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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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Kazansky, Peter
University of Southampton
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (41/41 displayed)
- 2017Ultrafast laser-induced birefringence in various porosity silica glasses: from fused silica to aerogelcitations
- 2015Functional birefringent elements imprinted by femtosecond laser nanostructuring of multi-component glass
- 2015Revealing the nanoparticles aspect ratio in the glass-metal nanocomposites irradiated with femtosecond lasercitations
- 2015Glass-metal nanocomposite modification by femtosecond laser irradiation
- 2014High-purity, broadband, entangled photon pairs generated in poled silica fibers
- 2014Multi-watt all-fiber frequency doubled lasercitations
- 2014All-fiber frequency-doubled visible lasercitations
- 2013Extraordinary anisotropy of ultrafast laser writing in glasscitations
- 2013Laser assisted modification of poled silver-doped nanocomposite soda-lime glass
- 2012Exciton mediated self-organization in glass driven by ultrashort light pulsescitations
- 2011Light coupling and enhanced backscattering in layered plasmonic nanocompositescitations
- 2011Type II parametric downconversion in a poled fiber
- 2010Measurement of X(2) symmetry in a poled fibercitations
- 2010Enhanced light backscattering in thermally poled plasmonic nanocomposite and its application to vapour sensing
- 2010Leaky-modes excitation in thermally poled nanocomposite glass and their exploitation for saturable absorption
- 2010Saturation of absorption in noble metal doped nanocomposite glass film excited by evanescent light fieldcitations
- 2010Poling-assisted fabrication of plasmonic nanocomposite devices in glasscitations
- 2010The problem of achieving high second-order nonlinearities in glasses: The role of electric conductivity in poling of high index glassescitations
- 2010Aperiodically poled silica fibers for bandwidth control of quasi-phase-matched second-harmonic generationcitations
- 2009From type II upconversion to SPDC: a path to broadband polarization entanglement in poled fibers
- 2009High-average-power second-harmonic generation from periodically poled silica fiberscitations
- 2008Low loss photonic components in high index bismuth borate glass by femtosecond laser direct writingcitations
- 2008Ion-exchange-induced formation of glassy electrooptical and nonlinear optical nanomaterialcitations
- 2007Broadly tunable second-harmonic generation in periodically poled silica fiberscitations
- 2007Photon pair source based on parametric fluorescence in periodically poled twin-hole silica fibercitations
- 2007Recent advances in poling and nanostructuring of glass
- 2007Dissolution of embedded gold nanoparticles in sol-gel glass filmcitations
- 2006Creating unusual structures by ultrashort light pulses in glass
- 2006Bleaching of sol-gel glass film with embedded gold nanoparticles by thermal polingcitations
- 2006Breaking symmetry in glass by femtosecond laser irradiation
- 2005Electric field-assisted formation of percolated silver nanolayers inside glasscitations
- 2005Refractive index engineering in glass containing spherical silver nanoparticles using dc electric field
- 2005Origin and enhancement of the second-order non-linear optical susceptibility induced in bismuth borate glasses by thermal polingcitations
- 2004Enhanced stability of the second-order optical nonlinearity in poled glassescitations
- 2004Optical waveguides in electrooptical nanophase glass-ceramicscitations
- 2002Nonlinearity in poled tin-doped silica samples fabricated by sol-gel technique
- 2002Femtosecond laser direct-writing and poling of embedded grating structures
- 2001UV laser-induced current in germanosilicate fibres with built in electrodes
- 2001Thermally poled silica samples are structurally heterogeneous: Electron diffraction evidence of partial crystallizationcitations
- 2000Propagation of cold atoms along a miniature magnetic guidecitations
- 2000Memorized polarization-dependent light scattering in rare-earth-ion-doped glasscitations
Places of action
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conferencepaper
Nonlinearity in poled tin-doped silica samples fabricated by sol-gel technique
Abstract
Since its first proposal quasi-phase-matching (QPM) has been implemented in many materials to achieve efficient second-order nonlinear optical interactions. QPM provides flexibility and new possibilities for phase-matching, especially in materials where the birefringence is not high enough to compensate for the dispersion. Periodic poling of silica fibres exploits the potential of the QPM technology to extend the possibility of efficient frequency conversion to materials which have a widespread use in optical applications and offers several advantages. Thermal poling is the most reliable technique in terms of reproducibility and long-term stability of the induced nonlinearity. In this paper we present the results on induced nonlinearity we have achieved with thermal poling in two tin-doped silica samples fabricated by sol-gel technique [1]. The tin-content was estimated to be ~1.2 and 6%w/w. While the sample with lower Sn concentration appeared to be a glass, in the sample at high concentration, SnO2 segregated to give a glass ceramic. The second-order optical nonlinearity induced in glass by poling has been evaluated through a Maker fringe technique [2]. The second harmonic signal recorded for the poled samples is shown in figure 1. Data were fitted with d33 as free parameter. Assuming a nonlinear thickness of 5µm in the tin-doped samples, d33 is found to be ~0.20pm/V. The results confirm the good non-linearity of silica-based poled material prepared by sol-gel, whereas no relevant effects can be ascribed to the different phases of the SnO2 dopant at the indicated poling conditions. <br/><br/>Figure 1: Second harmonic signal (I2omega) as a function of the incident angle theta, for the poled glass-ceramic sample ([SnO2]~6%). The line represents the best fit achieved with d33=0.2026 pm/V.