Orientador: Cláudio Luiz Carvalho / Banca: Haroldo Naoyuki Nagashima / Banca: Isaias Gonzaga de Oliveira / Resumo: Com o surgimento da supercondutividade as pesquisas envolvendo aplicações desta, em especial no transporte de energia, obtiveram um avanço promissor ao longo dos anos. Assim, este trabalho objetivou a fabricação de fios supercondutores utilizando o método Powder-In-Tube (PIT), no qual foi inserido dentro de um tubo de prata o pó da cerâmica supercondutora do sistema BSCCO. Estudos preliminares foram feitos em pastilhas feitas com o mesmo material supercondutor e após alguns resultados foram confeccionados os fios supercondutores. Medidas de caracterização foram feitas dentre elas a difratometria de raios-X, medidas elétricas pelo método de quatro pontas e microscopia do tipo (FEG-MEV) equipado com EDS para determinar a morfologia e composição química dos elementos na amostra. Os resultados de difratometria de raios-X apresentaram a formação das fases desejadas do sistema BSCCO de diferentes concentrações dentre elas as fases Bi-2212 Bi- 2223 e Bi-2234 contidas nas amostras sintetizadas. As medidas elétricas detectaram uma queda abrupta na resistência elétrica dos fios mostrando a faixa de transição supercondutora das amostras estudadas. As medidas de densidade de corrente com base no critério de corrente de 1μV/cm, utilizadas nos fios confeccionados, foram obtidos valores da ordem de 1,30 - 3,90 (KA/m2). Nas imagens de microscopia vale ressaltar uma melhora na interação entre os grãos supercondutores nas amostras submetidas a um maior tempo de sinterização e também foi possível verificar e analisar através da extrusão a compactação do pó cerâmico dentro do tubo de prata. O EDS detectou a composição química dos elementos nas amostras bem como a concentração das fases em determinadas regiões analisadas / Abstract: With the emergence of superconductivity research involving applications of this, particularly in the transport of energy, had a promising advance over the years. This study aims to manufacture superconducting wires using the method Powder-In-Tube (PIT), which was inserted inside a tube of silver powder of superconducting ceramic BSCCO system. Preliminary studies were done on pellets made with the same superconducting material, and after some results were prepared the superconducting wires. Characterization measurements were made among them the X-ray diffraction, electrical measurements by the method of four points and type of microscopy (FEG-SEM) equipped with EDX to determine the morphology and chemical composition of the elements in the sample. The results of X-ray diffraction showed the formation of the desired phases for this type of superconductor, ie the BSCCO system between them was possible to determine the Bi-2212 phase, Bi-2223 and Bi-2234 contained in the synthesized samples. The electrical measurements have detected a sudden drop in electrical resistance of the wires showing the range of superconducting transition with good accuracy. It was possible to perform the calculation of current density in the wires made based on a criterion of 1 μV/cm were obtained and values of around 1,30- 3,90 (KA/m2). The values are consistent with the specifications of the samples and within the limits of our research. In microscopy images is noteworthy improvement in the interaction between the superconducting grains in samples submitted to a higher sintering time and it was possible to verify and analyze the compaction of ceramic powder into silver tube through the extrusion process. The EDX detected the chemical composition of the elements in the samples in a qualitative way / Mestre

Orientador: Cláudio Luiz Carvalho / Banca: Victor Ciro Solano Reynoso / Banca: Alexander Polasek / Resumo: Devido a grande preocupação em se desenvolver novos materiais e técnicas para suprir a necessidade por novos recursos e atender com maior comodidade e eficiência a população mundial, estão surgindo novas áreas de pesquisas que visam suprir esta deficiência, seja criando novas tecnologias, ou mesmo aprimorando as técnicas existentes a fim de se obter um melhor aproveitamento dos recursos já existentes. Assim, estamos nos interessando por um ramo da ciência pouco conhecido, mas com um potencial muito elevado a ser descoberto, estamos falando dos materiais supercondutores, que pouco se sabe a respeito deles, porém muito já se faz com os mesmos. Desta maneira estamos apostando numa área mista, onde não usaremos os materiais supercondutores como sendo meramente condutores de energia e sim como dispositivos eletrônicos. Então, começamos o nosso trabalho, desenvolvendo materiais supercondutores na forma de filmes finos que é a base para o desenvolvimento desses dispositivos. Sendo assim escolhemos o sistema BSCCO, que tem como base os seguintes elementos, Bismuto, Estrôncio, Cálcio, Cobre e Oxigênio e que pode apresentar uma temperatura de transição da fase condutora para a fase supercondutora na faixa de 35 - 110K. Deste modo, nos propomos a estudar este tipo de material e desenvolver filmes finos, capazes de serem usados como ...(Resumo completo, clicar acesso eletronico abaixo) / Abstract: Due to great concern in developing new materials and techniques to supply the need for new resources and to assist with larger comfort and efficiency the world population, new areas of researches that seek to supply this deficiency are appearing, by creating new technologies, or even improving the existent techniques in order to obtain a better use of the resources already existent. Like this, we are being interested in a branch of the little known science, but with a very high potential to be discovered, we are talking about the superconductor materials, that little it is known regarding them. However it is much already done with the same ones. In this way we are betting in a mixed area, where we won't use the superconducting materials as being merely drivers of energy but like electronic devices. Then, we began our work, developing superconductor materials in the form of thin films that is the base for the development of those devices. The system BSCCO was chose because it has composed by the following elements, Bismuth, Strontium, Calcium, Copper and Oxygen and that it may present a transition temperature of the conductive phase for the superconductive phase in the range of 35 - 110K. This way, we have studied this material type and to develop thin films, capable of be used as base for electronic devices. In our work we ...(Complete abstract click electronic access below) / Mestre

