<p>Nanometer-scale metallic structures have been widely and intensively studied over the last decade because of their remarkable plasmonic properties that can enhance local electromagnetic (EM) fields. However, most plasmonic applications are restricted to the visible and near infrared photon energies due to the limitations of the surface plasmon resonance energies of the most commonly used plasmonic metals: Au and Ag. Plasmonic applications in ultraviolet (UV) are of great interest because Raman scattering sections are larger and do not overlap fluorescence spectra. UV plasmonics also benefit from high spatial resolution and low penetration depth. However, an appropriate UV plasmonic material must be identified.</p><p>We proposed and demonstrated that gallium is a highly-promising and compelling material for UV nanoplasmonics through synthesis of size-controlled nanoparticle arrays, EM modeling of local field enhancement, ellipsometric and spatial characterization of the arrays, and analytical measurement of UV- enhanced Raman and fluorescence spectra. Self-assembled arrays of hemispherical gallium nanoparticles deposited by molecular beam epitaxy on a sapphire support are characterized with spatial and ellipsometric measurements. Spin-casting a thin film of crystal violet upon these nanoparticles permitted the demonstration of surface-enhanced Raman spectra, fluorescence, and molecular photodegradation following excitation by a HeCd laser operating at 325 nm (UV). Measured local Raman enhancement factors exceeding 10<super>7</super> demonstrated the potential of gallium nanoparticle arrays for plasmonically-enhanced ultraviolet detection and remediation.</p> / Dissertation

The behaviour of surface plasmon polaritons (SPPs) in nanoscale geometries is studied using numerical methods supported by theory and experiment. First, we derive the behaviour of SPPs at graded metal-dielectric interfaces, including dispersion relations, field profiles, propagation velocities, losses, and cutoff wavelength. Numerical simulations show excellent agreement with analytic solutions. In the second part of the thesis we design hybrid vanadium dioxide-plasmonic based absorption switches. The switches are designed and optimized using optical, electrical and thermal simulations. 5 $\mu$m switch designs have extinction ratios exceeding 30 dB and require powers of 10 mW. A switch is fabricated based on the proposed design. A 7 $\mu$m experimental switch reaches 16.4 dB of extinction and requires 64 mW of power, making it one of the most efficient optical switches ever demonstrated in terms of extinction and power consumption. Numerical simulations predict experimental results with a high degree of accuracy.

The behaviour of surface plasmon polaritons (SPPs) in nanoscale geometries is studied using numerical methods supported by theory and experiment. First, we derive the behaviour of SPPs at graded metal-dielectric interfaces, including dispersion relations, field profiles, propagation velocities, losses, and cutoff wavelength. Numerical simulations show excellent agreement with analytic solutions. In the second part of the thesis we design hybrid vanadium dioxide-plasmonic based absorption switches. The switches are designed and optimized using optical, electrical and thermal simulations. 5 $\mu$m switch designs have extinction ratios exceeding 30 dB and require powers of 10 mW. A switch is fabricated based on the proposed design. A 7 $\mu$m experimental switch reaches 16.4 dB of extinction and requires 64 mW of power, making it one of the most efficient optical switches ever demonstrated in terms of extinction and power consumption. Numerical simulations predict experimental results with a high degree of accuracy.

We have numerically investigated the influence of a nanoscale silicon tip in proximity to an illuminated gold nanoparticle. We describe how the position of the high-permittivity tip and the size of a nanoparticle impact the absorption, peak electric field and surface plasmon resonance wavelength under different illumination conditions. We detail the finite element method (FEM) approach we have used for this, whereby we specify a volume excitation field analytically and calculate the difference between this source field and the total field (i.e., scattered-field formulation). We show that a nanoscale tip can locally enhance the absorption of the particle as well as the peak electric field at length scales far smaller than the wavelength of the incident light.

