The interaction of light and matter at nanoscale is the subject of study of this dissertation. Particularly, the coupling of light to surface plasmons and their applications in the fields of spectroscopy and sensing is the focus of this work. In terms of spectroscopy, the simple reason of using light to study the chemical structures of different materials is the fact that the energy of light lies in the range of vibrational and electronic transitions of matter. Further, the ability to squeeze light to subwavelength dimensions opens up new possibilities of designing nano-optical devices. In this work we explore surface plasmons for two major applications: (i) Directivity enhanced Raman spectroscopy and (ii) Chemical/biological sensing. Here a new enhancement phenomenon has been demonstrated experimentally in regards to Raman spectroscopy. Typically, Raman enhancement is considered in terms of local fields only. Here we show the use of directive nanoantennas to provide additional enhancement of two orders of magnitude. The nanoantenna design is optimal in the sense that almost all of the scattered light is coupled into the numerical aperture of the collecting lens. It is shown that the additional enhancement from directivity pushes the sensitivity to single molecule regime. Further, the out of plane radiation and simplicity of the design makes it an ideal candidate for use with typical commercial microscope setups. Extra ordinary transmission through nanohole arrays in metallic films is studied for refractive index sensing. Bulk resolution of 6×10-7 is demonstrated by optimizing array dimensions, wavelength of operation, noise reduction and consideration of sensitivity of the detecting CCD camera. Self-assembled nanostructures are investigated for spectroscopic applications. Time dependent studies of nanorods assembled in end-to-end and side-by-side configurations are conducted. The end-to-end configuration results in higher local field enhancements whereas; the side-by-side configuration shows a reduction in local fields because of the cancellation of radial field components between the neighbouring nanorods. It should be noted that higher fields are desirable for Raman spectroscopy. Grating structures have been analysed using reduced coupled mode theory. In most cases, only three lowest order modes prove to be sufficient for accurate description of the system response. Here we present design guidelines for broadband operation and optimization of high quality factor resonators. Finally the complex reflection coefficient from arbitrary terminated nanorods has been investigated. Phase of reflection plays an important role in the determination of resonance wavelength of nanoantennas. It is shown that the localized surface plasmon resonance of nanoparticles can be considered in terms of propagating surface plasmons along a nanorod of similar geometry where the length of the nanorod approaches zero accompanied with π degrees of phase of reflection. The contributions made in this work can prove useful in the fields of analytical chemistry and biomedical sensing. The directive nanoantenna can find applications in a number of areas such as light emitting devices, photovoltaics, single photon sources and high resolution microscopy. Our work related to EOT based sensing is already approaching the resolution of commercially available refractive index sensors with the added advantage of multiplexed detection. / Graduate

Les réseaux de nanotrous sont des structures plasmoniques ayant un énorme potentiel en tant que transducteurs pour la conception de biocapteurs. De telles structures sont prometteuses pour l’élaboration de biocapteurs capable d’effectuer du criblage à haut débit. L’intérêt de travailler avec des réseaux de nanotrous est dû à la simplicité d’excitation des polaritons de plasmons de surface en transmission directe, à la sensibilité et à la facilité de fabrication de ces senseurs. L’architecture de tels réseaux métalliques permet la conception de nanostructures ayant de multiples propriétés plasmoniques. L’intensité, la signature spectrale et la sensibilité du signal plasmonique sont grandement affectées par l’aspect physique du réseau de nanotrous. L’optimisation du signal plasmonique nécessite ainsi un ajustement du diamètre des trous, de la périodicité et de la composition métallique