In this thesis, the physical properties of certain multi-functional organic crystals were studied in detail. This study involves the growth of single crystals of Glucuronic acidγ-lactone (GAL), Imidazoliumtartarate (IMLT), (Bis)imidazoliumtartarate (BIMLT), and Diisopropylammonium iodide (DPI) and investigations of their optical, dielectric, piezoelectric, pyroelectric, and ferroelectric properties as a function of temperature and dependence on crystal structure in these organic crystals. Piezoelectric resonance was observed at certain frequencies when dielectric constant was monitored along the b-plate of GAL crystals. The electro-mechanical coupling coefficient estimated at the resonance near 1 MHz frequency revealed an exceptionally large value in GAL similar to that in inorganic lead titanate. The dependence of the piezoelectric resonance frequency on temperature was studied in detail. These crystals showed excellent second- and third-order nonlinear optical properties as well as high laser damage threshold. The high values of χ(2) andχ(3), laser damage threshold, and low UV cut-off makes GAL crystals an interesting prospect for NLO and laser applications. Towards this goal, GAL crystals were studied in detail with regard to determination of directions of dielectric axes, optic axes, and collinear phase-matching. Single crystals of another promising NLO organic crystal, IMLT were also grown which showed interesting dielectric, piezoelectric, and NLO properties. The dielectric dispersion with temperature provided an insight to the polarization mechanisms. Like GAL, IMLT also exhibits piezoelectric resonance. The existence of only one easy axis of vibration in IMLT enabled the candidate to identify the first resonance peak as corresponding to the fundamental mode of oscillation in the sample. This also helped to determine many piezoelectric parameters. By angular phase matching, one direction of phase matching in IMLT was identified. The conversion efficiency of IMLT along this direction was determined which was high in comparison to that in a standard KDP crystal. At piezoelectric resonance frequencies, the electro-optic response due to photo-elastic contributions is enhanced. Single crystals of organic ferroelectric BIMLT were grown by mixing two moles of imidazole with one mole of l-tartaric acid. The controversy with regard to the phase transition temperature of BIMLT was clarified by the DSC and structural analysis in this work. Previously, studies on BIMLT were limited to polycrystalline samples and single crystals with inclusions primarily due to the difficulty in growing good quality single crystals from aqueous solution. However, by experimenting the growth process using different solvents, good quality single crystals were achieved without the trapping of mother solution. This remarkable find is a notable result in these crystals for ferroelectric applications. The mechanism of ferroelectricity in BIMLT is mainly attributed to the transfer of protons along N–H---O hydrogen bonds in the direction of b-axis. Interestingly, the values of spontaneous polarization and Curie-temperature in the organic ferroelectric material DPI were significantly high and comparable to several popular inorganic ferroelectrics. The polarization obtained in this material is the highest among reported organic ferroelectrics. In addition to the high Curie temperature and spontaneous polarization, there were unique phase transitions that were revealed in DPI. The mechanism of ferroelectricity is quite complex, mainly being displacive type on account of the change in orientation of dipoles with electric field. Some contribution to ferroelectricity comes from the order-disorder nature of Nitrogen atom.

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No. of bitstreams: 1 TeseRRGP.pdf: 3041523 bytes, checksum: f8585bab1f9c1565717516794f4e8831 (MD5) Previous issue date: 2015-09-04 / Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES) / This study analyses the relationships between synthesis routes and physical properties of the composite system 67.5(PbMg1/3Nb2/3O3) +32.5(PbTiO3), or simply PMN-PT, as ferroelectric phase and BaFe12O19, or BaM, as magnetic phase. The choice of phases was based on the exceptional properties that both PMN-PT and BaM possess: solid solutions of the complex perovskite PMN-PT in both monocrystalline and polycrystalline forms, particularly those whose composition lies within the region of morphotropic boundary phases, have the largest known piezoelectric coefficients. BaM, or barium hexaferrite, presents relatively high property anisotropy due to its hexagonal crystal structure (expressed in particles that grow in nonequiaxed format) and easy magnetization along the c-Crystallographic axis. Thus, the main objective of this work was to obtain and characterize magnetoelectric composites (either volumetric or as two-dimensional nanostructures) textured from PMN-PT/BaM, by exploiting the quasi-piezomagnectic characteristics and the microstructural, crystallographic and magnetic anisotropyof the BaM phase. With a molar ratio of 80/20 between the ferroelectric and magnetic phases, different routes of synthesis and processing were used for the production of threedimensional ceramic composites with 0-3 connectivity, or thin films with 0-3 and 2-2 connectivity.The Pechini, sol-gel, co-precipitation,and solid state reaction techniques were applied for the synthesis of powders and/or solutions; the pressure-assisted sintering method was used for the densification of three-dimensional bodies; and the spin-coating technique was employed for the deposition of films. Physical, electrical, magnetic and magnetoelectric characterizations were performed in order to clarify the influence of the BaM phase upon composites of different configurations. In a prospective yet not exhaustive manner, relations were assessed among the experimental parameters of the various synthesis routes (with greater focus on the barium hexaferrite phase) and the production of