
Proceedings Paper
Optical control of THz reflectivity with surface wavesFormat | Member Price | Non-Member Price |
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Paper Abstract
We propose an experimental demonstration of a THz modulator with a visible optical command. The device is a n-doped
GaAs grating with subwavelength dimensions. The principle of this modulator is the control of the THz resonant
absorption by surface waves supported by the grating. This absorption is modulated with low power visible light, leading
to a modulation of the reflected THz beam. From experimental polarized THz reflectivity measurement of the grating,
we show that a depletion layer at the surface of the doped GaAs has to be taken into account to correctly describe the
observed resonant absorption. From experimental observation and modeling we are able to ascribe this absorption to the
coupling of incident THz light with surface plasmon-phonon polariton mode propagating along each wall of the grating.
Thus, each wall acts as a nano-antenna that resonantly absorbs light. The grating can be viewed as a metamaterial
composed of individual resonators. The theoretical model indicates that the reflectivity dip linked to the surface wave is
sensible to the electronic density in the walls of the grating. We performed an experiment to measure the THz
reflectivity while illuminating the grating with visible photons having energy higher than the bandgap of GaAs. The
created photoelectrons change the effective mode index, leading to a shift of the resonant absorption frequency. This
demonstrates the modulation of THz radiation around 8.5 THz with a visible optical command at room temperature.
Paper Details
Date Published: 7 September 2011
PDF: 11 pages
Proc. SPIE 8119, Terahertz Emitters, Receivers, and Applications II, 81190H (7 September 2011); doi: 10.1117/12.895531
Published in SPIE Proceedings Vol. 8119:
Terahertz Emitters, Receivers, and Applications II
Manijeh Razeghi; Nicolas Péré-Laperne; Henry O. Everitt; John M. Zavada; Tariq Manzur, Editor(s)
PDF: 11 pages
Proc. SPIE 8119, Terahertz Emitters, Receivers, and Applications II, 81190H (7 September 2011); doi: 10.1117/12.895531
Show Author Affiliations
S. Vassant, Institut d'Optique, CNRS, Univ. Paris Sud 11 (France)
Lab. de Photonique et Nanostructures, CNRS (France)
F. Pardo, Lab. de Photonique et Nanostructures, CNRS (France)
P. Bouchon, Lab. de Photonique et Nanostructures, CNRS (France)
Lab. de Photonique et Nanostructures, CNRS (France)
F. Pardo, Lab. de Photonique et Nanostructures, CNRS (France)
P. Bouchon, Lab. de Photonique et Nanostructures, CNRS (France)
F. Marquier, Institut d'Optique, CNRS, Univ. Paris Sud 11 (France)
J. J. Greffet, Institut d'Optique, CNRS, Univ. Paris Sud 11 (France)
J. L. Pelouard, Lab. de Photonique et Nanostructures, CNRS (France)
J. J. Greffet, Institut d'Optique, CNRS, Univ. Paris Sud 11 (France)
J. L. Pelouard, Lab. de Photonique et Nanostructures, CNRS (France)
Published in SPIE Proceedings Vol. 8119:
Terahertz Emitters, Receivers, and Applications II
Manijeh Razeghi; Nicolas Péré-Laperne; Henry O. Everitt; John M. Zavada; Tariq Manzur, Editor(s)
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