Esta tese tem como objetivo contribuir para o conhecimento e desenvolvimento das células solares sensibilizadas por corantes, através da elaboração de novas espécies supramoleculares e de estudos fundamentais de caracterização do filme de TiO2-P25 e da interface TiO2-Corante pela técnica de microscopia Raman confocal. Os estudos de microcopia Raman confocal da distribuição das fases cristalinas rutilo e anatase em filmes de TiO2-P25 (Degussa) mostraram que a fase rutilo está presente em agregados de diferentes tamanhos (de 250 nm a 3 µm) distribuídos na fase anatase e que estes agregados permaneceram mesmo após os processos de preparação da suspensão coloidal. Na presença do corante N3, verificou-se que a irradiação com laser em 532 nm, usando potência acima de 25 mW cm-2, provoca a absorção e posterior combustão do filme interfacial, com drásticas mudanças na morfologia visualizadas por microscopia Raman confocal, revelando a ocorrência da transformação de anatase em rutilo na região de incidência do feixe de laser. Outro ponto investigado nesta tese, foi a síntese e aplicação de novos sensibilizadores supramoleculares em células solares sensibilizadas por corante (DSC), visando diminuir os processos de recombinação e melhor aproveitamento do espectro solar através da estabilização do corante foto-oxidado e da transferência vetorial de elétron/energia. Além dos trabalhos com novas porfirinas supramoleculares, reproduzidas no apêndice, esta tese apresenta um estudo detalhado de uma série, formada por três espécies diméricas, constituídas pelas unidades [Ru(dcbH2)Cl]+ e [Ru(dmb)2Cl]+, unidas por ligantes ponte com dimensões lineares crescentes, isto é: bpy, bpe e bpeb (dcbH2= ácido-2,2\'-bipiridina-4,4\'-dicarboxílico, dmb= 4,4\'-dimetil-2,2\'- bipiridina, bpy= 4,4\'-bipiridina, bpe= trans-1,2-bis(4-piridil)-etileno e bpeb= trans-1,4- bis[2-(piridil)etenil]-benzeno). O rendimento global das DSCs correspondentes cresceram com o aumento do tamanho da ponte, passando de 2,78 % para o corante dim-Ru-bpy, para 2,89 e 3,25 % nos corantes dim-Ru-bpe e dim-Rbpeb, respectivamente. Foi observado que os valores de Jsc e η têm correlação linear com a distância de separação do buraco e da superfície do eletrodo de TiO2, ratificando que o processo de retardação da recombinação de carga, causado pelo aumento da ponte, é um fator muito importante para esta classe de compostos. Os resultados de IPCE mostraram que a unidade [Ru(dmb)2Cl(P)]+ também é responsável pela fotoinjeção de elétrons no TiO2. Assim, a excitação de qualquer uma das unidades, sempre acaba formando a espécie TiO2(e-)-Ru-Ru(h+) no filme interfacial. Os resultados confirmam as expectativas esperadas no planejamento energético vetorial, no qual o HOMO foi centrado na unidade distante da superfície e o LUMO ficou sobre a dcbH2 diretamente ancorada no superfície do TiO2. / This thesis encompasses our efforts to improve the knowledge and contribute to the development of dye-sensitized solar cells, by focusing on supramolecular design of new dyes and on critical aspects of the morphology of the TiO2-P25 and TiO2-Dye interfaces, as probed by confocal Raman microscopy. According to Raman imaging of the crystalline phase distribution of TiO2-P25 (Degussa) rutile was present as aggregates of different sizes (from 250 nm to 3 µm) dispersed in the 25 nm anatase powder, persisting even after applying criterious procedures for generating uniform colloidal suspensions. In addition, the irradiation of TiO2-P25 films containing adsorbed N3 dye, using a 532 nm laser (power over to 25 mW cm-2) led to the absorption and instantaneous combustion of the dye, promoting drastic local changes associated with the anatase to rutile conversion. The design and application of new supramolecular sensitizers in DSC has also been pursued, aiming an improvement of efficiency by slowing down the electron-hole recombination process, while enhancing the light harvesting effects in the visible range by means of vectorial electron/energy transfer. Studies concerning another efficient supramolecular porphyrin dye, have also been performed and published (Appendix). As the main subject, a series of dimeric species have been reported. They were based on the [Ru(dcbH2)Cl]+ and [Ru(dmb)2Cl]+ units connected by linear bridging ligands of increasing lengths, such as: bpy, bpe and bpeb (dcbH2= 2,2\'-bipyridine-4,4\'-dicarboxylic acid, dmb= 4,4\'-dimethyl-2,2\'-bipyridine, bpy= 4,4\'-bipyridine, bpe= trans-1,2-bis(4- pyridyl)-ethylene e bpeb= trans-1,4-bis[2-(4-pyridyl)ethenyl]-benzene). The overall yield of the corresponding DSCs increased with the bridging ligand length, from 2.78 % for dim-Ru-bpy, to 2.89 % and 3.25 % for dim-Ru-bpe and dim-Ru-bpeb, respectively. The electrochemical parameters associated with the short circuit current exhibited a linear correlation with the hole separation distance between the TiO2 electrode and the binuclear dye terminal, confirming that the retardation of charge recombination through the increasing distance is indeed a relevant factor for this series of compounds. The IPCE results indicated that the [Ru(dmb)2Cl(P)]+ unit is also involved in electron transfer, such that the dye excitation always leads the TiO2(e-)-Ru-Ru(h+) species. This conclusion confirmed the success of the supramolecular design and vectorial transfer strategy, in which the HOMO center was placed far away from the surface, but in communication with the LUMO center located at the dcbH2 group anchored on TiO2.

