by Tong Wai Yin Alex. / Thesis (M.Phil.)--Chinese University of Hong Kong, 1996. / Includes bibliographical references (leaf 55). / by Tong Wai Yin Alex. / Acknowledgement / Biographical Sketch / Abstract / Table of contents / Chapter Chapter 1 --- Introduction --- p.1 / Chapter Chapter 2 --- Nonlinear Optics in dye-doped solid --- p.4 / Chapter 2.1 --- Nonlinear Optics --- p.4 / Chapter 2.2 --- Photophysics of dye molecules --- p.6 / Chapter 2.3 --- Nonlinear effect in dye-doped solid --- p.8 / Chapter Chapter 3 --- Sol-Gel Silica --- p.11 / Chapter 3.1 --- The formation of dye-doped sol-gel silica --- p.11 / Chapter 3.2 --- The physical properties --- p.15 / Chapter 3.3 --- The optical properties --- p.16 / Chapter Chapter 4 --- Saturation Absorption --- p.18 / Chapter 4.1 --- Saturation Absorption in Fluorescein 548 dye-doped solid --- p.18 / Chapter 4.2 --- Experimental Details --- p.19 / Chapter 4.3 --- Results and Discussion --- p.19 / Chapter 4.4 --- Conclusion --- p.30 / Chapter Chapter 5 --- Optical Phase Conjucation --- p.31 / Chapter 5.1 --- OPC Theory --- p.31 / Chapter 5.11 --- The Distortion Correction Theorem --- p.32 / Chapter 5.12 --- The Proof of the Distortion Theorem --- p.32 / Chapter 5.13 --- The generation of Phase Conjucate Waves --- p.34 / Chapter 5.2 --- Degenerate Four Wave Mixing --- p.35 / Chapter 5.21 --- Geometries of DFWM --- p.35 / Chapter 5.22 --- DFWM Theory --- p.37 / Chapter 5.23 --- DFWM in Absorbing Media --- p.40 / Chapter 5.3 --- Experimental Details --- p.44 / Chapter 5.4 --- Results and Discussion --- p.46 / Chapter 5.5 --- Conclusion --- p.53 / Chapter Chapter 6 --- Conclusion and Suggestions for future work --- p.54 / Reference

Wang Jun. / Thesis (M.Phil.)--Chinese University of Hong Kong, 2003. / Includes bibliographical references (leaves 74-79). / Abstracts in English and Chinese. / Acknowledgements --- p.i / List of publications --- p.ii / Abstract (In English) --- p.iii / Abstract (In Chinese) --- p.v / Table of contents --- p.vii / List of figures --- p.x / List of tables --- p.xiv / Chapter Chapter I --- Introduction --- p.1 / Chapter Chapter II --- Dye-doped sol-gel zirconia and zirconia-organically modified silicate waveguides --- p.6 / Chapter 2.1 --- General sol-gel process --- p.6 / Chapter 2.2 --- Dye-doped sol-gel zirconia and zirconia-ORMOSIL waveguides --- p.7 / Chapter Chapter III --- Basic theory and experiment setup of distributed feedback waveguide lasers --- p.13 / Chapter 3.1 --- Coupled-wave theory of distributed feedback lasers --- p.13 / Chapter 3.2 --- Introduction on the theory of planar optical waveguide --- p.16 / Chapter 3.3 --- Experiment setup design of DFB waveguide lasers --- p.19 / Chapter Chapter IV --- Zirconia and zirconia-organically modified silicate distributed feedback waveguide lasers tunable in the visible --- p.23 / Chapter Chapter V --- Tunable multi-wavelength distributed feedback zirconia waveguide lasers --- p.35 / Chapter 5.1 --- Brief introduction on multi-wavelength lasers --- p.35 / Chapter 5.2 --- R6G-doped zirconia multi-mode waveguides --- p.36 / Chapter 5.3 --- Experimental results and discussion --- p.39 / Chapter 5.3.1. --- Dual- and quadruple-wavelength DFB waveguide lasers --- p.39 / Chapter 5.3.2. --- The dispersion characteristics of multi-wavelength DFB waveguide lasers --- p.44 / Chapter 5.3.3. --- Determination of waveguide parameters by the DFB technique --- p.48 / Chapter 5.4 --- Summary --- p.51 / Chapter Chapter VI --- Distributed feedback laser action in sol-gel glass symmetric waveguides --- p.53 / Chapter 6.1 --- The fabrication of dye-doped glass symmetric waveguides --- p.54 / Chapter 6.2 --- Experimental results and discussion --- p.56 / Chapter 6.2.1. --- DFB laser action in sol-gel glass symmetric-asymmetric waveguide --- p.56 / Chapter 6.2.2. --- Dispersion characteristics of DFB symmetric and asymmetric waveguide lasers --- p.61 / Chapter 6.3 --- Summary --- p.65 / Chapter Chapter VII --- Summary --- p.69 / References --- p.74

A molecular nitrogen laser was constructed and preliminary tests were performed to establish the fact that lasing action was taking place. The purpose was to show that a high energy pump source of ultraviolet radiation could be constucted, given a limited budget and expertise, which would be of the quality required to perform spectrographic research.Ball State UniversityMuncie, IN 57406

