Made available in DSpace on 2014-10-09T12:51:59Z (GMT). No. of bitstreams: 0 / Made available in DSpace on 2014-10-09T14:07:05Z (GMT). No. of bitstreams: 0 / Nesse trabalho foram estudados os compostos intermetalicos do tipo RAg (R = Nd, Gd e Ho) por calculos teoricos desenvolvidos dentro do formalismo da Teoria do Funcional Densidade (DFT). O metodo APW+lo (Augmented Planes Waves + lo- cal orbitals) foi aplicado para resolver a equacao de Kohn-Sham e a Aproximacao do Gradiente Generalizado (GGA) usada para tratar de forma aproximada o potencial de troca-correlacao. O codigo computacional utilizado foi o WIEN2k. As atividades foram focalizadas em duas frentes. Numa delas, determinou-se a fase magnetica do estado fundamental dos compos- tos HoAg e NdAg. Para isso, simulou-se as 4 estruturas magneticas possiveis (para as celulas cristalinas cubicas) desses dois sistemas (uma ferromagnetica (0,0,0) e as antifer-romagneticas: (0,0,¼), (¼,¼,0) e (¼,¼,¼)) e com a confeccao de gra¯cos de energia das celulas cristalinas dessas estruturas magneticas pela variacao dos volumes de tais celulas, chegou-se na estrutura magnetica (¼,¼,0) como a mais provavel para o estado fundamental magnetico de ambos os compostos. Tambem observou-se que o sistema de NdAg apre- senta uma pequena diferenca entre as energias das estruturas antiferromagnetica (¼,¼,0) e ferromagnetica. Creditou-se a esse efeito a explicacao de encontrar-se na literatura re- sultados experimentais diferentes para a estrutura magnetica do composto de NdAg puro e dopado com o atomo de 140Ce (entrando no sitio do Nd). Acredita-se que a dopagem do NdAg com o atomo de 140Ce (em uma porcao reduzida), gera alteracao no sinal da integral de troca (acoplamento RKKY), mudando-o de positivo para negativo, e isso implica na modficacao da fase magnetica do estado fundamental, passando da estrutura (¼,¼,0) µa 0,0,0). Assim, com a informacao anterior da estrutura magnetica do composto de NdAg quando dopado com o atomo de 140Ce, entrou-se na segunda etapa do estudo. Nela, fez-se os calculos das estruturas eletronicas usando a aproximacao de supercelulas nos compostos de GdAg e NdAg dopados com o atomo de Ce, garantindo que esse substituisse um atomo de terra rara nas supercelulas cristalinas montadas para determinar no Ce o campo hiperfino magnetico e suas componentes geradoras. Os compostos de GdAg e NdAg (dopados com Ce), respectivamente, tiveram suas celulas cristalinas montadas ferromagnetica e antiferromagneticamente. Utilizou-se a polarizacao orbital (DFT+U) nos eletrons da camada 4f das terras raras (excluindo-se o atomo de Gd que nao apresenta momento angular). Dessa forma, em ambos os sistemas foi possivel fazer varias simulacoes, nas quais a camada 4f do atomo de Ce foi populada de maneiras diferentes, afim de se obter varios valores de momento angular e com isso diversos resultados de campo hiperfino orbital foram conseguidos; assim, automaticamente o campo magnetico hiperfino tambem assumiu diferentes valores. Escolheu-se os sub-estados da camada 4f do Ce para serem simulados por meio da regra de Hund. Como esperado o campo hiperfino magnetico orbital gerado na camada 4f e a principal componente do campo hiper¯no total no atomo de Ce e ele apresenta sinal contrario µa componente de contato. Apesar dos resultados teoricos do campo hiperfino magnetico terem consideravel discrepancia dos resultados experimentais, pode-se verificar que o unico eletron da camada 4f do atomo de Ce (nos dois compostos) possivelmente esta em um dos seguintes sub-estados da camada 4f: ml = ¡2, ml = ¡1 ou ainda uma combinacao dos dois. / Dissertação (Mestrado) / IPEN/D / Instituto de Pesquisas Energeticas e Nucleares - IPEN-CNEN/SP

