Ce document présente une étude des mécanismes de relaxation de fullerènes induits par photoexcitation. Nous avons exploré les processus d'ionisation et de fragmentation de ces systèmes modèles suite à une irradiation par différentes sources de lumière : impulsion femtoseconde, laser à électron libre (IR lointain) et Synchrotron (XUV). Afin d'étudier ces mécanismes, nous utilisons l’imagerie par cartographie de vitesse qui nous permet de suivre l'évolution de la distribution angulaire de vitesse des particules émises. Suivant la durée, l'intensité et la longueur d'onde de l'excitation utilisée, la nature des mécanismes change drastiquement (mécanismes statistiques, ionisation cohérente en champ fort, autoionization de plasmons, etc…). Plusieurs approches théoriques sont utilisées allant du modèle Weisskopf pour les processus statistiques à la résolution de l'équation de Schrödinger dépendante du temps pour les processus cohérents. Cette étude permet de relier les mécanismes de relaxation intervenant à différentes échelles de temps / This document presents a study of relaxation mechanisms of fullerenes induced by photoexcitation. We have investigated ionization and fragmentation processes of these model systems under irradiation by various light sources: femtosecond pulse, free electron laser (far IR) and Synchrotron (XUV). To study these mechanisms, we use the velocity map imaging technique which allows us to follow the evolution of the angular distribution and velocity of the emitted particles. The nature of the relaxation mechanisms changes drastically (statistical mechanisms, coherent ionization in strong field, autoionization of plasmons, etc.) depending on the pulse duration, its intensity and the wavelength. Several theoretical approaches have been used including a Weisskopf modelling for the statistical processes and direct treatment of the time dependant Schrödinger equation for the coherent processes. This study allows us building bridges between the relaxation mechanisms occurring on various scales of time

Au cours des dernières années, le développement des cellules organiques à réseaux interpénétrés a permis d’améliorer les rendements de conversion photovoltaïque (PV). Ces dispositifs incorporent une couche active constituée d’un mélange d’un matériau donneur d’électron (D) et d’un matériau accepteur d’électron (A). La réalisation de ces cellules requiert une optimisation minutieuse de ce mélange et de la morphologie de cette couche photo-active qui en résulte. Cette dernière peut cependant évoluer spontanément vers une ségrégation de phase, généralement délétère pour les performances PV. Une solution possible, et relativement peu étudiée, consiste à lier chimiquement le donneur D et l’accepteur A par un espaceur non-conjugué. Les travaux décrits dans ce manuscrit portent sur la synthèse et la caractérisation d’assemblages moléculaires de type D-σ-A ainsi que leur utilisation comme matériau dit « unique » pour la fabrication de cellules solaires organiques mono composant. Une première famille de dyades et triades à base d’un bloc donneur de type quaterthiophène a été étudiée. Cette partie décrit la méthodologie générale d’assemblage des blocs D et A via une réaction de cycloaddition de type Huisgen. Au cours des chapitres suivant, plusieurs dyades basées sur un bloc donneur « push-pull » ont été synthétisées puis caractérisées. Les performances PV de ces composés ont été évaluées au sein de cellules solaires mono-composant et les meilleurs rendements de conversion, atteignant 1.4 %, rivalisent avec l’état de l’art. / Over the last few years, the development of bulk heterojunction organic solar cells (BHJ OSCs) led to significant increase in photovoltaic (PV) efficiency. Such devices are based on interpenetrated networks of an electron-donor material (D) and an electron-acceptor material (A) constituting the active layer. Nevertheless a careful optimization of the morphology is required to reach high power conversion efficiency. Furthermore, this optimized morphology can evolve towards spontaneous phase segregation which can be detrimental for the PV performances. To circumvent these limitations, a relatively unexplored approach relies on the use of a material where the donor and the acceptor moieties are covalently linked to each other through a nonconjugated π-connector. In this context, the work reported herein describes the synthesis and characterization of various molecular D-σ-A assemblies, as well as their preliminary evaluation as “unique” material for the realisation of single component organic solar cells (SC-OSCs). A first family of dyads and triads, based on quaterthiophene moieties as donor block, was studied. A general methodology to assemble the two D and A blocks via a Huisgen-type click-chemistry is described. Then, in the next chapters, several dyads based on a “push-pull” donor block have been synthesized and characterized. The PV performances of these compounds have been evaluated in SC-OSCs leading to power conversion efficiency up to 1.4 %, a value close to the state of the art.