Optical metamaterials are artificial media that exhibit new properties from structuring on the nanometric scale. One of the main researches in metamaterials investigates materials with negative refractive index, which can allow the development of perfect lens and other exciting potential applications. In this thesis, we theoretically study the properties of negative-index optical fishnet metamaterials, especially the origin of their negative-valued refractive index, and also associated theoretical problems. The thesis can be divided into 4 parts. In the first part we study the light scattering at an interface between air and a semi-infinite fishnet metamaterial. With a fully-vectorial numerical method, we calculate the scattering coefficients of the interface and find that the energy transport inside the fishnet is due to a single Bloch mode, the fundamental one. Based on the single-interface scattering coefficients and the effective index of this Bloch mode we propose a new algorithm for retrieving effective optical parameters of the metamaterial. The approach emphasizes the key role played by the fundamental Bloch mode and provides retrieved parameters that are more accurate or stable than those obtained by classical methods based only on light reflection and transmission through finite-thickness metamaterial slabs. Due to the importance of the fundamental Bloch mode in the light transport in metamaterials, in the second part, based on the Bloch mode orthogonality we derive closed-form expressions for the scattering coefficients at an interface between two periodic media with slightly different geometrical parameters, which is a computationally demanding electromagnetic problem. We show that the analytical expressions are very accurate for various geometries, including dielectric waveguides and metallic metamaterials. Thus they can be useful for designing and engineering stacks of periodic structures. As shown in the first part, the fundamental Bloch mode is central to explain the negative refraction phenomenon in fishnet metamaterials. In the third part, we derive an accurate semi-analytical model for the complex propagation constant of the fishnet fundamental Bloch mode. This is achieved by analyzing light propagation and scattering inside the fishnet. The model shows that the origin of broad-band negative index of fishnets can be mainly understood as a plasmon resonance in the transversal metal-insulator-metal (MIM) channels. The plasmon resonance enhances the 'magnetic' response of fishnet and the losses associated to this resonance can be compensated by including gain in the dielectric layers of the fishnet. Furthermore, the model allows an easy and precise geometrical tailoring of fishnet metamaterials. As shown in the third part, it is the plasmon resonance in metal-insulator-metal (MIM) structures that induces the negative index of fishnet metamaterials. In the last part, we study the asymptotic behavior of 3D MIM nanoresonators, as the resonator size is shrunk below the diffraction limit. In particular we show that the quality factor increases from 10 to 100 when the resonator volume is scaled down from (λ/2n)3 to (λ/50)3. We provide a comprehensive study with a semi-analytical Fabry-Perot model. The model remains accurate over the whole size scale even in the quasi-static regime for which retardation effects are not expected. This important and counterintuitive result indicates that both localized plasmon resonances in nanoparticles and delocalized resonance in elongated plasmonic nanowires can be possibly understood as a wave-retardation based antenna problem.

Reducing the absorber thickness is an attractive solution to decrease the production cost of solar cells. Furthermore, it allows to reduce the amount of material needed and improve the current collection in the cell. This thesis has been focused on the design of nanostructures to enhance light absorption in very small semiconductor volumes in order to achieve efficient ultra-thin solar cells. First, we have proposed an original light-trapping concept for ultra-thin amorphous silicon (a-Si:H) solar cells. A one-dimensional metallic grating is patterned on the front surface of the cell deposited on a metallic mirror. Broadband multi-resonant absorption has been demonstrated for both light polarizations. The metallic grating is also used as an alternative transparent electrode in order to reduce optical losses in the front contact. A detailed analysis of the multi-resonant absorption mechanism has been carried out through numerical calculations. The fabrication and optical characterization of ultra-thin a-Si:H solar cells with metallic gratings have validated the multi-resonant approach.Second, we have proposed a design with a two-dimensional metallic grid as a resonant front contact for very thin (25 nm) gallium arsenide (GaAs) layers. We have shown through the design and fabrication of a proof-of-concept structure the potential of metallic nanogrids to confine efficiently light absorption with an ultra-thin GaAs layer.Finally, advanced light-trapping structures could also allow a thickness reduction of crystalline silicon wafers of a factor 20 to 100 with respect to state-of-the-art cells. We have developed a process to transfer micron-thick epitaxial crystalline silicon (c-Si) layers onto a low-cost host substrate. Inverted nanopyramids have also been fabricated in crystalline silicon in order to achieve a broadband anti-reflection effect. It opens promising perspectives towards the realization of double-sided nanopatterned ultra-thin c-Si cells.