No description available.

Esta tese tem como objetivo contribuir para o conhecimento e desenvolvimento das células solares sensibilizadas por corantes, através da elaboração de novas espécies supramoleculares e de estudos fundamentais de caracterização do filme de TiO2-P25 e da interface TiO2-Corante pela técnica de microscopia Raman confocal. Os estudos de microcopia Raman confocal da distribuição das fases cristalinas rutilo e anatase em filmes de TiO2-P25 (Degussa) mostraram que a fase rutilo está presente em agregados de diferentes tamanhos (de 250 nm a 3 µm) distribuídos na fase anatase e que estes agregados permaneceram mesmo após os processos de preparação da suspensão coloidal. Na presença do corante N3, verificou-se que a irradiação com laser em 532 nm, usando potência acima de 25 mW cm-2, provoca a absorção e posterior combustão do filme interfacial, com drásticas mudanças na morfologia visualizadas por microscopia Raman confocal, revelando a ocorrência da transformação de anatase em rutilo na região de incidência do feixe de laser. Outro ponto investigado nesta tese, foi a síntese e aplicação de novos sensibilizadores supramoleculares em células solares sensibilizadas por corante (DSC), visando diminuir os processos de recombinação e melhor aproveitamento do espectro solar através da estabilização do corante foto-oxidado e da transferência vetorial de elétron/energia. Além dos trabalhos com novas porfirinas supramoleculares, reproduzidas no apêndice, esta tese apresenta um estudo detalhado de uma série, formada por três espécies diméricas, constituídas pelas unidades [Ru(dcbH2)Cl]+ e [Ru(dmb)2Cl]+, unidas por ligantes ponte com dimensões lineares crescentes, isto é: bpy, bpe e bpeb (dcbH2= ácido-2,2\'-bipiridina-4,4\'-dicarboxílico, dmb= 4,4\'-dimetil-2,2\'- bipiridina, bpy= 4,4\'-bipiridina, bpe= trans-1,2-bis(4-piridil)-etileno e bpeb= trans-1,4- bis[2-(piridil)etenil]-benzeno). O rendimento global das DSCs correspondentes cresceram com o aumento do tamanho da ponte, passando de 2,78 % para o corante dim-Ru-bpy, para 2,89 e 3,25 % nos corantes dim-Ru-bpe e dim-Rbpeb, respectivamente. Foi observado que os valores de Jsc e η têm correlação linear com a distância de separação do buraco e da superfície do eletrodo de TiO2, ratificando que o processo de retardação da recombinação de carga, causado pelo aumento da ponte, é um fator muito importante para esta classe de compostos. Os resultados de IPCE mostraram que a unidade [Ru(dmb)2Cl(P)]+ também é responsável pela fotoinjeção de elétrons no TiO2. Assim, a excitação de qualquer uma das unidades, sempre acaba formando a espécie TiO2(e-)-Ru-Ru(h+) no filme interfacial. Os resultados confirmam as expectativas esperadas no planejamento energético vetorial, no qual o HOMO foi centrado na unidade distante da superfície e o LUMO ficou sobre a dcbH2 diretamente ancorada no superfície do TiO2. / This thesis encompasses our efforts to improve the knowledge and contribute to the development of dye-sensitized solar cells, by focusing on supramolecular design of new dyes and on critical aspects of the morphology of the TiO2-P25 and TiO2-Dye interfaces, as probed by confocal Raman microscopy. According to Raman imaging of the crystalline phase distribution of TiO2-P25 (Degussa) rutile was present as aggregates of different sizes (from 250 nm to 3 µm) dispersed in the 25 nm anatase powder, persisting even after applying criterious procedures for generating uniform colloidal suspensions. In addition, the irradiation of TiO2-P25 films containing adsorbed N3 dye, using a 532 nm laser (power over to 25 mW cm-2) led to the absorption and instantaneous combustion of the dye, promoting drastic local changes associated with the anatase to rutile conversion. The design and application of new supramolecular sensitizers in DSC has also been pursued, aiming an improvement of efficiency by slowing down the electron-hole recombination process, while enhancing the light harvesting effects in the visible range by means of vectorial electron/energy transfer. Studies concerning another efficient supramolecular porphyrin dye, have also been performed and published (Appendix). As the main subject, a series of dimeric species have been reported. They were based on the [Ru(dcbH2)Cl]+ and [Ru(dmb)2Cl]+ units connected by linear bridging ligands of increasing lengths, such as: bpy, bpe and bpeb (dcbH2= 2,2\'-bipyridine-4,4\'-dicarboxylic acid, dmb= 4,4\'-dimethyl-2,2\'-bipyridine, bpy= 4,4\'-bipyridine, bpe= trans-1,2-bis(4- pyridyl)-ethylene e bpeb= trans-1,4-bis[2-(4-pyridyl)ethenyl]-benzene). The overall yield of the corresponding DSCs increased with the bridging ligand length, from 2.78 % for dim-Ru-bpy, to 2.89 % and 3.25 % for dim-Ru-bpe and dim-Ru-bpeb, respectively. The electrochemical parameters associated with the short circuit current exhibited a linear correlation with the hole separation distance between the TiO2 electrode and the binuclear dye terminal, confirming that the retardation of charge recombination through the increasing distance is indeed a relevant factor for this series of compounds. The IPCE results indicated that the [Ru(dmb)2Cl(P)]+ unit is also involved in electron transfer, such that the dye excitation always leads the TiO2(e-)-Ru-Ru(h+) species. This conclusion confirmed the success of the supramolecular design and vectorial transfer strategy, in which the HOMO center was placed far away from the surface, but in communication with the LUMO center located at the dcbH2 group anchored on TiO2.

