Nonlinear excitation of polariton cavity modes in ZnO single nanocombs
Tunable second harmonic (SH) polaritons have been efficiently generated in ZnO nanocombs, when the material is excited close to half of the band-gap. The nonlinear signal couples to the nanocavity modes, and, as a result, Fabry-Pérot resonances with high Q factors of about 500 are detected. Due to t...
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Optical Society of American (OSA)
2014
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| LEADER | 10945caa a22010217a 4500 | ||
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| 001 | PAPER-14295 | ||
| 003 | AR-BaUEN | ||
| 005 | 20241223093828.0 | ||
| 008 | 190411s2014 xx ||||fo|||| 00| 0 eng|d | ||
| 024 | 7 | |2 scopus |a 2-s2.0-84896376897 | |
| 040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
| 100 | 1 | |a Capeluto, María Gabriela | |
| 245 | 1 | 0 | |a Nonlinear excitation of polariton cavity modes in ZnO single nanocombs |
| 260 | |b Optical Society of American (OSA) |c 2014 | ||
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| 506 | |2 openaire |e Política editorial | ||
| 520 | 3 | |a Tunable second harmonic (SH) polaritons have been efficiently generated in ZnO nanocombs, when the material is excited close to half of the band-gap. The nonlinear signal couples to the nanocavity modes, and, as a result, Fabry-Pérot resonances with high Q factors of about 500 are detected. Due to the low effective volume of the confined modes, matterlight interaction is very much enhanced. This effect lowers the velocity of the SH polariton in the material by 50 times, and increases the SH confinement inside the nanocavity due to this higher refractive index. We also show that the SH phase-matching condition is achieved through LOphonon mediation. Finally, birrefringence of the crystal produces a strong SH intensity dependence on the input polarization, with a high polarization contrast, which could be used as a mechanism for light switching in the nanoscale. © 2014 Optical Society of America. |l eng | |
| 593 | |a Laboratorio de Electrónica Cuántica, Depto. de Física, FCEyN, UBA, 1428 Buenos Aires, Argentina | ||
| 593 | |a IFIBA-CONICET-UBA, 1428 Buenos Aires, Argentina | ||
| 593 | |a Laboratorio de Física del Sólido, Depto. de Física, FACET, UNT, 4000 S.M. de Tucumán, Argentina | ||
| 593 | |a CONICET, Argentina | ||
| 593 | |a Laboratorio de Nanomateriales y de Propiedades Dieléctricas, Depto. de Física, FACET, UNT, 4000 S.M. de Tucumán, Argentina | ||
| 690 | 1 | 0 | |a ENERGY GAP |
| 690 | 1 | 0 | |a PHASE MATCHING |
| 690 | 1 | 0 | |a PHONONS |
| 690 | 1 | 0 | |a PHOTONS |
| 690 | 1 | 0 | |a POLARIZATION |
| 690 | 1 | 0 | |a Q FACTOR MEASUREMENT |
| 690 | 1 | 0 | |a REFRACTIVE INDEX |
| 690 | 1 | 0 | |a ZINC OXIDE |
| 690 | 1 | 0 | |a EFFECTIVE VOLUME |
| 690 | 1 | 0 | |a INPUT POLARIZATION |
| 690 | 1 | 0 | |a INTENSITY DEPENDENCE |
| 690 | 1 | 0 | |a NONLINEAR EXCITATION |
| 690 | 1 | 0 | |a NONLINEAR SIGNALS |
| 690 | 1 | 0 | |a PHASE MATCHING CONDITIONS |
| 690 | 1 | 0 | |a POLARIZATION CONTRAST |
| 690 | 1 | 0 | |a SECOND HARMONICS |
| 690 | 1 | 0 | |a QUANTUM THEORY |
| 700 | 1 | |a Grinblat, G. | |
| 700 | 1 | |a Tirado, M. | |
| 700 | 1 | |a Comedi, David Mario | |
| 700 | 1 | |a Bragas, Andrea Verónica | |
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