218 resultados para Fullerene


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The nonlinear amplitude modulation dynamics of electrostatic oscillations of massive charged defects in a three-component pair plasma is investigated; i.e. doped pair-ion plasmas (anticipating the injection of a massive charged component in the background; e.g. in fullerene experiments). Ton-acoustic oscillations in electron-positron-ion (e-p-i) plasmas are also covered, in the appropriate limit. Linear and nonlinear effects (MI, envelope modes) are discussed. The role of the temperature and density ratio between the pair species is stressed.

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The propagation of small amplitude stationary profile nonlinear electrostatic excitations in a pair plasma is investigated, mainly drawing inspiration from experiments on fullerene pair-ion plasmas. Two distinct pair ion species are considered of opposite polarity and same mass, in addition to a massive charged background species, which is assumed to be stationary, given the frequency scale of interest. In the pair-ion context, the third species is thought of as a background defect (e.g. charged dust) component. On the other hand, the model also applies formally to electron-positron-ion (e-p-i) plasmas, if one neglects electron-positron annihilation. A two-fluid plasma model is employed, incorporating both Lorentz and Coriolis forces, thus taking into account the interplay between the gyroscopic (Larmor) frequency ?c and the (intrinsic) plasma rotation frequency O0. By employing a multi-dimensional reductive perturbation technique, a Zakharov-Kuznetsov (ZK) type equation is derived for the evolution of the electric potential perturbation. Assuming an arbitrary direction of propagation, with respect to the magnetic field, we derive the exact form of nonlinear solutions, and study their characteristics. A parametric analysis is carried out, as regards the effect of the dusty plasma composition (background number density), species temperature(s) and the relative strength of rotation to Larmor frequencies. It is shown that the Larmor and mechanical rotation affect the pulse dynamics via a parallel-to-transverse mode coupling diffusion term, which in fact diverges at ?c ? ±2O0. Pulses collapse at this limit, as nonlinearity fails to balance dispersion. The analysis is complemented by investigating critical plasma compositions, in fact near-symmetric (T- ˜ T+) “pure” (n- ˜ n+) pair plasmas, i.e. when the concentration of the 3rd background species is negligible, case in which the (quadratic) nonlinearity vanishes, so one needs to resort to higher order nonlinear theory. A modified ZK equation is derived and analyzed. Our results are of relevance in pair-ion (fullerene) experiments and also potentially in astrophysical environments, e.g. in pulsars.

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The cell-specific delivery of polynucleic acids (e.g., DNA, RNA), gene therapy, has the potential to treat various diseases. In this chapter we discuss the use of organic electronic materials as non-viral gene delivery vectors and the great potential for electrochemically triggered gene delivery. We highlight some examples in this chapter based on fullerenes (bucky balls and carbon nanotubes), graphenes and electroactive polymers, particularly those that include experiments in vivo.

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The structure and properties of melt mixed high-density polyethylene/multi-walled carbon nanotube (HDPE/MWCNT) composites processed by compression molding and blown film extrusion were investigated to assess the influence of processing route on properties. The addition of MWCNTs leads to a more elastic response during deformations that result in a more uniform thick-ness distribution in the blown films. Blown film composites exhibit better mechanical properties due to the enhanced orientation and disentanglement of MWCNTs. At a blow up ratio (BUR) of 3 the breaking strength and elongation in the machine direction of the film with 4 wt % MWCNTs are 239% and 1054% higher than those of compression molded (CM) samples. Resistivity of the composite films increases significantly with increasing BURs due to the destruction of conductive pathways. These pathways can be recovered partially using an appropriate annealing process. At 8 wt % MWCNTs, there is a sufficient density of nanotubes to maintain a robust network even at high BURs.

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Double photoionization accompanied by loss of n C atoms (n=0, 2, 4, 6) was investigated by merging beams of Xe@C60+ ions and synchrotron radiation and measuring the yields of product ions. The giant 4d dipole resonance of the caged Xe atom has a prominent signature in the cross section for these product channels, which together account for 6.2 ± 1.4 of the total Xe 4d oscillator strength of 10. Compared to that for a free Xe atom, the oscillator strength is redistributed in photon energy due to multipath interference of outgoing Xe 4d photoelectron waves that may be transmitted or reflected by the spherical C60+ molecular cage, yielding so-called confinement resonances. The data are compared with an earlier measurement and with theoretical predictions for this single-molecule photoelectron interferometer system. Relativistic R-matrix calculations for the Xe atom in a spherical potential shell representing the fullerene cage show the sensitivity of the interference pattern to the molecular geometry. © 2013 American Physical Society.