This thesis presents a series of studies of quenched random disorder (QRD) on liquid crystals. We have used high-resolution AC-Calorimetry, high-resolution X-Ray Diffraction (XRD), X-Ray Intensity Fluctuation Spectroscopy (XIFS), Turbidity, Integrated Low-Angle Light Scattering (ILALS), as well as Polarizing Microscopy to characterize the effects of a nano-colloidal dispersions of aerosils in the phase transitions of several liquid crystals. The aerosil ($SIL$) is made of 70~AA~ diameter SiO$_{2}$ particles coated with hydroxyl (-OH) groups. The coating allows the $SIL$ particles to hydrogen-bond together, to form a very low density gel in an organic solvent. This provides the quenched random disorder. The liquid crystals of interest are: octyloxycyanobiphenyl ($8OCB$), 4-extit{n}-pentylphenylthiol-4'-extit{n}-octyloxybenzoate (ar{8}$S5), 4'-transbutyl-4-cyano-4-heptyl-bicyclohexane ($CCN47$), and octylcyanobiphenyl ($8CB$). Studies have been carried out as a function of aerosil concentration and temperature spanning the following phase transitions, Isotropic to Nematic (emph{I-N}), nematic to smectic-emph{A} (emph{N-SmA}), smectic-emph{A} to smectic-emph{C} (emph{SmA-SmC}), and crystallization.

Les travaux présentés dans ce manuscrit portent sur la conception, simulation et réalisation des nouvelles structures des commutateurs hyperfréquences basées sur l’intégration des couches minces des matériaux innovants fonctionnels tels que les matériaux à changement de phase (PCM) et les matériaux à transition de phase (PTM). Le principe de fonctionnement de ces composants repose sur le changement de résistivité présenter par ces matériaux. Nous avons exploité le changement de résistivité réversible du GeTe de la famille des matériaux à changement de phase (PCM) entre les deux états : amorphe à forte résistivité et cristallin à faible résistivité, pour réaliser une nouvelle structure d’un simple commutateur SPST. Ensuite, nous avons intégré ce commutateur dans une nouvelle structure de la matrice de commutation DPDT (Double Port Double Throw) à base de PCM pour l’application dans la charge utile du satellite. Nous avons utilisé la transition isolant-métal présenté par le dioxyde de vanadium (VO2) de la famille des matériaux à transition de phase, pour réaliser une nouvelle structure de commutateur simple à deux terminaux sur une très large bande de fréquence (100 MHz–220 GHz). / The work presented in this manuscript focuses on the design, simulation and realization of new microwave switches structures based on the integration of thin layers of innovative functional materials such as phase change materials (PCM) and phase transition materials. (PTM). The operating principle of these components is based on the change of resistivity present by these materials. We exploited the reversible resistivity change of GeTe of phase change materials family between the two states: amorphous with high resistivity and crystalline with low resistivity to realize a new structure of SPST switch. Then, we have integrated this switch structure on a new structure of DPDT (Double Port Double Throw) switch matrix based on phase change materials for application in satellite payload. We have used the insulatingmetal transition presented by the vanadium dioxide (VO2) of phase transition materials family to realize a new two terminals simple switch structure on a very wide frequency band (100 MHz–220 GHz).

