Há muitos agentes terapêuticos comercializados sob forma racêmica. Os enantiômeros podem apresentar diferenças significativas nos perfis farmacocinético e farmacodinâmico. O uso do enantiômero puro em formulações farmacêuticas pode resultar em melhor ajuste de dose e menos efeitos adversos. A atropina, um alcalóide natural da Atropa belladonna, é a mistura racêmica de l-hiosciamina e d-hiosciamina. Este fármaco é principalmente utilizado para dilatar a pupila e como um antiespasmódico. Para quantificar estes enantiômeros, foram desenvolvidos métodos analíticos utilizando a cromatografia líquida de alta eficiência (CLAE) com as fases estacionárias quirais Chiralcel-OD® e Chiral-AGP®. Para quantificar estes enantiômeros em soluções oftálmicas, foi realizada a validação com sucesso de um método por CLAE, empregando uma coluna Chiral-AGP®, a 20°C. A fase móvel foi uma solução tampão fosfato (contendo 10 mM de 1-octanosulfonato de sódio e 7,5 mM de trietilamina, ajustada para pH 7,0 com ácido fosfórico) e acetonitrila (99:1 v/v). A vazão foi de 0,6 mL/min, com detecção ultravioleta em 205 nm. No intervalo de concentração de 14,0 µg/mL a 26,0 µg/mL, o método é linear (r > 0,9999), exato (100,1% - 100,5%) e preciso (RSDsistema ≤ 0,6%; RSDintra-dia ≤ 1,1%; RSDentre-dias ≤ 0,9%). O método é específico e os testes de validação asseguram que as soluções de padrão e amostra são estáveis até 72 horas. O planejamento fatorial assegura a robustez com variação de ±10% nos componentes da fase móvel e 2°C na temperatura da coluna. / There are many therapeutic agents commercialized under racemic form. The enantiomers can show significant differences in the pharmacokinetic and pharmacodynamic profiles. The use of pure enantiomer in pharmaceutical formulations can result in better adjustment of dose and less adverse effects. Atropine, an alkaloid of the Atropa belladonna, is a racemic mixture of l-hyoscyamine and d-hyoscyamine. This drug is mainly used to dilate the pupil and as an antispasmodic agent. To quantify these enantiomers analytical methods were developed, using high performance liquid chromatography (HPLC) with chiral stationary phases Chiralcel OD® and Chiral AGP®. To quantify these enantiomers in ophthalmic solutions the validation of a HPLC method was performed using a Chiral AGP® column at 20°C. The mobile phase consisted of a buffered phosphate solution (containing 10 mM 1-octanesulfonic acid sodium salt and 7.5 mM triethylamine, adjusted to pH 7.0 with ortho-phosphoric acid) and acetonitrile (99:1 v/v). The flow rate was 0.6 mL/min, with ultraviolet detection at 205 nm. In the concentration range from 14.0 mg/mL to 26.0 mg/mL, the method is linear (r > 0.9999), exact (100.1% - 100.5%) and precise (RSDsystem ≤ 0.6%; RSDintra-day ≤ 1.1%; RSDinter day ≤ 0.9%). The method is specific and the validation tests assure that standard and sample solutions are stable for up to 72 hours. The factorial design assures the robustness with variation of ± 10% in the mobile phase components and 2°C of column temperature.

Strong light matter interactions in metallic nanoparticles (NPs), especially those made of noble metals such as Gold and Silver is at the heart of much ongoing research in nanoplasmonics. Individual NPs can support collective excitations (Plasmon’s) of the electron plasma at certain wavelengths, known as the localized surface Plasmon resonance (LSPR) which provides a powerful platform for various sensing, imaging and therapeutic applications. For a collection of NPs their optical properties can be signify cannily different from isolated particles, an effect which originates in the electromagnetic interactions between the localised Plasmon modes. An interesting aspect of such interactions is their strong dependence on the geometry of NP collection and accordingly new optical properties can arise. While this problem has been well considered in one and two dimensions with periodic as well as with random arrays of NPs, three dimensional systems are yet to be fully explored. In particular, there are challenges in the successful de-sign and fabrication of three dimensional (3D) plasmonic metamaterials at optical frequencies. In the work presented in this thesis we present a detail investigation of the theoretical and experimental aspects of plasmonic interactions in two geometrically different three dimensional plasmonic nanostructured systems - a chiral system consisting of achiral plasmonic nanoparticles arranged in a helical geometry and an achiral system consisting of achiral plasmonic nanoparticle arrays stacked vertically into three dimensional geometry. The helical arrangement of achiral plasmonic nanoparticles were realised using a wafer scale technique known as Glancing Angle Deposition (GLAD). The measured chiro-optical response which arises solely from the interactions of the individual achiral plasmonic NPs was found to be one of the largest reported value in the visible. Semi analytical calculation based on couple dipole approximation was able to model the experimental chiro-optical response including all the variabilities present in the experimental system. Various strategies based on antiparticle spacing, oriented elliptical nanoparticles, dielectric constant value of the dielectric template were explored such as to engineer a strong and tunable chiro-optical response. A key point of the experimental system despite the presence of variabilities, was that the measured chiro-optical response showed less than 10 % variability along the sample surface. Additionally we could exploit the strong near held interactions of the plasmonic nanoparticles to achieve a strongly nonlinear circular differential response of two photon photoluminescent from the helically arranged nanoparticles. In addition to these plasmonic chiral systems, our study also includes investigation of light matter interactions in purely dielectric chiral systems of solid and core shell helical geometry. The chiro-optical response was found to be similar for both the systems and depend strongly on their helical geometry. A core-shell helical geometry provides an easy route for tuning the chiro-optical response over the entire visible and near IR range by simply