Plasmonic properties of self-assembled silver nanoparticles/nanowires array on periodically patterned Si (100) substrate are reported with special attention on the mechanism of nanoparticles self-assembly. The advantage of this bottom up approach over other self-assembling and lithographic methods is the flexibility to tune array periodicity down to 20 nm with interparticle gaps as low as 5 nm along the ripple. Ripple pattern have shallow modulation (~2 nm) still particles self-assembly was observed in non-shadow deposition. Therefore adatoms diffusion and kinetics is important on ripple surface for the self-assembly. PVD e-beam evaporation method used for deposition has proven to be superior to sputter deposition due to lower incident flux and lower atom energy. It was found that particles self-assembly largely dependent on angle of incidence, substrate temperature, and deposition direction due to ripple asymmetric tilt. Ostwald ripening observed during annealing on ripples substrate has striking dependency on ripple periodicity and was found to be different compared to Ostwald ripening on flat Si surface. In-situ RBS measurements of deposited silver on flat and rippled substrate confirmed different sticking of atoms on the two surfaces. The difference between maximum and minimum of the calculated local flux show a peak at an incidence angle of 70o with respect to surface normal. This explains the best alignment of particles at this angle of incidence compare to others. Self-assembled nanoparticles are optically anisotropic, i.e. they exhibit a direction dependent shift in LSPR. The reason of the observed anisotropy is a direction dependent plasmonic coupling. Different in plane and out of the plane dielectric coefficients calculated by modelling Jones matrix elements, confirms that nanoparticle/nanowire array are biaxial anisotropic (ex ¹ ey ¹ ez). The nanoparticles are predominantlyinsulating while nanowires are both metallic and insulating depending on the dimension. Silver nanoparticles/nanowires self-aligned on pre-patterned rippled substrate are presented for the first time as an active SERS substrate. Anisotropic SERS response in such arrays is attributed to different field enhancement along and across the ripples. Strong plasmonic coupling in elongated nanoparticles chain results in significantly higher SERS intensity then spherical nanoparticles/nanowires and non-ordered nanoparticles. Higher SERS intensity across the nanowires array in comparison to along the array (bulk silver) confirms electromagnetic field enhancement (hot-junction) is responsible for SERS phenomenon. Self-assembly of cobalt nanoparticle on ripple pattern substrate is also reported. Due to less adatom mobility and higher sticking cobalt self-assembly is possible only at much higher temperature. A strong uniaxial magnetic anisotropy was observed not observed for non ordered cobalt particles.

La détection et l'identification des substances biologiques ou chimiques peuvent être accomplies par des biocapteurs. On exige des biocapteurs d'être simple et rapide à utiliser, d'avoir une taille réduite, et d'être suffisamment sensible afin de pouvoir détecter des molécules en petite quantité. Des dispositifs plasmoniques se sont révélés adaptés pour l'usage en tant qu'élément transducteur des biocapteurs. Les plasmon-polaritons de surface (SPP) sont des oscillations collectives du nuage électronique des métaux, couplées à des ondes électromagnétiques. Leur fréquence de résonance dépend de l'indice de réfraction de leur environnement diélectrique. Ceci permet de sonder de manière efficace la présence des molécules par la modification de l'indice de réfraction engendrée par celles-ci. La technique reposant sur ce principe s'appelle la détection par résonance des plasmons de surface (SPR sensing en anglais). De plus, les SPP confinent le champ électrique incident à des volumes sub-longueurs d'onde et l'exaltent ainsi. Les molécules qui se situent dans ces zones de forte exaltation du champ électrique interagissent plus efficacement avec la lumière incidente par l'intermédiaire du SPP, tel que leur section efficace de l'absorption infrarouge (IR) augmente. La spectroscopie IR est une technique standard d'identification de molécules en quantités suffisantes. Pour améliorer la sensibilité, la