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Fullerenhaltige Bulk-Heterojunction-Solarzellen auf Polymerbasis zeigen derzeit eine geringe Langzeitstabilität, die unter anderem auf der Entmischung der Bulkphasen beruht. In dieser Arbeit wurden daher auf neuartige Weise Blockcopolymere entwickelt, die zur Stabilisierung der Phasen dienen können. Ausgehend von Poly-3-hexylthiophen-Makroinitiatoren wurde ein zweiter Block mit reaktivem Comonomer polymerisiert, das zur Anbindung von reinem Fullerens bzw. von Fullerenderivaten diente. Die fullerenfunktionalisierten Polymere wurden in Modell-Systeme eingemischt und zeigten erste Verbesserungen bezüglich der Phasenstabilisierung.:1 Einleitung und Zielstellung 2 Grundlagen 2.1 Polymere Solarzellen 2.1.1 Theoretische Grundlagen und Funktionsweise 2.1.2 Materialien und Materialoptimierung 2.1.3 Stabilisierung der Blendmorphologien 2.2 Blockcopolymere – Eigenschaften und Aufbau 2.2.1 Kontrolliert radikalische Polymerisationen 2.2.2 Kumada-Catalyst Transfer Polycondensation 2.3 Fullerene – Eigenschaften und Funktionalisierung 3 Ergebnisse und Diskussion 3.1 Darstellung von Akzeptor-Polymeren 3.1.1 Synthese der Copolymere 3.1.2 Bingel-Reaktion 3.1.3 Polymeranaloge Reaktionen und Anbindung von Fullerenen an Copolymere 3.2 Synthesen von Donor-Akzeptor-Blockcopolymeren 3.2.1 Synthese und Charakterisierung des Makroinitiators und der Blockcopolymere 3.2.2 Polymeranaloge Reaktionen an Blockcopolymeren 3.3 Charakterisierung der Eigenschaften von Donor-Akzeptor-Blockcopolymeren in Blends 3.3.1 Blends mit fullerenhaltigen Blockcopolymeren 3.3.2 Blends mit azidfunktionalisiertem Blockcopolymer 3.3.3 Solarzellen-Tests 4 Zusammenfassung und Ausblick 5 Experimenteller Teil 5.1 Verwendete Chemikalien und Reagenzien 5.2 Geräte und Hilfsmittel 5.3 Synthesen niedermolekularer Verbindungen 5.4 Polymersynthesen 5.5 Polymeranaloge Reaktionen 6 Literaturverzeichnis Anhang

Indiana University-Purdue University Indianapolis (IUPUI) / As mass production of carbon nanoparticles (CNPs) continues to rise, the likelihood of occupational and environmental exposure raises the potential for exposure‐related health hazards. Although many groups have studied the effects of CNPs on biological systems, very few studies have examined the effects of exposure of cells, tissues or organisms to low, physiologically relevant concentrations of CNPs. Three of the most common types of CNPs are single wall nanotubes (SWNT), multi wall nanotubes (MWNT) and fullerenes (C60). We used electrophysiological techniques to test the effects of CNP exposure (40 μg/cm2 – 4 ng/cm2) on barrier function and hormonal responses of well characterized cell lines representing barrier epithelia from the kidney (mpkCCDcl4) and airways (Calu‐3). mpkCCDcl4 is a cell line representing principal cell type that lines the distal nephron in an electrically tight epithelia that aids in salt and water homeostasis and Calu‐3 is one of the few cell lines that produces features of a differentiated, functional human airway epithelium in vivo. These cell lines respond to hormones that regulate salt/water reabsorption (mpkCCDcl4) and chloride secretion (Calu‐3). In mpkCCDcl4 cells, after 48 hour exposure, the transepithelial electrical resistance (TEER) was unaffected by high concentrations (40 – 0.4 μg/cm2) of C60 or SWNT while lower, more relevant levels (< 0.04 μg/cm2) caused a decrease in TEER. MWNT decreased TEER at both high and low concentrations. CNT exposure for 48 hour did not change the transepithelial ion transport in response to anti‐diuretic hormone (ADH). In Calu‐3 cells, after 48 h of exposure to CNPs, fullerenes did not show any effect on TEER whereas the nanotubes significantly decreased TEER over a range of concentrations (4 μg/cm2‐0.004 ng/cm2). The ion transport response to epinephrine was also significantly decreased by the nanotubes but not by fullerenes. To look at the effect of exposure times, airway cells were exposed to same concentrations of CNPs for 24 and 1h. While the 48 h and 24 h exposures exhibited similar effects, there was no effect seen after 1h in terms of TEER or hormonal responses. In both the cell lines the magnitude of the transepithelial resistance change does not indicate a decrease in cellular viability but would be most consistent with more subtle changes (e.g., modifications of the cytoskeleton or changes in the composition of the cellular membrane). These changes in both the cell lines manifested as an inverse relationship with CNP concentration, were further corroborated by an inverse correlation between dose and changes in protein expression as indicated by proteomic analysis. These results indicate a functional impact of CNPs on epithelial cells at concentrations lower than have been previously studied and suggest caution with regard to increasing CNP levels due to increasing environmental pollution.