ceramic composites of PMNPT/ BaM system. It was found that the final characteristics of the prepared materials, particularly the hysteresis behavior of the magnetoelectric coefficient as a function of applied magnetic field, were highly susceptible to variations in the morphology, size and orientation of barium hexaferrite grains, which, in turn, depended on the synthesis and sintering routes applied. / Realizaram-se estudos de síntese e de caracterização das propriedades físicas do sistema compósito 67,5(PbMg1/3Nb2/3O3) +32,5(PbTiO3), ou simplesmente PMN-PT, como fase ferroelétrica, e da BaFe12O19, ou BaM, como fase magnética. A escolha dessas fases baseou-se nas propriedades excepcionais que ambas apresentam. A perovskita complexa PMN-PT, tanto na forma monocristalina como policristalina, apresenta soluções sólidas com os maiores coeficientes piezoelétricos conhecidos, particularmente as de composição na região do contorno morfotrópico de fases, como é o caso da 32,5%mol de PT. A fase BaM, ou hexaferrita de bário, apresenta relativamente alta anisotropia de propriedades magnéticas devido à sua estrutura cristalográfica hexagonal (refletida em partículas que crescem em formato não equiaxial) e fácil magnetização ao longo do eixo cristalográfico-c. O objetivo principal deste trabalho foi a obtenção e a caracterização de compósitos magnetoelétricos (volumétricos ou como nanoestruturas bidimensionais) texturados de PMN-PT/BaM, explorando-se as características quasi-piezomagnéticas e a anisotropia microestrutural/cristalográfica/magnética da fase BaM. Com uma proporção molar de 80/20 entre a fase ferroelétrica e a magnética, foram utilizadas diferentes rotas de síntese e de processamento de materiais para a produção de compósitos com conectividade 0-3, quando no caso de corpos cerâmicos volumétricos; ou 0-3 e 2-2, quando no caso de filmes finos. Os métodos Pechini, sol-gel, de copreciptação e de reação no estado sólido foram utilizadas na síntese dos pós e/ou soluções; o método de sinterização assistida por pressão, para a densificação dos corpos volumétricos, e a técnica “spin-coating”, para a deposição dos filmes. As caracterizações físicas, elétricas, magnéticas e magnetoelétricas buscaram evidenciar a influência das propriedades da fase BaM nas diferentes configurações de compósitos. De forma prospectiva e ainda não exaustiva, foram avaliadas as relações entre os parâmetros experimentais das diversas rotas de síntese (com maior foco na fase hexaferrita de bário) e a produção de compósitos cerâmicos do sistema PMN-PT/BaM. Encontrou-se que as características finais dos materiais preparados, em especial o comportamento histerético do coeficiente magnetoelétrico em função do campo magnético aplicado, foram altamente susceptíveis às variações da morfologia, tamanho e orientação dos grãos da hexaferrita de bário, que, por sua vez, dependem das rotas de síntese e de sinterização aplicadas.

A presente tese descreve a síntese e caracterização de 10 novas séries de moléculas na forma de banana contendo os anéis isoxazolina e isoxazol como reais candidatos na preparação de cristais líquidos polares. Foram avaliados parâmetros estruturais tais como o tipo de função conectora do centro curvado com os braços mesogênicos, a natureza do heterociclo e a sua posição relativa ao núcleo. A síntese dos compostos contou com a metodologia de preparação do anel isoxazolina, a cicloadição [3+2] 1,3-dipolar entre alcenos e óxidos de nitrila, os quais foram gerados pelas oximas preparadas a partir de aldeídos alifáticos e aromáticos. Todas as isoxazolinas foram oxidadas aos seus respectivos isoxazóis utilizando dióxido de manganês. Foram utilizadas ainda reações de alquilação, redução, desproteção, hidrogenólise, olefinação, adição de aminas à aldeídos e esterificação. Todas as moléculas sintetizadas foram caracterizadas por RMN de 1H e 13C, além de serem observadas por MOLP para determinação dos seus pontos de fusão. As moléculas que apresentaram comportamento mesomórfico foram ainda caracterizadas por DSC, XRD e voltagem triangular. No capítulo 3 é descrita a síntese dos isoftalatos 19a-b, 20a-b, 26a-b e 27a-b. No subgrupo dos Isoftalatos derivados de isoxazóis e isoxazolinas 3,5-diarilsubstituídos foi possível a síntese apenas do composto 11d que não apresentou comportamento líquido cristalino No subgrupo dos isoftalatos derivados de isoxazóis e isoxazolinas 3-alquil-5-arilsubstituídos as isoxazolinas 19a-b não apresentaram comportamento líquido-cristalino. Foram encontradas mesofases para os compostos 20a-b que ainda não foram determinadas com as técnicas disponíveis. Os isoxazóis 20a-b apresentaram uma provável Blue Phase logo após o resfriamento do isotrópico, que rapidamente se converte em uma provável mesofase monotrópica ferroelétrica com texturas e padrão de XRD peculiares até então não observada na literatura. No subgrupo dos isoftalatos derivados de isoxazóis e isoxazolinas 3-aril-5-alquilsubstituídos 26a-b e 27a-b não foi observado comportamento líquido-cristalino. O capítulo 4 descreve a síntese das isoftaliminas 35, 36, 44, 45, 50a-b, 51a-b, 56a-d, 57a-d, 63a-b e 64a-b. No subgrupo dos isoxazóis e isoxazolinas 3,5-diarilsubstituídos 35, 36, 44 e 45 foram observadas as mesofases B7 e B1 apenas com a inversão da orientação do anel isoxazol como braçomesogênicos dos compostos finais, enquanto que as isoxazolinas não apresentaram mesofases. A mesofase B7 do composto 36 apresentou comportamento antiferroelétrico enquanto que a mesofase B1 do composto 45 não mostrou resposta frente ao campo elétrico aplicado, além disso, o XRD mostrou que tal mesofase colunar B1 pode ser uma fase 3D modulada. No subgrupo das isoxazolinas e isoxazóis 3-alquil-5-arilsubstituídos 50a-b e 51a-b foram observadas fases do tipo DC para as isoxazolinas 50a-b, a qual deve ser confirmada por FFTEM. No subgrupo dos materiais 3-aril-5-alquilsubstituídos 56a-d, 57a-d, 63a-b e 64a-b foram observadas mesofases SmXPF para os compostos 56b-d. Os isoxazóis 57a-d apresentaram texturas similares, porém