Made available in DSpace on 2016-03-15T19:38:54Z (GMT). No. of bitstreams: 1 RODRIGO MENDES GEROSA.pdf: 6396087 bytes, checksum: b904e08a314dcda72a403496699b5206 (MD5) Previous issue date: 2015-08-26 / Fundo Mackenzie de Pesquisa / This thesis describes the development of new photonic devices produced by micromanipulation of the optical fibers properties, i.e., the change, in the micrometer scale, of the fiber s optical and/or geometrical properties. In this context, three lines of research have been followed, using different optical fiber processing techniques and considering different types of devices. In the first line, the coupling of two cores in a photonic crystal fiber with three initially uncoupled cores was demonstrated. The couplers had an insertion loss estimated at ~1 dB and exhibited spectral modulations with a depth up to 18 dB. They also showed high sensitivity to polarization, which can be exploited in fiber polarization beamsplitters. For this work, we used a technique that modifies the fiber structure by applying local differential pressure and heating. In the second line, a Rhodamine dye laser was develop with a fully fiber integrated optofluidic cavity. It was possible to maintain a high flow of the dye solution, up to 400 μL / min, which allowed the use of a pump laser with a high repetition rate (1 kHz), and, at the same time, the degradation of the gain medium was not observed. An optical conversion rate of up to 9% and a pump energy threshold lower than 1 mJ were obtained. A splicing technique was used, in which an angled cleaved capillary fiber was fused to a conventional fiber, thereby leaving a side inlet open for the fluid flow. The third line aimed at the incorporation of carbon nanomaterials to optical fibers. In this case, two approaches were employed: in one of them, polymeric films, with a thickness of 20 μm, containing carbon nanotubes were produced on the face of optical fiber patchcords; such patchcords have been inserted into erbium-doped fiber laser cavities to act as saturable absorbers in order to obtain mode-locking operation. Pulses with durations down to 364 fs were obtained with 10.2 nm bandwidths. The films were formed when a micro-droplet of a carbon nanotube suspension on an optical adhesive was placed on the surface of optical fiber connectors, with the use of a micropipette. Within the same line, photonic crystal fibers (PCFs) with homogeneous graphene oxide films covering the inner walls of their capillaries were obtained. The homogeneity was confirmed by Raman spectroscopy and by the loss per fiber length, as measured by the cut back method. A PCF was also spliced to conventional connectorized fiber patchcords and incorporated into a laser cavity to generate pulses. The film production was consisted of inserting a graphene oxide suspension into the PCF capillaries, after which the solvent was dried. / Essa tese descreve o desenvolvimento de novos dispositivos fotônicos produzidos a partir da micromanipulação das propriedades de fibras ópticas, isto é, da alteração em escala micrométrica, das propriedades ópticas e/ou geométricas destas. Nesse contexto, três linhas de trabalho foram seguidas, utilizando diferentes técnicas de processamento de fibras ópticas e levando à demonstração de diferentes tipos de dispositivos. Na primeira linha foi demostrado o acoplamento de dois núcleos em uma fibra de cristal fotônico com três núcleos inicialmente desacoplados. Os acopladores apresentaram uma perda de inserção estimada de ~1 dB e exibiram modulações espectrais com uma profundidade de até 18 dB. Apresentaram também uma sensibilidade elevada à polarização, que pode ser explorada em divisores de polarização (polarization beamsplitters) a fibra. Para isso foi utilizada uma técnica de alteração da estrutura da fibra através da aplicação de pressão diferencial e aquecimento local,. Na segunda linha foi desenvolvido um laser do corante Rodamina com uma cavidade optofluídica totalmente integrada em fibra. Nela, era possível manter um alto fluxo da solução de corante, de até 400 μl/min, o que permitiu utilizar um laser de bombeio com alta taxa de repetição (1kHz) sem observar-se degradação do meio de ganho. Uma taxa de conversão óptica de até 9% e uma energia de limiar (threshold) menor que 1 μJ foram obtidas. Utilizou-se aqui uma técnica de emenda através da qual uma fibra capilar clivada em ângulo era emendada com uma fibra convencional, deixando assim uma entrada lateral para fluidos. A terceira linha visou incorporar nanomateriais de carbono a fibras ópticas. Nesse caso duas abordagens foram empregadas: em uma, filmes poliméricos com espessuras de 20 μm e contendo nanotubos de carbono foram produzidos na face de conectores de cordões de fibra ópticas; esse cordões foram inseridos em cavidades laser a fibra dopada com érbio para atuar como absorvedores saturáveis para a obtenção de mode locking. Com isso foram obtidos pulsos de até 364 fs e espectros com larguras de banda de 10,2 nm. Os filmes foram formados a partir de uma microgota de uma suspensão de nanotubos de carbono em adesivos ópticos que foi colocada sobre a face de conectores de fibra óptica com uma micropipeta. Ainda na mesma linha obtiveram-se fibras de cristal fotônico (PCFs) com filmes de óxido de grafeno homogêneos no interior de seus capilares. A homogeneidade foi comprovada através de espectroscopia Raman e pela medida da perda em função do comprimento das fibras, realizada através do método cut back. Uma PCF foi, ainda, emendada a cordões de fibra convencional conectorizados e incorporada a cavidades laser para geração de pulsos. A produção dos filmes foi realizada através da inserção de uma suspensão de óxido de grafeno nos capilares de PCFs de núcleo sólido, após o qual o solvente era secado.