changing the shell thickness as well as shell material. The measured response of the samples was found to be very large and very uniform over the sample surface. Since the material system is based entirely on dielectrics, losses are minimal and hence could possibly serve as an alternative to conventional plasmonic chiro-optical materials. Finally we demonstrated the used of an achiral three dimensional plasmonic nanostructure as a SERS (surface enhance Raman spectroscopy) substrate. The structure consisted of porous 3D metallic NP arrays that are held in place by dielectric rods. For practically important applications, the enhancement factor, as well as the spatial density of the metallic NPs within the laser illumination volume, arranged in a porous 3D array needs to be large, such that any molecule in the vicinity of the metal NP gives rise to an enhanced Raman signal. Having a large number of metallic NPs within the laser illumination volume, increases the probability of a target molecule to come in the vicinity of the metal NPs. This has been achieved in the structures reported here, where high enhancement factor (EF) in conjunction with large surface area available in a three dimensional structure, makes the 3D NP arrays attractive candidates as SERS substrates.

No description available.

We study the masses of the low-lying charm and bottom mesons within the framework of heavy-hadron chiral perturbation theory. We work to third order in the chiral expansion, where meson loops contribute. In contrast to previous approaches, we use physical meson masses in evaluating these loops. This ensures that their imaginary parts are consistent with the observed widths of the D-mesons. The lowest odd- and even-parity, strange and non-strange mesons provide enough constraints to determine only certain linear combinations of the low-energy constants (LECs) in the effective Lagrangian. We comment on how lattice QCD could provide further information to disentangle these constants. Then we use the results from the charm sector to predict the spectrum of odd- and even-parity of the bottom mesons. The predicted masses from our theory are in good agreement with experimentally measured masses for the case of the odd-parity sector. For the even-parity sector, the $B$-meson states have not yet been observed; thus, our results provide useful information for experimentalists investigating such states. The near degeneracy of nonstrange and strange scalar $B$ mesons is confirmed in our predictions using $\mathrm{HHChPT}$. Finally,we show why previous approaches of using $\mathrm{HHChPT}$ in studying the mass degeneracy in the scalar states of charm and bottom meson sectors gave unsatisfactory results. Interactions between these heavy mesons are treated using effective theories similar to those used to study nuclear forces. We first look at a strongly-interacting channel which produces a bound or virtual state and a dimer state which couples weakly to a weakly-interacting channel to produce a narrow resonance. We also look at the short-range interactions in two channels. We consider two cases: two channels where one has a strong $s$-wave interaction which produces bound or virtual states, and a dimer state which couples weakly to weakly-coupled channels which in turn can produce narrow resonances. For each of these systems, we use well-defined power-counting schemes. The results can be used to investigate resonances in the charmonium and bottomonium systems. We demonstrate how the method can be applied to the $X(3872)$. The widths of the $X(3872)$ for decay processes to $\bar{D}^0 D^{*0}$ and $\bar{D}^0D^0\pi$ are calculated. We use these results to obtain the line shapes of the $X(3872)$ under different assumptions about the nature of this state.

Le développement de méthodes de synthèse asymétriques a largement été exploré au cours des vingt dernières années et en particulier par le biais de réactifs organométalliques. Bien que ces processus mènent à d’excellents résultats en terme d’énantiodiscrimination, l’objectif de cette thèse a été de développer de nouveaux outils de synthèse peu onéreux, respectueux des fonctions sensibles environantes et permettant l’accès aux composés attendus avec de bons rendements et excès énantiomériques. Dans cet optique, des triorganozincates de lithium chiraux ont été étudiés. Des méthodes d’alkylation et d’arylation 1,2 énantiosélectives d’aldéhydes, comportant comme partenaire chiral la (R)-N-(2-iso-butoxybenzyl)-1- phenyléthanamine, ont ainsi été développées et mises en application sur divers aldéhydes. Les alcools secondaires correspondants ont été obtenus avec de bons rendements (jusqu'à 83%) et d’excellents excès énantiomériques (jusqu'à 99%). Ces procédures ont ensuite été appliquées à la synthèse asymétrique de produits naturels et/ou bioactifs tels que la Spiromastilactone A, la (R)-Néobénodine et la (R)-Orphénadrine. Par ailleurs, la synthèse de nouveaux ligands de type amino-alcool a été développée dans le but ultime de désymétriser des substrats de type imines cycliques. / The development of new asymetric methodologies have been widely explored during the last twenty years and in particular through organometallic reagents. Although these processes lead to excellent results in terms of enantiodiscrimination, the goal of this thesis was to develop new tools: cheap, chemoselective and allowing the access to the desired compounds with high yields and enantiomeric excesses. In this context, chiral lithium triorganozincates have been studied. Enantioselective nucleophilic 1,2 alkylation and arylation of aldehydes reactions, including (R)-N-(2-iso-butoxybenzyl)-1-phenylethanamine as the chiral ligand, have been optimized toward various aldehydes. The expected secondary chiral alcohols have been obtained with good yields (up to 83%) and high enantiomeric excesses (up to 99%).These processes have been then applied to the asymmetric synthesis of naturals and/or bioactive compounds as Spiromastilactone A, (R)-Neobenodine and (R)-Orphenadrine. Finally, the access to new amino-alcohols have been developed with the ultimate goal to engage those species as the chiral partner when reacting chiral lithium zincates with imines.