du réseau. L'agencement de l'ensemble de ces paramètres permet d'identifier une structure optimale possédant une périodicité de 1000 nm, un diamètre des nanotrous de 600-650 nm et un film métallique ayant une épaisseur de 125 nm d'or. Ce type de transducteur a une sensibilité en solution de 500-600 nm/RIU pour des bandes plasmoniques situées entre 600-700 nm. L'intérêt de travailler avec cette structure est la possibilité d'exciter les plasmons de polaritons de surface (SPPs) selon deux modes d'excitation : en transmission exaltée (EOT) ou en réflexion totale interne par résonance des plasmons de surface (SPR). Une comparaison entre les propriétés plasmoniques des senseurs selon les modes d'excitation permet de déterminer expérimentalement que le couplage de la lumière avec les ondes de SPP de Bloch (BW-SPPs) en transmission directe résulte en un champ électromagnétique davantage propagatif que localisé. D'un point de vue analytique, la biodétection de l'IgG en SPR est 6 fois plus sensible par rapport au mode EOT pour une même structure. Une étude du signal plasmonique associé au BW-SPP pour un certain mode de diffraction démontre que la distance de pénétration de ces structures en EOT est d'environ 140 nm. La limite de détection de l'IgG humain pour un réseau de nanotrous de 1000 nm de périodicité est d'environ 50 nM en EOT. Ce mémoire démontre la viabilité des réseaux de nanotrous pour effectuer de la biodétection par criblage à haut débit lors de prochaines recherches. L'investigation de l'effet de l'angle d'excitation en transmission exaltée par rapport au signal plasmonique associé au mode (1,0) d'un réseau de nanotrous de 820 nm d'or démontre que la sensibilité en solution n'est pas proportionnelle à la sensibilité en surface du senseur. En fait, une optimisation de l'angle d'incidence pour le mode (1,0) de diffraction des BW-SPP permet d'amplifier la sensibilité en surface du senseur jusqu'à 3-fois pour un angle de 13,3°. Ce mémoire démontre ainsi la nécessité d'optimiser l'angle d'excitation et les propriétés physiques du senseur afin de développer un transducteur de grande sensibilité basé sur l'excitation en transmission de réseaux de nanotrous. / This research aims at developing a multiplexed biosensor for protein detection based on the nanohole array technology. Gold nanohole arrays exhibit distinct plasmonics properties depending on the excitation mode of the surface plasmon polaritons (SPPs). The interest of working with nanohole arrays is related to their high sensitivity, ease of fabrication and simple setup of excitation in transmission. The architecture of nanohole arrays leads to a nanostructure having multiple plasmonics properties. The intensity, the spectral signature and the sensitivity of the plasmonic signal were highly affected by the shape of the nanohole arrays. Varying the diameter of the holes, the periodicity and the metallic composition of the array were used to optimize the plasmonic signal. The optimal structure was found to have a periodicity of 1000 nm, a diameter of 600-650 nm and a metallic film with a thickness of 125 nm of gold. Such a transducer exhibits a bulk refractive index sensitivity of 500-600 nm/RIU for plasmonic bands absorbing around 600-700 nm. Surface plasmon resonance (SPR) in the Kretschmann configuration and enhanced optical transmission (EOT) mode were compared using large gold nanohole arrays (1000 nm periodicity, 600 nm diameter and 125 nm depth) in order to assess their relative analytical performance. Biodetection of IgG was found to be 6 times more sensitive with SPR in the Kretschmann configuration than in EOT mode for the same structure. The decay length of the electromagnetic field in EOT mode was determined experimentally to be around 140 nm with a layer-by-layer polyelectrolyte deposition. This results suggests that the plasmonic properties of EOT for nanohole arrays is much more associated to a Bloch wave SPPs mode rather than a localized SPR. Variation of the incident angle of excitation of the BW-SPPs in transmission leads to a higher surface sensitivity for the (1,0) diffraction mode for gold nanohole arrays of 820 nm periodicity. Optimization of the physical properties and the excitation angle of the nanohole arrays is essential in order to develop a transducer having a potential towards multiplexed biosensors.

