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Estudo da orientação molecular em filmes automontados de azopolímeros por meio da técnica de geração de segundo harmônico (SHG) / Molecular orientation in self-assembled azo-polymer thin films studied by second harmonic generation (SHG).Lopes, Fábio Juliano da Silva 17 August 2006 (has links)
Filmes ultrafinos de polímeros que contém azocromóforos são importantes para muitas aplicações como armazenamento óptico, formação de grades de relevo superficiais, alinhamento de camadas de cristal líquido e dispositivos ópticos com propriedades não-lineares. Dentre as muitas técnicas de fabricação de filmes orgânicos ultrafinos, a técnica de Automontagem eletrostática camada a camada (Layer-by-Layer, LBL) é muito atrativa devido a sua simplicidade e versatilidade, permitindo o controle na espessura e na composição dos filmes em escalas nanométricas. Contudo, a completa caracterização estrutural de tais filmes enfrenta dificuldades devido à falta de técnicas experimentais apropriadas. Utilizamos a Geração de Segundo Harmônico (SHG) para estudar a orientação molecular de filmes automontados de um polieletrólito catiônico (PAH - Poli(alilamina hidroclorada)) e um polieletrólito aniônico contendo azocromóforos como grupos laterais (Ma-co-DR13) sobre substrato de vidro. O sinal de SHG é proporcional à susceptibilidade não-linear de segunda ordem do filme, que por sua vez depende da distribuição orientacional dos azocromóforos nesse filme. Os resultados indicam que existem uma orientação preferencial dos azocromóforos, que leva a uma não-linearidade óptica significativa. Entretanto, a intensidade do sinal e a anisotropia não são homogêneas por toda a amostra, indicando a presença de domínios orientacionais, que é verificado por meio da Microscopia a Ângulo de Brewster (BAM). O sinal médio de SHG não aumenta com a espessura do filme, indicando que a ordem orientacional das sucessivas bicamadas são independentes. Analisando o sinal de SHG em função das polarizações de saída e entrada, alguns parâmetros da distribuição orientacional dos azocromóforos podem ser deduzidos. Ajustando as medidas de SHG a uma distribuição modelo concluímos que os cromóforos possuem uma certa distribuição angular com um ângulo médio em relação à superfície do plano de aproximadamente 40° e uma pequena anisotropia ao longo do plano do filme. Utilizamos também o Método da Máxima Entropia (MEM) para determinar a distribuição mais larga possível compatível com nossos dados experimentais e comparar então com a distribuição modelo obtida através dos procedimentos de ajuste. / Ultrathin films of polymers containing azochromophores are important for many applications such as optical data storage, formation of surface relief gratings, liquid crystal alignment layers and non-linear optical devices. Among several techniques for fabricating organic thin films, the Layer-By-Layer electrostatic self-assembly (LBL) is very attractive due to its simplicity and versatility, allowing one to control film thickness and composition in the nanometer scale. However, thorough structural characterization of such films is often difficult due to lack of appropriate experimental techniques. We have used optical second-harmonic generation (SHG) to study the molecular orientation of Layer-by-Layer films of a cationic polyelectrolyte ((PAH - Poly(allylamine hydrochloride)) and a anionic polyelectrolyte containing azochromophores with azo side groups (PAH/Ma-co-DR13) on a glass substrate. The SHG signal is proportional to the second-order nonlinear susceptibility of the film, which in turn depends on the orientational distribution of the azo chromophores in the film. The results indicate that there is a preferential orientation of the azo chromophores in the film, leading to a significant optical nonlinearity. However, both the signal strength and its anisotropy are not homogeneous throughout the sample, indicating the presence of orientational domains. This is verified through Brewster Angle Microscopy (BAM). The average SHG signal does not increase with film thickness, indicating that the orientational order of successive bilayers are independent. Analyzing the SHG signal as a function of the input and output polarizations, a few parameters of the azochromophore orientational distribution can be deduced. Fitting the SHG signal to a simple model distribution, we have concluded that the chromophores have an angular distribution with a mean tilt from the surface plane of approximately 41° and a slight in-plane anisotropy. We have also used the Maximum-Entropy Method (MEM) to determine the widest orientational distribution compatible with our data and compared it to the model distribution obtained by the fitting procedure.