Le ligand nacnacxylH (xyl = C6Me2H3) et les ligands dikétimines N-alkyle substitués (nacnacCH(Me)PhH, nacnacBnH and nacnaciPrH) ont été préparés avec de bons rendements à l’exception du nacnaciPrH (23%) en utilisant un protocole en une étape et à l’aide d’un montage Dean-Stark. La réaction du S,S-nacnacCH(Me)PhH et du nacnacBnH avec le nBuLi dans le THF conduit au S,S-nacnacCH(Me)PhLi(THF) et au nacnacBnLi(THF). Les tentatives de bromation de ces composés par le N-bromosuccinimide conduisent plutôt aux ligands S,S-succnacnacCH(Me)PhH et succnacnacBnH (succ = succinimido) substitués par un groupement succinimido sur le carbone  La chloration par le N-chlorosuccinimide conduit au produit désiré, mais avec des impuretés. La réaction de ces ligands avec le CuOtBu (ou bien MesCu, où Mes = C6Me3H2, et une quantité catalytique de CuOtBu) en présence de bases de Lewis donne les (nacnacxylCu)2(-toluène), nacnacxylCuCNC6H3(Me)2, nacnacCH(Me)PhCuL (L = PPh3, PMe3, CNC6H3(Me)2, DMAP, lutidine, Py, MeCN), nacnacBnCuL (L = PPh3, CNC6H3(Me)2, styrène, trans-stilbene, phenylvinylether, acrylonitrile, diphenylacetylène), nacnaciPrCuL (L = PPh3, CNC6H3(Me)2, MeCN) et le succnacnacCH(Me)PhCuL (PPh3, CNC6H3(Me)2, pyridine). Tous ces complexes sont jaunes et sensibles à l’air et à l’humidité. En l’absence de fortes bases de Lewis, on n’observe pas de réaction entre les précurseurs de cuivre et les ligands N-alkyle substitués. Les études RMN des complexes dans le C6D6 ne présentent pas de complexe de toluène mais un mélange à l’équilibre du (nacnacxylCu)2(-C6D6) et nacnacxylCu(C6D6) dans une proportion de 2 pour 1. Alors que l’addition de plus de cinquante équivalents soit de THF, soit de toluène n’induit aucun changement des spectres RMN, l’addition de 2 équivalents de MeCN conduit instantanément au complexe nacnacxylCu(MeCN). De plus, le (nacnacxylylCu)2(-C6D6) ne se coordone ni ne réagit avec le N2O, même après avoir été chauffé à 60°C pendant treize jours. En présence de DPA (diphenylacétylène), la réaction du nacnacBnH avec le CuOtBu conduit au dimère ponté (nacnacBnCu)2(µ-DPA). L’addition d’un excès de DPA (10-12 équivalents) transforme le dimère ponté en complexe lié en position terminale nacnacBnCuDPA. Les nacnacRH (R = CH(Me)Ph et i-Pr) ne forment pas de complexe ni avec les oléfines ni avec le DPA. Une réactivité similaire a été observée avec les complexes de nacnacCH(Me)PhCu(NCMe) et nacnaci-PrCu(NCMe). Tandis que le complexe lié en position terminale par MeCN a été isolé et caractérisé, l’équilibre en solution nous laisse suspecter la formation d’un complexe d’acétonitrile ponté. Des études de réactivité comparatives ont été menées sur quelques complexes de cuivre. La Morpholine ne réagit pas avec le nacnacBnCu(acrylonitrile) contrairement à l’acrylonitrile libre. L’expérience de l’échange d’oléfine montre que l’acrylonitrile (une oléfine électro-attractrice) se lie plus fortement que les autres oléfines, mettant ainsi en évidence l’importance de la rétrodonation  face à la donation La rétrodonation est cependant faible comparée aux autres complexes de styrène structurellement caractérisés. Les complexes nacnacCH(Me)PhCuL (L = PPh3 et MeCN) ont été employés dans la cyclopropanation catalytique du styrène et dans l’addition conjuguée du ZnEt2 sur la 2-cyclohexénone, mais les résultats indiquent que le ligand dikétimine est éliminé avant son entrée dans le cycle catalytique. Par conséquent, il n’y a pas d’induction chirale. Les complexes tétra coordinées de cuivre avec les nacnacRCu(phen) (R = Bn, CH(Me)Ph et Phen = 1,10-phenanthroline, 2-Mes-1,10-phenanthroline, 2,9-dimethyl-1,10-phenanthroline (dmp) et 2,9-diphenyl-1,10-phenanthroline (dpp)) ont été synthétisés. Ces complexes sont d’une intense couleur bleue et des interactions d’empilement entre l’un des cycles phényle des ligands nacnac et la phénanthroline ont été observées dans les structures à l’état solide. Les mesures en absorption UV-visible ont été effectuées dans le toluène et les bandes MLCT sont déplacées vers le rouge par rapport à celles des complexes de cuivre et bisphénanthroline. Tous ces composés émettent à l’état solide mais les complexes 1,10-phenanthroline et 2-Mes-1,10-phenanthroline n’émettent pas en solution. Pour renforcer les interactions d’empilement , les nouveaux ligands nacnacRH (R = CH2C6H2(OMe)3, CH2C6F5) et leurs complexes de cuivre respectifs ont été préparés avec du dmp et dpp. Afin de permettre la comparaison, le nacnaciBuCu(dmp) a été synthétisé. Alors que les complexes dmp montrent une augmentation des interactions intramoléculaires - avec les substituants phényle du ligand dikétimine et de la phénanthroline, les complexes dpp ne révèlent pas de telles interactions. Les complexes perfluorés montrent, en absorption et en émission, un déplacement