não apresentaram mesofase, mas os mesmos seguem o mesmo padrão de difração das isoxazolinas do capítulo 3. Apenas a isoxazolina 63b dos compostos perfluorados apresentou mesofase No capítulo 5 é descrita a síntese de ésteres não-simétricos contendo os heterociclos isoxazol e isoxazolinas como núcleo central 71a-f, 82, 83, 84 e 85. No primeiro subgrupo todos os ésteres cinâmicos 71a-f apresentaram comportamento mesomórfico com grandes faixas de temperaturas nas mesofases. No segundo subgrupo as isoxazolinas 82 e 83 apresentaram comportamento completamente distinto, onde só foi observada a formação de uma mesofase SmB para o composto que tem a posição éster localizada na direção do nitrogênio do heterociclo. Já os isoxazóis 84 e 85 deste subgrupo apresentaram as mesofases N e SmC em temperaturas bastante similares, porém, a observação desses materiais em uma cela alinhada revelou o crescimento de filamentos na transição N-SmC apenas para o composto 85, o qual também possui a porção éster na direção do nitrogênio do anel isoxazol. O capítulo 6 traz a síntese dos ésteres e iminas simétricos 88, 89, 94 e 95 utilizando os heterociclos como núcleo central, os quais apresentaram mesofases SmC e N. Além disso, o diéster 89 derivado de isoxazol apresentou a mesma característica que o composto 85 do capítulo 5, apresentando uma transição N-SmC com crescimento de filamentos perpendiculares à direção de alinhamento da amostra dentro da cela, podendo estar relacionada à uma mesofase NTB. / This thesis describe the synthesis and characterization of 10 new series of banana shaped molecules containing the isoxazoline and isoxazole rings as real players for preparation of polar liquid crystals. It was evaluate structural parameters such as the type of connecting function of the bent core with the mesogenic arms, the heterocycle nature and its position relative to the central core. The synthesis of the compounds included the methodology of preparation of the isoxazoline ring, the [3 + 2] 1,3-dipolar cycloaddition between alkenes and nitrile oxides, which were generated by the oximes prepared from aliphatic and aromatic aldehydes. Furthermore, all isoxazolines were oxidized to its respective isoxazoles using manganese dioxide. Besides the described methodologies, alkylation, reduction, deprotection, hydrogenolysis, olefination, addition of amines to the aldehydes and esterification reactions were used. All the synthesized molecules were characterized by 1H NMR and 13C NMR, and also observed by POM for determination of its melting points. The molecules previously analyzed by POM that showed mesomorphic behavior were characterized by DSC, XRD and triangular voltage still. Chapter 3 describes the synthesis of isophthalates 19a-b, 20a-b, 26a-b e 27a-b. In the subgroup of isophthalates derived from isoxazoles and isoxazolines 3,5-diarylsubstituted it was possible to synthesize only compound 11d which did not show liquid crystalline behavior In the subgroup of the isophthalates derived from isoxazoles and isoxazolines 3-alkyl-5-arylsubstituted the isoxazolines 19a-b did not show liquid crystalline behavior. It was found mesophases for compounds 20a-b that still could not be determined with the available techniques. The isoxazoles 20a-b presented a probable Blue Phase soon after cooling from the isotropic which quickly converts into a probable ferroelectric monotropic mesophase with peculiar textures and pattern of XRD until then not observed in the literature. In the subgroup of the isophthalates of isoxazoles and isoxazolines 3-aryl-5-alkylsubstituted 26a-b and 27a-b no liquid crystalline behavior was observed. Chapter 4 describes the synthesis of isophthalimines 35, 36, 44, 45, 50a-b, 51a-b, 56a-d, 57a-d, 63a-b and 64a-b. In the subgroup of the isoxazoles 3,5-diarylsubstituted 35, 36, 44 and 45 the B7 and B1 mesophases were observed only with the inversion of the isoxazole ring orientation as mesogenic arm of thefinal compounds whereas the isoxazolines did not present mesophases. The B7 mesophase of the compound 36 showed antiferroelectric switching while the B1 mesophase of the compound 45 showed no response to the applied electric field, in addition, the XRD showed that such B1 columnar mesophase could be a 3D modulated phase one. In the subgroup of 3-alkyl-5-arylsubstituted isoxazolines and isoxazoles 50a-b and 51a-b DC phases were observed for isoxazolines 50a-b which should be confirmed by FFTEM. The SmXPF mesophase were observed for componds 56b-d in the subgroup of 3-aryl-5-alkylsubstituted materials 56a-d, 57a-d, 63a-b e 64a-b. The isoxazoles 57a-d presented similar textures although did not showed mesophase, but they follow the same diffraction pattern of the chapter 3 isoxazolines. Only the isoxazoline 63b of the perfluorinated compounds showed mesophase In chapter 5 is described the synthesis of non-symmetric esters containing isoxazol and isoxazolines heterocycles as central core 71a-f, 82, 83, 84 e 85. In the first subgroup all the cinnamic esters 71a-f showed mesomorphic behavior with large mesophases temperature ranges. In the second subgroup the isoxazolines 82 and 83 showed completely different behavior which only was observed the SmB mesophase formation for compound having the ester position towards the heterocycle nitrogen. Furthermore, the isoxazoles 84 and 85 of this subgroup showed the N and SmC mesophases at very similar temperatures, however, the observation of these materials in an aligned cell revealed the filamentary growth in the N-SmC transition only for compound 85, which also has the ester moiety in the direction of the isoxazole ring nitrogen. Chapter 6 brings forward the synthesis of symmetrical esters and imines 88, 89, 94 and 95 using the heterocycles as the central cores, which showed SmC and N mesophases. Moreover, the isoxazole derived diester 89 showed the same feature as compound 85 of Chapter 5, exhibiting a N-SmC transition with filament growth perpendicular to the rubbing direction of the cell which may be related to a NTB mesophase.