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Estudo da orientação molecular em filmes automontados de azopolímeros por meio da técnica de geração de segundo harmônico (SHG) / Molecular orientation in self-assembled azo-polymer thin films studied by second harmonic generation (SHG).Fábio Juliano da Silva Lopes 17 August 2006 (has links)
Filmes ultrafinos de polímeros que contém azocromóforos são importantes para muitas aplicações como armazenamento óptico, formação de grades de relevo superficiais, alinhamento de camadas de cristal líquido e dispositivos ópticos com propriedades não-lineares. Dentre as muitas técnicas de fabricação de filmes orgânicos ultrafinos, a técnica de Automontagem eletrostática camada a camada (Layer-by-Layer, LBL) é muito atrativa devido a sua simplicidade e versatilidade, permitindo o controle na espessura e na composição dos filmes em escalas nanométricas. Contudo, a completa caracterização estrutural de tais filmes enfrenta dificuldades devido à falta de técnicas experimentais apropriadas. Utilizamos a Geração de Segundo Harmônico (SHG) para estudar a orientação molecular de filmes automontados de um polieletrólito catiônico (PAH - Poli(alilamina hidroclorada)) e um polieletrólito aniônico contendo azocromóforos como grupos laterais (Ma-co-DR13) sobre substrato de vidro. O sinal de SHG é proporcional à susceptibilidade não-linear de segunda ordem do filme, que por sua vez depende da distribuição orientacional dos azocromóforos nesse filme. Os resultados indicam que existem uma orientação preferencial dos azocromóforos, que leva a uma não-linearidade óptica significativa. Entretanto, a intensidade do sinal e a anisotropia não são homogêneas por toda a amostra, indicando a presença de domínios orientacionais, que é verificado por meio da Microscopia a Ângulo de Brewster (BAM). O sinal médio de SHG não aumenta com a espessura do filme, indicando que a ordem orientacional das sucessivas bicamadas são independentes. Analisando o sinal de SHG em função das polarizações de saída e entrada, alguns parâmetros da distribuição orientacional dos azocromóforos podem ser deduzidos. Ajustando as medidas de SHG a uma distribuição modelo concluímos que os cromóforos possuem uma certa distribuição angular com um ângulo médio em relação à superfície do plano de aproximadamente 40° e uma pequena anisotropia ao longo do plano do filme. Utilizamos também o Método da Máxima Entropia (MEM) para determinar a distribuição mais larga possível compatível com nossos dados experimentais e comparar então com a distribuição modelo obtida através dos procedimentos de ajuste. / Ultrathin films of polymers containing azochromophores are important for many applications such as optical data storage, formation of surface relief gratings, liquid crystal alignment layers and non-linear optical devices. Among several techniques for fabricating organic thin films, the Layer-By-Layer electrostatic self-assembly (LBL) is very attractive due to its simplicity and versatility, allowing one to control film thickness and composition in the nanometer scale. However, thorough structural characterization of such films is often difficult due to lack of appropriate experimental techniques. We have used optical second-harmonic generation (SHG) to study the molecular orientation of Layer-by-Layer films of a cationic polyelectrolyte ((PAH - Poly(allylamine hydrochloride)) and a anionic polyelectrolyte containing azochromophores with azo side groups (PAH/Ma-co-DR13) on a glass substrate. The SHG signal is proportional to the second-order nonlinear susceptibility of the film, which in turn depends on the orientational distribution of the azo chromophores in the film. The results indicate that there is a preferential orientation of the azo chromophores in the film, leading to a significant optical nonlinearity. However, both the signal strength and its anisotropy are not homogeneous throughout the sample, indicating the presence of orientational domains. This is verified through Brewster Angle Microscopy (BAM). The average SHG signal does not increase with film thickness, indicating that the orientational order of successive bilayers are independent. Analyzing the SHG signal as a function of the input and output polarizations, a few parameters of the azochromophore orientational distribution can be deduced. Fitting the SHG signal to a simple model distribution, we have concluded that the chromophores have an angular distribution with a mean tilt from the surface plane of approximately 41° and a slight in-plane anisotropy. We have also used the Maximum-Entropy Method (MEM) to determine the widest orientational distribution compatible with our data and compared it to the model distribution obtained by the fitting procedure.
