The optical properties of gold in the visible are dominated by the response of the free conduction electrons to light. In gold nanostructures, the surface charge density adopts a configuration that is constrained by the shape of the nanoparticles. As a result, the scattering of light by gold nanoparticles exhibits a resonant response characterised by a strong scattering and absorption in a narrow range of frequencies. The spectral range of this \emph{localised surface plasmon resonance} (LSPR) can be tuned by varying the size and shape of the gold nanoparticle --- the nanoparticles act as nanoscale antennas for the visible light. Confirmation of this scaling rule is obtained by conducting experiments with nanoparticles of varying size and aspect ratio. Such particles are fabricated by electron-beam lithography, and characterised by dark-field spectroscopy. Not only does the LSPR shift in frequency with a change of particle size, but its spectral lineshape is also modified. The intensity and width of the LSPR are dictated by a variety of factors that are related to the intrinsic material properties (the complex dielectric function of gold), and to the particle geometry and environment. The optical response of small gold nanorods is well described by a simple oscillating dipole model --- the incident electromagnetic field induces a current in the particle that re-radiates light (scattering). A series of refinements can be made to model more accurately the optical response of realistic particles. If the dipole moment characterising the particle is allowed to vary in phase across the particle, retardation effects provide a correction for the effective dipole moment of the particle. As the particle size approaches the wave length in the surrounding medium, the dipolar approximation breaks down and higher order multipoles need to be considered. The Mie theory provides a very accurate description of the response of spheres of arbitrary size. Further, the T-matrix and other numerical techniques can be employed to accurately reproduce the scattering properties of particles of arbitrary shapes. When the scattering sample consists of a collection of gold nanoparticles, the collective optical response is affected by two key factors. First, the measured LSPR is a convolution of the distribution of particle sizes with the individual response of a single particle. This leads to an inhomogeneous broadening of the LSPR lineshape. Second, the light that is scattered by one such particle near resonance can strongly affect its neighbours which scatter light in proportion to the net field they experience, that is the sum of the incident field plus the perturbation arising from the neighbouring particles. The onset of such multiple scattering events is observed even for particle separations that are several times larger than the particle size. Several regimes of interaction can be distinguished according to the ratio separation / wavelength. First, when the particles are in close proximity (separation $\ll$ wavelength), near-field interactions dominate and result in a spectral shift of the LSPR accompanied with a spectral broadening. Second, when the separation is commensurate with the wavelength, a coherent interaction can develop that couples a large number of particles. In ordered arrays, such coupling gives rise to a geometrical resonance that can strongly affect the LSPR of the particles. In particular a sharp spectral feature is observed that depends on both the single particle response and the geometrical arrangement of the particles in the array. The coherence of such multiple scattering in diffractive arrays of gold nanoparticles can be broken by introducing disorder in the distribution of particle sizes, or in the particle positions. The optical properties of an irregular array reflect the departure from a periodic system and the spectral lineshape evolves as the level of disorder is increased. In the limit of uncorrelated positions, the diffractive coupling is suppressed and the response of the collection of the particles rejoins the response of isolated particles.