Les sismologues ont révélé l'existence d'une anisotropie sismique complexe dans la graine terrestre. Cette thèse, en deux parties, présente deux approches différentes pour, d'une part, expliquer l'existence de cette anisotropie avec des modèles de graine numérique et, d'autre part, étudier l'effet des transformations de phase sur cette anisotropie.Dans un premier temps, nous avons construit un outil de simulation de la propagation des rais sismiques à travers une graine numérique, afin d'étudier la possibilité de reproduire numériquement les données sismologiques et de contraindre la dynamique et la minéralogie de la graine. Nous concluons qu'aucune structure du fer cubique ne permet de développer une anisotropie sismique significative. Seule la structure hexagonale compacte permet de le faire. Parmi les modèles géodynamiques quadripolaires étudiés, la croissance équatoriale préférentielle est le processus dynamique qui présente le meilleur accord avec les observations de dépendance à la profondeur et d'anisotropie polaire. L'ajout d'une stratification chimique permet d'amplifier d'environ 40% l'anisotropie globale mais augmente la dispersion des résidus sismiques, ce qui n'est pas conforme aux observations de dépendance à la profondeur. Enfin, une croissance dendritique (texture de solidification) est peu compatible avec une anisotropie principale Nord-Sud. Il apparaît clairement qu'aucun de ces modèles géodynamiques ne permet d'obtenir une amplitude d'anisotropie suffisante en utilisant les propriétés élastiques publiées pour le fer dans la graine. A l'issue de ce travail, de nombreux autres processus dynamiques restent encore à étudier, tels que les forces de Lorentz et la translation-convection thermique, processus bipolaire qui présente un fort intérêt pour la caractérisation de la composante hémisphérique de l'anisotropie sismique.Dans un deuxième temps, nous avons procédé à des expériences de transition de phase α-ε (fer cubique centré vers fer hexagonal compact) dans le fer pur. Nous avons simulé les textures résultantes à l'aide du mécanisme de Burgers. Nous avons confronté nos simulations aux résultats expérimentaux. Nous avons pu confirmer la validité du mécanisme de transformation de Burgers. Nous avons trouvé une forte sélection de variant sous l'effet de la contrainte non-hydrostatique dans le sens direct α→ε, produisant de fortes textures. Dans le sens inverse ε→α, on observe des textures finales très faibles, voire aléatoires. Appliqués avec prudence au cas de la graine terrestre, nos résultats indiquent que la transformation de phase du fer hexagonal à cubique ne peut pas expliquer la forte anisotropie observée. Nous avons aussi noté une mémoire de texture partielle, déjà documentée pour d'autres métaux de transition. Enfin, nous avons procédé à des tests préliminaires en cellule diamant en rotation. Les résultats de ces expériences de cisaillement ont également montré un très bon accord avec les simulations fondées sur le mécanisme de Burgers. En revanche, nous avons pu constater de grands écarts entre nos résultats expérimentaux et les simulations en cisaillement présentées dans la littérature [Levitas et al., 2010], notamment en termes de gradient de contraintes. / Seismologists revealed the existence of a complex seismic anisotropy in the Earth's inner core. In this thesis we took two different approaches in order to characterize the anisotropy: in a first part, we tried to explain this anisotropy using formation models of inner core and, in a second part, we considered the impact of eventual phase transitions on anisotropy.Firstly, we simulate the propagation of seismic rays through a numerically grown inner core, in order to measure the seismic anisotropy to compare with actual observations and to constrain the dynamics and mineralogy of the inner core. We conclude that no cubic structure of iron may produce a significant global anisotropy. Only the hexagonal compact phase of iron may produce a measurable signal. Considering a panel of quadripolar geodynamical models, we observe that simple preferential equatorial growth is the most consistent with seismological observations of a polar anisotropy and depth dependence of seismic residuals. Chemical stratification amplifies the global anisotropy by about 40%, but at the same time increases the scatter of residuals in a way that is poorly compatible with the observed depth dependence. Finally the addition of dendritic growth (solidification texture) prohibits the emergence of a first order North-South anisotropy. Independently of the geodynamical model it appears clearly that none of these geodynamical models the development of an anisotropy consistent with observations when using the published elastic properties of iron at inner core conditions. Following this work, several geodynamical models remain to be studied such as magnetic forcing (Lorentz forces). Models involving translation-thermal convection are of great interest as they may account for the hemispherical component of the seismic anisotropy.Secondly, we performed experiments on the α-ε (cubic centered to hexagonal compact iron) phase transition in pure iron. We compare our experimental texture results with our simulations of the transformation considering Burgers mechanism. We confirm here the Burgers atomic path as the mechanism activated during the α-ε transformation in iron. We find direct evidence of a strong variant selection controlled by non-hydrostatic stresses in the diamond anvil cell during the forward α→ε transformation, producing strong textures. The opposite will occur with the reverse ε→α phase transition where an almost complete randomization is to be expected. Our observations can be applied with some caution to the Earth's inner core and show that the strong seismic anisotropy in the inner core may not be explained by the occurrence of a hexagonal to cubic phase transition in the inner core. A limited texture memory effect was brought into light, already documented for other transition metals. At last, we performed a preliminary study on the effect of shear on the α-ε phase transition in pure iron using a rotational cell. Again the α-ε phase transformation in iron can be modelized by the Burgers mechanism. We find that simulations in the literature [Levitas et al., 2010] fail to reproduce our experimental results, particularly in terms of stress field.