This dissertation is focused on the interaction between femtosecond laser and patterned two-dimensional gold nanostructures. The sample was prepared by two different lithographic techniques, the nanosphere lithography and the electron beam lithography. Characterization was carried out with scanning electron microscopy, transmission electron microscopy, atomic force microscopy, and UV-vis absorption spectroscopy. Femtosecond transient absorption spectroscopy was used to answer a number of fundamental questions regarding the laser-nanostructure interaction. Under a low density irradiation of a femtosecond laser, we examined the effect of the lattice crystallinity on the electron-phonon relaxation in monolayer periodic array nanoparticles prepared with nanosphere lithography. We found that the electron-phonon relaxation rate was faster in polycrystalline nanoparticles and decreases greatly in single crystalline nanospheres, which is explained by the presence of high density grain boundaries. The ultrafast laser-induced coherent phonon oscillations in patterned gold nanoparticles are also fully characterized. We studied the effect of size, shape, thickness, monitoring wavelength, and materials of the prismatic array nanoparticles on the period of their coherent phonon oscillations. In a gold nanodisk pair system, we found that the fractional change in the vibration frequency increases exponentially with decreasing the ratio of the interparticle separation to the particle diameter, which is explained by the coupling of the induced electric field in one nanodisk by the strong surface plasmon field of its pair partner. Based on the coherent phonon oscillation of gold caps on a polystyrene sphere monolayer array, a new all-optical gigahertz modulation technique is developed. Under a high density irradiation of a femtosecond laser, the melting and ablation processes can be induced in gold nanoparticles. We studied femtosecond laser induced shape and localized surface plasmon resonance band changes of gold prismatic array nanoparticles. We also observed that the femtosecond laser irradiation of the nanoprisms at the surface plasmon resonance absorption maximum can cause them to detach from the substrate and 'fly away'. Atomic force microscopy and scanning electron microscopy measurements revealed that the displaced nanoparticles are thinner and smaller than the undisplaced ones, which supports an atomic ablation mechanism.

L ’intérêt des nano-particules pour le domaine de l ’optique visible a été suscité lors du premier rapport rédigé par Faraday en 1857 et qui a initié les bases de la production de nanoparticules métalliques en vue de leur propriété optiques inattendues (coloration des solutions). Plus récemment, le contrôle et le guidage de la lumière basés sur l’excitation de résonance plasmon dans les nanostructures a permis beaucoup d’applications liées à la vie quotidienne et impliquant la lumière. La résonance plasmonique de structures métalliques estun phénomène essentiel qui conduit à des propriétés optiques uniques à travers l’interaction de la lumière avecles électrons libres du métal. L’excitation de la résonance plasmon localisé (LSPR) permet d’exalter localement l’énergie électromagnétique comme dans le cas des nano-antennes mais aussi d’acheminer la lumière à travers des canaux de dimensions sub-l sur de grandes distances distances grâce à l’excitation du Plasmonde Surface Propagatif (PSP). Au cours de cette thèse, nous avons étendu un algorithme existant afin de calculer la réponse optique (sections efficaces de diffusion et d’absorption) de NPs ayant une forme géométrie quelconque. Ce type de NP anisotrope (vis-à-vis de la polarisation incidente) peut présenter à la résonance plasmonique une section efficace de diffusion 25 fois supérieure à celle géométrique. De plus, une étude systématique importante a été effectuée afin d’optimiser la géométrie de tels Nps.En ce qui concerne la PSP qui est impliqué dans la transmission exaltée à travers les matrices d’ouvertures annulaires AAA, nous avons entrepris une étude systématique des propriétés de l’excitation du mode particul particulier sans coupure de ces nano - guides. Il s’agit du mode Transverse Electrique et Magnétique (TEM). Une étude numérique complète est alors effectuée pour correctement concevoir la structure avant qu’elle ne soit expérimentalement fabriquée et caractérisée. Pour palier certaines contraintes expérimentale, une structure inclinée est proposée et étudiée dans le cas d’un métal parfaitement conducteur. Nous avons démontrée numériquement et analytiquement certaines propriétés intrinsèques de la structure montrant un coefficient de d’au moins 50% d’un faisceau incident non polarisé indépendamment des conditions d’éclairage (polarisation,angle et plan d’incidence). Lorsque le mode TEM est excité, le flux laminaire de l’énergie à travers la structure présente une déviation géante sur de très petites distances inférieures à la longueur d’onde. Les résultats présentés dans cette thèse pourraient être considérés comme une contribution importante à la compréhension du phénomène de transmission exaltée basé sur l’excitation de ce type de mode guidé. / The release of the rst report by Faraday in 1857 set the foundation of the production of metal nanoparticlesand their unexpected optical properties (coloring). More