Cette thèse traite avec des équations aux dérivées partielles provenant de la physique mathématique. En particulier, à partir de modèles 3D ferromagnétisme et ferroélectricité, nous obtenons des modèles 1D et 2D par l'intermédiaire de processus asymptotiques basés sur des méthodes de réduction de dimension. Le modèle 3D ferromagnétisme a été proposé par W.F. Brown depuis lesannées 40. Il est également possible d'utiliser un modèle dynamique, décrivant l'aimantation au cours du temps, en utilisant un système introduit par L.D. Landau et E.M. Lifschitz en 1935. Pour le modèle ferroélectrique, nous nous référons aux papiers de P. Chandra et P.B. Littlewood, W. Zhang et K. Bhattacharya et au livre de T. Mitsui, I. Taksuzaki et E. Nakamura.Ma thèse est constituée de trois parties :Au début, je considère l'énergie micromagnétique avec des coefficients dégénératifs dans un fil mince. Après avoir montrer l'existence de minimiseurs du problème, j'identifie l'énergie limite lorsque la section du fil tend vers zéro.Dans la deuxième partie, j'étudie le comportement asymptotique des solutions dépendant du temps des problèmes micromagnétique dans une multi-structure constituée de la jonction de deux fils minces. En supposant que les volumes des deux fils tendent vers zéro avec la même vitesse. On obtient un problème limite couplé par une condition de jonction. Le problème limite reste non-convexe, mais devient complètement local.Dans le dernier chapitre, à partir d’un modèle variationnel 3D non convexe et non-local pour la polarisation électrique dans un matériau ferroélectrique, et à l'aide d'un processus asymptotique basé sur la réduction de dimension, j'analyse des phénomènes de jonction pour deux films minces ferroélectriques joints orthogonaux. Selon la façon dont la réduction se passe, on obtienttrois modèles différents de dimension 2. On remarque qu’un effet de mémoire du processus de réduction apparaît, ce dernier dépend de la compétition entre les épaisseurs des deux films: Le paramètre de guidage est la limite du rapport des épaisseurs des deux films / This thesis deals with partial differential equations coming from mathematical physics. Particularly, starting from 3D models for ferromagnetism and ferroelectricity, we derive 1D and 2D models via asymptotic processes based on dimensional reduction methods. The 3D model for ferromagnetism was proposed by W.F. Brown in the 40s and it is based on a system introduced by L.D. Landau and E.M. Lifschitz in 1935. About the ferroelectric model, we refer tothe papers of P. Chandra and P.B. Littlewood, W. Zhang and K. Bhattacharya and to the book of T. Mitsui, I. Taksuzaki, and E. Nakamura.This thesis based on three works:At the beginning, we consider micromagnetic energy, with some degenerating coefficients, in a thin wire. After showing the existence of minimizers, we identify the limit energy as the section of the wire vanishes.In the second part, we study the asymptotic behavior of the solutions of a time dependent micromagnetic problem in a multi-structure consisting of two joined thin wires. We assume that the volumes of the two wires vanish with same rate. We obtain two 1D limit problems coupled by a junction condition on the magnetization. The limit problem remains non-convex, but now it becomes completely local.In the last chapter, starting from a non-convex and nonlocal 3D variational model for the electric polarization in a ferroelectric material, and using an asymptotic process based on dimensional reduction, we analyze junction phenomena for two orthogonal joined ferroelectric thin films. We obtain three different 2D-variational models for joined thin films, depending on how the reduction happens. We note that, a memory effect of the reduction process appears, and it depends on the competition of the relative thickness of the two films: The guide parameter is the limit of the ratio between these two small thickness

Pós nanocristalinos de Ba1-xCaxTiO3(0≤ x ≤ 0.30) foram sintetizados pela primeira vez por meio do método dos precursores poliméricos modificados, em temperaturas relativamente baixas (500°C). Para a densificação dos corpos cerâmicos duas técnicas distintas foram utilizadas: a sinterização convencional, utilizando um forno elétrico; e a sinterização a laser, na qual um laser de CO2 foi utilizado como principal fonte de calor. Os corpos cerâmicos sinterizados pelas duas técnicas apresentaram um tamanho médio de grãos em torno de 500 nm, porém uma maior densidade relativa foi obtida nas cerâmicas sinterizadas a laser, chegando a 99%, além de boa transparência, ∼42% a 940 nm para a amostra com 30 mol% de Ca com espessura de 0.5 mm. Também verificamos por meio de simulação numérica, que a equação de condução de calor na aproximação linear, considerando uma fonte de calor com perfil gaussiano, descreve qualitativamente o comportamento observado durante a sinterização a laser no seu estágio final. Por meio da técnica de espectroscopia de impedância foi feita a caracterização dielétrica dos corpos cerâmicos, nos quais três pontos principais foram estudados: i) o efeito do tamanho de grãos; ii) a influência da concentração de Ca; e iii) a influência do método de sinterização. Com a variação do tamanho do grão foram observadas mudanças na intensidade do pico de transição ferro-paraelétrica, na temperatura de Curie e na permissividade relativa à temperatura ambiente. Para concentrações de Ca até 15 mol%, as cerâmicas apresentaram uma transição de Curie estreita semelhante ao