Quantum information processing (QIP) has the potential to reduce the complexity of many classically ‘hard’ computational problems. To implement quantum information algorithms, a suitable physical quantum computer architecture must be identified. One approach is to store quantum information in the electron spins of an array of paramagnetic N@C₆₀ endohedral fullerene molecules, using the electron-electron dipolar interaction to permit the formation of the entangled quantum states needed to implement QIP. This thesis explores two different chemical methods to create two-spin centre arrays that contain N@C₆₀. The first method uses a double 2,3 dipolar cycloaddition reaction to a dibenzaldehyde-terminated oligo-p-phenylene polyethynylene (OPE) unit , to create an (S_3/2, S_3/2) N@C₆₀-N@C₆₀ dimer with a fixed spin centre separation of 2.7 nm. The second approach is via a self-assembly scheme in which a Lewis base functionalised N@C₆₀ molecule coordinates to an antiferromagnetic metallic ring magnet to form a (S_3/2, S_3/2) two-spin centre N@C₆₀-Cr₇Ni system with an inter-spin separation of 1.4 nm. In both systems, a significant perturbation of the electron spin transition energies is observed using CW ESR, this perturbation is shown to be well accounted for by the inclusion of an electron-electron dipolar coupling term in the electron spin Hamiltonians. To create entanglement in an ensemble of two-spin centre molecules, the dipolar coupling interaction must lie within a narrow distribution. To achieve this not only the separation but also the orientation of the inter-spin axis with respect to the applied magnetic field must be controlled for which a method of macroscopic alignment is required. The potential of using a uniaxially drawn liquid crystal elastomer to exert uniaxial order on fullerene dimers is tested, finding that the degree of alignment is insufficient, possibly a result of the propensity for the fullerene molecules to phase separate from the elastomer. This phase separation is shown to restrict N@C₆₀ phase coherence lifetime to 1.4 µs at 40 K due to instantaneous spin diffusion. The electron spin environment of both N@C₆₀ and an N@C₆₀-C₆₀ dimer in a polymer matrix is examined using polystyrene as the host matrix. By deuteration of the polystyrene matrix, a maximum phase coherence lifetimes of 48 µs and 21 µs are measured for the N@C₆₀ and N@C₆₀-C₆₀ dimer, respectively. The concept of reading out the electron spin state of N@C₆₀ molecules by coupling it to a spin system that can be probed using optically detected magnetic resonance (ODMR) such as an NV- centre has been previously suggested. To this end, the photostability of N@C₆₀ under 637 nm laser illumination has been examined in solution. The effect of the presence of an atmospheric concentration of oxygen is striking, affording a 57-fold retardation in the photodecomposition of N@C₆₀ compared to a degassed solution. When ambient oxygen is present, the average number of excitations that are required to cause decomposition is ≈60000. Finally, for future UV photophysics experiments involving N@C₆₀, the best solvent to use was found to be decalin, finding that it significantly slowed decomposition of N@C₆₀ in both ambient and degassed solutions. The conclusions of this work make a significant contribution to the field of QIP with N@C₆₀, showing that there is a bright future for N@C₆₀.