spectroscopie vibrationnelle d'absorption exaltée par la surface (SEIRA pour surface enhanced infrared absorption en anglais) est particulièrement bien adaptée.Alors que la plasmonique s'est principalement développée dans le visible via les métaux nobles, les semi-conducteurs III-V fortement dopés présentent une alternative intéressante pour la plasmonique dans le moyen IR. Leur fonction diélectrique ressemble à celle des métaux nobles dans le visible, mais décalée dans le moyen IR. Leur densité de charges moindre que celle de l'or permet de réduire considérablement leurs pertes. La spectroscopie SEIRA utilise des nanoantennes plasmoniques dont les résonances se situent dans l'IR pour couvrir la gamme spectrale des modes vibrationnels moléculaires. L'InAsSb fortement dopé accordé en maille sur un substrat en GaSb présente des propriétés plasmoniques au-delà de 5 µm de longueurs d'onde.Dans ce manuscrit, nous proposons des nanostructures en InAsSb:Si/GaSb pour développer un biocapteur utilisant les techniques de SEIRA et de SPR "sensing". Les nanostructures ont été réalisées soit par photolithographie et gravure chimique humide soit par lithographie interférentielle et gravure par plasma réactif. Les caractérisations optiques ont été effectuées par spectroscopie IR à transformée de Fourier. Des calculs numériques par la méthode des différences finies dans le domaine temporel (FDTD) ont permis d'étudier l'effet des paramètres géométriques sur la réponse optique des structures. Deux types de structure ont été proposés : des réseaux unidimensionnels ainsi que des réseaux bidimensionnels de nanoantennes rectangulaires supportant des résonances de plasmon de surface localisé (LSPR) dans les deux directions de polarisation de la lumière par rapport aux axes de la structure. Ce type de structures permet ainsi une réponse optique ayant des résonances dans deux bandes spectrales différentes. Les techniques de SPR "sensing" et de SEIRA ont été démontrées pour l'ensemble des structures uni- et bidimensionnelles. Différents types d'analytes comme les polymères et le benzaldéhyde vanilline ont servi de systèmes de tests pour les structures plasmoniques. Les sensibilités se situent entre 10² et 10^3 nm/RIU. Les facteurs d'augmentation des signaux vibrationnels obtenus sont compris dans une gamme de 1,2 à 5,7 et les facteurs d'exaltation ont été évalués autour de 10^3 à 10^4 pour les réseaux bidimensionnels de nanoantennes plasmoniques. / The detection and identification of biological and chemical substances can be performed with biosensors. Biosensors are required to be simple and rapid to use, small, and sensitive in order to detect minute amounts of analyte molecules. Plasmonic devices have proven their utility as biosensing transducers. Surface plasmon-polaritons (SPP), collective oscillations of the electron cloud in metallic media coupled to an electromagnetic wave, are sensitive to the refractive index of their environment, providing thus an efficient way to probe the presence of molecules by the refractive index modification. This technique is called surface plasmon resonance (SPR) sensing. Moreover, SPP confine the incident electric field to sub-wavelength dimensions and enhance the field strength. Molecules located in these so-called field hotspots interact more efficiently with incident light due to a coupling mechanism mediated by the SPP, so that their infrared (IR) absorption cross section is increased. While IR spectroscopy is a standard tool for molecular identification, it does not provide sufficient sensitivity for the detection of smallest quantities. Exploiting the surface enhanced IR absorption (SEIRA) due to the plasmonic enhancement enables the detection of small amounts of analyte.While surface plasmons were mainly discovered using noble metals such as gold and silver, nowadays other material systems are also considered which display complementary or improved properties compared to the standard materials in plasmonics, especially to enlarge the spectral range where plasmonic effects can be observed and exploited. Material science enables to tailor the dielectric function of a material and consequently to control the plasmonic properties. Highly doped III-V semiconductors constitute an alternative to gold and silver for mid-IR plasmonics, due to their