The features of surface plasmon resonance in gold cluster films

The internal reflection of nanosized gold cluster films was studied using the technique of polarization modulation of electromagnetic radiation in the Kretschmann geometry. We measured the reflection coefficients Rs and Rp of s- and p-polarized radiation, respectively, as well as their polarizati...

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Published in:Semiconductor Physics Quantum Electronics & Optoelectronics
Date:2009
Main Authors: Maksimenko, L.S., Matyash, I.E., Rudenko, S.P., Serdega, B.K.
Format: Article
Language:English
Published: Інститут фізики напівпровідників імені В.Є. Лашкарьова НАН України 2009
Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/118687
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Journal Title:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Cite this:The features of surface plasmon resonance in gold cluster films / L.S. Maksimenko, I.E. Matyash, S.P. Rudenko, B.K. Serdega // Semiconductor Physics Quantum Electronics & Optoelectronics. — 2009. — Т. 12, № 2. — С. 129-134. — Бібліогр.: 13 назв. — англ.

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Digital Library of Periodicals of National Academy of Sciences of Ukraine
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Summary:The internal reflection of nanosized gold cluster films was studied using the technique of polarization modulation of electromagnetic radiation in the Kretschmann geometry. We measured the reflection coefficients Rs and Rp of s- and p-polarized radiation, respectively, as well as their polarization difference ∆R = Rs − Rp, as function of the light incidence angle in the 0.4÷1.6 µm wavelength range. A topological size effect was found; it consists in dependence of the value and sign of curvature of the polarization difference characteristics on the film surface properties. It is shown that the sign of curvature of ∆R characteristics depends on the radiation wavelength λ and indicates resonance interaction with a metal film of either p-polarized radiation only or that of both polarizations. The spectral characteristic of the topological size effect in the resonance interaction is obtained from the condition of isotropic reflection, ∆R = Rs − Rp = 0, and its dependence on the radiation wavelength.
ISSN:1560-8034