BaTiO3,enquanto que para concentrações maiores, uma transição de fase difusa foi observada. A sinterização a laser resultou em corpos cerâmicos com constante dielétrica 30% maior, e menor perda dielétrica do que as cerâmicas sinterizadas convencionalmente. Finalmente, foi proposto um modelo baseando-se na formação de vacâncias de oxigênio para o aumento da condutividade elétrica com a substituição de Ca. / Ba1-xCaxTiO3 (0 ≤ x ≤ 0.30) nanocrystalline powders were successfully synthesized for the first time at relative low temperature (500 °C) by a modified polymeric precursor method. The densification of the ceramics was made by two distinct techniques: conventional sintering using an electric furnace; and by a laser sintering process in which a CO2 laser is used as the main heating source. It was achieved dense ceramics with an average grain size about 500 nm from both techniques. However, the laser sintered ceramics presented a higher relative density (99 %) and a transparency of 42% at 940 nm in the sample with 30 mol% of Ca. By numerical simulation of the thermal conduction equation on the linear approximation case and taking account a thermal source with a gaussian profile, it was possible to describe qualitatively the final stage of the laser sintering process. The dielectric characterization of the ceramic bodies were carried out by the impedance spectroscopy technique and three main effects were studied: i) the grain size effect; ii) the Ca concentration influence; and, iii) the sintering technique influence. Modifying the grain size led to changes in the ferro-paraelectric transition magnitude, on the Curie temperature value and in the relative permittivity at room temperature. For Ca2+ concentrations up to 15 mol% the sintered ceramics presented a sharp Curie transition like BaTiO3,while for higher Ca concentrations a diffuse phase transition was observed. The laser sintered ceramics presented a dielectric constant 30% higher than the conventional sintering and a lower dielectric loss. Finally, we have proposed a model based on the oxygen vacancies formation to explain the conductivity increase with the Ca2+ substitution.

Este trabalho descreve um estudo sistemático da influência da adição do átomo de lantânio na estrutura da fase Bi4Ti3O12 (BIT) e do átomo érbio na fase Bi3,25La0,75Ti3O12 (BLT075) no que tange seu processo de síntese e suas propriedades estruturais, microestruturais e elétricas. Cerâmicas de composição nominal Bi4-xLaxTi3O12 (BLTx) com 0 x 2 mol % e Bi3,25La0,75Ti3O12 (BLT075) com substituição no sítio do La3+ (BLExT) e no sítio do Ti4+ (BLTEx) com 0 x 0,06 mol %, foram preparadas através do método de síntese por reação do estado sólido. Os dados de difração de raios X (DRX) das amostras BLTx mostram a formação de uma solução sólida para todas as amostras, exceto para amostra contendo 2 mol% de La3+. Verificou-se que a adição de La3+ leva a um aumento da temperatura de sinterização e diminui o tamanho médio dos grãos, alterando sua morfologia de grão na forma de placas para uma forma mais esférica. Quanto às propriedades dielétricas, amostras BLTx com x 1 mol% apresentam um comportamento característico de um ferroelétrico normal, enquanto que quando x > 1 mol%, observa-se um pequeno deslocamento da temperatura de máximo da permissividade dielétrica (Tm) com a freqüência, indicando a existência de um comportamento típico de materiais ferroelétricos relaxores. Os resultados de espectroscopia Raman sugerem que os íons La3+ tendem a ocupar preferencialmente o sítio do Bi3+ das camadas peroviskitas quando x < 1,0 mol %, enquanto que quando x >1,0 mol %, o processo de incorporação também ocorre no sítio do Bi3+ nas camadas de Bi2O2. De acordo com a analise dos espectros XANES e XPS, a estrutura local e eletrônica dos átomos de Ti, Bi e La, não são afetadas de forma significativa pela adição de lantânio.Em relação às amostras dos sistemas BLExT e BLTEx, os dados de DRX mostram somente a presença de fases secundárias nas composições x= 0,04 e 0,06 mol% do sistema no BLTEx. A sinterização à 1115oC possibilitou obter amostras apresentando uma densidade relativa superior a da amostra não dopada BLT075. A adição de Er3+ causa mudanças na morfologia, diminuindo o tamanho médio dos grãos no sistema BLExT e aumentando no sistema BLTEx. Através de medidas elétricas, foi observado um decréscimo no valor Tm em ambos os casos. Quando x > 0,02 mol%, o comportamento de Tm é dominado pelo limite de solubilidade para o sistema BLExT. De acordo com os dados de XAS, a estrutura local e eletrônica dos átomos de Ti e Er não são afetadas de forma significativa pela adição de érbio. / This work describes a systematic study of the influence of the lanthanum atom addition in the Bi4Ti3O12 (BIT) phase and the erbium atom addition in the Bi3,25La0,75Ti3O12 (BLT075) phase in terms of their synthesis process and its structural, microstructural and electrical properties. Ceramics of nominal composition Bi4-xLaxTi3O12 (BLTx) with 0 x 2 mol% and Bi3,25La0, 75Ti3O12 (BLT075) with Er3+ replacing the La3+ atoms (BLExT) and replacing Ti4+ atoms (BLTEx) with 0 x 0, 06 mol%, were prepared by the solid state reaction method. X-ray diffraction (XRD) data of BLTx samples shows the formation of a solid solution for all samples, except for sample containing 2 mol% of La3+. It was found that the addition of La3+ leads to an increase in the sintering temperature, a decrease in the average size of grains and a modification on the grain from plates