Conselho Nacional de Desenvolvimento CientÃfico e TecnolÃgico / FundaÃÃo Cearense de Apoio ao Desenvolvimento Cientifico e TecnolÃgico / No presente trabalho foram realizadas medidas de espalhamento Raman polarizado em cristais de L-metionina e de DL-alanina (dois aminoÃcidos) e em diversas amostras de nanotubos de carbono de parede simples (SWNT). As medidas de espalhamento Raman em cristais de L-metionina foram realizadas no intervalo espectral entre 50 cm-1 e 3100 cm-1 desde a temperatura ambiente atà a temperatura de 17 K. No intervalo de temperatura estudado a estrutura da L-metionina manteve-se estÃvel. à temperatura ambiente tambÃm foram realizadas medidas Raman em altas pressÃes hidrostÃticas. A mÃxima pressÃo atingida foi de 4,7 GPa e diversas modificaÃÃes nos modos associados Ãs unidades CO2, NH3, CC, CS, CH, CH2 e CH3 sugerem que a L-metionina sofre um transiÃÃo estrutural de fase em torno de 2,1 GPa com histerese de aproximadamente 0,8 GPa. No cristal de DL-alanina foram realizadas medidas de espalhamento Raman no intervalo de temperatura de 15 K a 295 K. Embora nenhuma mudanÃa significativa tenha sido observada neste intervalo de temperatura, os resultados sÃo importantes para se entender o comportamento de uma molÃcula fundamental na constituiÃÃo das proteÃnas. Medidas de espalhamento Raman em SWNTâs foram realizadas em amostras preparadas pela tÃcnica de arco voltÃico, utilizando-se vÃrios catalisadores metÃlicos. As amostras foram divididas em duas sÃries: A primeira com os catalisadores à base de MnNiCo e a segunda à base de FeNiCo. Em ambas as sÃries observou-se que a inserÃÃo de CÃrio (Ce) foi responsÃvel por tornar a distribuiÃÃo de diÃmetros do subconjunto ressonante com a energia 2,41 eV mais estreita. AlÃm disso, o mÃximo da distribuiÃÃo à deslocado para o azul, provavelmente em conseqÃÃncia da seleÃÃo de tubos de menor diÃmetro dentro do subconjunto estudado. A inserÃÃo de ZircÃnio (Zr) à segunda sÃrie nÃo trouxe mudanÃas significativas. Foram realizadas medidas de espalhamento Raman em funÃÃo da pressÃo hidrostÃtica em uma amostra comercial de SWNT. Como fluido transmissor foram utilizadas soluÃÃes de dois surfactantes: o dodecil sulfato de sÃdio (SDS) e o Ãcido plurÃnico F127 (F127). Devido à baixa relaÃÃo sinal-ruÃdo, nÃo foi possÃvel estudar o comportamento dos modos de respiraÃÃo radial (RBM), mas pela descontinuidade do grÃfico da freqÃÃncia em funÃÃo da pressÃo dos modos tangenciais em aproximadamente 2 GPa à provÃvel que os nanotubos sofram uma transiÃÃo de fase estrutural nessa pressÃo, com deformaÃÃo da seÃÃo circular dos tubos como predito por estudos teÃricos. Dois conjuntos de amostras contendo diferentes nÃveis de inserÃÃo de lÃtio tambÃm foram estudados por espectroscopia Raman. Cada conjunto era formado por uma amostra sem lÃtio, uma com lÃtio e a terceira com inserÃÃo parcial de lÃtio (obtida pela lavagem da amostra que contÃm lÃtio). Nos dois conjuntos a inserÃÃo foi eficiente, contudo o mecanismo de inserÃÃo à diferente de uma sÃrie para outra. Na primeira sÃrie o catalisador utilizado para a inserÃÃo de lÃtio foi LiNi0,5Co0,5O2. Com este composto o lÃtio à intercalado intersticialmente e pode ser removido quase que completamente pela lavagem da amostra. Jà na segunda sÃrie o composto utilizado foi LiCO3/NiO/CoO o que fez com que o lÃtio fosse intercalado dentro dos tubos de modo a nÃo ser removido pela lavagem da amostra. / This work describes polarized Raman scattering measurements in L-methionine and in DL-alanine (two amino acids) crystals and in several samples of single-walled carbon nanotubes (SWNT). In L-methionine crystal the Raman spectra were obtained from 17 K to 295 K in the spectral range from 50 cm-1 to 3100 cm-1, but no indication of a phase transition was observed. At room temperature, Raman scattering measurements were also performed for pressure up to 5 GPa. Several changes observed in the spectra were interpreted as due to structural phase transition undergone by L-methionine crystal at ~ 2.1 GPa. The results for decompression show that the phase transition is reversible with a hysteresis of ~ 0.8 GPa. In DL-alanine crystal the Raman spectra were obtained at temperatures from 15 K to 295 K over the spectral range 50 cm-1 - 3100 cm-1. No evidence of structural phase transition was found in this range of temperature, although information about diverse modes of the crystal were furnished. Samples of SWNTâs studied were prepared with metallic catalysts using the arc voltaic method. MnNiCo was the main compound of the first series and FeNiCo, the main compound of the second. In both sets it was observed that Cerium (Ce) insertion induces in the sub-set, probed with the 2.41 eV excitation energy, a narrowing of the diameter distribution favoring the tubes with smaller diameter. The Raman scattering measurements in a commercial sample of SWNTâs show a discontinuity at about 2 GPa. The discontinuity was represented by a changing in the slope of the frequency versus pressure for tangential modes. The measurement was performed twice, using two different solutions of surfactants, sodium dodecil sulfate (SDS) and plurocic acid F127 (F127), and the results were similar. The anomaly was interpreted as due to the deformation of the tubes as predicted theoretically. Two sets of three samples of SWNTâs containing different levels of lithium insertion were also analyzed by Raman spectroscopy. Each set of sample was formed by a sample with lithium, a sample without lithium and a sample with partial insertion of lithium. The results show that the lithium is efficiently intercalated with both lithium containing compound (LiCO3/NiO/CoO and LiNi0.5Co0.5O2), but the mechanism of intercalation differs from one to the other. The intercalation is unstable when lithium is intercalated interstitially (LiNi0.5Co0.5O2) and it can be removed almost completely by washing the sample, but if the lithium is intercalated inside the tubes (LiCO3/NiO/CoO) it can not be removed by the same process.

