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For the quadrupole mode, another Fano dip is observed in the radiative power spectrum (n = 2) in Figure 2a at 568 nm between the bonding mode and the anti-bonding mode for d = 25 nm.
Comparing these spectra with those of a nanomatryoshka reveals that a Fano dip divides the dipole mode of the nanoshell into two parts - the anti-symmetric bonding mode and the symmetric anti-bonding mode.
The λ res are found in the wavelength range of 1.2 2.5 μm for bonding mode and 0.6 1.3 μm for anti-bonding mode, respectively.
These results in the splitting of the plasmon mode into two resonance modes, i.e., "bonding" mode (ranging in longer wavelengths) and "anti-bonding" mode (ranging in shorter wavelengths) [24].
For the side-to-side pair, the opposite is the case and the symmetric mode has higher energy than the anti-symmetric mode, making the anti-symmetric mode the bonding mode and the symmetric mode the anti-bonding mode.
The electric field, surface charge distribution, and far-field radiation pattern in the x-z plane of the dipolar bonding mode (820 nm), the Fano dip (740 nm), and the dipolar anti-bonding mode (648 nm) are studied and shown in Figures 5, 6, and 7, respectively.
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Two of the bonding modes for Cp are illustrated in the following structure, which contains both η3- and η5-C5H5 ligands.
b Schematic charge densities corresponding to bonding modes of the cases 1 4.
Only the dipolar and quadrupolar bonding modes (( {left|{omega}_rightrangle}_n ), n = 1, 2) are maintained in the spectrum.
In Figure 2, the bonding modes (|ω −〉 n ) of nanoegg with different core offset D are shown.
The number of bonding modes has been observed for the thiosemicarbazones in their neutral or anionic forms [27].
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