, an electric dipole, the driving current is supplied externally in the circuit. For optical antennas, the oscillations are generated by the incident EM field
, Interface along the x ? y plane between a metal and a dielectric
, Scanning electron micrographs of different optical antenna designs. (a) Hertzian dimmer antenna, 2012.
, (c) Bowtie antenna and (d) Yagi-Uda antenna. SEM image courtesy of Xiao Yu, PhD student at the ICB lab
, Black dots correspond to experimental data. The red and blue lines correspond to fits to the Drude and Drude-Lorentz models
, The red dashed squares point to its interband transitions (b)
, (a) one-photon absorption, (b) direct two-photon resonance mediated by a virtual state, (c) resonant sequential two-photon absorption, (d) relaxed sequential absorption. Adapted with permission from, vol.120, 1994.
, A femtosecond laser pulse generates surface plasmons in the particle which exponentially decay into hot electrons and holes within ? 10 fs. (c) Coulomb electron-electron interactions lead to the decay of the most energetic electrons in a few tenths of femtoseconds and eventually relax back to ambient temperature in the picosecond scale thanks to the coupling with phonons. Shaded areas represent the initial Fermi-Dirac distribution of electronic states, points indicate the occupancies of different energy levels, Schematic representation of the hot electron generation in gold nanostructures. (a) A gold nanostructure is initially in thermal equilibrium at T = T 0 . (b)
, 73 3.6.1 (a) SEM micrograph of a 5 µm × 150 nm AuNW electrically contacted at the distal end. Another electrode is separated 50 nm from the nanowire to apply a potential difference across the gap. (b) Schematic of the electrical connection at distal-end region of the nanowire. (c) Excitation laser filtered optical image showing the generated N-PL throughout the AuNW. The dashed squared area is zoomed in and showed at the bottom of the image. The circle indicates the monitored area, PL spectra of the 7.0 µm studied AuNW (a) at different positions along the nanowire and (b
, 3 (a) N-PL emission spectra at the distal end of a 5.0 µm long AuNW under the action of a 14 V bias and without any bias applied. The acquisition time is fixed at t acq = 0.2 s. Wide field optical images of the filtered nonlinear emission of the same nanowire under (b) 0 V and (c) 14 V bias applied, vol.6
, High resolution transmission electron microscope (HRTEM) image showing the crystallinity of the synthesized silver nanowires. Image provided by the group of G.V.P. Kumar in IISER Pune, India. The inset represents the corresponding fast Fourier Transform. SEM images of (b) a typical nanowire and its two terminations (c,d). The AgNW diameter is around 530 nm, p.80
, Leakage radiation (LR) is emitted under the phase-match angle range represented by ?. An oil-immersion objective collects the leakage radiation. The transversal polarization is indicated by the blue arrows. The zoomed area corresponds to the dashed square, p.82
, Arrows point to the straight lines resulting from the excitation of two leaky modes. (c) Profiles at the edges of the nanowire for the dashed area indicated in (a). (d) Cross section of the Fourier plane shown in (b) at k y /k 0 = 0 for the multiple leaky modes excitation showed in (a), a) Wide-field image of the relative intensity distribution of the leaky mode in a 12.6 µm long AgNW. A bright-field image of the same nanowire is shown at the left. (b
Recipes for spin coating the two PMMA layers needed for e-beam lithography. . 30 2.3.2 Recipes for spin coating the AZ nLOF, p.31, 2070. ,
, Azimuthal wavevector spread angles for the Fourier plane images shown in fig
Gérard Colas des Francs, and Alexandre Bouhelier. Electrical Command of the Nonlinear Photoluminescence in Plasmonic Antennas. Preparing for submission ,
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, ? Electrical Command of the Nonlinear Photo-luminescence of Plasmonic Gap Antennas Surface Plasmon Photonics 8 SPP8 2017
, ? Electrical Command of the Linear and Nonlinear responses of Plasmonic Gap Antennas Journeés de l'Ecole Doctorale Carnot-Pasteur, 2017.
, ? Electrical Command of the Nonlinear Photoluminescence of Plasmonic Gap Antennas Summer School on Plasmonics 4 SSOP4 2017
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