Sélection in vivo par phage display dans un modèle de sténose valvulaire aortique chez la souris pour la découverte de nouveaux peptides ciblant la valve aortique

La sténose valvulaire aortique (SVA) est la maladie des valves cardiaques la plus répandue dans les pays développés qui touche les personnes âgées. La SVA est un processus actif caractérisé par des dépôts de lipides, de l’inflammation, de la fibrose et une calcification active des feuillets qui progresse vers un épaississement et durcissement de la valve aortique et une diminution de l’aire de la valve aortique. Nous avons émis l’hypothèse que la pathogénèse de la SVA modifie progressivement l’endothélium de la valve aortique, ce qui engendre l’expression de biomarqueurs spécifiques aux tissus et à la maladie. On rapporte dans cet étude, l’utilisation de la technique de sélection in vivo par phage display d’une librairie de peptides aléatoires afin de trouver de nouveaux peptides candidats qui se lieraient à des biomarqueurs spécifiques à la valve aortique malade d’une souris. Des souris ATX (LDLr-/-;Tg(hApoB+/+)) âgées atteintes de la SVA ont été utilisées pour la sélection in vivo d’une librairie de peptides aléatoires de 7 acides aminés contraints ou linéaires. Après 4 tours de criblage, on a caractérisé 14 phages différents qui ont été séparés en 5 motifs consensus pour la librairie linéaire et 11 phages différents qui représentent 5 différents motifs consensus pour la libraire de peptides contraints. La spécificité de 4 phages candidats de la librairie linéaire et de 5 phages de la librairie contrainte a été étudiée par l’immunomarquage des peptides d’intérêt exprimés par les phages sur les coupes de tissus de la valve aortique malade par rapport aux tissus contrôles du foie, du rein, de la rate, du ventricule et du poumon. Parmi eux, 6 phages représentent des peptides candidats intéressants qui ont besoin d’être testés davantage pour évaluer leur spécificité in vivo à la valve. Bien qu’il reste encore de la validation à effectuer, les peptides candidats spécifiques trouvés peuvent représenter des agents moléculaires d’imagerie utiles ou des transporteurs dans la livraison de drogue qui ciblent la valve aortique malade.

Evidence for polaron conduction in nanostructured manganese ferrite

Nanoparticles of manganese ferrite were prepared by the chemical co-precipitation technique. The dielectric parameters, namely, real and imaginary dielectric permittivity (ε and ε ), ac conductivity (σac) and dielectric loss tangent (tan δ), were measured in the frequency range of 100 kHz–8MHz at different temperatures. The variations of dielectric dispersion (ε ) and dielectric absorption (ε ) with frequency and temperature were also investigated. The variation of dielectric permittivity with frequency and temperature followed the Maxwell–Wagner model based on interfacial polarization in consonance with Koops phenomenological theory. The dielectric loss tangent and hence ε exhibited a relaxation at certain frequencies and at relatively higher temperatures. The dispersion of dielectric permittivity and broadening of the dielectric absorption suggest the possibility of a distribution of relaxation time and the existence of multiple equilibrium states in manganese ferrite. The activation energy estimated from the dielectric relaxation is found to be high and is characteristic of polaron conduction in the nanosized manganese ferrite. The ac conductivity followed a power law dependence σac = Bωn typical of charge transport assisted by a hopping or tunnelling process. The observed minimum in the temperature dependence of the frequency exponent n strongly suggests that tunnelling of the large polarons is the dominant transport process

Studies on the resonance Raman spectra of polyaniline obtained with near-IR excitation

The effects of near-IR (NIR) laser power over the Raman spectra of poly(aniline) emeraldine salt (PANIES) and base (PANI-EB) were investigated. The reasons for the existence of several bands from 1324 to 1500 cm-1 in the Raman spectra of poly(aniline) obtained at NIR region were also studied. The bands from 1324 to 1375 cm-` were associated to vC-N of polarons with different conjugation lengths and the bands from 1450 to 1500 cm-1 in Raman spectra of PANI emeraldine and pernigraniline base forms were correlated to vC=N modes associated with quinoid units having different conjugation lengths. The increase of laser power at 1064.0 run causes the deprotonation of PANI-ES and the formation of cross-linking segments having phenazine and/or oxazine rings. For PANI-EB only a small spectral change is observed when the laser power is increased, owing to the low absorption of this form in the NIR region. Copyright (c) 2007 John Wiley & Sons, Ltd.