A liquid Cooled below its normal freezing temperature is known as a supercooled liquid. On further cooling, supercooled liquids crystallize to thermodynamically stable, ordered structures. Alternatively, if the cooling rate is fast enough, the crystallization may be avoided altogether. Below a particular temperature during rapid cooling the liquid will solidify into a disordered, amorphous phase -also known as the glassy phase of matter. This particular temperature is termed the ”glass transition temperature” (Tg). Unlike a crystalline solid, a glass is neither a thermodynamically stable phase nor does it possess long range molecular ordering. Very slow structural relaxation (in the time scale of ∼ 100 s) is always present in the glassy phase. Thus, this phase is often referred to as a metastable phase of matter. Experimental and theoretical studies related to the behavior of supercooled liquids are the subject matter of many investigations for the last few decades [1]. These studies find their applications in diverse fields such as geology, cryopreservation, glaciology and atmospheric science. However, properties of supercooled liquids and the corresponding amorphous phase are not completely understood at present, particularly for hydrogen bonded (H-bonded) systems. This thesis concerns both the crystallization and the glass formation process of H-bonded systems. The systems of interest are water, the commonly accepted universal solvent, and the aqueous binary mixture of glycerol and water. The technique of molecular probing is often used to study the cooperativety and rotational diffusion of supercooled liquids and for determination of the glass transition temperature. For the present set of work, a molecular probe technique called spin probe ESR is extensively used. Electron paramagnetic resonance or electron spin resonance (EPR/ESR) measures the electronic energy level separation and is well known for the high sensitivity. All of the systems studied in the present set of work are diamagnetic. This issue is circumvented by dissolving paramagnetic spin probe molecules, which are usually organic free radicals with one N-O group, into the systems. Spin probes are added in very low concentrations (~10-3M) to minimize the effect on the host system and also to avoid mutual interactions between them. The unpaired electron delocalized in the direction of the N-O bond serves as the paramagnetic center required for an ESR experiment. The splitting of electron energy level due to the external magnetic field (Zeeman splitting) can give rise to resonance absorption of energy if exposed to a microwave of appropriate frequency. There is also a magnetic coupling (hyperfine) between the spin of the unpaired electron and nuclear spin of the nearby nitrogen atom. The hyperfine coupling splits each electron energy levels, to the first order, symmetrically into three levels. The transitions between these levels -subject to appropriate selection rules -give rise to the ESR spectrum [2]. The spectral shape in a magnetic field sweep ESR experiment appears complex if randomly oriented spin probes are dispersed in an amorphous or polycrystalline solid matrix. The high degree of mobility in probe molecules, present in a liquid solution, can average out the individual anisotropy of magnetic tensors to get a spectrum of three equally spaced liens. Experiments can be performed spanning a spin probe reorientation timescale of 10-7-10-12 s typically in the temperature range of 4.2 -300K. In chapter one we have given a brief overview of the supercooled liquids and the phase transitions related to the present work. Particular emphasis has been given to the dynamical features of the supercooled liquid close to its glass transition temperature and their classification based on the degree of ’fragility’ [3]. Brief general introductions of the systems studied in each of the following chapters are also provided. Then, the details of ESR spectroscopy and a quantum mechanical picture of the method of spin probe ESR have been discussed [4]. A separate section has been devoted to the numerical and analytical methods used to analyze the spectrum to extract information related to the spin probe dynamics [5]. The chapter concludes with a description of the ESR spectrometer. In chapter two we have studied the glass transition and dynamics of the supercooled water by the method of spin probe ESR. The vitrification has been done by direct exposure of the bulk water sample, doped with the spin probe TEMPOL, to the liquid helium flow. The vitrified matrix turns into the ultraviscous liquid above the putative glass transition temperature of ~136 K which further transforms to cubic ice (Ic) above TX ~150 K. The supercooled fraction of water, along with the spin probes which are treated as impurities by the crystallized surroundings, remain trapped inside the veins or triple junctions of the ice grains which serve as the interfacial reservoir of impurities in a polycrystalline ice matrix. The spectra for the entire temperature range have been analyzed with the help of in-depth computation by modelling the reorientation of TEMPOL in terms of the jump angle θs and the rotational correlation time τ [5]. This model, based on a homogeneous mobility scenario of the spin probe, works nicely except in the temperature range of 140-180 K. Dynamical heterogeneity (DH) is apparent