Emergence of Fano response in trimer structure with asymmetric permittivity

Contribution of Multipolar Moments in Each Eigenmode at Wavelength of 611 nm

Contribution of Multipolar Moments in Each Eigenmode at Wavelength of 508 nm

Difference between the Ratio of the Interference Term ($C_{\mathrm{i}\mathrm{n}\mathrm{t}}$) Relative to the Scattering Cross Section ($C_{\mathrm{s}\mathrm{c}\mathrm{a}}$) for Each Variation of $d_1$^a

^a Differences are relative to default value ${d_1} = 80\;{\rm nm}$.

Difference between the Ratio of the Interference Term ($C_{\mathrm{i}\mathrm{n}\mathrm{t}}$) Relative to the Scattering Cross Section ($C_{\mathrm{s}\mathrm{c}\mathrm{a}}$) for Each Variation of $d_2$^a

^a Differences are calculated relative to the default value ${d_2} = 55\;{\rm nm}$.

Table 1.

Contribution of Multipolar Moments in Each Eigenmode at Wavelength of 611 nm

Table 2.

Contribution of Multipolar Moments in Each Eigenmode at Wavelength of 508 nm

Table 3.

Difference between the Ratio of the Interference Term ($C_{\mathrm{i}\mathrm{n}\mathrm{t}}$) Relative to the Scattering Cross Section ($C_{\mathrm{s}\mathrm{c}\mathrm{a}}$) for Each Variation of $d_1$^a

^a Differences are relative to default value ${d_1} = 80\;{\rm nm}$.

Table 4.

Difference between the Ratio of the Interference Term ($C_{\mathrm{i}\mathrm{n}\mathrm{t}}$) Relative to the Scattering Cross Section ($C_{\mathrm{s}\mathrm{c}\mathrm{a}}$) for Each Variation of $d_2$^a

^a Differences are calculated relative to the default value ${d_2} = 55\;{\rm nm}$.