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A presente dissertação descreve a síntese e o estudo de propriedades fotofísicas e biológicas de sistemas baseados em ftalocianinas. Os sistemas sintetizados consistem em ftalocianinas contendo unidades de D-galactose, ciclodextrinas, [60]fulereno ou porfirinas. Na primeira parte da dissertação aborda-se a síntese de ftalocianinas substituídas com unidades de D-galactose, com o intuito de serem utilizadas como fotossensibilizadores em terapia fotodinâmica. A eficiência de geração de oxigénio singuleto induzida pelas glicoftalocianinas, bem como a sua actividade fotodinâmica in vitro em células HeLa são avaliadas. Adicionalmente são descritos os estudos de MALDI-MS/MS de dois pares de glicoftalocianinas isoméricas. Numa segunda parte, descrevem-se a síntese e a caracterização de sistemas supramoleculares de ftalocianinas ligadas a ciclodextrinas ou [60]fulereno. Foram desenvolvidas metodologias sintéticas para obter complexos ftalocianínicos de ruténio(II) substituídos axialmente com derivados de ciclodextrinas, e complexos ftalocianínicos de zinco(II) ligados covalentemente a ciclodextrinas. Descreve-se também a síntese de uma díade ftalocianina- [60]fulereno. A estratégia sintética envolve um peculiar primeiro passo, uma reacção de aminação redutiva, no qual se obtém uma ftalocianina funcionalizada com glicina, seguida da habitual reacção de cicloadição 1,3- dipolar. Na terceira parte, abordam-se sistemas dador-aceitador de díades porfirinaftalocianina, como modelos promissores para mimetizar sistemas fotossintéticos naturais. Diferentes tipos de díades porfirina-ftalocianina, ligadas através do grupo fenilo da posição meso ou da posição β-pirrólica da porfirina, são sintetizadas e caracterizadas. As abordagens sintéticas envolvem reacções de aminação catalisadas por paládio e reacções de condensação cruzada de dois ftalonitrilos adequadamente substituídos. Também se descrevem processos de transferência de energia e electrónica fotoinduzidos que se formam a partir das díades porfirina-ftalocianina.

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The solid-fluid transition properties of the n - 6 Lennard-Jones system are studied by means of extensive free energy calculations. Different values of the parameter n which regulates the steepness of the short-range repulsive interaction are investigated. Furthermore, the free energies of the n < 12 systems are calculated using the n = 12 system as a reference. The method relies on a generalization of the multiple histogram method that combines independent canonical ensemble simulations performed with different Hamiltonians and computes the free energy difference between them. The phase behavior of the fullerene C60 solid is studied by performing NPT simulations using atomistic models which treat each carbon in the molecule as a separate interaction site with additional bond charges. In particular, the transition from an orientationally frozen phase at low temperatures to one where the molecules are freely rotating at higher temperatures is studied as a function of applied pressure. The adsorption of molecular hydrogen in the zeolite NaA is investigated by means of grand-canonical Monte Carlo, in a wide range of temperatures and imposed gas pressures, and results are compared with available experimental data. A potential model is used that comprises three main interactions: van der Waals, Coulomb and induced polarization by the permanent electric field in the zeolite.

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Dissertação de mestrado, Biologia Marinha, Faculdade de Ciências e Tecnologia, Universidadde do Algarve, 2015

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Trabalho Final de Mestrado para obtenção do Grau de Mestre em Engenharia Química e Biológica

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Le fullerène C60 est une molécule sphérique composée exclusivement d'atomes de carbone. Ce composé possède une surface aromatique convexe homogène et peut s'associer, entre autres, avec des molécules possédant des surfaces aromatiques par des interactions non-covalentes. Le triptycène est une molécule en forme de "Y" qui possède des surfaces aromatiques convexes. Cette molécule possède l'habileté de s'associer avec le C60 par des interactions de type π qui sont amplifiées par la complémentarité des surfaces concaves et convexes impliquées dans les arrangements cristallins. Nous avons synthétisé des dérivés triptycényles portant des groupements fonctionnels aux extrémités des bras de ce noyau de façon à étendre les cavités disponibles pour interagir avec le C60. En effet, nous avons découvert que les atomes de chlore, de brome et d'iode ainsi que les groupements méthyle permettent d'étendre les surfaces disponibles pour interagir avec les fullerènes C60 et C70. Nous avons étudié les associations entre les dérivés triptycényles et les fullerènes par l'analyse des structures cristallographiques résolues par diffraction des rayons-X. De plus, nous avons étudié les associations entre les molécules considérées par l'analyse des surfaces d'Hirshfeld entourant les fullerènes. Découlant de ces études, l'effet d'amplification des atomes de chlore, de brome et d'iode ainsi que les groupements méthyle a été employé pour identifier de nouveaux solvants aptes à solubiliser efficacement le C60.