significatif vers le bleu, alors que les complexes substitués par un groupements isobutyle présentent des transitions déplacées vers le rouge. Alors que les intensités de luminescence et les durées de vie sont faibles, les déplacements réduits de Stokes et les pics étroits de luminescence comparables indiquent une réduction des distorsions de l’état excité. / The ligand nacnacxylH (xyl = C6Me2H3) and the N-alkyl substituted diketimine ligands (nacnacCH(Me)PhH, nacnacBnH and nacnaciPrH) have been prepared in good yields except nacnaciPrH (23%) using a one-step procedure with the help of a Dean-Stark apparatus. Reaction of S,S-nacnacCH(Me)PhH and nacnacBnH with nBuLi in THF gave S,S-nacnacCH(Me)PhLi(THF) and nacnacBnLi(THF). Attempts to brominate these THF adducts with N-bromosuccinimide gave instead the -carbon substituted succinimido ligands S,S-succnacnacCH(Me)PhH and succnacnacBnH (succ = succinimido). Chlorination with N-chlorosuccinimide, afforded the desired product albeit with significant amounts of impurities. Reaction of these ligands with CuOtBu (or MesCu and catalytic amounts of CuOtBu, Mes = C6Me3H2) in the presence of Lewis bases gave (nacnacxylCu)2(-toluene), nacnacxylCuCNC6H3(Me)2, nacnacCH(Me)PhCuL (L = PPh3, PMe3, CNC6H3(Me)2, DMAP, lutidine, Py, MeCN), nacnacBnCuL (L = PPh3, CNC6H3(Me)2, styrene, trans-stilbene, phenylvinylether, acrylonitrile, diphenylacetylene), nacnaciPrCuL (L = PPh3, CNC6H3(Me)2, MeCN) and succnacnacCH(Me)PhCuL (PPh3, CNC6H3(Me)2, pyridine). All complexes are yellow and sensitive to air and moisture. There was no reaction between the copper precursors and the N-alkyl substituted ligands in the absence of strong Lewis bases. NMR studies of the complex (nacnacxylCu)2(-toluene) in C6D6, showed no toluene adduct but an equilibrium mixture of (nacnacxylCu)2(-C6D6) and nacnacxylCu(C6D6) in a ratio of 2:1. While addition of up to 50 equiv of either toluene or THF did not cause any significant change in the 1H NMR spectrum, addition of 2 equiv MeCN gave instantaneously the nacnacxylCu(MeCN) complex. In addition, (nacnacxylylCu)2(-C6D6) did not coordinate or react with N2O even after heating at 60 oC for thirteen days. In the presence of DPA (diphenylacetylene), reaction of nacnacBnH with CuOtBu yields the bridged dimer (nacnacBnCu)2(µ-DPA). Addition of excess DPA (10-12 equiv) converts the bridged dimer to the terminally bound complex nacnacBnCuDPA. NacnacRH (R = CH(Me)Ph and i-Pr) did not form complexes with olefins or with DPA. Similar reactivity was observed in nacnacCH(Me)PhCu(NCMe) and nacnaci-PrCu(NCMe) complexes. While the terminally bound MeCN complex was isolated and characterized, equilibrium in solution led us to suspect the formation of a bridged acetonitrile adduct. Reactivity and comparative studies were performed with several copper complexes. Morpholine did not react with nacnacBnCu(acrylonitrile) while free acrylonitrile does. Olefin exchange experiment showed that acrylonitrile (an electron withdrawing olefin) binds stronger than the other olefins examined, showing the importance of -backbonding relative to -donation. -Backbonding is, however, still low when compared other structurally characterized transition metal styrene complexes. Complexes nacnacCH(Me)PhCuL (L = PPh3 and MeCN) have been employed in catalytic cyclopropanation of styrene and the conjugate addition of ZnEt2 to 2-cyclohexenone, but results indicate that the diketimine ligand is lost before it enters the catalytic cycle. Hence, there was no chiral induction. Four-coordinate copper(I) complexes of the form nacnacRCu(phen) (R = Bn, CH(Me)Ph and Phen = 1,10-phenanthroline, 2-Mes-1,10-phenanthroline, 2,9-dimethyl-1,10-phenanthroline (dmp) and 2,9-diphenyl-1,10-phenanthroline (dpp)) were also prepared. The complexes are intensely blue in colour and intramolecular -stacking interactions between one of the phenyl rings of nacnac ligand with the phenanthroline were observed in the solid state structures. UV-vis absorption measurements were performed in toluene and the MLCT bands are red-shifted relative to those of bisphenanthroline copper complexes. All compounds are emissive in the solid state, but 1,10-phenanthroline and 2-Mes-1,10-phenanthroline complexes do not emit in solution. To buttress the -stacking interactions, the new ligands nacnacRH (R = CH2C6H2(OMe)3, CH2C6F5) and their respective copper complexes with dmp and dpp were prepared. For the sake of comparison, nacnaciBuCu(dmp) was prepared. While the dmp complexes showed enhanced -intramolecular interactions with both phenyl substituents of the diketimine ligand and the phenanthroline, dpp revealed no such interactions. The perfluorinated complex showed a significant blue-shift in absorption and emission spectra when compared to the other complexes, while the isobutyl substituted complex displayed red-shifted transitions. While luminescence intensities and lifetimes were low, reduced Stoke shifts and comparable sharp luminescence peaks indicate reduced distortions in the excited state.

