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...
Збережено в:
| Дата: | 2009 |
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| Автори: | , , , |
| Формат: | Стаття |
| Мова: | English |
| Опубліковано: |
Інститут фізики напівпровідників імені В.Є. Лашкарьова НАН України
2009
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| Назва видання: | Semiconductor Physics Quantum Electronics & Optoelectronics |
| Онлайн доступ: | https://nasplib.isofts.kiev.ua/handle/123456789/118687 |
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| Назва журналу: | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
| Цитувати: | 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. |
Репозитарії
Digital Library of Periodicals of National Academy of Sciences of Ukraine| Резюме: | 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. |
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