dielectric function which resembles the one of the noble metals, but shifted to the mid-IR spectral range. Indeed, InAsSb in the IR is even less lossy than gold in the visible. SEIRA using plasmonic resonances spectrally tuned to molecular absorption lines, or resonant SEIRA, requires nanoantenna substrates displaying their resonances in the IR. Highly doped InAsSb grown lattice matched on GaSb substrates is an interesting material system for this task. InAsSb is plasmonic for wavelengths above approximately 5 µm.In this work, we propose InAsSb:Si/GaSb nanostructures as SEIRA and SPR substrates for an application in biosensing devices. InAsSb nanoantennas on GaSb substrates have been prepared using photolithography and wet chemical etching by a citric acid: hydrogen peroxyde solution or alternatively, by interferential lithography and reactive ion etching, especially to reduce the lattice parameter. An optical characterization of the structures was performed by FTIR spectroscopy, supported by numerical finite-difference time-domain (FDTD) calculations which were also applied to study the impact of geometrical parameters on the optical response. Notably, two types of structure designs were proposed: one-dimensional periodic gratings and two-dimensional arrays of rectangular shaped nanoantennas which provide localized surface plasmon resonances (LSPR) in both polarization directions contrary to the gratings and enable hence a dual band optical response. SPR sensing and SEIRA have successfully been demonstrated using both types of structures, with proof-of-concept analytes such as different polymers and the aromatic compound vanillin with absorption features at high IR wavelengths. A bulk sensitivity in the range of 10² to 10^3 nm/RIU was reached. The vibrational signals increased of factors ranging between approximately 1.2-5.7, and the SEIRA enhancement was estimated to be in the range of 10^3 to 10^4 for the rectangular nanoantenna arrays.

Plasmon coupling is known to cause distance dependent red-shifts of the characteristic plasmon resonance and localize strong electric fields to the gap between individual nanoparticles. These effects form the basis of nanoscale plasmonic sensors designed by creating specic structures of coupled nanoparticles. The simplest of these structures, a nanoparticle dimer, can easily be assembled through molecular self-assembly, resulting in a structure called a plasmon ruler. These plasmon rulers are crucial tools for the measurement of nanoscale distances, but the impact of the molecular linker on the plasmonic response of the coupled system remains insufficiently understood. In this dissertation, plasmons rulers composed of 40 nm gold nanoparticles are utilized to systematically investigate the potential effects of one molecular linker, DNA, on the strength of the plasmon coupling at a variety of interparticle separations. The strength of the plasmon coupling is determined based on the shifting of the plasmon resonance, which, at separations below 2.7 nm, is significantly blue-shifted when compared to expected values from electromagnetic simulations and experiments without DNA linkers. This deviation indicates a reduced charge accumulation on the nanoparticles in the gap region and is ascribed to DNA-mediated charge transfer. Enhancements to the charge transfer capabilities of the DNA were also investigated, through the deposition of interstitial palladium nanocrystals on the DNA linkers. The deposition of these nanocrystals results in a variety of structural changes to the plasmon rulers, associated with blue- and red-shifts of the plasmon resonance relative to electromagnetic simulations without gap material and experimental spectra of structures without molecular or metallic linkers. The relative blue-shift of the resonance results from a variety of scenarios, including short interparticle separations bridged by DNA or palladium nanocrystals, the build-up of palladium nanocrystals within the gap, or the incorporation of discrete palladium nanoparticles in the DNA linkers. The underlying mechanisms of the observed spectral shifts are analyzed. The red-shifted resonances resulted from a significant build-up of palladium nanocrystals in the gap, effectively linking the gold nanoparticles and forming a hybrid nanorod-like structure.