Les molécules chirales représentent environ 60% des médicaments présents sur le marché pharmaceutique et plus de 80% des médicaments en développement avec plus de 150 milliards de dollars de chiffre d’affaire pour l’année 2002. Les intermédiaires chiraux sont fortement demandés dans l’industrie pharmaceutique atteignant 15 milliards de dollars de chiffre d’affaire en 2009. D’autres domaines en sont demandeurs avec une répartition d’environ 15% dans l’agrochimie et 5% pour la parfumerie. L’obtention de composés d’intérêt pharmaceutique de façon asymétrique est un réel défi et une réelle nécessité. Ces molécules possèdent une architecture spatiale qui entraîne des interactions spécifiques et des affinités particulières avec les enzymes ou des récepteurs biologiques chiraux. L’utilisation de catalyseurs pour accéder à des composés organiques chiraux et plus précisément l’oxydation d’alcanes prochiraux ou d’oléfines constitue un domaine en essor ces dernières décennies. Pour parvenir à synthétiser des molécules chirales, l’industrie pharmaceutique s’est tournée vers l’utilisation de biocatalyseurs en partie pour réaliser différentes réactions stéréo-contrôlées avec la nécessité de séparer les mélanges racémiques par résolution enzymatique. Cependant, les biocatalyseurs présentent un inconvénient majeur qui est généralement le faible rendement en composé chiral recherché et nécessite un savoir faire pour la manipulation de ces enzymes. Les métalloporphyrines sont des catalyseurs comportant un macrocycle tétrapyrrolique et différentes fonctionnalisations en positions méso. Ces molécules ont fait l’objet de nombreuses études qui ont conduit à la synthèse de métalloporphyrines chirales très complexes. Malheureusement, leur synthèse est souvent longue avec de faibles rendements et leur application à un nombre limité de substrats ne permet pas leur généralisation. Ce travail de thèse, développé pour la première fois au laboratoire, s’inscrit dans le cadre d'un contrat CIFRE, dans le but de parvenir à la synthèse de porphyrines chirales facilement accessibles, applicables dans des réactions d’oxydation énantiosélectives efficacement (stabilité). Le premier objectif visé est la synthèse de porphyrines chirales dont la structure ciblée comporte des groupements hétérocycliques azotés chiraux en position méso, reliés par une liaison carbone-hétéroatome (C-N). Nous avons pu atteindre 4 séries de porphyrines qui ont été évaluées dans des réactions d’oxydation énantiosélectives (époxydation, hydroxylation). Le deuxième objectif visé est d’exploiter les propriétés électroniques particulières des porphyrines permettant l’application des porphyrines en tant que photosensibilisant après photoactivation en thérapie anticancéreuse. L’étude des paramètres physiques est primordiale pour déterminer la longueur d’onde d’activation et le rendement quantique. Nous avons souhaité utiliser nos porphyrines et leurs précurseurs en tant qu’agents antiparasitaires, sans photoactivation dans un premier temps, conduisant à la découverte d’activités très intéressantes sur certaines espèce de leishmanies. Enfin, leur application sur P. falciparum nous a permis d’isoler une molécule avec une activité très intéressante. Dans les deux cas, des manipulations avec photoactivation sont en cours. / Chiral molecules represent about 60% of drugs in pharmaceutical market and over 80% of drugs in development with more than 150 billion dollars in 2002. Chiral intermediates are in high demand in the pharmaceutical industry producing a turnover of 15 billion dollars in 2009. Other areas are seekers of chiral molecules with a distribution of about 15% in agrochemicals and 5% for the perfume. Asymmetrically production of compounds of pharmaceutical interest is a real challenge. These molecules have a spatial architecture that results in specific interactions and affinity with the enzymes or biological chiral receptors. The use of catalysts to synthesis chiral organic compounds, and more specifically to oxidize alkenes and alkanes having prochiral positions, is a very important area extensively studied in recent decades with few positive results. To achieve the synthesis of chiral molecules, the pharmaceutical industry has turned to the use of biocatalysts, in part, to perform various stereo-controlled reactions with systematically followed by separation of the different isomers by different methodes. However, biocatalysts have a major disadvantage relative to low yields of chiral compound and requires expertise for handling these