recently, controlling and guiding light via plasmonicresonance in nanostructures enable a lot of applications affecting everyday life that involves light. Plasmonresonance of metallic structures is a key phenomenon that allows unique optical properties through the interactionof light with the free electrons of the metal. The excitation of Localized Surface Plasmon Resonance(LSPR) leads to turn-on large local enhancements of electromagnetic energy as within antennas or to routelight as waveguide to desired region with high transmission through the excitation of Propagating SurfacePlasmon (PSP). During this thesis, we have developed an existing algorithm in order to calculate the opticalresponse of NPs of any shape. We have especially determined the localized energy enhancement factor interm of optical response of nano-antenna. This anisotropic (polarization dependent) NPs type can feature, atplasmon resonance, scattering efciency factor higher than 25. Moreover, an important systematic study hasbeen performed in order to optimize design of such NPs.Concerning the PSP that are involved in the enhanced transmission through Annular Aperture Arrays (AAAs),we systematically study the properties of the excitation of the peculiar Transverse ElectroMagnetic (TEM) guidedmode inside such nano-apertures. A complete numerical study is performed to correctly design the structurebefore it is experimentally characterized. For reasons associated to fabrication constraints and efciency,a slanted AAA made in perfectly conducting metal is proposed and studied. We numerically and analyticallydemonstrate some intrinsic properties of the structure showing a transmission coefcient of at least 50%ofan un-polarized incident beam independently of the illumination configuration (polarization, angle, and planeof incidence). At the TEM peak transmission, the laminar flow of the energy through the structure can exhibitgiant deviation over very small distances ( ). The results presented in this thesis could be considered as animportant contribution to the understanding of the enhanced transmission phenomenon based on the excitationof guided modes

Cette thèse présente la conception et la mise en œuvre d'un imageur CMOS pour être utilisé dans biocapteurs intégrés basés sur Résonance Plasmonique de Surface (SPR). Tout d'abord, les conditions optimales pour la résonance plasmon dans une interface compatible CMOS / post-CMOS sont obtenus par modélisation avec COMSOL. Deuxièmement, un imageur CMOS de Colonne Actif (CMOS-ACS) du 32x32 pixels est mis en œuvre sur une technologie CMOS 0,35 um. Dans une interface d'or-eau avec une excitation de prisme, on constate que pour les prismes avec des indices de réfraction de 1,55 et 1,46, le couplage optimal avec le plasmon est obtenu pour des films d'or d'une épaisseur de 50 et 45 nm, respectivement. Dans ces conditions, environ 99,19% et 99,99% de l'énergie de la lumière incidente est transférée à le surface plasmon pour les deux prismes respectivement, à condition que la lumière incidente, avec une longueur d'onde de 633 nm, arrive avec un angle d'incidence de 68,45° et 79,05° respectivement. Il est également obtenu qu'un changement de RIU 10-4 de l'indice de réfraction du milieu diélectrique, produit un changement de 0,01 ° dans l'angle de résonance de plasmons qui, dans un schéma de modulation d'intensité de lumière produit une variation de 0,08% dans la lumière réfléchie au photodétecteur. En ce qui concerne le imageur CMOS, une photodiode n-well/p-substrate est choisi comme l'élément de photodétection, en raison de sa faible capacité de jonction, ce qui conduit à un rendement élevé et le gain de conversion élevé comparativement à une photodiode n-diff/p-substrate. Des simulations sur ordinateur avec Cadence et Silvaco produit une capacité de jonction de 31 FF et 135 fF respectivement. Le pixel de l'imageur est basé sur une configuration à trois transistors (3T) et présente un facteur de remplissage de 61%. Le circuit de lecture utilise une technique de capteur de colonne actif (ACS) pour réduire le bruit à motif fixe (Fixed Pattern Noise ou FPN en anglais) liée au le Capteur à Pixels Actif (APS) traditionnelle. En outre, Non-Corrélés Echantillonnage Double (Non-Correlated Double Sampling ou NCDS en anglais) et Delta double échantillonnage (DDS) sont utilisés comme techniques de réduction du bruit. Un montage optique expérimental est utilisé pour caractériser les performances de l'imageur, et nous avons obtenu un gain en conversion de 7,3 uV/e-, une capacité de jonction de la photodiode de 22 fF, un bruit de lecture de 324,5 uV, ce qui équivaut à 45 électrons, et une gamme dynamique de 50,5 dB. Les avantages de l'ACS et NCDS-DDS sont observées dans le niveau faible de FPN du pixel et de la colonne, avec une valeur de 0,09% et 0,06% respectivement. Le travail présenté dans cette thèse est une première étape vers l'objectif de développer une plateforme entièrement intégrée SPR pour biocapteurs, incorporant source de lumière, l'interface SPR, canal microfluidique, les éléments d'optique et imageur CMOS. / This dissertation presents the design and implementation of a CMOS imager for use in integrated biosensors based on Surface Plasmon Resonance. First, the optimal conditions for plasmon resonance in a CMOS/Post-CMOS compatible interface are obtained by COMSOL