), eigenpermittivity, and residuum of the dimer-modes which dominate the scattering efficiency of Fig. 10. Positions of the peaks of the total scattering efficiency.
From: Full-wave electromagnetic modes and hybridization in nanoparticle dimers
Mode | \({{\boldsymbol{x}}}_{{\boldsymbol{emq}}}^{{\boldsymbol{\perp }}}\) | \({{\boldsymbol{\omega }}}_{{\boldsymbol{emq}}}^{{\boldsymbol{\perp }}}\) [Prad/s] | \({{\boldsymbol{\varepsilon }}}_{{\boldsymbol{emq}}}^{{\boldsymbol{\perp }}}\) | \({{\boldsymbol{\rho }}}_{{\boldsymbol{emq}}}^{{\boldsymbol{\perp }}}\) | # peak | x |
|---|---|---|---|---|---|---|
\({{\bf{d}}}_{e1,2}^{\perp }\) | 0.760 | 2.29 | 16.11 − 2.23i | 0.149 | (1) | 0.771 |
\({{\bf{d}}}_{e0,1}^{||}\) | 1.696 | 5.08 | −0.70 − 3.96i | 1.038 | (2) | 0.901 |
\({{\bf{d}}}_{e0,3}^{\perp }\) | 1.126 | 3.37 | 15.67 − 2.50i | 0.168 | (3) | 1.099 |
\({{\bf{d}}}_{e2,1}^{\perp }\) | 1.099 | 3.29 | 15.99 − 0.32i | 0.021 | (3) | 1.099 |
\({{\bf{d}}}_{e1,8}^{\perp }\) | 1.366 | 4.09 | 16.00 − 0.26i | 0.017 | (4) | 1.336 |
\({{\bf{d}}}_{e3,1}^{\perp }\) | 1.421 | 4.26 | 15.98 − 0.05i | 0.004 | (5) | 1.423 |
\({{\bf{d}}}_{e1,12}^{\perp }\) | 1.571 | 4.71 | 15.96 − 1.02i | 0.068 | (6) | 1.584 |
\({{\bf{d}}}_{e1,14}^{\perp }\) | 1.692 | 5.07 | 15.99 − 0.07i | 0.005 | (7) | 1.688 |
