Abstract
We analyze microstructure, linear and nonlinear optical properties of planar waveguides produced by implantation of MeV Ag ions into LiNbO3. Linear optical properties are described by the parameters of waveguide propagation modes and optical absorption spectra. Nonlinear properties are described by the nonlinear refractive index. Operation of the implanted crystal as an optical waveguide is due to modification of the linear refractive index of the implanted region. The samples as implanted do not show any light-guiding. The implanted region has amorphous and porous microstructure with the refractive index lower than the substrate. Heat treatment of the implanted samples produces planar light-guiding layer near the implanted surface. High-resolution electron microscopy reveals re-crystallization of the host between the surface and the nuclear stopping region in the form of randomly oriented crystalline grains. They make up a light-guiding layer isolated from the bulk crystal by the nuclear stopping layer with low refractive index. Optical absorption of the sample as implanted has a peak at 430 nm. This peak is due to the surface plasmon resonance in nano-clusters of metallic silver. Heat treatment of the samples shifts the absorption peak to 545 nm. This is more likely due to the increase of the refractive index back to the value for the crystalline LiNbO3. The nonlinear refractive index of the samples at 532 nm (of the order of 10-10 cm2 W-1) was measured with the Z-scan technique using a picosecond laser source. Possible applications of the waveguides include ultra-fast photonic switches and modulators.
Original language | English |
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Pages (from-to) | 750-757 |
Number of pages | 8 |
Journal | Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms |
Volume | 166 |
DOIs | |
State | Published - May 2 2000 |
Event | 10th International Conference on Radiation Effects in Insulators - Jena, Ger Duration: Jul 18 1999 → Jul 23 1999 |
Funding
This research was supported by the NASA Alliance for Nonlinear Optics (NASA Grant NAG5-6532), the Division of Material Sciences, US Department of Energy (Contract DE-AC05-96OR22464 with Lockheed Martin Energy Research Corp.), and US Army Research Office (grant DAAH04-96-1-190) and by the National Centre for HREM, The Netherlands.
Funders | Funder number |
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Division of Material Sciences | |
NASA Alliance for Nonlinear Optics | |
National Centre for HREM | |
U.S. Department of Energy | DE-AC05-96OR22464 |
National Aeronautics and Space Administration | NAG5-6532 |
Army Research Office | DAAH04-96-1-190 |