in this temperature range and a more mobile (fast) component, as compared to the one corresponding to the very slow dynamics of TEMPOL at lower temperatures (slow), is observed. The relative weight of the fast and the slow component changes with temperature and above ~180 K the entire spectrum changes into the motionally narrowed triplet. The temperature dependence of the slow component of τ shows a change in slope at a temperature close to the putative glass transition temperature of water. The fast component of τ exhibits a fragile, i.e. non-Arrhenius character at high temperature with a crossover to a strong, i.e. Arrhenius behavior below ~225 K, close to the hypothesized fragile-to-strong crossover (FSC) for water at TFSC ~228 K. The breakdown of the Debye-Stokes-Einstein (DSE) law is observed when the τ values are combined with the available viscosity data of water to evaluate the DSE ratio, paralleling the SE breakdown which has recently been observed in nanoconfined water [6]. The dynamical heterogeneity is thought to be closely associated with the static structural heterogeneities of supercooled water. The existence of large scale structural fluctuations spanning a range of low-and high-density phases of liquid water have been associated with the heterogeneous dynamics sensed by TEMPOL. Motivated by the Arrhenius like behavior of the slow component, it has been identified with the low density liquid (LDL). The fragile nature of the fast component at high temperature may be identified with that of the high density liquid (HDL) which is the predominant fraction in liquid or weakly supercooled water [6]. Chapter three reports the studies on freezing and dynamics of the supercooled water trapped inside the veins of a polycrystalline ice matrix by dissolving spin probes TEMPO and TEMPOL into it. When a millimolar spin probe aqueous solution is cooled below the freezing point of water, the spin probes -driven by the mechanism described above migrate to the liquid environment inside the ice veins. Local concentration of the probe molecules inside the veins can go up to 1-10 M [7]. Bulk crystallization is evident in differential scanning calorimetry (DSC) studies whereas the liquid environment of the spin probe below the bulk freezing is confirmed by its narrow triplet ESR spectrum. A sudden collapse of this narrow triplet into a single broad line indicates the freezing of the trapped water fraction which usually happens well below the DSC freezing point for both the probes. The spin probe detected freezing point of this interstitial water is found to be largely dependent on the properties and the amount of the dissolved probe molecules. An explanation is sought in terms of the ’destructuring effect’ on the tetrahedral ordering of the water H-bond network by both the high local concentration of the spin probes and the hydrogen bond strength, formed between the water and the spin probe molecules through the polar groups of the latter [8, 9]. These two factors are thought to play important roles in determining the reorientational dynamics of the spin probe molecules, as well. The rotational correlation times of the two probes exhibit a crossover owing to the different mobility of their salvation shells in the more ordered supercooled water. The observed relaxation behavior of this confined water using the probe TEMPO, which has little effect on water H-bond network, is found in agreement with the previous experimental investigations on water confined in a nanochannel [10]. In chapter four, the glass transition, relaxation and the free volume of the glycerol-water (G-W) system are studied over the glycerol concentration range of 5 -85 mol% with TEMPO as the spin probe. G-W mixture is intrinsically inhomogeneous due to the well established phase segregation below a critical glycerol concentration of 40 mol%. In the inhomogeneous regime the water molecules tend to form cooperative domains besides the mesoscopic G-W mixture [11]. Samples are quenched by rapid cooling down to 4.2 K inside the spectrometer cryostat. Spectra were recorded on slow heating of the sample in the temperature range of 130 -305 K. The glass transition temperature is correlated to the sharp transition of the extrema separation of the ESR spectrum. The glass transition temperatures are found to follow a concentration dependence which is closely associated to the mesoscopic inhomogeneities of the G-W system. The steady enhancement in fragility of the G-W system with the addition of water is evident from the temperature dependence of the spin probe correlation time τ for the entire concentration range. In the temperature range of 283 -303 K, the DSE law is followed i.e. the spin probe reorientation process is found to be strongly coupled to the system viscosity. In this regime, the τ values have been used along with the available viscosity data to calculate the effective volume V of the spin probe for the entire concentration range. The spin probe effective volume is a measure of the available free volume of the host matrix. A drastic change in the quantity is seen in the vicinity of the 40 mol% glycerol concentration owing to a similar structural change of the matrix due to the formation of mesoscopic scale inhomogeneities below the critical concentration [12]. The thesis concludes with a discussion about the possible future directions of research.