modelling. Second, a 32x32-pixel CMOS-Active Column Sensor (CMOS-ACS) is implemented on 0.35 um CMOS technology. In a gold-water interface with prism excitation, it is found that for prisms showing refractive indexes of 1.55 and 1.46, optimal plasmon coupling is obtained for gold films with thicknesses of 50 and 45 nm respectively. Under these conditions, approximately 99.19% and 99.99% of the incident light's energy is transferred to the surface plasmon for both prism respectively, provided that the incident light, with a wavelength of 633 nm, arrives with incidence angles of 68.45° and 79.05° respectively. It is also obtained that a change of 10-4 RIU in the refractive index of the dielectric medium, produces a change of 0.01° in the plasmon resonance angle, which under a light intensity modulation scheme produces a change of 0.08% in the reflected light's energy reaching the photodetector. Concerning the CMOS imager, a n-well/p-substrate photodiode is selected as the photosensing element, due to its low junction capacitance, which results in high efficiency and high conversion gain compared to the n-diff/p-substrate photodiode. Computer simulations with Cadence and Silvaco produced a junction capacitance of 31 fF and 135 fF respectively. The imager's pixel is based on a three-transistor (3T) configuration and shows a fill factor of 61%. The readout circuitry employs an Active Column Sensor (ACS) technique to reduce the Fixed Pattern Noise (FPN) associated with traditional Active Pixel Sensors (APS). Additionally, Non-Correlated Double Sampling (NCDS) and Delta Double Sampling (DDS) are used as noise reduction techniques. An experimental optical setup is used to characterize the performance of the imager, obtaining a conversion gain of 7.3 uV/e-, a photodiode junction capacitance of 21.9 fF, a read noise of 324.5 uV, equivalent to ~45 e- and a dynamic range of 50.5 dB. The benefits of ACS and NCDS-DDS are observed in the low pixel and column FPN of 0.09% and 0.06% respectively. The work presented in this thesis is a first step towards the goal of developing a fully integrated SPR-biosensing platform incorporating light source, SPR interface, microfluidic channel, optical elements and CMOS imager.

Le sujet de ma thèse est l’étude de la diffraction par des trous sub-longueur percés dans des films métalliques, ainsi que la compréhension du rôle des plasmons de surface (SPs) dans la diffraction en champ lointain. Nous avons construit un goniomètre « fait maison » de haute qualité. Une série de trous unique percés dans un film opaque et variant continûment de k • r >> 1 à k • r << 1 ont été explorées. Ici, k est le vecteur d'onde de l'onde incidente et r est le rayon du trou. Les résultats expérimentaux indiquent que la diffraction de la lumière par un trou unique peut être séparée en quatre régimes, dépendant de la polarisation incidente. Une expression analytique simple révèle pour la première fois, l’implication de deux facteurs compétitifs: l'un lié aux plasmons de surface, et l'autre provenant du couplage du champ aux modes de guide d'onde de l'ouverture. Lorsque le trou est entouré par des corrugations concentriques (structure d'oeil de boeuf), et est illuminé avec les rainures sur le côté de sortie, l'effet de collimation est observé: la diffraction en champ lointain est confinée dans un très petit angle solide. L’influence des paramètres géométrique sur la figure de diffraction de l’œil de bœuf a été étudié et des motifs de diffraction dont la largeur est inférieure à 1 ° dans le champ lointain ont été atteints. Un autre mode de surface (CWs), différent des SPs, a été étudié sur des films de tungstène. Il a été démontré que les CWs permettent également d’obtenir un effet de collimation. À titre de comparaison, nous avons montré que la transmission exaltée est bien plus faible pour les CWs que pour les SPs sur nanostructures. / The theme of my thesis is to investigate the diffraction behavior of subwavelength holes in metal films, and to understand the surface plasmons’ (SPs) role in aperture far-field diffraction. We have built a home-made goniometer setup with high-level quality. A series of single hole continuously ranging from k•r>>1 to k•r<<1 in a flat opaque film were explored, where k is the wavevector of the incident wave and r is the radius of the hole. The experimental results indicated that the diffraction of single hole can be classified into four regimes, depending on the input polarization. A simple analytical expression reveals for the first time the subtle interplay of two competing factors: one related to surface plasmon excitation and the other originating in the coupling of the field to the waveguide mode of the aperture. When the hole is surrounded by concentric grooves (bull’s eye structure) and is illuminated with the grooves on the output side, the beaming effect occurs: far-field diffraction is confined in very small solid angle. The effects of geometrical parameters on bull’s eye diffraction have been studied and the diffraction patterns with the width less than 1° in the far field have been achieved. Another surface waves (CWs) different from SPs on tungsten films were studied. It was demonstrated that the CWs have beaming effect as well. By comparison we showed that CWs display much weaker enhancement in transmission than SPs through nanostructures.

