Depuis plusieurs années, les nanotubes de carbones (NTCs) présentent un important potentiel dans le secteur des applications biomédicales (imagerie médicale, vectorisation de médicaments, etc.). Toutes ces applications impliquent des modifications au niveau de la paroi des NTCs par le biais de fonctionnalisations chimiques afin de pouvoir y greffer des molécules d’intérêt. Il existe deux principales voies de fonctionnalisation impliquant différents types d’interactions et des changements plus ou moins conséquents au niveau des NTCs. D’une part, la fonctionnalisation covalente, la plus largement utilisée, conduit à la formation de liaisons covalentes stables mais modifie en même temps la structure et donc les propriétés intrinsèques des NTCs. D’autre part, les NTCs peuvent être fonctionnalisés de manière non-covalente, c’est-à-dire par le biais d’interactions faibles (interactions hydrophobes, π- π stacking, interactions ioniques, etc.), ce qui n’affecte pas la structure des NTCs. Les objectifs de cette thèse ont été, dans un premier temps, de déterminer le meilleur processus de purification des nanotubes de carbone biparois (DWNTs) synthétisés par CCVD au CIRIMAT afin d’en éliminer toutes traces de nanoparticules métalliques mais surtout d'espèces carbonées indésirables (carbone désorganisé), le but étant de partir d’un échantillon oxydé le plus pur possible et dans lequel le carbone n'est présent que sous forme de NTCs. Ainsi, toute éventuelle compétition entre les différentes espèces carbonées, pouvant rendre impossible toute conclusion claire, est évitée. Les DWNTs ont été choisis comme structure idéale pour représenter à la fois les NTCs mono-paroi (morphologie similaire) et les NTCs multi-parois de manière générale. Les protocoles de fonctionnalisations covalente et non-covalente des DWNTs purifiés ont été mis au point dans un deuxième temps. Le choix des molécules d’intérêt à greffer s’est porté principalement sur des fluorophores (isothiocyanate de fluorescéine FITC ; Cy5 ; une streptocyanine uniquement fluorescente par liaison covalente), permettant ainsi une visualisation directe de la fonctionnalisation. La détermination des taux de greffage, réalisée grâce à différentes techniques de caractérisation, a soulevé les questions de la stabilité dans le temps de la fonctionnalisation non-covalente et de la quantité réellement greffée de façon covalente sur les NTCs lorsque cette voie est choisie. Enfin, les DWNTs ainsi fonctionnalisés ont été par la suite incubés en présence de plusieurs types de cellules afin de tester leur détection in vitro et la stabilité de la fonctionnalisation dans ce type d'environnement. La co-localisation des DWNTs fluorescents au niveau des cellules a été rendue possible par le croisement des résultats obtenus par les microscopies confocales de fluorescence et Raman. / For many years now, carbon nanotubes (CNTs) show an important potential for biomedical applications (medical imaging, targeted drug delivery, tissue engineering, cancer treatment). All these applications involve modifications of the CNTs walls, through chemical functionalisation, in order to make possible the attachment of molecules of interest. There are two main approaches for functionalisation, involving different interactions and more or less substantial changes in CNTs. On the one hand, the most widely used is the covalent functionalisation that leads to stable covalent bonds but also modifies the structure and thus the inherent properties of CNTs. On the other hand, CNTs can be functionalised by a non-covalent way, that is, through weak interactions (hydrophobic interactions, π- π stacking, ionic interactions, etc.), which do not affect the structure of CNTs. The goals of this thesis were, in a first phase, to determine the best purification strategy for double-walled carbon nanotubes (DWNTs), synthesized by a Catalytic Chemical Vapour Deposition process developed at the CIRIMAT, in order to remove all traces of metal nanoparticles but especially of unwanted carbonaceous species (disorganised carbon); the aim was to start from the cleanest oxidised sample in which CNTs are the only form of carbon, in order to avoid any competition between different carbon species, making then impossible to get a clear conclusion. DWNTs were selected as an ideal structure which would represent both single-walled CNTs (similar morphology) and multi-walled CNTs in general. The protocols of covalent and non-covalent functionalisations of purified DWNTs were developed in a second stage. The choice of the molecules of interest to graft mainly fell on fluorophores (fluorescein isothiocyanate FITC; Cy5; a streptocyanine only fluorescent when it is covalently attached), thus allowing a direct observation of the functionalisation. Grafting ratios could be determined thanks to the combination of several characterisation techniques, which raised some questions on the stability with time of the non-covalent functionalisation, and on what is really covalently grafted on the CNTs when this way is chosen. Finally, such functionalised DWNTs were incubated with several types of cells to test their in vitro detection and the functionalisation stability in this kind of environment. Co-localisation of fluorescent DWNTs in the cells was achieved by comparison of the results obtained from confocal fluorescence and confocal Raman microscopies.