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Nanostructured Assemblies Based On Metal Colloids And Monolayers: Preparation, Characterisation And Studies Towards Novel ApplicationsDevarajan, Supriya 07 1900 (has links)
Nanoscience dominates virtually every field of science and technology in the 21st century. Nanoparticles are of fundamental interest since they possess unique size- dependent properties (optical, electrical, mechanical, chemical, magnetic etc.), which are quite different from the bulk and the atomic state. Bimetallic nanoparticles are of particular interest since they combine the advantages of the individual monometallic counterparts.
The present study focuses on bimetallic nanoparticles containing gold as one of the constituents. Au-Pd, Au-Pt and Au-Ag bimetallic/alloy nanoparticles have been prepared by four different synthetic methods, and characterised by a variety of techniques, with an emphasis on Au-Ag alloy systems in the solution phase as well as in the form of nanostructured films on solid substrates. Au- Ag alloy nanoparticles have been used to demonstrate two different applications. The first is the use of Au-Ag monolayer protected alloy clusters in demonstrating single electron charging events in the solution phase as well as in the dry state. Single electron transfer events involving nanosized particles are being probed extensively due to their potential applications in the field of electronics. The second is an analytical application, involving the use of trisodium citrate capped Au-Ag alloy hydrosols as substrates for surface enhanced Raman and resonance Raman scattering [SE(R)RS] studies. The sols have been used for single molecule detection purposes.
Various organic molecules such as quinones, phthalocyanines and methyl violet have been self- assembled in a stepwise manner on the nanoparticulate as well as bulk Au, Ag and Au-Ag surfaces, and characterised extensively by spectroscopic, electrochemical and spectroelectrochemical techniques.
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Multiwavelength Surface Plasmon Resonance Sensor Designs for Chemical and Biochemical DetectionEarp, Ronald Lee Jr. 08 July 1998 (has links)
Surface plasmon resonance (SPR) sensors using multiwavelength light coupling are investigated to probe changes in refractive index that occur as a result of chemical or biochemical processes. Traditional SPR sensors have used angle modulation to facilitate detection at the sensor surface; however, the multiwavelength approach is novel and brings new functionality to SPR sensors.
The multiwavelength sensors are constructed on both fiber optic and bulk waveguides such as prisms. A thin metal film is deposited on the waveguide surface to support the surface plasmon (SP) mode. The evanescent field produced by light propagating through the waveguide can be coupled into the surface plasmon mode thus attenuating the transmitted light. This coupling is dependent upon phase matching between the light wavevector and the surface plasmon wavevector. The wavevectors are directly related to the wavelength of light, thickness of analyte on the sensor surface and the refractive index of the analyte. As these parameters change, the light output from the sensor will be affected. Other thin films can be subsequently deposited on the metal to functionalize the sensor surface for a particular analyte of interest. A theoretical background and details of the sensor construction is given.
The developed sensors are tested in a variety of application systems. Experimental results for refractive index sensing in bulk liquid applications is shown. Observed sensitivity approaches that of conventional SPR techniques. Alkyl-thiol monolayer systems are studied to investigate kinetics of formation and the thickness resolution of the sensor. A biochemical system is investigated to compare the sensors with other immunoassay techniques. Ionic self-assembled monolayer (ISAM) systems are investigated to probe structure and determine their usefulness as an immobilization layer for biochemical species.
A mathematical model based on Fresnel reflection equations is developed to predict sensor response. This model can be used to selectively vary sensor parameters to optimize the response for a specific analyte system or to calculate system parameters based on experimental results. Results from the various experiments are compared with the model.
Experimental results and interpretations are discussed along with future work and potential improvements. Classical SPR sensors are also discussed along with comparisons with the multiwavelength sensors. Future improvements to SPR sensors design are considered, as is the application of the technology to high-throughput drug screening for pharmaceuticals. / Ph. D.
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