Submitted by Irene Nascimento (irene.kessia@ufpe.br) on 2017-01-30T18:17:26Z No. of bitstreams: 2 license_rdf: 1232 bytes, checksum: 66e71c371cc565284e70f40736c94386 (MD5) DISSERTACAO_LEO_DEFESA - FINAL - CATALOGADA PDF.pdf: 4585329 bytes, checksum: 4b70c80127866cd2da97a6217bb6a34f (MD5) / Made available in DSpace on 2017-01-30T18:17:27Z (GMT). No. of bitstreams: 2 license_rdf: 1232 bytes, checksum: 66e71c371cc565284e70f40736c94386 (MD5) DISSERTACAO_LEO_DEFESA - FINAL - CATALOGADA PDF.pdf: 4585329 bytes, checksum: 4b70c80127866cd2da97a6217bb6a34f (MD5) Previous issue date: 2016-08-16 / CNPQ / Um dos principais desafios no projeto de sensores baseados em Ressonância de Plasmons de Superfície — RPS — é maximizar sua sensibilidade. Neste trabalho é proposto o uso de dois algoritmos heurísticos, Monte Carlo e Enxame de Partículas, para otimização de sensores baseados em RPS em interfaces planares, i.e, nas configurações de Kretschmann e de Otto, sem o auxílio da aproximação lorentziana para a curva de ressonância. Devido à natureza probabilística dos algoritmos, consegue-se obter um método simples e robusto para atingir essa otimização. É feita uma comparação quanto à eficiência computacional dos algoritmos em relação ao método tradicional de otimização, ficando demonstrado que o método de Enxame de Partículas é o mais eficiente em relação às outras técnicas. Com o emprego desse método, a dependência espectral dos parâmetros ótimos é obtida para sensores utilizando vários metais nas configurações de Kretschmann e de Otto, tanto para aplicações em meios gasosos quanto em meios aquosos. Um aplicativo foi desenvolvido e sua funcionalidade demonstrada, que pode ser executado diretamente via web, com base na metodologia proposta, para otimização de sensores RPS em interfaces planares. / One of the main challenges in the design of surface plasmon resonance – SPR – sensor systems is to maximize their sensitivity. In this work one proposes the use of two heuristic algorithms, Monte Carlo and Particle Swarm, for optimization of SPR sensors in planar interfaces, i.e, in the Kretschmann and Otto configurations, without use of the Lorentzian approximation to the resonance curve. Because of the probabilistic nature of the algorithms, one manages to obtain a simple and robust method to achieve optimization. A comparison is made on the computational efficiency of the algorithm relative to the traditional method of optimization, showing that the particle swarm optimization method is more efficient compared to other techniques. By employing this method, the spectral dependence of optimum parameters is obtained for sensors using a wide range of metal films in the Kretschmann and Otto configurations, both for applications in gaseous an in aqueous media. An app was developed and its functionality can be demonstrated, by direct execution via web, based on the proposed methodology for optimization of SPR sensors on planar interfaces.

This report examines the cross sections of silver microresonators subjected to an incident light with different polarization. The microresonators had different geometries with and without broken symmetries. Cross section profiles for different microresonator configurations are interesting for the division of Material Physics, Uppsala University, when designing metamaterials to tune the optical response of the material. The goal is to form an insight of how the optical response can be tuned by choosing different geometries, varying the size and polarization of the incident light. In this project computer simulations in COMSOL were made to simulate the optical response of different microresonators. When the incident light interact with the silver microresonators plasmonic excitations is generated which in turn interacts with the light changing the phase and therefore the optical response. By increasing the radius of the disk silver microresonantors the resonance was found to shift to lower energies. For a geometry with a disk microresonator inside a ring microresonator the Fano resonances were dependent of the radius of the disk microresonator.

