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In our calculation we cannot consider the partial embedding of the concentric-shell fullerenes in the Ag substrate which will also influence the plasmon energy. The EELS spectra of an isotropic dielectric sphere embedded in a dielectric material have already been formulated in, and
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In our calculation we cannot consider the partial embedding of the concentric-shell fullerenes in the Ag substrate which will also influence the plasmon energy. The EELS spectra of an isotropic dielectric sphere embedded in a dielectric material have already been formulated in N. Zabala and A. Rivacoba, Phys. Rev. B48, 14 534 (1993);
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where the authors emphasized the existence of a new mode (an interface mode) at lower energy
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Kinematic effects can also affect the relative intensity of plasmon resonance: as seen in Sec. III, at lower primary energy, the electrons excite low-energy resonances with higher probability. This could also play a role in the observed intensity of the radial mode compared to the tangential one
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Kinematic effects can also affect the relative intensity of plasmon resonance: as seen in Sec. III, at lower primary energy, the electrons excite low-energy resonances with higher probability. This could also play a role in the observed intensity of the radial mode compared to the tangential one.
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