to a more spherical morphology. The dielectric properties of BLTx samples with x 1 mol% show a behavior characteristic of a normal ferroelectric whereas when x> 1 mol%, there is a small displacement of the temperature of maximum dielectric permittivity (Tm) with the frequency, indicating the existence of a typical behavior of a relaxor ferroelectric material. The Raman spectroscopy results suggest that La3+ ions tend to preferentially occupy the Bi3+ site in the peroviskite layer when x <1.0 mol%, whereas when x> 1.0 mol%, the process of incorporation occurred also in the Bi3+ site of the Bi2O2 layer. According to the analysis of XANES and XPS spectra, the local structure of atoms and electronic structure of Ti, Bi and La atoms of BLTx samples are not affected significantly by the addition of lanthanum. For samples of BLExT and BLTEx systems, the XRD data shows only the presence of a secondary phase in the x = 0.04 and 0.06 mol% compositions of the BLTEx system. The sintering at 1115 °C allowed to obtain samples presenting a relative high density than the sample BLT075 undoped sample. The addition of Er3+ induces significative changes in grain morphology by decreasing the average size of grains in the BLExT system and by increasing the BLTEx system. Through electrical measurements, it was observed a decrease in the Tm value in both cases. In the BLExT system, when x> 0.02 mol%, the behavior of Tm is dominated by the solubility limit. According to the XAS data, the local and electronic structure of Ti and Er atoms are not affected significantly by the addition of erbium.

Orientador: Lisandro Pavie Cardoso / Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Fisica Gleb Wataghin / Made available in DSpace on 2018-08-06T02:28:50Z (GMT). No. of bitstreams: 1 DosSantos_AdenilsonOliveira_D.pdf: 4430176 bytes, checksum: 30089a1aff00bfd64635f23601dd3039 (MD5) Previous issue date: 2006 / Resumo: Como primeira contribuição deste trabalho, as varreduras Renninger (VR) da difração múltipla de raios-X foram empregadas no estudo da transição de fase estrutural do Sal de Rochelle (monoclínica-ortorrômbica) induzida por temperatura. Devido ao caráter tridimensional e sensibilidade dessa técnica acompanhamos as deformações na célula unitária com a temperatura, através do deslocamento dos picos secundários com maior sensibilidade. Foi possível determinar os parâmetros de rede e simular cada VR com o programa UMWEG. Os picos secundários de 4-feixes ( 0 0 0 ) ( 0 0 10 )( 1 0 9 )(1 0 1 ) e (0 0 0 )( 0 0 10 )( 2 3 0 )(2 3 10 ) da fase ortorrômbica foram medidos na VR para 24ºC (Tc). Os coeficientes de expansão térmica do sal de Rochelle também foram obtidos, e estão em bom acordo com a literatura. Como segunda contribuição, usamos a VR na determinação precisa dos parâmetros de rede dos materiais magnetocalóricos PrAl2, NdAl2e PrNi5. Implementamos uma rotina baseada na simulação da VR com o programa UMWEG, através da qual escolhe-se o comprimento de onda adequado para a medida de picos secundários muito sensíveis à distorção na célula unitária. Na aplicação no caso do PrAl2 usamos o caso de 4-feixes ( 0 0 0 )( 6 0 0 )( 1 3 7 )( 7 3 7 ) com 2.... =6.663(3)º e obtivemos com grande precisão a=8,03332(7)Å. O efeito de polimento mecânico na superfície dessa amostra foi analisado pelo mapeamento das reflexões de superfície (BSD) e o comportamento mosaico do cristal foi evidenciado. Nas outras medidas, como utilizamos a mesma geometria da estação XRD1, não foi possível obter a melhor condição para a rotina apresentada, mas foram obtidos para o NdAl2 (a=7,9972(5)Å) e PrNi5 (a=4,9590(8)Å e c=3,9794(5)Å) com boa precisão. Outra contribuição foi o estudo do efeito de campo elétrico no cristal orgânico MBANP através do monitoramento por curvas de rocking da reflexão ( 10 0 0 ). Observou-se uma histerese "asa de borboleta", ainda não observada em cristais orgânicos, e sem modelo para cristais monoclínicos. Cálculos usando mecânica quântica para moléculas isoladas de MBANP mostram que as principais características da forma de histerese podem ser explicadas em termos de mudanças induzidas pelo campo elétrico nos perfis de carga e na geometria de moléculas isoladas de MBANP / Abstract: As the first contribution of this work, the Renninger scan (RS) of the X-ray multiple diffraction were used in the study of the Rochelle salt structural phase transition (monoclinic-orthorhombic) induced by temperature. Due to its three-dimensional feature and sensitivity of the technique was possible to follow the unit cell deformations with temperature, through the angular shifts of the most sensitive secondary peaks. We were able to determine the lattice parameters as well as to simulate each RS by using the UMWEG program. The ( 0 0 0 )( 0 0 10 )( 1 0 9 )(1 0 1 ) and ( 0 0 0 )( 0 0 10 )( 2 3 0 )(2 3 10 ) 4-beam peaks for the orthorhombic phase were measured in the RS at 24ºC (Tc). Rochelle salt thermal expansion coefficients were also obtained in good agreement with literature values. As the second contribution, we have also used the RS in the precise lattice parameter determination of PrAl2 , NdAl2 and PrNi5 magnetocaloric materials. We have implemented a routine based on the RS simulation (UMWEG program), through which, one can choose the adequate wavelength to measure the most sensitive secondary peaks to the unit cell variations. The application of thid method in the case of PrAl 2, has allowed to measure the ( 0 0 0 )( 6 0 0 )( 1 3 7 )( 7 3 7 ) 4- beam case that presents 