This thesis summarizes the methods of preparation and optical properties of hybrid assemblies of Au NPs and cadmium selenide (CdSe) QDs. First chap-ter deals with the literature survey and theoretical aspects of plasmonics and discussions on optical excitations of metal (plasmons) and semiconducting QDs (excitons). Variation of energy levels of CdSe QDs and its optical properties i e. absorption and emission properties under strong confinement regime have been discussed with respect to effective mass approximation (EMA) model. This is followed by the discussion on optical properties of Au NPs and rods, describing absorption properties, based on Mie theory. Size and shape depen-dent variation of absorption properties. Theoretical discussions of collective effects in QDs assemblies and plasmonic interactions with the QDs assemblies i.e. plasmonic Dicke effect and metal nanoantenna interaction with CdSe QDs arrays is provided. In the second chapter a discussion on experimental techniques used for the study is provided. It starts with a discussion on the synthesis methods for CdSe QDs and Au NPs/rods with different capping ligands. Different techniques of preparation of CdSe QDs assemblies and their hybrid with metallic nanoparti-cles has been discussed. Further discussion on optical microscopy techniques, confocal, near field scanning microscopy (NSOM), Brewster angle microscopy and electron microscopy techniques i. e transmission electron microscopy and scanning electron microscopy and thermogravimetry analysis of the samples is provided. In the third chapter the details of the different self-assembly methods of preparation of hybrid assemblies of CdSe QDs and Au NPs /rods are given. The different strategies are used for different type of hybrids. In first method of Langmuir-Blodgett (LB) , effect of different capping agents, core size, and number ratios of Au NPs/rods to CdSe QDs, effect of anisotropy of Au NPs on the LB films of CdSe QDs assemblies is discussed. In another method of dip coating several control parameters like dip time, concentration of the solution and dip speed of transferring an aligned GNRs is given. Finally a combination of LB and dip coating methods is described for transferring aligned GNRs over a compact layer of CdSe QDs. At the end, a section is devoted to hit and trials of self-assemblies of hybrid of GNRs and CdSe QDs using LB method, the failures of which resulted in devising a method which uses a combination of LB and dip coating. In fourth chapter effects of plasmons on the collective emission of CdSe QDs assemblies are investigated. A plasmonic tuning of photoluminescence from semiconducting QD assemblies using Au NP in different ratio and different packing density has been discussed. We have described how the emission from a closed pack assemblies, prepared with different packing densities depends on the packing density and extent of spectral overlap between QD photolumi-nescence and the metal nanoparticle absorbance. We have provided possible evidence for plasmon mediated coherent emission enhancement from some of these assemblies from the case of strong spectral overlap between CdSe QDs and Au nanoparticle. In fifth chapter, we have demonstrated non local far field enhancement of PL in QDs assemblies induced by isolated and partially aligned GNRs nano-antenna located on such assemblies. It is shown that the emission is also anisotropic with the maxima being near such GNRs assembly which decays to finite, nonzero and significantly large values even away from the vicinity of any such assemblies. For this novel effect it is shown to have a clear spec-tral dependence. It is shown to be maximum when the longitudinal surface plasmon resonance absorption maxima is resonant with the CdSe QD photolu-minescence maxima and the excitation wavelength and is always non-existent for the off resonant case. We have also shown that finite difference time do-main simulations could model some of the observed near field effects but the far field effects could not be modelled in such simulations.