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<p>Currently, fossil fuels and nuclear power are our primary energy sources. However, both have critical disadvantages due to the limited supply and the hazard issues. Renewable energy research becomes one of most important research topics in the 21st century. Nanostructured materials show unique electrochemical properties in various energy conversion or storage devices. This dissertation starts with fundamental optical studies of nanomaterials (carbon nanotubes), followed by synthesizing novel nanomaterials for energy conversion (solar cells) and storage (lithium ion batteries) devices. </p><p> (1) There is an on-going debate concerning the ability of double walled carbon nanotubes (DWNTs) to exhibit photoluminescence (PL). We aim to clearly resolve this debate through the study of carefully separated DWNTs using density gradient ultra-centrifugation (DGU). Here, we clearly show that light is emitted from the inner wall of DWNTs. Interestingly, it was found that a very narrow range of diameters of the inner walls of DWNTs is required for photoluminescence (PL) to be observable. All other diameters led to complete PL quenching in DWNTs. (2) Inexpensive dye sensitized solar cells (DSSCs) on flexible plastic substrates have a bright future, but they require low temperature annealing (< 200°C). The method to fabricate low temperature DSSCs should resolve poor electron transfer between titanium dioxide (TiO2) nanoparticles (NPs) due to their incomplete contiguity and insulating layer of organic residues from binders in the photoactive film. Here, we have developed uniform CNTs/TiO2 composites for low temperature DSSCs by using modified sol gel method. DSSCs were fabricated to study incorporating functionalized few walled carbon nanotubes (f-FWNTs) effect on TiO2 NPs. Incorporating f-FWNTs can be beneficial for the low temperature annealing process of DSSCs to overcome extremely poor electron transport through TiO2 photoactive film. Incorporating f-FWNTs with TiO2 active layer improves electrons transport in some degree, but this advantage is limited. (3) Conductive fillers, such as amorphous carbon, carbon nanotube and graphene, have been mixed with nanostructured metal oxide materials to improve the performance of electrode materials in energy storage devices. However, ineffective junctions between conductive fillers are limiting the overall conductivity of the electrode. Therefore, we developed a convenient, inexpensive and scalable method for synthesizing hybrid carbon and titanium dioxide (C/TiO2) co-gels and co-aerogels to improve their electrochemical capacity in lithium ions batteries (LIBs). The monolith of the hybrid C/TiO2 co-aerogel can be directly used as active electrodes without the addition of binders. As a result, the capacitance of LIB anodes using the hybrid co-aerogel is significantly improved over current LIBs based on carbon/titanium oxide composite. Other metal oxides could also form co-gels with carbon to improve their potentials in numerous electrochemical, photocatalytic, and photoelectronic devices.</p> / Dissertation

One of the most significant issues in nanocomposite performance is improving the dispersion of carbon nanotubes (CNTs) in thermosetting or thermoplastic polymers in order to gain good mechanical properties. Several studies have investigated the fabrication of nanocomposites based on carbon nanotubes and analysed properties, but there is still insufficient data on their structure-property relationships. This thesis has investigated the central importance of stress transfer Raman studies in epoxy composites reinforced with single-walled carbon nanotubes (SWCNTs), double-walled carbon nanotubes (DWCNTs) and multiwall carbon nanotubes (MWCNTs) to elucidate the reinforcing ability of the CNTs in an epoxy matrix. This project was undertaken to synthesise and characterize MWCNTs and determine the effect of different weight fractions of untreated MWCNTs on the stress transfer efficiency at the MWCNTS / epoxy interface and on the stiffness of the thermomechanical properties of the MWCNTS / epoxy composites. It was undertaken to assess the stress transfer efficiency at the CNT / epoxy interface and at the inter-walls of the CNTs with tensile deformation and with cyclic loading.Optimized conditions of the injection chemical vapour deposition method (CVD), such as long injection times were applied to produce MWCNTs with a high yield, high aspect ratio and well-defined