Análise do modelo t-J e sua aplicação aos compostos de óxidos de cobre

Neste trabalho estudamos modelos teóricos que descrevem sistemas eletrônicos fortemente correlacionados, em especial o modelo t-J, e suas aplicações a compostos de óxidos de cobre, notadamente os compostos que apresentam supercondutividade de alta temperatura crítica e o composto Sr2CuO2Cl2. No primeiro capítulo do trabalho, fazemos uma exposição de três modelos que envolvem o tratamento das interações elétron-elétron, que são os modelos de Hubbard de uma banda, o modelo de Heisenberg e o modelo t-J. Na dedução deste último fazemos uma expansão canônica do hamiltoniano de Hubbard, no limite de acoplamento forte, levando-nos a obter um novo hamiltoniano que pode ser utilizado para descrever um sistema antiferromagnético bidimensional na presen- ça de lacunas, que é exatamente o que caracteriza os compostos supercondutores de alta temperatura crítica na sua fase de baixa dopagem.Após termos obtido o hamiltoniano que descreve o modelo t-J, aplicamos à este uma descrição de polarons de spin, numa representação de holons, que são férmions sem spin, e spinons, que são bósons que carregam somente os graus de liberdade de spin. Utilizando uma função de Green para descrever a propagação do polaron pela rede, obtemos uma equação para a sua autoenergia somando uma série de diagramas de Feynman, sendo que para este cálculo utilizamos a aproxima ção de Born autoconsistente[1]. Do ponto de vista numérico demonstramos que a equação integral de Dyson resultante do tratamento anterior não requer um procedimento iterativo para sua solução, e com isto conseguimos trabalhar com sistemas com grande número de partículas. Os resultados mostram, como um aspecto novo, que o tempo de vida média do holon tem um valor bastante grande no ponto (π,0 ) da rede recíproca, perto da singularidade de Van Hove mencionada na literatura[2]. Este aspecto, e suas implicações, é amplamente discutido neste capítulo. No capítulo 3 estudamos o modelo estendido t-t'-J, com tunelamento à segundos vizinhos e a incorporação dos termos de três sítios[3]. Fazemos a mesma formulação do capítulo anterior, e discutimos as aplicações dos nossos resultados ao óxido mencionado anteriormente. Finalmente, no último capítulo apresentamos uma aplicação original do modelo t-J à uma rede retangular, levemente distorcida, e demonstramos que os resultados do capítulo 3 são reproduzidos sem necessidade de introduzir termos de tunelamento adicionais no hamiltoniano. Esta aplicação pode se tornar relevante para o estudo das fases de tiras encontradas recentemente nesses materiais de óxidos de cobre.

Propriedades física de molécilas orgânicas e compostos do tipo perovskita CdSiO3 e CaPbO3

In the first part of this work our concern was to investigate the thermal effects in organic crystals using the theory of the polarons. To analyse such effect, we used the Fröhlich s Hamiltonian, that describes the dynamics of the polarons, using a treatment based on the quantum mechanics, to elucidate the electron-phonon interaction. Many are the forms to analyzing the polaronic phenomenon. However, the measure of the dielectric function can supply important information about the small polarons hopping process. Besides, the dielectric function measures the answer to an applied external electric field, and it is an important tool for the understanding of the many-body effects in the normal state of a polaronic system. We calculate the dielectric function and its dependence on temperature using the Hartree-Fock decoupling method. The dieletric function s dependence on the temperature is depicted by through a 3D graph. We also analyzed the so called Arrhenius resistivity, as a functionof the temperature, which is an important tool to characterize the conductivity of an organic molecule. In the second part we analyzed two perovskita type crystalline oxides, namely the cadmium silicate triclinic (CdSiO3) and the calcium plumbate orthorhombic (CaPbO3), respectively. These materials are normally denominated ABO3 and they have been especially investigated for displaying ferroelectric, piezoelectric, dielectrics, semiconductors and superconductors properties. We found our results through ab initio method within the functional density theory (DFT) in the GGA-PBE and LDA-CAPZ approximations. After the geometry optimization for the two structure using the in two approximations, we found the structure parameters and compared them with the experimental data. We still determined further the angles of connection for the two analyzed cases. Soon after the convergence of the energy, we determined their band structures, fundamental information to characterize the nature of the material, as well as their dielectrics functions, optical absorption, partial density of states and effective masses of electrons and holes

Structural and dielectric properties of relaxor Sr0.5Ba0.5Bi2Nb2O9 ceramic

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Espectros fractais em sistemas nanoestruturados e cristais fotônicos

The study of the elementary excitations such as photons, phonons, plasmons, polaritons, polarons, excitons and magnons, in crystalline solids and nanostructures systems are nowdays important active field for research works in solid state physics as well as in statistical physics. With this aim in mind, this work has two distinct parts. In the first one, we investigate the propagation of excitons polaritons in nanostructured periodic and quasiperiodic multilayers, from the description of the behavior for bulk and surface modes in their individual constituents. Through analytical, as well as computational numerical calculation, we obtain the spectra for both surface and bulk exciton-polaritons modes in the superstructures. Besides, we investigate also how the quasiperiodicity modifies the band structure related to the periodic case, stressing their amazing self-similar behavior leaving to their fractal/multifractal aspects. Afterwards, we present our results related to the so-called photonic crystals, the eletromagnetic analogue of the electronic crystalline structure. We consider periodic and quasiperiodic structures, in which one of their component presents a negative refractive index. This unusual optic characteristic is obtained when the electric permissivity and the magnetic permeability µ are both negatives for the same range of angular frequency ω of the incident wave. The given curves show how the transmission of the photon waves is modified, with a striking self-similar profile. Moreover, we analyze the modification of the usual Planck´s thermal spectrum when we use a quasiperiodic fotonic superlattice as a filter.