A caracterização das propriedades ópticas de moléculas de DNA, tais como a absorção e a fluorescência por excitação, são importantes para a determinação de parâmetros usados no desenvolvimento de biossensores fotônicos. O estudo da absorção óptica do DNA, obtido por diferentes métodos tem se mostrado muito eficiente na determinação do grau de pureza do material genético obtido por amplificação, ou extração e purificação do DNA total. Por outro lado, a fluorescência por excitação a partir de um marcador cromóforo é uma técnica importante em processos de quantificação de massa, em técnicas tais como a eletroforese em gel de agarose. Devido à baixa fluorescência de moléculas de DNA na região visível do espectro, entre 500-600nm, utiliza-se destes marcadores que se ligam à molécula e que são opticamente ativos nesta região para detecção de sua emissão de fluorescência. Neste trabalho foi realizado um estudo da fluorescência do DNA, obtido a partir de uma amplificação por transcriptase reversa do RNA (RT-PCR), na região de 400nm a 600nm, sem adição de marcador e utilizando excitação por um e dois fótons (405nm e 800nm) através da técnica de microscopia confocal. As amostras contendo solução de dsDNA (237ng/μL) foram depositadas sobre um filme de prata de 200nm de espessura que também é crescido previamente sobre um substrato de vidro. Sobre o filme metálico é fabricado nanoestruturas metálicas por de litografia por feixe de íons com um microscópio de duplo feixe FEI Quanta 3D 200i. As nanoestruturas são formadas por arranjos concêntricos de anéis com diâmetros de até 20 μm, largura 50nm e separados por 400nm. Quando a excitação do material genético ocorre sobre a nanoestrtutura o laser gera na nanoestrutura plasmon-polaritons de superfície (SPP) que interagem com as moléculas de dsDNA na solução. Observa-se que nas regiões onde as nanoestruturas são fabricadas que a intensidade de fluorescência da macromolécula é muito maior do que a obtida fora da estrutura e sobre o filme metálico. Os efeitos da interação entre SPPs e as moléculas aumentam a atividade óptica (taxa de emissão) e podem servir como base para a fabricação de sensores fotônicos ultrasensíveis. Concluindo, os efeitos dos campos plasmônicos sobre o fluoróforo são significativos e foram observados pela diminuição do tempo de vida das moléculas e o aumento da sua fluorescência. / The characterization of the optical properties of DNA molecules, such as absorption and excitation fluorescence, is important to the determination of the parameters used for the preparation of photonic biosensors. The study of optical absorption of DNA, obtained through different methods, currently has a high sensitivity to determine the degree of purity of the genetic material obtained by amplification, extraction and purification of the total DNA. On the other hand, excitation fluorescence using a marker is an important technique in mass quantification processes together with techniques such as agarose gel electrophoresis. Because of low fluorescence of DNA molecules, in the visible region of the spectrum, between 500-600nm, the use of labels that bind to the molecule are critically for the detection of their fluorescence emission. In this work we studied the DNA fluorescence, obtained from a RNA reverse transcriptase (RT-PCR) amplification, in the region from 400nm to 600nm, without the addition of a marker as a fluorophore and using confocal microscopy with one and two photons (405nm and 800nm). The solutions of dsDNA (237ng/μL) were dropped on a silver film with 200nm tackiness deposited on a glass substrate. In the silver film nanostructures were fabricated ion beam lithography with FEI Quanta 3D 200i dual beam microscope. The nanostructures are formed by concentric arrangements of rings with diameters up to 20 μm, width 50nm and separated by 400nm. When the excitation of the genetic material occurs on a nanostructure an excited surface plasmon-polaritons (SPP) is responsible for the DNA excitation. It is observed in these regions an increase of the fluorescence intensity many times higher than one obtained out of the nanostructure on the silver film. The effects of the interaction between SPPs and molecules increase the optical activity of the molecule (emission rate) and can serve as the basis of photonic sensors. Concluding, the effects of the plasmon fields on the fluorophore are significant and were observed by decreasing the life time of the molecules and the increasing of their fluorescence.

