2022
DOI: 10.15407/hftp13.04.476
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An influence of the adsorbed molecules layer on the localized surface plasmons in the spherical metallic nanoparticles

Abstract: An influence of the adsorbed molecules layer on the optical characteristics of the spherical metallic nanoparticles has been studied in the work. In order to do this one considers the additional term which takes into account the scattering of electrons at the interface between metal and adsorbate. The analytical expressions for the frequency dependences for the parameter of coherence loss due to the scattering at the interface “metal – adsorbed layer” have been obtained. It has been found that the presence of … Show more

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Cited by 2 publications
(1 citation statement)
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“…For the third maximum (𝜆 (3) max ≈ 480 nm for Ag@TC and 𝜆 (3) max ≈ 550 nm for Au@TC), and ℏ𝜔 (3) res = 2.11 eV for Ag@TC and ℏ𝜔 (3) res = 1.62 eV for Au@TC, which correspond to 𝜆 (3) max ≈ 765 nm and 𝜆 (3) max ≈ 590 nm, i.e., the theoretical and experimental values 𝜆 (3) max are close for Au@TC while the values 𝜆 (3) max are significantly different for Ag@TC the values differ significantly. In our opinion, this can be associated with the fact that the theoretical values of resonant frequencies ℏ𝜔 (𝑖) res were estimated in non-dissipative approximation, while under an increase of the wavelength (decrease of the frequency) of the incident light for the particles of the indicated size, the relaxation processes, associated with the electron scattering both by the surface of the particle and with the additional chemical damping at the interface "metal -J-aggregate" interface (see, for example, [74,75]), may be essential. Nevertheless, the authors are aware that this issue requires a more detailed research and will be the subject of subsequent works of the authors.…”
Section: The Results Of Calculations and Discussionmentioning
confidence: 99%
“…For the third maximum (𝜆 (3) max ≈ 480 nm for Ag@TC and 𝜆 (3) max ≈ 550 nm for Au@TC), and ℏ𝜔 (3) res = 2.11 eV for Ag@TC and ℏ𝜔 (3) res = 1.62 eV for Au@TC, which correspond to 𝜆 (3) max ≈ 765 nm and 𝜆 (3) max ≈ 590 nm, i.e., the theoretical and experimental values 𝜆 (3) max are close for Au@TC while the values 𝜆 (3) max are significantly different for Ag@TC the values differ significantly. In our opinion, this can be associated with the fact that the theoretical values of resonant frequencies ℏ𝜔 (𝑖) res were estimated in non-dissipative approximation, while under an increase of the wavelength (decrease of the frequency) of the incident light for the particles of the indicated size, the relaxation processes, associated with the electron scattering both by the surface of the particle and with the additional chemical damping at the interface "metal -J-aggregate" interface (see, for example, [74,75]), may be essential. Nevertheless, the authors are aware that this issue requires a more detailed research and will be the subject of subsequent works of the authors.…”
Section: The Results Of Calculations and Discussionmentioning
confidence: 99%