enzymes. Metalloporphyrins are tetrapyrrolic macrocyle substituted in meso position with various functional groups and incorporating metals (Fe, Mn, Co, Ru). These molecules have been extensively studied and led to the synthesis of many complex chiral metalloporphyrins. Unfortunately, their synthesis is often long with low yields and their application to a limited number of substrates is a major drawback. The first objective of this work is the synthesis of original chiral porphyrins. The targeted structure contains chiral heterocyclic nitrogen groups in two meso positions, connected by a carbon-heteoatom bond (C-N). We were able to reach 4 porphyrins-series that have been evaluated as catalyst in oxidation reactions (epoxidation, hydroxylation). The second objective is to take advantage of specific electronic properties of porphyrins for applications as photosensitizer after photoactivation for cancer by photodynamic therapy. The use of this therapy increased during last decades but poor specificity and solubility of the different porphyrins used in clinic against many cancers prompt us to investigate this area. The study of the physical parameters is essential to determine wavelength activation and quantum yield of a photosensitizer. We wanted to use our porphyrins and their precursors as antiparasitic agents, with and without photoactivation against L. donovani, L. major, T. brucei brucei. Malaria is caused by a protist of the genus of Plasmodium. This parasite has an iron deficiency on one hand and cannot biosynthesize certain amino acids. Strucure analogy of porphyrins with heme led us to evaluate antimalarial activity of several porphyrins against P. falciparum.

Dans cette thèse, je présente une étude que j'ai réalisée à l'université Paris-sud sous la direction de Thierry Jolicœur sur les phases des Hall Quantiques Fractionnaire (HQF) dans la géométrie du cylindre.Après une rapide introduction dans le premier chapitre, je présente dans le second quelques concepts de base de l'effet HQF et j'introduit certains aspects de la géométrie cylindrique.Le chapitre 3 est consacré à l'étude de la limite du cylindre fin, c'est à dire lorsque la circonférence du cylindre est de l'ordre de quelques longueurs magnétiques. Dans cette limite, on sait que la fonction d'onde de Laughlin au remplissage 1/q se réduit à un cristal unidimensionnel, où une orbitale sur q est occupée. Dans le but d'étudier un limite intermédiaire, nous conservons les quatre premiers termes du développement de l’Hamiltonien lorsque la circonférence est petite devant la longueur magnétique. On trouve alors une expression exacte de l'état fondamental au moyen d'opérateurs de "squeezing" ou de produits de matrices. Nous trouvons également une écriture similaire pour les quasi- trous, les quasi-électron et la branche magnétoroton.Dans les chapitres 4 et 5, je me concentre sur l'étude des excitations de bord chirales des phases de HQF. Je présente une étude microscopique de ces états de bord dans la géométrie du cylindre, lorsque les quasi-particules peuvent passer d'un bord à l'autre par effet tunnel. J'étudie d'abord dans le chapitre 4 la phase de HQF principale dont l'état fondamental est bien décrit par la fonction d'onde de Laughlin. Pour un échelle d'énergie plus faible que le gap du volume, le théorie effective est donnée par un fluide d'électrons unidimensionnel bien particulier : un liquide de Luttinger chiral. À l'aide de diagonalisations numériques exactes, nous étudions le spectre des états de bord formé de le combinaison des deux bord contre-propageant sur chacun des cotés du cylindre. Nous montrons que les deux bords se combinent pour former un liquide de Luttinger non-chiral, où le terme de courant reflète le transfert de quasi-particules entre les bords. Cela nous permet d'estimer numériquement les paramètre de Luttinger pour un faible nombre de particules, et nous trouvons une valeur cohérente avec la théorie de X. G. Wen.J'analyse ensuite dans le chapitre 5 les modes de bord des phases de HQF au remplissage 5/2. À partir une construction basée sur la Théorie des Champs Conformes (TCC), Moore et Read (Nucl. Phys. B, 1991) ont proposé que la physique essentielle de cette phase soit décrite par un état apparié de fermion composites. Une propriété importante de cet état est que ses excitations émergentes permutent sous une statistique non-abéliène. Lorsqu'elles sont localisées sur les bords, ces excitations sont décrites par un boson chiral et un fermion de Majorana. Dans la géométrie du cylindre, nous montrons que le spectre des excitations de bord est fomé des tours conformes du modèle IsingxU(1). De plus, par une méthode Monte-Carlo, nous estimons les différentes dimensions d'échelle sur des grands systèmes (environ 50 électrons), et nous trouvons