This thesis entitled “Electronic Structure and Bonding in Metallaboranes and Main Group Compounds” consists of five chapters. Chapter 1 gives an exposition of concepts and techniques used in understanding the electronic structure and bonding in some chemically interesting molecules. Heuristics concepts like isolobal analogy and electron counting rules are used in analyzing and predicting some novel chemical systems. A brief description of computational techniques such as density functional theory (DFT) based methods are used to quantitatively examine the structures and energies of these systems. In chapter 2 we present a critical analysis of bonding in neutral and dianionic stannadiphospholes and compare the potential energy surfaces with the isoelectronic Cp+ and Cp- species. The analysis indicates that Sn can be a better isolobal analogue to P+ than to BH or CH+. In chapter 3 we present new strategy to stabilize B2H4 in planar configuration using transition metal fragments. This requires the metal to donate two electrons into the empty B-B π orbital. Such complexes present a unique case study to the classical DCD model of metal-π complex. In chapter 4 we study the bonding in some recently synthesized metallaboranes which does not follow conventional electron counting rules. The complex and non-canonical nature of these metallaboranes feature some unique bonding patterns which are elucidated using theoretical techniques. In the final chapter we present new approach to build metal coated boron fullerenes. We use electron counting rules to device new structures which show enhanced metal boron bonding.

Trifluoromethylierung von Mischungen hoeherer Fullerene mit CF3I wurde in Ampullen bei 400-420 Grad Celsius und 500-600 Grad Celsius durchgefuehrt. Die Produktmischungen wurden mittels mehrstufiger HPLC getrennt. In mehreren Versuchen konnten aus den isolierten HPLC-Fraktionen Kristalle fuer die Roentgenstrukturanalyse gewonnen werden. Die folgenden Strukturen der CF3-Derivate der Fullerene C84, C86 und C88 wurden bestimmt: 1 Isomer von C84(4)(CF3)12, C84(11)(CF3)10, C84(11)(CF3)12, C84(11)(CF3)16, C84(16)(CF3)8, C84(16)(CF3)14, C84(18)(CF3)10, C84(18)(CF3)12, C84(22)(CF3)20, C84(23)(CF3)8, C84(22)(CF3)10, C84(22)(CF3)12, C84(22)(CF3)18, C86(17)(CF3)10, C86(17)(CF3)16, C88(33)(CF3)16, C88(33)(CF3)18 und C88(33)(CF3)20. 2 Isomere von C84(22)(CF3)12, C84(22)(CF3)14 und C84(23)(CF3)14. 3 Isomere von C84(11)(CF3)14. 4 Isomere von C84(22)(CF3)16. Die Additionsmuster der Strukturen wurden diskutiert. Die experimentell nachgewiesenen Strukturen wurden mit berechneten Modellstrukturen verglichen. Dabei wurde auch die Stabilitaet der experimentellen Strukturen vorausgesagt. Zusaetzlich wurden die moeglichen Reaktionspfade fuer die Bildung hoeherer Derivate ausgehend von niedrigen Derivaten diskutiert. Sie zeigen, dass die Regioselektivitaet der Addition vom Kaefigisomer abhaengig ist. Die Reaktionspfade von vier Fullerenkaefigen werden in dieser Arbeit vorgestellt. C84(11)(CF3)10 --> C84(11)(CF3)16 C84(22)(CF3)2 --> C84(22)(CF3)20 C84(23)(CF3)10 --> C84(23)(CF3)18 C86(17)(CF3)10 --> C86(17)(CF3)16 / Trifluoromethylation of higher fullerene mixtures with CF3I was performed in ampoules at 400 to 420 degree Celsius and 500 to 600 degree Celsius. The obtained product mixtures were separated by multistep HPLC. Subsequent crystal growth and X-ray diffraction measurements allowed for structural characterization of the CF3 derivatives of fullerenes C84, C86 and C88 listed as the following. 1 isomer of C84(4)(CF3)12, C84(11)(CF3)10, C84(11)(CF3)12, C84(11)(CF3)16, C84(16)(CF3)8, C84(16)(CF3)14, C84(18)(CF3)10, C84(18)(CF3)12, C84(22)(CF3)20, C84(23)(CF3)8, C84(22)(CF3)10, C84(22)(CF3)12, C84(22)(CF3)18, C86(17)(CF3)10, C86(17)(CF3)16, C88(33)(CF3)16, C88(33)(CF3)18 and C88(33)(CF3)20. 2 isomers of C84(22)(CF3)12, C84(22)(CF3)14 and C84(23)(CF3)14. 3 isomers of C84(11)(CF3)14. 4 isomers of C84(22)(CF3)16. The molecular structures of isolated isomers were discussed in terms of their addition patterns and relative formation energies. DFT calculations were used to predict stable molecular structures of the CF3 derivatives. Calculated model structures have been compared with the experimental ones. In addition, the reaction pathways from the lower derivatives to higher ones of selected compounds were predicted. The pathways indicate the regioselectivity of additions depending on the fullerene cage isomer. Reaction pathways are presented for four fullerene cages in this work. C84(11)(CF3)10 --> C84(11)(CF3)16 C84(22)(CF3)2 --> C84(22)(CF3)20 C84(23)(CF3)10 --> C84(23)(CF3)18 C86(17)(CF3)10 --> C86(17)(CF3)16