Les vésicules extracellulaires (VEs) sont des nanovésicules circulantes (30 à 100nm de diamètre) libérées dans l'espace extracellulaire par la plupart des cellules humaines, suite à leur activation ou à leur apoptose. Les VEs se divisent en 3 grandes catégories ; les exosomes (Exo), les microparticules (MPs) et les corps apoptotiques (cAPO). Les VEs sont présentes à l'état physiologique dans les différents fluides biologiques du corps humain et jouent un rôle majeur dans différents processus physio-pathologiques. De nos jours, plusieurs techniques, certaines en routine, sont utilisées pour étudier les VEs. Cependant, aucune d'entre elles ne permet de déterminer à la fois leur concentration, leur taille et leurs caractéristiques biochimiques. Un consensus existe sur la nécessité de combiner des techniques pour disposer enfin d'une caractérisation fine et complète des VEs. Il est d'un intérêt majeur de développer des plateformes analytiques dédiées à ces VEs en vue d'améliorer la qualification des échantillons biologiques et de découvrir de nouveaux biomarqueurs de pathologies humaines ou de bio-indicateurs de suivi thérapeutique.Notre projet consiste à développer une plateforme NanoBioAnalytique (NBA) combinant trois techniques : l'imagerie par Résonance des Plasmons de Surface (SPRi), la Microscopie à Force Atomique (AFM) et la Spectrométrie de Masse (MS). L'enjeu est de développer une interface biopuce-instruments qui permettra d'effectuer des investigations multiphysiques et multiéchelles apportant, en une stratégie globale, les informations plus complètes sur les différentes populations de VEs.[...]Ces travaux ont montré la capacité de notre plateforme à détecter sélectivement, et simultanément, différentes sous-populations des VEs co-existantes dans un échantillon complexe tel que du plasma, en s'appuyant sur l'expression différentielle des marqueurs protéiques membranaires. Les taux de capture se sont avérés être directement corrélés à la concentration des vésicules dans l'échantillon injecté. L'analyse AFM a permis de déterminer la distribution en taille de différentes sous-populations de VEs et permettre une analyse différentielle de la distribution en taille sur la gamme 20 nm - 1000 nm. Enfin, des études protéomiques "sur-puce" ont été également engagées afin de caractériser la composition en protéines des VEs libérées sous différentes conditions. Cette analyse a permis d'établir des premiers profils protéomiques différentiels des VEs dans les échantillons étudiés.La plateforme NBA est une méthode efficace pour caractériser et quantifier les VEs, sans marquage et avec une grande sensibilité, sur une large gamme dynamique (environ 10(7) à 10(12) particules/mL) cohérente avec celle existante en fluide physiologique et sur une plage de taille couvrant 2 décades. Elle s'inscrit parmi les approches les plus prometteuses pour l'investigation des VEs en complément de la cytométrie en flux. La grande adaptabilité de cette méthode d'analyse des VEs ouvre de larges perspectives de déploiement dans les secteurs de la Santé, de l'Environnement et de l'Agro-alimentaire. / Extracellular vesicles (EVs) are small vesicles (30 to 1000 nm) released from different cell types, upon activation or apoptosis, and present in most body fluids (Blood, Urine….). Based on the current state of knowledge of their biogenesis and biochemical properties, EVs can be devided into three distinct populations: exosomes (EXO), microparticles (MPs) and apoptotic bodies (APOb). EVs have been found to play important biological roles and are also biomarkers of different pathologies. […] The first step consists of the injection of the samples containing EVs onto the biochip surface. This step is accomplished by SPR technique that allows label-free monitoring of EVs immunocapture onto the surface of a biochip presenting different specific bioreceptors. Following the capture of EVs, a nanometrological investigation of the biochip surface by AFM is engaged to characterize the physical properties of captured vesicles (size, morphology, etc..). Owning a nanometrical resolution, AFM can discriminate between individual EVs and vesicles or protein aggregates, leading to an accurate characterization of individual vesicles. The coupling of SPR technique with AFM was adapted to offer a representative global view of each array of bioreceptors and to measure the size of thousands of individual EVs. A proteomic investigation was also engaged to characterize the proteomic compositions of the different subpopulations of EVs. Such an investigation could contribute to the understanding of EVs biogenesis, biology and pathophysiology. To evaluate the potential of our platform to detect, quantify and characterize nanoparticles, two calibration particles, which cover the lower and upper size range of EVs, were chosen: (i) virus-like particles of 50 nm of diameter, also called CP50, and (ii) protein-functionnalized synthetic beads of 920 nm of diameter, called CP920. The capture tests in SPR showed a specific capture of these two calibration particles with their specific bioreceptors, immobilized onto the biochip surface, regardless the complexity of the media in which they were diluted. Also, a positive correlation was obtained between the capture level, measured by SPR, and the particle 9