BSCCO-2212 is a high-temperature cuprate superconductor whose microscopic behavior is currently poorly understood. In particular, it is unclear whether its order parameter is consistent with s-wave or d-wave symmetry. It has been suggested that its order parameter might take one of several forms that are consistent with d-wave behavior. We present some calculations using the many-body theory approach to superconductivity that suggest that such order parameters would lead to a suppression of the critical temperature in the presence of impurities. Because some experiments have suggested the critical temperature of BSCCO-2212 is relatively independent of the concentration of impurities, this lends support to the hypothesis that its order parameter has s-wave symmetry.

No description available.

While in conventional superconductors coupling between electrons and phonons is known to be responsible for the electron pairing, for the high temperature superconductors the pairing media remains under debates. Since the interactions of electrons with other degrees of freedom (phonons, magnetic excitations, etc) manifest themselves by an additional renormalization in the electronic dispersion, they can be investigated by means of Angle Resolved Photoelectron Spectroscopy. In the work renormalization in two families of high Tc cuprates have been studied. Along the diagonal of the two-dimensional BZ, the renormalization effects are represented by an unusual band dispersion that develops a so-called ‘‘kink’’. In the vicinity of the (pi, 0) point of the BZ, where the order parameter reaches its maximum, the renormalization is noticeably stronger and makes itself evident even in the shape of a single spectral line measured for a fixed momentum. It was shown that for the Bi-2212 samples substitution of Cu atoms in Cu-O plane changes renormalization features in ARPES spectra both in nodal and antinodal parts of the Brillouin zone. The smearing of the dip in the in the spectral line shape measured at (pi; 0) point can be well explained by coupling of electrons to the magnetic resonance mode. The effect of Zn and Ni substitution on the antinodal ARPES spectra was shown to be in good agreement with the influence of these impurities on magnetic resonance mode seen in inelastic neutron scattering experiments. This, in addition to the previous ARPES studies of temperature and doping dependence of peak-dip-hump structure, mass renormalization near antinodal region and a kink in the nodal part of Brillouin zone, provides further evidence that the coupling to magnetic excitations, rather than to phonons, is responsible for the observed unusual renormalization. Unlike the well studied Bi-2212 family of cuprates, photoemission on YBCO-123 turns out to be much more complicated. The observed spectra have a strong contribution from a heavily overdoped surface component with the hole doping level of about x~0.30, which is weakly dependent on the sample stochiometry. Absence of any signs of superconductivity in the spectra of the overdoped component was argued to result from the unusually high doping level. This conclusion is supported by the fact that the overdoped bands give rise to the Fermi surface and band structure consistent with the predictions of the LDA calculations, as well as, by the dependence of the photoemission matrix element on the excitation energy, which closely follows that of the superconducting bulk component. Specific experimental geometry was used to enhance the signal coming from the superconducting component. In particular, experiments with circularly polarized light bundled with simple theoretical considerations enabled better separation of the surface and the bulk components. This type of experiments also suggests that the overdoped component is mainly localized in the topmost CuO2 bilayer, while the next bilayers in the YBCO-123 structure already represent bulk properties and retain superconductivity. Using partially Ca substituted samples it was possible to obtain spectra with a suppressed overdoped component. The likely reason for the suppression is a shift of the most probable cleavage plane from the Ba–O interface to the Y layer. Spectra from the Ca substituted sample clearly reveal a sizable superconducting gap, and strong renormalization effects in the vicinity of the antinodal point. The fact that the renormalization vanishes above Tc and has strong momentum dependence, diminishing away from the (pi; 0)/(0; pi) point, strongly suggests that the reason for this renormalization in YBCO-123 is coupling of the electronic subsystem to spin resonance, similar to the case of Bi-2212.