G' Raman peak. The morphology and size of CNTs were observed by scanning electron microscopy (SEM) and transmission electron microscopy (TEM) while their thermal stability was examined by Thermogravimetric analysis (TGA). Both Raman spectroscopy and mechanical testing (static and dynamic) were utilized in this study. The Raman spectroscopy research consisted of following the G'-band frequency and linewidth as well as the intensity of radial breathing modes (RBMs) during tensile deformation. The stress-induced Raman shifts in the nanocomposites have been shown to be controlled by the number of carbon nanolayers. A theory has been developed to determine and simulate the stress transfer efficiency parameter, (k_i) for MWCNTs. Tensile tests and dynamic mechanical testing were used to assess the mechanical properties of the nanocomposites.The most obvious finding to be drawn from the present study is that the reinforcement of the epoxy resin with different loadings of MWCNTs is useful, but the best reinforcement was at low loadings of MWCNTs. One of the more significant findings to emerge from this study is that (k_i) between the inner walls of the DWCNTs and MWCNTs are quite similar (~0.7), which suggest that (k_i) may be similar for all CVD MWCNTs and DWCNTs. The second major finding was that there were RBM intensity variations for the SWCNTs and DWCNTs in the hot-cured epoxy composites and that for the DWCNTs both the inner and outer nanotube walls are stressed during deformation

Le remplissage des nanotubes de carbone (NTC) est considéré comme une approche relativement simple permettant de synthétiser des nanocristaux du fait de l'effet de confinement 1D imposé par la cavité centrale des NTC, qui peut être seulement de l'ordre du nanomètre ou moins, notamment dans le cas des NTC monoparoi et en particulier des NTC biparois (DWCNT) sur lesquels nous avons concentré nos efforts. De tels nanocristaux devraient avoir des propriétés physiques (électriques, magnétiques) différentes de celles de leurs équivalents à l'état massif du fait de la modification de la coordinence des atomes ou des ions les composant. Parmi les différentes méthodes existantes pour le remplissage des NTC, (in situ pendant la synthèse, a posteriori à partir de solutions), la méthode faisant intervenir des matériaux fondus est la plus populaire pour le remplissage par des matériaux inorganiques. Elle permet en effet d'atteindre des taux de remplissage raisonnablement élevés et demeure assez simple à mettre en œuvre. Cependant, elle fait preuve d'un certain nombre de limitations (techniques) qui posent problème dans le cas de matériaux à haut point de fusion (typiquement > 1000°C), dont la réactivité avec le carbone à haute température pourrait être gênante (carboréduction des oxydes par exemples), ou encore dont la faible mouillabilité vis-à-vis du carbone à l'état fondu est rédhibitoire (métaux par exemple). Il est possible de palier à cette difficulté en procédant par étapes successives et en remplissant d'abord les NTC avec un précurseur puis d'utiliser la cavité interne des NTC comme des nanoréacteurs afin de procéder dans un second temps à une transformation in situ. Dans ces travaux, nous avons étudié (1) le remplissage de DWCNT avec de l'iode ainsi qu'avec différents iodures métalliques en mettant en œuvre essentiellement la méthode des sels fondus. Nous avons étudié en détails l'influence des paramètres physico-chimiques du matériau de remplissage (réactivité chimique sous la forme en particulier du potentiel rédox du couple iodure métallique / métal, mais aussi viscosité, tension de surface, pression de vapeur saturante en milieu fondu) mais aussi du NTC (texture cylindrique ou "en arrêtes de poisson", diamètre, nombre de parois) sur le taux de remplissage. (2) Nous avons étudié en détail un certain nombre de structures inhabituelles de nanomatériaux confinés dans les DWCNT, en faisant appel à la modélisation structurale et à la simulation d'images de microscopie électronique sur la base de ces modèles pour guider notre analyse. (3) Nous avons enfin étudié différentes réactions in situ dans les DWCNT telles que la sulfuration, la réduction sous hydrogène ou encore la fluoration afin de synthétiser des nanocristaux originaux et de les caractériser en détails à l'aide d'outils tels que par exemple le MET Haute Résolution et la spectroscopie de perte d'énergie des électrons (EELS). / Filling carbon nanotubes (CNTs) has been considered as an easy approach to synthesize various