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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Tranchant, Laurent
Institut photonique d'analyse non-destructive européen des matériaux anciens
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (7/7 displayed)
- 2017Polaritonic figure of merit of plane structurescitations
- 2015Guided near-field radiative heat transfer : study of nanostructures supporting surface phonon-polaritons
- 2015Measurement of the in-plane thermal conductivity of SiO2 thin films due to surface phonon-polaritons
- 2015Focusing of surface phonon-polaritons along conical and wedge polar nanostructurescitations
- 2014Fresnel-like formulas for the reflection and transmission of surface phonon-polaritons at a dielectric interfacecitations
- 2014Effects of anisotropy and size of polar nano thin films on their thermal conductivity due to surface phonon-polaritonscitations
- 2013Anomalous thermal conductivity by surface phonon-polaritons of polar nano thin films due to their asymmetric surrounding mediacitations
Places of action
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article
Focusing of surface phonon-polaritons along conical and wedge polar nanostructures
Abstract
International audience ; Focusing of surface phonon-polaritons propagating toward the tip of a cone and the edge of a wedge is theoretically analyzed and compared. Based on Maxwell's equations, explicit expressions for the dispersion relations in each structure are determined and solved numerically for a propagation parameter driving the surface phonon-polariton energy density. For conical and wedge structures of SiO2, it is found that: (1) the cone (wedge) supports the polariton focusing only for aperture angles in the interval 18°–68° (21°–51°), and within the range of excitation frequencies from 32.1 THz (31.5 THz) to 33.9 THz (33.9 THz). In this frequency interval, the real part of the SiO2 permittivity is negative and the presence of polaritons is significant. (2) The polariton focusing efficiency of both the cone and wedge reaches its maximum values at the critical frequency fcr=33.6 THz and at different aperture angles of about αopt=45° and αopt=30°, respectively. (3) When the polaritons travel from 100 nm to 5 nm toward the tip of the cone with this optimum angle, their Poynting vector increases by a factor of 12, which is about four times larger than the corresponding one provided by the wedge and indicates that the cone is more efficient than the wedge for the focusing of surface phonon-polaritons.