Cette thèse porte sur l’étude d’un système modèle de nanoparticules (NP) d’or supportées sur TiO2(110) en vue de mieux comprendre la corrélation entre propriétés morphologiques, structurales et de résonances plasmoniques locales (LSPR) des NP. Des mesures in situ de diffusion de rayons X en incidence rasante à grands angles (GIXD) et à petits angles (GISAXS) et de spectroscopie de réflectance différentielle de surface (SDRS) ont été réalisées pendant la croissance des NP déposées par épitaxie par jet moléculaire en ultra-vide.L’étude du LSPR par SDRS, avec décomposition des signaux en polarisation s et p et réalisée simultanément avec le GISAXS, a permis de relier la variation de la fréquence de résonance des NP à celle de leur diamètre moyen, dans la gamme de 2 à 6 nm.De manière générale, la position du pic plasmonique dérive vers le bleu avec la diminution de la taille des NP mais avec un comportement qui dépend de l’état de surface des substrats. Dans un cas, les polarisations s et p suivent la même variation alors que dans l’autre non. Cet effet a été analysé en décomposant la fréquence plasmon en modes dipolaires parallèle (A//, qui contribue aux deux polarisations s et p) et perpendiculaire (Az, qui contribue à la seule polarisation p) à la surface.Lorsque A// domine (positions des pics plasmoniques s et p identiques, pour une taille donnée de NP), la position en longueur d’onde du pic plasmonique dérive vers le bleu avec la diminution de la taille de la même façon que pour des NP enterrées. Cet effet de taille intrinsèque, d’origine quantique, peut être décrit par un effet de spill out des électrons s qui débordent au-delà du rayon de la NP et de la diminution de l’écrantage des électrons d à la surface de la NP. L’interaction avec le substrat provoque un décalage global de la fréquence de vibration vers le rouge par rapport aux NP d’or dans le vide.Pour l’autre échantillon (s 6 = p), la contribution du mode A z devient notable au-dessous de 5 nm. L’influence du substrat sur ce mode est différente, son effet augmente quand la taille diminue, contrecarrant l’effet de taille intrinsèque Dans ce cas, la dérive de la position du LSPR vers le bleu avec la diminution de la taille est plus lente en polarisation p qu’en polarisation s.Ces comportements sont à relier aux mesures de GIXD, réalisées en fin de croissance, qui ont montré des épitaxies différentes dans les deux cas. Dans l’un (s = p), une grande partie des NP sont orientées avec la direction [110] de l’or alignée le long des rangées d’oxygène pontant de TiO2(110) alors que dansl’autre (s /= p) les NP présentent un fort désordre orientationnel attribué à une surface avec un très grand nombre de marches. / This thesis concerns the study of supported gold nanoparticles (NP) onTiO2(110) as a model system. The aim is improving the comprehension ofthe correlation between morphological and structural properties andlocal surface plasmon resonances (LSPR) of the NP.In situ measurements during NP growth were performed by grazingincidence X-ray diffraction (GIXD), grazing incidence small angle X-raydiffusion (GISAXS) and surface differential reflectance spectroscopy(SDRS). NP were deposited by molecular beam epitaxy in ultra-high vacuum.Simultaneous study of LSPR phenomena by SDRS and GISAXS allowed thedescription of resonance frequency evolution with the NP mean diameterincrease from 2 to 6 nm.Typically, position of the plasmon peak in both p and s measuredpolarizations is found to blue-shift when NP size decreases, butdetailed behavior is influenced by TiO2(110) surface state.At the same NP dimension, in one case plasmon pics position is the samefor both s and p polarization, whereas in the second studied sample theyare different, but only in the small size range (diameter<5nm). Thisphenomenon was analyzed thanks to the decomposition of plasmonexcitation into parallel (A//, contributing to both s and p signal) andperpendicular (Az, contributing only to p polarization) modes withrespect to the surface.When A// dominates (same peak positions for s and p polarizations at thesame NP mean diameter) the observed blue-shift with size decrease isvery close to that reported in literature for embedded Au NP. Thissuggests that the underlying quantum size effect, due to s-electronsspill-out and diminishing of d-electrons screening for surface atoms, isan intrinsic property of the NP. Interaction with the substrate inducesa global red-shift compared to NP in vacuum.In the other case (s /= p for sizes smaller than 5 nm), Az contributionin noticeable. Substrate influence on this mode is different, its effectincreases as size decreases, countering the intrinsic size effect.Blue-shift with size decrease is slowed down in p polarization comparedto the s one. These results were linked to GIXD measurements performedafter NP growth. They show epitaxial differences between the two studiedcases. In the former (p=s), a fair amount of NP is oriented such thatgold [110] direction is aligned with the TiO2(110) surface bridgingoxygen arrays. In the second case (p/=s), NP show a strong orientationaldisorder, possibly due to the presence of a large amount of steps on theTiO2(110) surface.