Magnetic properties of poly(3-hexylthiophene)

A room temperature ferromagnetic phase is observed in samples of poly(3-hexylthiophene) partially doped with ClO (4) over bar. The magnetic behavior presents a strong dependence on the sample preparation conditions, in particular, a dependence with the final potential of the sample after reduction. The origin of the ferromagnetism is proposed to be associated with interactions between spin 1/2 polarons formed in the polymeric chain upon doping. The dependence of saturation and spontaneous magnetization as the function of the final potential after reduction shows a way to control the magnetic properties of this polymer. (C) 2008 Elsevier B.V. All rights reserved.

Simultaneous observation of the magnetic and electric behavior in a correlated system near a metal-semiconductor transition: ESR in pellets of conducting polymers

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Dielectric investigations of vanadium modified barium zirconium titanate ceramics obtained from mixed oxide method

Vanadium modified barium zirconium titanate ceramics Ba(Zr(0.10)Ti(0.90))O(3):2V (BZT:2V) were prepared from the mixed oxide method. According to X-ray diffraction analysis, addition of vanadium leads to ceramics free of secondary phases. Electrical characteristics reveal a dielectric permittivity at around 15,000 with low dielectric loss with a remnant polarization (P(r))of 8 mu C/cm(2) at 2 kV/cm. From the obtained results, we assume that vanadium substitution in the BZT lattice affects dielectric characteristics due to the electron-relaxation-mode in which carriers (polarons, protons, and so on) are coupled with existing dielectric modes. (C) 2009 Published by Elsevier B.V.

Room temperature ferromagnetic behavior in pressed pellets of doped poly (3-methylthiophene)

Room temperature ferromagnetic behavior has been observed in pressed pellets of doped poly(3-methylthiophene). In this work we show that thermoremance data taken in two different ways favours the interpretation of data in terms of the Dzialoshinski-Moriya anisotropic superexchange interaction of the polarons via dopant anions giving rise to weak ferromagnetism.

The ferromagnetic behaviour of conducting polymers revisited

The magnetic properties of doped pellets of poly(3-methylthiophene) showing room temperature ferromagnetic behaviour have been discussed in a previous article. The magnetic behaviour was attributed to a weak ferromagnetic phase, due to the superexchange interaction of polarons via the dopant anions. The Dzialoshinsky-Morya interaction among canted spins was proposed to explain the ferromagnetism. In this article the main conclusions of that work concerning the magnetic behaviour are revised. The basic assumption now is that the magnetic moments are spin 1/2 polarons that can interact antiferromagnetically and/or ferromagnetically. In the small crystalline regions of the polymer, which are identified with the polymer portion that remains ferromagnetic at room temperature, the interaction gives rise to S = 0 and 1 bipolarons and the S = 1 triplet state is lower in energy. In the disordered region, disorder will prevent the complete S = 1 and 0 coupling and bands of polarons ferromagnetically and antiferromagnetically coupled will appear. Using this approach, all the magnetization data can be qualitatively explained, as well as the electron spin resonance data.

Magnetic field dependent magnetization of a conducting plasticized poly(aniline) film

We report magnetic data of free standing films of poly( aniline) (PANI) protonated with a plasticizing di-ester of succinic acid. The data have been obtained using the electron spin resonance (ESR) technique at two different frequencies, X-band (9.4 GHz) and Q-band ( 34 GHz), on one hand, and by magnetization measurements in broad ranges of temperatures and magnetic fields on the other hand. All the data can be explained assuming a transition as a function of temperature from delocalized magnetic moments in the valence band to localized positive polarons in several antiferromagnetically correlated bands. By increasing the magnetic field, the magnetic properties are affected in several ways. An intra-band admixture of states occurs; it contributes to increase the spins' localization and finally promotes an antiferromagnetic-metamagnetic transition.

Magnetic field dependence of the magnetic susceptibility and the specific heat of the doped plasticized polyaniline (PANI-DB3EPSA)0.5

Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)

Polaronic ferromagnetism in conducting polymers

Ferromagnetic behavior at room temperature is reported in metal-free-conducting polymer samples of poly(3-methylthiophene) doped with ClO 4 -. Magnetic moments associated with spin 1/2 positive polarons are possibly interacting through a Dzialoshinski-Moriya anisotropic superexchange via the dopant anions, giving rise to weak ferromagnetism. © 2001 Elsevier Science B.V. All rights reserved.