des valeurs en accord avec les prédictions de la TCC.Dans le dernier chapitre de ce manuscrit, je présente un travail que j'ai réalisé à UBC (Vancouver) en collaboration avec Marcel Franz sur les phase de Hall quantiques de spin induites dans le graphène par des adatomes. Dans ce système, les adatomes induisent un couplage spin-orbite sur les électrons des la feuille de graphène et introduisent du désordre qui est susceptible de détruire le gap spectral. Nous montrons dans ce chapitre que le gap spectral est préservé lorsque des valeurs réalistes de paramètres sont usités. De plus, au moyen de calculs analytiques à base énergie et de diagonalisations numériques exactes, nous identifions un signal caractéristique dans la densité d'états locale mettant en évidence la présence d'un gap topologique. Ce signal pourrait être observé au moyen d'un microscope à effet tunnel. / I present in this thesis a study that I did in the university Paris-sud under the supervision of Thierry Jolicœur onto Fractional Quantum Hall (FQH) phases in the cylinder geometry. After a short introduction in the first chapter, I present some basic concept relative to the FQH effect in the second one and introduce some essential features relative to the cylinder geometry, useful for the chapters 3, 4, and 5. The chapter 3 is dedicated to the study of the thin cylinder limit, i.e. when the circumference of the cylinder is of the order of a few magnetic length. In this limit, it is known that the Laughlin wave function at the filling factor 1/q is reduced to a one dimensional crystal in the lowest Landau level orbitals where one every q orbitals is occupied. We Taylor expand the Hamiltonian when the circumference is small compare to the magnetic length in order to study an intermediate limit. When only the first four terms of the development are kept, it is possible to find exact representations of the ground state with "squeezing" operators or matrix products. We also find similar representations for quasiholes, quasielectrons and the magnetorton branch. These results have been published in the article Phys. Rev. B 85, 155116 (2012). In the chapter 4 and 5 I focus onto the gapless chiral edge excitations of FQH phases. I present a microscopic study of those edges states in the cylindrical geometry where quasiparticles are able to tunnel between edges. I first study the principal FQH phase at the filling fraction 1/3 whose ground state is well described by the Laughlin wave function in the chapter 4. For an energy scale lower than the bulk gap, the effective theory is given by a very peculiar one dimensional electron fluid localized at the edge: a chiral Luttinger liquid. Using numerical exact diagonalizations, we study the spectrum of edge modes formed by the two counter-propagating edges on each side of the cylinder. We show that the two edges combine to form a non-chiral Luttinger liquid, where the current term reflects the transfer of quasiparticles between edges. This allows us to estimate numerically the Luttinger parameter for a small number of particles and find it coherent with the one predicted by X. G. Wen theory. We published this work in Phys. Rev. B 86, 115214 (2012). I then analyze edge modes of the FQH phase at filling fraction 5/2 in the chapter 5. From a Conformal Field Theory (CFT) based construction, Moore and Read (Nucl. Phys. B, 1991) proposed that the essential physics of this phase is described by a paired state of composite fermions. A striking property of this state is that emergent excitations braid with non-Abelian statistics. When localized along the edge, those excitations are described through a chiral boson and a Majorana fermion. In the cylinder geometry, we show that the spectrum of edge excitations is composed of all conformal towers of the IsingxU(1) model. In addition, with a Monte Carlo method, we estimate the various scaling dimensions for large systems (about 50 electrons), and find them consistent with the CFT predictions.In the last chapter of my manuscript, I present a work that I did in UBC (Vancouver) in collaboration with Marcel Franz onto quantum spin Hall phases in graphene induced by adatoms. In this system, adatoms induce a spin orbit coupling for electrons in the graphene sheet and create some disorder which might be responsible for destruction the spectral gap. We show in this chapter and in the article [Phys. Rev. B 89, 201410(R) (2014)] that the spectral gap remains open for a realistic range of parameters. In addition, with analytical computations in the low energy approximation and numerical exact diagonalizations, we find characteristic signal in the local density of states highlighting the presence of topological gap. This signal might be observed in scanning tunneling spectroscopy experiments.

