An optical nanoantenna made of plasmonic chain resonators
We propose a novel structure that behaves like an optical antenna and converts evanescent waves into propagating waves. The system comprises metallic subwavelength cylinders distributed in a dual-period array. It is illuminated by an evanescent wave generated by total internal reflection in a close...
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| Formato: | Capítulo de libro |
| Lenguaje: | Inglés |
| Publicado: |
2011
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| Acceso en línea: | Registro en Scopus DOI Handle Registro en la Biblioteca Digital |
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| LEADER | 13286caa a22012257a 4500 | ||
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| 001 | PAPER-23716 | ||
| 003 | AR-BaUEN | ||
| 005 | 20250609082904.0 | ||
| 008 | 190411s2011 xx ||||fo|||| 00| 0 eng|d | ||
| 024 | 7 | |2 scopus |a 2-s2.0-79952685390 | |
| 040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
| 100 | 1 | |a Lester, Marcelo Fabián | |
| 245 | 1 | 3 | |a An optical nanoantenna made of plasmonic chain resonators |
| 260 | |c 2011 | ||
| 270 | 1 | 0 | |m Lester, M.; Grupo Optica de Sólidos-Elfo, Instituto de Física Arroyo Seco, Universidad Nacional Del Centro de la Provincia de Buenos Aires, Pinto 399 (cp 7000), Buenos Aires, Argentina; email: mlester@exa.unicen.edu.ar |
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| 506 | |2 openaire |e Política editorial | ||
| 520 | 3 | |a We propose a novel structure that behaves like an optical antenna and converts evanescent waves into propagating waves. The system comprises metallic subwavelength cylinders distributed in a dual-period array. It is illuminated by an evanescent wave generated by total internal reflection in a close interface. For particular wavelengths, the system exhibits resonances and the inhomogeneous wave is converted into propagating waves that radiate to the far field. This effect can be controlled by varying the geometrical parameters of the structure, such as the period and the inclination angle. Therefore, the transmitted intensity can be sent to a predesigned direction. This structure could be used in highly sensitive detection devices, among other applications. © 2011 IOP Publishing Ltd. |l eng | |
| 593 | |a Grupo Optica de Sólidos-Elfo, Instituto de Física Arroyo Seco, Universidad Nacional Del Centro de la Provincia de Buenos Aires, Pinto 399 (cp 7000), Buenos Aires, Argentina | ||
| 593 | |a Grupo de Electromagnetismo Aplicado, Departamento de Física, IFIBA (CONICET) Ciudad Universitaria, C1428EHA Buenos Aires, Argentina | ||
| 593 | |a Consejo Nacional de Investigaciones Científicas y Técnicas, CONICET, Argentina | ||
| 690 | 1 | 0 | |a DIFFRACTION AND SCATTERING |
| 690 | 1 | 0 | |a SUBWAVELENGTH STRUCTURES |
| 690 | 1 | 0 | |a SURFACE PLASMONS |
| 690 | 1 | 0 | |a DIFFRACTION AND SCATTERING |
| 690 | 1 | 0 | |a EVANESCENT WAVE |
| 690 | 1 | 0 | |a FAR FIELD |
| 690 | 1 | 0 | |a GEOMETRICAL PARAMETERS |
| 690 | 1 | 0 | |a HIGHLY SENSITIVE |
| 690 | 1 | 0 | |a INCLINATION ANGLES |
| 690 | 1 | 0 | |a INHOMOGENEOUS WAVES |
| 690 | 1 | 0 | |a NANOANTENNAS |
| 690 | 1 | 0 | |a NOVEL STRUCTURES |
| 690 | 1 | 0 | |a OPTICAL ANTENNAS |
| 690 | 1 | 0 | |a OTHER APPLICATIONS |
| 690 | 1 | 0 | |a PLASMONIC |
| 690 | 1 | 0 | |a SUB-WAVELENGTH |
| 690 | 1 | 0 | |a SUB-WAVELENGTH STRUCTURES |
| 690 | 1 | 0 | |a SURFACE PLASMONS |
| 690 | 1 | 0 | |a TOTAL INTERNAL REFLECTIONS |
| 690 | 1 | 0 | |a TRANSMITTED INTENSITIES |
| 690 | 1 | 0 | |a CYLINDERS (SHAPES) |
| 690 | 1 | 0 | |a DIFFRACTION |
| 690 | 1 | 0 | |a ELECTROMAGNETIC WAVE REFLECTION |
| 690 | 1 | 0 | |a REACTIVE ION ETCHING |
| 690 | 1 | 0 | |a REFRACTIVE INDEX |
| 690 | 1 | 0 | |a WAVE TRANSMISSION |
| 690 | 1 | 0 | |a PLASMONS |
| 700 | 1 | |a Skigin, D.C. | |
| 773 | 0 | |d 2011 |g v. 13 |k n. 3 |p J. Opt. |x 20408978 |t Journal of Optics | |
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