Orientador: Cláudio Luiz Carvalho / Banca: Rafael Zadorosny / Banca: Carlos Yujiro Shigue / Resumo: Com a descoberta dos supercondutores de alta temperatura crítica na década de 80, as propriedades elétricas desses materiais passaram a ser intensamente estudadas, principalmente por meio do processo de dopagem. Desta forma, este trabalho teve por objetivo estudar os efeitos da dopagem nas propriedades elétricas do sistema supercondutor BSCCO com fórmula estequiométrica Bi1,6Pb0,4Sr2-xRExCa2Cu3O10+δ, por meio da substituição do elemento terra rara (RE), lantânio (La), em sítios de Sr, onde 0≤x≤2,0, em intervalos de 0,5. As soluções precursoras foram preparadas baseadas no método de Pechini, obtendo-se uma resina polimérica submetida a tratamento térmico de 200oC/10h, resultando em um material na forma de pó, o qual foi levado novamente a tratamento térmico entre 400oC a 810oC. Com o pó, foram preparadas pastilhas, submetendo-as a um novo tratamento térmico de 810oC/+31h. Para se conhecer as principais características das amostras, foram feitas a caracterização estrutural por meio da técnica de Difratometria de Raios X (DRX) para todos os tratamentos térmicos realizados; a caracterização elétrica, pelo método de quatro pontas dc; para a caracterização morfológica e química, a técnica de microscopia eletrônica de varredura (MEV), juntamente com a técnica de Espectroscopia por Energia Dispersiva de Raios X (EDX); e medidas magnéticas ac e dc para a caracterização magnética das amostras. Os resultados apontaram uma degradação das propriedades de supercondução, além de mudanças estruturais, morfológicas e magnéticas com o aumento da concentração de dopante / Abstract: With the discovery of high critical temperature superconductors in the 80, the electrical properties of these materials became intensively studied, mainly through the doping process. Thus, the objective of this work was the study of the effects of doping on the electrical properties of BSCCO superconducting system with stoichiometric formula Bi1,6Pb0,4Sr2-xRExCa2Cu3O10+δ, by the substitution of rare earth element (RE), lanthanum (La) in the sites of Sr, where 0 ≤ x ≤ 2.0, in interval of 0.5. The precursor solutions were prepared based by Pechini method, obtaining a polymer resin subjected to heat treatment at 200° 10h, which results in a material in C/ a powder. In sequence, futher heat treatments between 400oC to 810oC were made. With the powder were prepared bulks by subjecting them to a new heat treatment at 810° C/+31h. To know the main characteristics of the samples, structural characterization were made by the technique of X-Ray Diffraction (XRD) for all heat treated samples; the electrical characterization was made by the dc four probe method; for the morphological and chemical characterization by the technique of Scanning Electron Microscopy (SEM), together with the technique of Energy Dispersive X-ray Spectroscopy (EDX); and ac and dc magnetic measurements to magnetic characterization of the sample. The results shown a degradation of superconducting properties, as a consequence of structural, morphology and magnetic changes with the dopant concentration increase / Mestre

Ce travail concerne l'épitaxie par jets moléculaires de films de BiSrCaCuO. On y présente un dispositif de pilotage de la croissance grâce à la diffraction d'électrons rapides RHEED, comprenant également des logiciels d'analyse permettant de corréler l'évolution du diagramme RHEED, avec les propriétés physiques (composition, structure et morphologie, transport ...). Cette analyse, appliquée au cas de films appauvris en Bi, permet de les décrire comme une nanostructure d'intercroissance, en partie ordonnée suivant un modèle " mur de briques " où deux types de nanophases alternent en quinconce : Bi-2212 et Bi-2PRQ d'épaisseur double. Selon la composition moyenne des films, trois familles de nanophases 2PRQ sont identifiées, qui correspondent à des modèles structuraux spécifiques : stoechiométriques Bi-2267, riches en Sr Bi-2446, riches en Cu Bi-2429 comportant des plans Cu2O3 de type échelles. Les conditions physiques pour la synthèse de chaque famille nanostructurée sont décrites.