nanocrystals since the inserted materials are forced to adopt a nearly one-dimensional morphology arising from their very high aspect ratio, especially in the case of single-walled CNTs (SWCNTs) or double-walled CNTs (DWCNTs). Nanocrystals/nanowires of transition metals, especially those with very narrow diameters, are predicted to exhibit peculiar magnetic property differing from the bulk metals. Filling CNTs provides a possible way for the synthesis of such metal nanocrystals/nanowires. There are several methods for filling CNTs including the in situ method, gas phase method, molten phase method, solution method, etc. Among them, molten phase has been very popular for filling various types of nanotubes due to the possibility to reach high filling rates, simplicity and versatility. However, for materials with high melting point such as metals, it is difficult to insert them into CNTs directly. To solve this problem, we also took advantage of the inner cavity of CNTs which not only templates the growth but also acts as a nanoreactor in order to perform chemical reactions. The insertion of materials with high melting point is typically achieved by first filling CNTs with a precursor, and then transforming the precursor into the desired 1D nanostructure by post-treatments. In this thesis, (i) filling DWCNTs with iodine and various halides via the molten phase method was performed and the influence of the relevant physical and chemical properties of the halides on the filling rate was investigated. The role of the redox potential as a main parameter driving the filling efficiency is pointed out, and explained; (ii) peculiar structures of the nanocrystals confined within DWCNTs were imaged by transmission electron microscopy (TEM) and corresponding modeling of the observed crystal nanostructures and related TEM images were proposed; (iii) different in situ transformations on the iodide-filled DWCNTs were attempted and the chemical composition of the encapsulated 1D nanocrystals before and after post-filling treatments was systematically identified by means of electron energy loss spectroscopy (EELS).

In this thesis, experimental studies are reported of ultrafast dynamics and third order optical nonlinear coefficients of carbon nanotubes, and time resolved coherent phonon dynamics of semiconductors and rare earth titanates. The thesis is divided into three parts. The first part presents (i) general introduction to theoretical background on nonlinear optical susceptibility and time resolved studies, and systems studied (chapter 1) and (ii) experimental techniques (chapter 2). The second part of the thesis deals with the measurements of third order nonlinear susceptibilities and ultrafast dynamics of single and double walled carbon nanotubes (chapter 3). The third part contains coherent phonon dynamics in semiconductors, Te (chapter 4), Bi2Te3 (chapter 5), and ZnTe (chapter 6) and spin-frustrated rare earth titanate insulators (chapter 7). Chapter 1: This chapter is a general introduction to the thesis. The chapter is divided into two parts: (i) light-matter interaction, and (ii) systems studied. Under light-matter interaction, we describe the required theoretical and conceptual background of nonlinear optical susceptibilities and time resolved carrier and phonon dynamics. In the next part, a brief summary of details of the systems studied, that include carbon nanotubes (single and double walled), semiconductors (Te, Bi2Te3 and ZnTe) and insulating spin-frustrated rare earth titanates (Gd2Ti2O7, Dy2Ti2O7 and Tb2Ti2O7), are presented. Chapter 2: Details of the ultrafast laser systems (femtosecond oscillator and amplifier), pulse width measurements and ultrafast experimental pump-probe and z-scan techniques, used in this thesis are given in this chapter. Chapter 3: Here the experimental results on the measurements of third order optical nonlinearity and ultrafast dynamics of single and double walled carbon nanotubes are presented. The chapter starts with a general overview of optical switching followed by known ultrafast dynamics and nonlinear studies on carbon nanotubes. In the next section, our theoretical modelling of nonlinear absorption and refraction in the limit of saturable absorption is described. The final two sections depict our results on single and double walled carbon nanotubes. These studies indicate that double walled carbon nanotubes are best candidates for ultrafast optical switching. Chapter 4: This chapter presents temperature and pump fluence