A caracterização das propriedades ópticas de moléculas de DNA, tais como a absorção e a fluorescência por excitação, são importantes para a determinação de parâmetros usados no desenvolvimento de biossensores fotônicos. O estudo da absorção óptica do DNA, obtido por diferentes métodos tem se mostrado muito eficiente na determinação do grau de pureza do material genético obtido por amplificação, ou extração e purificação do DNA total. Por outro lado, a fluorescência por excitação a partir de um marcador cromóforo é uma técnica importante em processos de quantificação de massa, em técnicas tais como a eletroforese em gel de agarose. Devido à baixa fluorescência de moléculas de DNA na região visível do espectro, entre 500-600nm, utiliza-se destes marcadores que se ligam à molécula e que são opticamente ativos nesta região para detecção de sua emissão de fluorescência. Neste trabalho foi realizado um estudo da fluorescência do DNA, obtido a partir de uma amplificação por transcriptase reversa do RNA (RT-PCR), na região de 400nm a 600nm, sem adição de marcador e utilizando excitação por um e dois fótons (405nm e 800nm) através da técnica de microscopia confocal. As amostras contendo solução de dsDNA (237ng/μL) foram depositadas sobre um filme de prata de 200nm de espessura que também é crescido previamente sobre um substrato de vidro. Sobre o filme metálico é fabricado nanoestruturas metálicas por de litografia por feixe de íons com um microscópio de duplo feixe FEI Quanta 3D 200i. As nanoestruturas são formadas por arranjos concêntricos de anéis com diâmetros de até 20 μm, largura 50nm e separados por 400nm. Quando a excitação do material genético ocorre sobre a nanoestrtutura o laser gera na nanoestrutura plasmon-polaritons de superfície (SPP) que interagem com as moléculas de dsDNA na solução. Observa-se que nas regiões onde as nanoestruturas são fabricadas que a intensidade de fluorescência da macromolécula é muito maior do que a obtida fora da estrutura e sobre o filme metálico. Os efeitos da interação entre SPPs e as moléculas aumentam a atividade óptica (taxa de emissão) e podem servir como base para a fabricação de sensores fotônicos ultrasensíveis. Concluindo, os efeitos dos campos plasmônicos sobre o fluoróforo são significativos e foram observados pela diminuição do tempo de vida das moléculas e o aumento da sua fluorescência. / The characterization of the optical properties of DNA molecules, such as absorption and excitation fluorescence, is important to the determination of the parameters used for the preparation of photonic biosensors. The study of optical absorption of DNA, obtained through different methods, currently has a high sensitivity to determine the degree of purity of the genetic material obtained by amplification, extraction and purification of the total DNA. On the other hand, excitation fluorescence using a marker is an important technique in mass quantification processes together with techniques such as agarose gel electrophoresis. Because of low fluorescence of DNA molecules, in the visible region of the spectrum, between 500-600nm, the use of labels that bind to the molecule are critically for the detection of their fluorescence emission. In this work we studied the DNA fluorescence, obtained from a RNA reverse transcriptase (RT-PCR) amplification, in the region from 400nm to 600nm, without the addition of a marker as a fluorophore and using confocal microscopy with one and two photons (405nm and 800nm). The solutions of dsDNA (237ng/μL) were dropped on a silver film with 200nm tackiness deposited on a glass substrate. In the silver film nanostructures were fabricated ion beam lithography with FEI Quanta 3D 200i dual beam microscope. The nanostructures are formed by concentric arrangements of rings with diameters up to 20 μm, width 50nm and separated by 400nm. When the excitation of the genetic material occurs on a nanostructure an excited surface plasmon-polaritons (SPP) is responsible for the DNA excitation. It is observed in these regions an increase of the fluorescence intensity many times higher than one obtained out of the nanostructure on the silver film. The effects of the interaction between SPPs and molecules increase the optical activity of the molecule (emission rate) and can serve as the basis of photonic sensors. Concluding, the effects of the plasmon fields on the fluorophore are significant and were observed by decreasing the life time of the molecules and the increasing of their fluorescence.

