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Composite thin films of PbTiO3 nano-crystals and high transparency polymer polyetherketone(PEK-c) for application of non-linear optical devices were prepared by spin coating. The size of PbTiO3 nano-crystals was estimated to be 30-40 nm using a transmission electron microscope. The refractive index and the mode propagation losses at 633 nm were measured using the prism coupling technique and improved photographic technique respectively. They were found to be 1.6545 and 2.00 dB cm-1 (fundamental mode),respectively. Moreover, it is observed that this loss is increased at higher mode indices.

参考文献

[1] S R Marder;B Kippelen .Design and Synthesis of Chromophores and Polymers for Electro-optic and Photorefractive Applications[J].Nature,1997,388:845-851.
[2] A Chan;V Chuyanov .Low-VπElectro-optic Modulator with a High-μβ Chromophore and a Constant-bias Field[J].Optics Letters,1998,23:478-480.
[3] M D Fontana;F Abdi;K Wojcik .Electro-optical Properties of a Single Domain PbTiO3 Crystal[J].Journal of Applied Physics,1995,77:2102-2106.
[4] T Chen;Y Yuan;J Xu.Interaction of Organic Solvents with a Novel Polyetheretherketone[J].CHINESE JOURNAL OF APPLIED CHEMISTRY,1988(05):52-56.
[5] Q. Ren;D. Xu;Y.T. Chow;Z.H. Lu;C.B. Ma;G.H. Zhang;H.P. Chan;P.L. Chu .Preparaton and characterization of a poled nanocrystal and polymer composite PbTiO_3/PEK-c film for electro-optic applications[J].Applied physics, A. Materials science & processing,2003(2):183-186.
[6] W Gleine;J Muller .Low-pressure Chemical Vapor Deposition Silicon-oxynitride Films for Integrated Optics[J].Applied Optics,1992,31:2036-2040.
[7] Y Okamura;S Yoshinaka;S Yamamoto .Measuring Mode Propagation Losses of Integrated Optical Waveguides:a Simple Method[J].Applied Optics,1983,22:3892-3894.
[8] Q Ren;Z G Wang .Measurement of PT-PEK-c Polymer Film Parameters using the Quasi-waveguide m-line Method[J].Journal of Materials Science and Letters,1997,16:1389-1391.
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