Grâce à leurs fortes acidités, les milieux superacides permettent d’accéder par polyprotonation à des intermédiaires superélectrophiles polycationiques, capables d’être piégés par des nucléophiles très faibles. Ces espèces très réactives ont permis de développer des méthodologies de synthèse sans équivalent en conditions « classiques ».Dans la première partie de ce travail, le comportement de composés organophosphorés dans le milieu HF/SbF5 a été évalué et les sites de protonation de différentes fonctions phosphorées ont pu être observés par RMN in situ à basse température. La réactivité d’oxydes de phosphines insaturés a également été évaluée et des composés organophosphorés cycliques et/ou fluorés ont été synthétisés avec de bons rendements. Des expériences de RMN in situ à basse température ont permis de mettre en évidence un intermédiaire superélectrophile de type phosphonium-carbénium inédit dont l’implication a été confirmée par des calculs théoriques.La deuxième partie est consacrée à l’exploitation de la contrainte benzylique d’espèces superélectrophiles. A partir d’éphédrines tosylées, des benzosultames cycliques ont été obtenus par cyclisation intramoléculaire diastéréospécifique dans l’acide trifluorométhanesulfonique. L’analyse des intermédiaires réactionnels par RMN a permis de révéler l’implication d’une contrainte benzylique contrôlant la spécificité de la réaction. Les benzosultames chiraux N-F obtenus après fluoration ont été utilisés comme réactifs de fluoration électrophile énantiosélective et la synthèse de dioxydes de méthanodibenzothiazocines chiraux inédits a également été envisagée. / Thanks to their exceptional acidity, superacid allow access to polycationic superelectrophiles by polyprotonation. These highly reactive species are capable of being trapped by very weak nucleophiles and can be used to develop new synthetic methodologies without equivalents under “classical” conditions. In the first part of this work, the behavior of organophosphorus compounds in HF/SbF5 was evaluated and the protonation sites of different phosphorus functions have been observed by low temperature NMR spectroscopy. The reactivity of unsaturated phosphine oxides has also been evaluated and cyclic and/or fluorinated organophosphorus compounds have been synthetized in good yields. In situ low-temperature NMR experiments revealed a phosphonium-carbenium superelectrophilic intermediate whose implication was confirmed by theoretical calculations. The second part deals with the study of the benzylic strain applied to superelectrophilic species. From tosylated ephedrines, cyclic benzosultams were obtained by diastereospecific intramolecular process in trifluoromethanesulfonic acid. Analysis of the reaction intermediates by NMR revealed the implication of a benzylic strain controlling the specificity of the reaction. After fluorination, the obtained N-F chiral benzosultams were used as enantioselective electrophilic fluorination reagents and the synthesis of new chiral methanodibenzothiazocine dioxides was also considered.

O presente trabalho consiste no estudo do papel da simetrial quiral no potencial nucleon-nucleon devido à troca de dois píons. Para o calculo do potencial foi levada em consideração a troca de dois píons não-correlacionados, envolvendo contribuicões com até um loop. A simetria quiral é introduzida no potencial através da sua realização não-linear, utilizando-se a Lagrangiana fenomenológica quiral de Weinberg. Os diagramas de Feynman construidos com os vértices dessa Lagragiana são ordenadas segundo potencias crescentes do momento, e calculados covariantemente. Os diagramas divergentes são regularizados covariantemente. Partindo do formalismo da equação de Bethe-Salpeter, relacionamos, em uma primeira etapa, as amplitudes de transição covariantes com o potencial, através do princípio da unitariedade elástica. O potencial, covariante e relativístico, e obtido no espaço dos momentos e é não-local e dependente da energia. Em uma segunda etapa, efetuamos a redução não-relativística do potencial e sua transformada de Fourier, obtendo um potencial local e independente da energia, que pode ser usado na equação de Schrödinger. O potencial obtido possui contribuições central, spin-orbita, tensorial e spin-spin. A parte dependente de isospin e semelhante à do potencial de Lemon e Partovi, sendo que as maiores modificações aparecem na parte isoescalar, principalmente no canal central, onde um substancial aumento de atração na região de 1.2 a 2.0 fm é observada. A fim de compararmos nosso potencial com a literatura, fixamos o valor de A como sendo 50 GeV, fazendo com que os efeitos do parâmetro de corte fiquem restritos à região r 0.5 fm. Os resultados obtidos foram comparados com o potencial fenomenológico de Argonne e revelaram razoável compatibilidade na maioria dos canais. Entretanto, existem discrepâncias importantes, possivelmente devidas a efeitos não estudados neste trabalho, tais como os devidos às ressonâncias A e p. / This work is devoted to the study of the role of chiral symmetry in the two pion exchange nucleon-nucleon potential. We consider only non-correlated two pion exchanges due to one loop contributions. Chiral symmetry is implemented in the potential through its non-linear realization, given by Weinberg\'s phenomenological Lagrangian. Feynman diagrams derived from this Lagrangian are arranged according to increasing powers of the momentum, and calculated covariantly. Divergent diagrams are regularizated covariantly. Starting from the Bethe-Salpeter equation, we relate the covariant transition amplitudes with the potential, using the elastic unitarity principle. The potential in momentum space is covariant, relativistic, non-local and energy dependent. Next, we perform its nonrelativistic reduction and Fourier transform, obtaining a potential which is local, energy independent and that can be used in the Schrödinger equation. This potential has central, spin-orbit, tensor and spin-spin components. The isospin dependent part is similar to that of the Lomon and Partovi potential, but important differences appear in the isoscalar part, especially in the central channel, where a substantial increase of attraction in the 1.2 to 2.0 fm region is observed. In order to compare our potential with the literature, we fixed the cutoff parameter at A = 50 GeV, restricting its effects to the r 0.5 fm region. Our results are compared with Argonne phenomenological potential, and a reasonable compatibility in most of the channels is found. However, there are also important discrepancies which may be due to effects not considered in this work, such as those due to A and the p ressonances.