Le but de cette thèse et de la recherche associée est une démonstration des avantages d’une combinaison de propriétés inhabituelles de nanostructures plasmoniques avec des aspects parmi les plus intéressants de l’optique non-linéaire. Pour cet effet, la modélisation analytique et numérique a été combiné avec le travail expérimental, qui comprenait la production de nanostructures et les mesures effectuées au moyen de la microscopie confocale non-linéaire résolue en polarisations et de la technique Z-scan modifiée (nommée “f-scan”).Il a été montré que l’anisotropie efficace de génération de seconde-harmonique dans les cristaux plasmoniques (formés par des réseaux rectangulaires de cavités tétraédriques sur une surface d’argent) peut être contrôlée par un choix approprié des paramètres de maille. Il a aussi été montré que cette anisotropie provient principalement d’une structure de bande photonique elle-même anisotrope, présentant une bande interdite plasmonique avec des états plasmoniques en bord de bande, permettant de renforcer le champ électrique local. Les arrangements chiraux bidimensionnels de nanoparticules triangulaires d’or, forment des “meta-molécules” plasmoniques énantiomériques, ont été analysés par microscopie non-linéaire à la lumière polarisée circulairement et par modélisation numérique, révélant un fort effet chiroptique par génération de seconde harmonique en rétro-réflexion. La petite taille des énantiomères uniques permet de créer “des filigranes” (“watermarks”) codés par la chiralité des meta-molécules, qui peuvent être lu par imagerie de la génération de seconde harmonique excitée par un rayon polarisé circulairement. Les caractéristiques quantitatives de la non-linéarité optique du troisième ordre et de l’efficacité d’absorption saturable des solutions aqueuses de fragments de graphène et de graphène dopé par des nanoparticules d’or a été effectuée par une nouvelle technique “f-scan”, qui a été créée et développée par incorporation d’une lentille à distance focale accordable dans une technique de Z-scan traditionnelle. Ces études ont montrées que le graphène présente une absorption saturable ultra-rapide très efficace, qui est parfois convertie en absorption saturable inverse. Il apparaît alors qu’une décoration du graphène par des nanoparticules d’or peut causer une légère amélioration du paramètre d’efficacité d’absorption saturable dans la plage spectrale de leurs résonances plasmoniques. En résumé, cette thèse présente une variété de propriétés optiques non-linéaires apparaissant dans les nanostructures plasmoniques. Différentes possibilités de contrôle de ces propriétés au moyen d’une démarche de nano-ingénierie, soutenue par des modélisations à la fois analytique et numérique ont été démontrées et analysées. Ces travaux ouvrent la voie à la fabrication et à l‘optimisation sur mesure de nouveaux nano-matériaux et nano-dispositifs photoniques reposant sur des effets de nano-plasmonique non-linéaire. / The aim of this thesis and the underlying research work is to demonstrate the benefits emerging from combination of the peculiar properties of plasmonic nanostructures with the most interesting aspects of nonlinear optics. For this purpose, analytical and numerical modeling was combined with experimental work, which included nanofabrication and measurements performed by means of polarization-resolved nonlinear confocal microscopy and by modified Z-scan technique (called "f-scan").It has been shown that the effective anisotropy of the second-harmonic generation in plasmonic crystals (formed by rectangular arrays of tetrahedral recesses in silver surface) can be controlled by proper choice of lattice constants. It also has been shown that this anisotropy arises mainly from the anisotropic photonic band structure, exhibiting plasmonic band gap with plasmonic band edge states, enabling enhancement of the local electric field.Two-dimensional chiral arrangements of triangular gold nanoparticles, forming plasmonic enantiomeric "meta-molecules", have been studied by nonlinear microscopy operating with circularly polarized light and by numerical modeling, revealing strong chiroptical effect in backscattered second-harmonic radiation. Small size of individual enantiomers allows to create "watermarks", encoded by the chirality of meta-molecules, which can be readout by imaging of second-harmonic generation excited by circularly polarized laser beam.Quantitative characterization of the third-order optical nonlinearity and saturable absorption efficiency of aqueous solutions of graphene and gold-nanoparticle decorated graphene has been performed by novel "f-scan" technique, which has been created and developed by incorporation of a focus-tunable lens into traditional Z-scan. These studies have shown that the graphene exhibits very efficient ultrafast saturable absorption, which is occasionally suppressed by reverse saturable absorption. Moreover, it turns out that decoration of graphene by gold nanoparticles may cause a slight improvement of the saturable absorption efficiency parameter within spectral range of their plasmon resonances.In summary, the following thesis presents various nonlinear optical properties of plasmonic nanostructures. Different possibilities of controlling these properties by means of nano-engineering, supported by analytical and numerical modeling, is also analyzed and demonstrated. This work opens up new perspectives for fabrication and rational design of novel photonic nano-materials and nano-devices based on nonlinear nanoplasmonic phenomena.