2.... =6.663(3)º and hence, to determine a=8.03332(7)Å, with high precision. PrAl2surface polishing effect was also analyzed by the secondary surface peak (BSD) mapping, through which, the crystal mosaic behavior was exhibited. For the other crystals, the same LNLS geometry was used and the best condition to applying the routine could not be obtained, however good precision lattice parameters were obtained for NdAl2 (a=7.9972(5)Å) and PrNi5 (a= 4.9590(8)Å and c= 3.9794(5)Å). Another contribution to the study of the electric field application in the MBANP organic crystal through the monitoring of ( 10 0 0 ) rocking curves was performed. It was observed a (butterfly wing) hysteresis, not yet observed for organic crystals and with no model suggested for monoclinic crystals. Quantum mechanical calculations on isolated MBANP molecules show that the main features of the hysteresis shape can be explained in terms of field-induced changes in the charge profiles and geometry of isolated MBANP molecules / Doutorado / Física da Matéria Condensada / Doutor em Ciências

O presente trabalho teve como objetivo o estudo das propriedades elétricas e estruturais das amostras cerâmicas pertencentes ao sistema Ba1-xRxTi1-yZryO3 (R=Ca,Sr). As amostras na forma de pó micro ou nanoestruturadas foram respectivamente obtidas através do método de mistura de óxidos e do método dos precursores poliméricos. Amostras cerâmicas apresentando grãos em uma escala micrométrica foram obtidas através do método tradicional de sinterização em alta temperatura enquanto amostras cerâmicas nanoestruturadas foram obtidas através da técnica de sinterização por plasma (Spark plasma Sintering ou SPS). Os resultados obtidos através da técnica de espectroscopia de impedância mostraram que com o aumento da quantidade de Zr na matriz as amostras passam de um estado ferroelétrico normal para um estado ferroelétrico relaxor e que este efeito é mais pronunciado nas amostras contendo cálcio. A partir dos resultados da difração de raios X em alta resolução, foi possível determinar os processos de transição de fase em função da substituição dos átomos de Ti por Zr além de identificar um processo de transição de fase espontânea na amostra contendo cálcio e 18 mol % de zircônia. Através das medidas do espectro de absorção de raios X e do espectro Raman foi possível mostrar que, independente da composição e da estrutura a longa distancia, apresentam certo grau de desordem local e que esta desordem local está principalmente associada ao fato do átomo de titânio estar fora de sua posição centro simétrica no octaedro TiO6 e que está desordem é comparável a observada no composto BaTiO3 tetragonal. A desordem química devido ao aumento da quantidade de átomos de Zr na matriz associada a esta desordem local levam ao aparecimento do estado relaxor. Finalmente, o estudo das amostras preparadas por SPS mostraram que é possível obter amostras de composição BaTi0,80Zr0,20O3 apresentando uma alta densidade e tamanho de grão nanométrico. Os resultados da espectroscopia de impedância destas amostras mostraram devido ao pequeno deslocamento da temperatura de máximo e do alargamento da curva de permissividade com a diminuição do tamanho de grão, não foi possível classificar essa amostra como apresentando um comportamento típico de um material ferroelétrico relaxor. / This work aimed to study the structural and electrical properties of ceramic samples belonging to the Ba1-xRxTi1-yZryO3 (R = Ca, Sr) system. The powder samples presenting a micro or nanosize were respectively obtained by using a mixture of oxides and by the modified polymeric precursor methods. Micrometer scale ceramic samples were obtained through the traditional method of sintering at high temperature while nano-sized particles ceramics were obtained using the spark Spark Plasma Sintering (SPS) technique. The results obtained using the technique of impedance spectroscopy showed that with an increasing amount of Zr in the matrix, samples change from a normal ferroelectric state to a relaxor ferroelectric state and that this effect is more pronounced in samples containing calcium. From the results of high resolution X-ray diffraction technique, it was possible to determine the phase transition processes due to the substitution of Ti atoms by Zr and, in addition, identify a process of spontaneous phase transition in the sample containing calcium and 18 mol% of zirconium. From the measurements of X-ray absorption Spectroscopy and Raman spectra it was possible to show that regardless of the composition and structure of long range order, the samples have some degree of local disorder and that this local disorder is primarily associated with the fact that the titanium atom being out of its symmetrical center position in the octahedron and is TiO6 disordered. This is comparable to the distorsion observed in tetragonal BaTiO3 sample. The chemical disorder due to the increase of Zr atoms in the matrix associated with this disorder is responsible of the occurrence of relaxor state. Finally, the study of samples prepared by SPS showed that it is possible to obtain samples with BaTi0,80Zr0,20O3 composition with a high-density and nanometeric grain size. The results of impedance spectroscopy on these samples show a small shift of the maximum temperature and a slight broadening of the permittivity curve with decreasing grain size. However, this result does not allowed to classify the samples as having a typical relaxor ferroelectric material behavior.