<p>Fullerenes have been shown to constitute a prototypical building block for truly nanometer-sized devices and exotic nanounit-based materials, e.g., high-temperature superconductors. This makes the detailed understanding of fullerene electronic states in compounds and at interfaces of primary importance, since the high symmetry of the molecule greatly </p><p>simplifies the starting point of the analysis. Carbon nanotubes, which combine one macroscopic with two nanoscopic dimensions, are perhaps of even greater practical interest.</p><p>Angle-dependent electron spectroscopies have been employed in the present work to study these materials, characterizing their structure, bonding, and electronic states. For solid C₆₀, the photoelectron angular distribution has been found to be essentially that of the free molecule, modified by solid state scattering; a similar distribution is found for K₃C_60.</p><p>The surface and bulk electronic structure of K₃C₆₀ has been identified by angle-dependent core and valence photoelectron spectroscopy (PES) and x-ray emission spectroscopy. An insulating surface layer has been identified for this high-temperature superconductor.</p><p>Angle-dependent valence PES is used to investigate the electronic states of C₆₀/Al(110). Electron correlations are found to be the origin of the splitting observed in the molecular orbitals, which is quite sensitive to the molecular orientation. The components of the highest occupied molecular orbital are differentiated according to their overlap with the substrate.</p><p>A rigid shift of valence- and core-levels has been observed even for ionic and covalent C₆₀compounds, reflecting the efficient static polarizability screening of the molecule. </p><p>The alignment of multi-walled carbon nanotubes has been investigated by x-ray absorption spectroscopy, using the spectral intensity ratio of π*- and *-resonances. Core level combined with valence PES shows that the degree of defect structure varies from position to position on the sample. Valence photoelectron spectra of defect-free sample spots closely resembles the total DOS of graphite.</p>

Fullerenes have been shown to constitute a prototypical building block for truly nanometer-sized devices and exotic nanounit-based materials, e.g., high-temperature superconductors. This makes the detailed understanding of fullerene electronic states in compounds and at interfaces of primary importance, since the high symmetry of the molecule greatly simplifies the starting point of the analysis. Carbon nanotubes, which combine one macroscopic with two nanoscopic dimensions, are perhaps of even greater practical interest. Angle-dependent electron spectroscopies have been employed in the present work to study these materials, characterizing their structure, bonding, and electronic states. For solid C60, the photoelectron angular distribution has been found to be essentially that of the free molecule, modified by solid state scattering; a similar distribution is found for K3C60. The surface and bulk electronic structure of K3C60 has been identified by angle-dependent core and valence photoelectron spectroscopy (PES) and x-ray emission spectroscopy. An insulating surface layer has been identified for this high-temperature superconductor. Angle-dependent valence PES is used to investigate the electronic states of C60/Al(110). Electron correlations are found to be the origin of the splitting observed in the molecular orbitals, which is quite sensitive to the molecular orientation. The components of the highest occupied molecular orbital are differentiated according to their overlap with the substrate. A rigid shift of valence- and core-levels has been observed even for ionic and covalent C60 compounds, reflecting the efficient static polarizability screening of the molecule. The alignment of multi-walled carbon nanotubes has been investigated by x-ray absorption spectroscopy, using the spectral intensity ratio of π*- and *-resonances. Core level combined with valence PES shows that the degree of defect structure varies from position to position on the sample. Valence photoelectron spectra of defect-free sample spots closely resembles the total DOS of graphite.