No description available.

This thesis describes work carried out on the research, development and implementation of new processes for the fabrication of surface plasmon waveguide biosensors. Fabrication of surface plasmon resonance (SPR) based waveguides embedded in a thick CYTOP cladding with the incorporation of fluidic channels was achieved with improved quality and operability compared to previous attempts. The fabrication flow was modified in key areas including lithography for feature definition, gold evaporation and the upper cladding deposition procedure. The combined result yielded devices with sharper resolution of waveguides, gold surfaces with minimal aberrations, reduced surface roughness and minimization of waveguide deformation due to reduction of solvent diffusion into the lower cladding. The fabricated waveguides consisted of a thin, 35 nm, patterned gold film, embedded in a thick, 18 µm, CYTOP fluoroploymer cladding. The gold devices were exposed by O2 plasma etching through the upper cladding to form fluidic channels for the facilitation of flow of an index matched sensing medium. Optical and physical characterization of devices revealed structures of significantly improved quality over previous attempts, rendering the platform competitive for biosensing applications.

This thesis describes work carried out on the research, development and implementation of new processes for the fabrication of surface plasmon waveguide biosensors. Fabrication of surface plasmon resonance (SPR) based waveguides embedded in a thick CYTOP cladding with the incorporation of fluidic channels was achieved with improved quality and operability compared to previous attempts. The fabrication flow was modified in key areas including lithography for feature definition, gold evaporation and the upper cladding deposition procedure. The combined result yielded devices with sharper resolution of waveguides, gold surfaces with minimal aberrations, reduced surface roughness and minimization of waveguide deformation due to reduction of solvent diffusion into the lower cladding. The fabricated waveguides consisted of a thin, 35 nm, patterned gold film, embedded in a thick, 18 µm, CYTOP fluoroploymer cladding. The gold devices were exposed by O2 plasma etching through the upper cladding to form fluidic channels for the facilitation of flow of an index matched sensing medium. Optical and physical characterization of devices revealed structures of significantly improved quality over previous attempts, rendering the platform competitive for biosensing applications.

In this thesis numerical methods are used to understand the individual and collective optical response of metal nanoparticles (MNPs). In particular, finite 1D assemblies of MNPs are characterized by analytical solutions to Maxwell's equations. Small particle solutions such as the well-established plasmon hybridization scheme as well as a novel circuit model explaining the intrinsic mechanisms of free electron dynamics help to characterize the optical response of single and coupled MNPs. Complex systems of closely spaced MNPs with small interparticle gaps are studied with the help of full scattering solutions to Maxwell's equations. It is shown that higher order plasmon modes facilitate strong near-fields between MNPs, and in linear chains foster specific optical attributes which are present in more complex systems, playing a key role in energy propagation along practical MNP waveguides.

A theoretical treatment is presented of a plasmonic interaction at an interface between a semiconductor and a dielectric, as opposed to the more traditional configuration whereby a metal/dielectric interface is investigated. Our work is to show that structures using semiconductors instead of metal to excite surface plasmon can support not only terahertz frequencies plasmons but also optical frequency (around 10 to power of 15 Hz) plasmons. / Thesis

Thesis (Ph. D.)--Oregon State University, 2009. / Printout. Includes bibliographical references (leaves 74-78). Also available on the World Wide Web.