By numerical methods, two models of anisotropic mixed quantum spin chains, consisting of spins of two different sizes, Sa = 1/2 and Sb = 1 as well as Sb = 3/2, are studied with respect to their critical properties at quantum phase transitions in a selected region of parameter space. The quantum spin chains are made up of basecells of four spins, according to the structure Sa − Sa − Sb − Sb. They are described by the XXZ Hamiltonian, that extends the quantum Heisenberg model by a variable anisotropic exchange interaction. As additional control parameter, an alternating exchange constant between nearest-neighbour spins is introduced. Insight gained by complementary application of exact diagonalization and quantum Monte Carlo simulations, as well as appropriate methods of analysis, is embedded in the broad existing knowledge on homogeneous quantum spin chains. In anisotropic homogeneous quantum spin chains, there exist phase boundaries with continuously varying critical exponents, the Gaussian critical lines, along which, in addition to standard scaling relations, further extended scaling relations hold. Reweighting methods, also applied to improved quantum Monte Carlo estimators, and finite-size scaling analysis of simulation data deliver a wealth of numerical results confirming the existence of a Gaussian critical line also in the mixed spin models considered. Extrapolation of exact data offers, apart from confirmation of simulation data, furthermore, insight into the conformal operator content of the model with Sb = 1. / Mittels numerischer Methoden werden zwei Modelle anisotroper gemischter Quantenspinketten, bestehend aus Spins zweier unterschiedlicher Größen, Sa = 1/2 und Sb = 1 sowie Sb = 3/2, hinsichtlich ihrer kritischen Eigenschaften an Quanten-Phasenübergängen in einem ausgewählten Parameterbereich untersucht. Die Quantenspinketten sind aus Basiszellen zu vier Spins, gemäß der Struktur Sa − Sa − Sb − Sb, aufgebaut. Sie werden durch den XXZ Hamiltonoperator beschrieben, der das isotrope Quanten-Heisenberg Modell um eine variable anistrope Austauschwechselwirkung erweitert. Als zusätzlicher Kontrollparameter wird eine alterniernde Kopplungskonstante zwischen unmittelbar benachbarten Spins eingeführt. Die durch komplementäre Anwendung exakter Diagonalisierung und Quanten-Monte-Carlo Simulationen, sowie entsprechender Analyseverfahren, gewonnenen Erkenntnisse werden in das umfangreiche existierende Wissen über homogene Quantenspinketten eingebettet. Im Speziellen treten in anisotropen homogenen Quantenspinketten Phasengrenzen mit kontinuierlich variierenden kritischen Exponenten auf, die Gaußschen kritischen Linien, auf denen neben den herkömmlichen auch erweiterte Skalenrelationen Gültigkeit besitzen. Umgewichtungsmethoden, speziell auch angewandt auf verbesserte Quanten-Monte-Carlo Schätzer, und Endlichkeitsskalenanalyse von Simulationsdaten liefern eine Fülle von numerischen Ergebnissen, die das Auftreten der Gaußschen kritischen Linie auch in den untersuchten gemischten Quantenspinketten bestätigen. Die Extrapolation exakter Daten bietet, neben der Bestätigung der Simulationsdaten, darüber hinaus Einblick in einen Teil des konformen Operatorinhalts des Modells mit Sb = 1.

Path integral Monte Carlo (PIMC) is a method suitable for quantum liquid simulations at finite temperature. We present in this thesis a study of PIMC dealing with the theory and algorithms related to it, and then two applications of PIMC to current research problems of quantum fluids in the Bolzmann regime. The first part encompasses a study of the different ingredients of a PIMC code: action, sampling and physical property estimators. Particular attention has been paid to Li-Broughton's higher order approximation to the action. Regarding sampling, several collective movement methods have been derived, including the bisection algorithm, that has been thoroughly tested. We also include a study of estimators for different physical properties, such as, the energy (through the thermodynamic and virial estimators), the pair distribution function, the structure factor, and the momentum distribution. In relation to the momentum distribution, we have developed a novel algorithm for its estimation, the trail method. It surmounts some of the problems exposed by previous approaches, such as the open chain method or McMillan's algorithm.The Richardson extrapolation used within PIMC simulations, is another contribution of this thesis. Up until now, this extrapolation has not been used in this context. We present studies of the energy dependence on the number of "beads", along with the betterment provide by the Richardson extrapolation. Inasmuch as our goal is to perform research of quantum liquids at finite temperature, we have produced a library of codes, written from scratch, that implement most of the features theoretically developed. The most elaborated parts of these codes are included in some of the appendixes.The second part shows two different applications of the algorithms coded. We present results of a PIMC calculation of the momentum distribution of Ne and normal 4He at low temperatures. In the range of temperatures analysed, exchanges can be disregarded and both systems are considered Boltzmann quantum liquids. Their quantum character is well reflected in their momentum distributions witch show clear departures from the classical limit. The PIMC momentum distributions which show clear departures from the classical limit. The PIMC momentum distributions are sampled using the trail method. Kinetic energies of both systems, as a function of temperature and at a fixed density, are also reported. Finally, the solid-liquid neon phase transition along the 35 K isotherm has been characterized.While thermodynamic properties of the solid phase are well known the behaviour of some properties, such as the energy or the dessity, during the trasition presen6 some uncertainties For example, experimental data for the place diagram, which determines solid and liquid boundaries, present sizeable differences. The temperature chosen is high enough so that Bose or Fermi statistics corrections are small, although the system is strongly quantum mechanical. The results obtained show a discontinuity in the kinetic energy during the transition.