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Le fullerène C60, une molécule sphérique, et le C70, un analogue ellisoïde, sont des composés aromatiques convexes constitués exclusivement d'atomes de carbone. La nature aromatique de la surface de ces cages de carbone rend possible leur association à l'état solide avec d'autres molécules aromatiques de topologie complémentaire. En particulier, l'association des fullerènes avec des composés présentant des motifs concaves aromatiques, via une association de type concave-convexe, est favorable. En effet, les interactions π•••π de type concave-convexe sont amplifiées grâce à la complémentarité topologique des partenaires impliqués. Le centrohexaindane est un hydrocarbure non planaire rigide qui a été synthétisé pour la première fois en 1988 par Kuck et collaborateurs. Cette molécule possède quatre surfaces aromatiques concaves orientées dans une géométrie tétraédrique qui sont susceptibles d'interagir favorablement avec les fullerènes. Nous avons ainsi avec succès cocristallisé le centrohexaindane avec les fullerènes C60 et C70. Puis, nous avons étudié les assemblages à l'état solide entre le centrohexaindane et les fullerènes par l'analyse des structures résolues via diffraction des rayons X. Les surfaces concaves aromatiques du centrohexaindane se sont révélées être propices à une association avec les fullerènes C60 et C70 via des interactions π•••π de type concave-convexe, tel que prévu. En outre, nous avons découvert que les liaisons C-H situées à la périphérie du centrohexaindane prennent part à une multitude de contacts C-H•••π avec les molécules de fullerène. Les échantillons de cocristaux composés de centrohexaindane et de fullerène ont aussi été caractérisés par diffraction de poudre des rayons X et par analyse thermogravimétrique dans le but d'en évaluer l'homogénéité.

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Les hétérojonctions formées de deux matériaux, un donneur et un accepteur (D/A), sont la base de la majorité des mélanges photovoltaïques organiques. Les mécanismes de séparation des charges dans ces systèmes représentent aujourd'hui l'un des sujets les plus chauds et les plus débattus dans ce domaine. Nous entrons au coeur de ce débat en choisissant un système D/A à base de phtalocyanine de cuivre (CuPc) et de fullerène (C60). Pour sonder les états excités de nos molécules et obtenir de l'information sur les phénomènes à l'interface D/A, nous réalisons une expérience pompe-sonde, appelée absorption photoinduite (PIA). Nous y mesurons le changement fractionnaire de transmission au travers de l'échantillon. Les mesures de PIA sont réalisées à l'état de quasi équilibre, à T=10K. Nous observons une modulation prononcée dans la région du photoblanchiment de l'état fondamental qui nous indique que la pompe induit un décalage du spectre d'absorption de l'état fondamental. Ce décalage peut être expliqué par deux processus : soit l'échantillon est chauffé par la pompe (effet thermique) ou bien des charges sont créées à l'interface entre les deux matériaux (effet Stark). La dépendance en température du spectre d'absorption entre 10K et 290K montre une signature thermique pour un changement de température de 80K. Grâce au ratio des raies Raman anti-Stokes et Stokes, nous démontrons que la pompe chauffe l'échantillon de 34 K, température insuffisante pour attribuer notre signal à un effet thermique. Nous évaporons ensuite la bicouche CuPc/C60 sur de l'ITO et du saphir, substrats qui possèdent des conductivités thermiques différentes et nous observons le même signal de PIA, excluant par le fait même l'hypothèse de l'effet thermique. Puisque notre étude est comparable à la spectroscopie à effet Stark, nous procédons à une analyse similaire en comparant notre signal de PIA au spectre de la transmittance et à ses dérivés première et seconde. Nous observons alors que notre signal reproduit presque parfaitement la dérivée seconde de la transmittance. Ces résultats sont conformes à une signature optique d'effet Stark due à la création de charges à l'interface D/A.

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Optical limiting and thermal lensing studies are carried out in C70–toluene solutions. The measurements are performed using 9-ns pulses generated from a frequencydoubled Nd:YAG laser at 532 nm. Optical limiting studies in fullerene molecules lead to the conclusion that reverse saturable absorption is the major mechanism for limiting. Analysis of thermal lensing measurements showed a quadratic dependence of thermal lens signal on incident laser energy, which also supports the view that optical limiting in C70 arises due to sequential two-photon absorption via excited triplet state (reverse saturable absorption).

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Optical limiting and thermo-optic properties of C60 in toluene are studied using 532 nm, 9 ns pulses from a frequency-doubled Nd:YAG laser. Optical limiting studies in these fullerene molecules lead to the conclusion that reverse saturable absorption is the major mechanism for limiting properties in these molecules. Thermal lensing measurements are also performed in fullerene solutions. The quadratic dependence of thermal lens signal on incident energy confirms that enhanced optical absorption by the sample via excited triplet state absorption may play a leading role in the limiting property.

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We compute the density-fluctuation spectrum of spherical 4HeN shells adsorbed on the outer surface of Cn fullerenes. The excitation spectrum is obtained within the random-phase approximation, with particle-hole elementary excitations and effective interaction extracted from a density-functional description of the shell structure. The presence of one or two solid helium layers adjacent to the adsorbing fullerene is phenomenologically accounted for. We illustrate our results for a selection of numbers of adsorbed atoms on C20, C60, and C120. The hydrodynamical model that has proven successful to describe helium excitations in the bulk and in restricted geometries permits to perform a rather exhaustive analysis of various fluid spherical systems, namely, spheres, cavities, free bubbles, and bound shells of variable size.