Organometal halide perovskite absorbers such as methylammonium lead iodide chloride (CH3NH3PbI3-xClx), have emerged as an exciting new material family for photovoltaics due to its appealing features that include suitable direct bandgap with intense light absorbance, band gap tunability, ultra-fast charge carrier generation, slow electron-hole recombination rates, long electron and hole diffusion lengths, microsecond-long balanced carrier mobilities, and ambipolarity. The standard method of preparing CH3NH3PbI3-xClx perovskite precursors is a tedious process involving multiple synthesis steps and, the chemicals being used (hydroiodic acid and methylamine) are quite expensive. This work describes a novel, single-step, simple, and cost-effective solution approach to prepare CH3NH3PbI3-xClx thin films by the direct reaction of the commercially available CH3NH3Cl (or MACl) and PbI2. A detailed analysis of the structural and optical properties of CH3NH3PbI3-xClx thin films deposited by aerosol assisted chemical vapor deposition is presented. Optimum growth conditions have been identified. It is shown that the deposited thin films are highly crystalline with intense optical absorbance. Charge carrier separation of these thin films can be enhanced by establishing a local internal electric field that can reduce electron-hole recombination resulting in increased photo current. The intrinsic ferroelectricity in nanoparticles of Barium Titanate (BaTiO3 -BTO) embedded in the solar absorber can generate such an internal field. A hybrid structure of CH3NH3PbI3-xClx perovskite and ferroelectric BTO nanocomposite FTO/TiO2/CH3NH3PbI3-xClx: BTO/P3HT/Cu as a new type of photovoltaic device is investigated. Aerosol assisted chemical vapor deposition process that is scalable to large-scale manufacturing was used for the growth of the multilayer structure. TiO2 and P3HT with additives were used as ETL and HTL respectively. The growth process of the solar absorber layer includes the nebulization of a mixture of PbI2 and CH3NH3Cl perovskite precursors and BTO nanoparticles dissolved in DMF, and injection of the aerosol into the growth chamber and subsequent deposition on TiO2. While high percentage of BTO in the film increases the carrier separation, it also leads to reduced carrier generation. A model was developed to guide the optimum BTO nanoparticle concentration in the nanocomposite films. Characterization of perovskite solar cells indicated that ferroelectric polarization of BTO nanoparticles leads to the increase of the width of depletion regions in the perovskite layer hence the photo current was increased by one order of magnitude after poling the devices. The ferroelectric polarization of BTO nanoparticles within the perovskite solar absorber provides a new perspective for tailoring the working mechanism and photovoltaic performance of perovskite solar cells.

Les cristaux liquides sont des matériaux organiques utilisés pour réaliser des dispositifs électroniques ; avant de les intégrer dans des applications, il est nécessaire d'étudier leurs propriétés physico-chimiques et diélectriques pour optimiser leurs performances. Ce travail de thèse est consacré aux nanocolloïdes obtenus par dispersion de nanoparticules ferroélectriques dans un cristal nématique ; il s'agit d'étudier l'influence des inclusions sur les transitions de phases et sur les propriétés diélectriques de la matrice. L'étude des transitions de phases à l'aide de l'Analyse Enthalpique Différentielle (AED) a mis en évidence l'influence des nanoparticules ferroélectriques ; ceci résulte de deux principaux effets ; la polarisation spontanée des nanoparticules et l'ancrage entre les molécules du cristal liquide et les inclusions. La caractérisation diélectrique a révélé le couplage entre la polarisation macroscopique des inclusions et le champ électrique ; ce couplage se manifeste par une augmentation des températures de transitions de phases par rapport à celles déterminées par l'AED. La compétition entre les effets de la polarisation sous champ électrique et de l'ancrage induit une modification des permittivités (parallèle et perpendiculaire) et de l'anisotropie diélectriques. L'utilisation des nanoparticules fortement polaires sélectionnées a confirmé l'importance de la polarisation macroscopique des nanoparticules pour améliorer les propriétés des nanocolloïdes étudiés ; en effet, de très faibles quantités de ces nanoparticules donnent lieu à des améliorations plus significatives que celles obtenues par les nanoparticules brutes. / Liquid crystals are organic materials used to make electronic devices ; before using this material in applications, it is necessary to study their physical-chemical and dielectric properties in order to optimize their performance. This study is devoted to the nanocolloids obtained by dispersing ferroelectric nanoparticles in a nematic liquid crystal ; it means an inclusion influences the phase transitions temperatures and the dielectric properties of the host. The phase transitions measured by using Differential scanning calorimetry (DSC) evidenced the ferroelectric nanoparticles influence ; which is attributed two effects : the nanoparticles spontaneous polarization and the anchoring effect between nanoparticles and liquid crystal. The dielectric characterisation revealed the coupling between the macroscopic polarization of the inclusions and the electric field ; this coupling is manafested by an increase of phase transition temperatures compared to those determined by DSC. The competition between the polarization effect under an electric field and the anchoring effect induces a modification of the permittivities (parallel and perpendicular) and the dielectric anisotropy. Using harvested nanoparticles, the study confirmed the importance of the nanoparticles polarization to increase the properties of the studied nanocolloids. In fact, very small quantity of the harvested nanoparticles presents more significant improvements than those obtained with the non-harvested nanoparticles.