dependent femtosecond time resolved reflectivity measurements on tellurium. The chapter starts with an overview of previous pump-probe reflectivity studies at room temperature on tellurium followed by our results. A totally symmetric A1 coherent phonon at 3.6 THz responsible for the oscillations in the reflectivity data is observed to be strongly positively chirped (i.e, phonon time period decreases at longer pump-probe delay times) with increasing photoexcited carrier density, more so at lower temperatures. We show for the first time that the temperature dependence of the coherent phonon frequency is anomalous (i.e, increasing with increasing temperature) at high photoexcited carrier density due to electron-phonon interaction. At the highest photoexcited carrier densities of ~ 1.4 x 1021cm-3 and the sample temperature of 3K, the lattice displacement of the coherent phonon mode is estimated to be as high as ~ 0.24 Å. Numerical simulations based on coupled effects of optical absorption and carrier diffusion reveal that the diffusion of carriers dominates the non-oscillatory electronic part of the time-resolved reflectivity. Finally, using the pump-probe experiments at low carrier density of 6 x 1018 cm-3, we separate the phonon anharmonicity to obtain the electron-phonon coupling contribution to the phonon frequency and linewidth. Chapter 5: This chapter begins with a introduction of previous ultrafast studies at room temperature on Bi2Te3 and then presents our results on the temperature dependent high pump fluence time resolved reflectivity measurements on Bi2Te3. The time resolved reflectivity data shows two coherently generated totally symmetric A1g modes at 1.85 THz and 3.6 THz at 296K which blue shift to 1.9 THz and 4.02 THz, respectively at 3K. At high photoexcited carrier density of ~ 1.7 x 1021cm-3, the phonon mode at 4.02 THz is two orders of magnitude higher positively chirped than the lower frequency mode at 1.9 THz. The chirp parameter, β is shown to vary inversely with temperature. The time evolution of these modes is studied using continuous wavelet transform of the time-resolved reflectivity data. The analysis shows that the build up time for the two coherent phonons is different. Chapter 6: This chapter starts with a general introduction on various as pects of ZnTe to be used in generation and detection of THz followed by our results on influence of carriers and sample temperature on coherent phonon and polariton generation in ZnTe. Combination of femtosecond Kerr, two photon absorption and impulsive stimulated Raman scattering experiments have been carried out to investigate the effect of pulse energy and crystal temperature on the generation of coherent polaritons and phonons in < 110 > cut ZnTe single crystals of three different resistivities. We demonstrate that the effect of two-photon induced free carriers on the creation of both the polaritons and phonons is largest at 4K where the free carrier lifetime is enhanced. Further, the temperature dependant impulsive stimulated Raman scattering on high and low purity ZnTe crystals allows us to unambiguously assign the phonon mode at 3.5 THz to the longitudinal acoustic mode at X-point in the Brillouin zone, LA(X) in contrast to the assignment as two-phonon process in earlier studies. Chapter 7: This chapter starts with an introduction on previous Raman studies on the pyrochlore systems accompanied by our results on the generation of coherent optical phonons in spin frustrated pyrochlore single crystals Dy2Ti2O7, Gd2Ti2O7 and Tb2Ti2O7 and their behavior as a function of sample temperature from 296K to 4K. At 4K, two coherent phonons are observed at 5.3 THz (5.0 THz) and ~ 9.3 THz (9.4 THz) for Dy2Ti2O7 (Gd2Ti2O7) whereas three coherent phonons are generated at ~ 4.8 THz, 8.6 THz and 9.6 THz for Tb2Ti2O7. In the case of spin-ice Dy2Ti2O7, a clear discontinuity is observed in the linewidths of both the coherent phonons as well as in the phase of low energy coherent phonon mode, indicating a subtle structural change as also suggested by Raman studies. In comparison, such changes are not seen in the coherent phonons of Gd2Ti2O7, and Tb2Ti2O7. Another important observation is the phase difference of ‘π’ between the modes in all the samples, thus suggesting that the driving forces behind the generation of these modes are different in nature unlike a purely impulsive or displacive mechanism. Chapter 8: This chapter summarizes our results reported in this thesis and gives future directions.