As ligas de FeRh apresentam um comportamento não usual quando encontradas próximas da composição equiatômica, sendo observada uma transição de fase magnetoestrutural de primeira ordem, na qual o sistema passa de um estado antiferromagnético para um estado ferromagnético com a temperatura crítica próxima da temperatura ambiente. A temperatura crítica de transição é fortemente dependente da composição da liga, das técnicas de produção e dimensionalidade da amostra, além de fatores externos como pressão e campo magnético. No presente trabalho foram depositados, via magnetron sputtering, filmes de FeRh (monocamadas) e FeRh/Fe (bicamadas) sobre substratos monocristalinos de MgO (001), sendo utilizado duas temperaturas de deposição diferentes: 798 K e 913 K. A estrutura cristalina dos filmes foi analisada através de técnicas de medidas de difração de raios X (varredura &theta - 2 &theta, varredura em &phi e rocking curves) e as composições e espessuras dos filmes foram analisadas por medidas de RBS. A principal diferença morfológica encontrada entre as amostras foi uma melhor uniformidade na distribuição de orientações dos grãos cristalinos nos filmes depositados na temperatura mais elevada. As propriedades magnéticas, medidas por meio de um VSM equipado com um criostato e um forno, evidenciaram diferenças entre as amostras depositadas nas diferentes temperaturas mencionadas, observando-se variações significativas nas temperaturas de transição de fase e diferentes larguras dos ciclos térmicos. Também foi observado, em todas as amostras, coexistência de fases antiferromagnética e ferromagnética na camada de FeRh, principalmente na região de baixas temperaturas. As amostras depositadas em 798 K foram mais favoráveis à formação da fase FeRh antiferromagnética e, no caso das bicamadas, também apresentaram um melhor acoplamento entre as camadas de FeRh e Fe que as amostras depositadas em 913 K, favorecendo um incremento do campo coercivo e da magnetização remanente relativa do sistema. / FeRh alloys, near the equiatomic composition, present an unusual magneto structural first-order phase transition in which the system changes from antiferromagnetic to ferromagnetic state at a critical temperature close to ambient temperature. The critical transition temperature is strongly dependent on the alloy composition, production techniques and dimensionality of the sample, as well as external factors such as pressure and magnetic field. In the present work, FeRh (monolayers) and FeRh/Fe (bilayers) films were deposited on monocrystalline MgO (001) substrates, via magnetron sputtering, at two different deposition temperatures: 798 K and 913 K. The crystalline structures of the films were analyzed by using different techniques of X-ray diffraction (&theta - 2 &theta scan, &phi scan and rocking curves). The compositions and thicknesses of the films were analyzed by RBS measurements. The main morphological difference between the samples was a better uniformity in the distribution of crystalline grain orientations in the films deposited at higher temperature. The magnetic properties, which were measured by a VSM equipped with a cryostat and an oven, revealed differences between the samples obtained at different temperatures. Significant variations in the critical phase transition temperatures and different widths of thermal cycles were observed. It was also observed, in all samples, coexistence of antiferromagnetic and ferromagnetic phases in the FeRh layer, mainly at low temperatures. The samples deposited at 798 K were more favorable to the formation of the antiferromagnetic FeRh phase. In addition, for the bilayers deposited at 798 K, it was observed a better coupling between the FeRh and Fe layers in comparison to samples deposited at 913 K, favoring an increase in the coercive field and the remanence magnetization.

Nanomateriais de fct-FePt, SmCo e Carbeto de Cobalto têm sido bastante estudados para a aplicação em gravação magnética e imãs de elevado desempenho, devido as suas energias magnetocristalinas e coercividades elevadas. Nanopartículas de FePt unidimensionais foram propostas na tentativa de obter melhora no alinhamento magnético das estruturas auto-organizadas. Neste trabalho, a formação de nanobastão e nanofios de FePt foi estudada através da presença de oleilamina e pequena quantidade de monóxido de carbono liberado pelo pentacarbonilferro(0). Estes dois parâmetros foram estudados a fim de analisar a influência no alongamento das nanopartículas e verificou-se que ambos atuam sinergicamente. Foram obtidos tanto nanofios de FePt ramificados de comprimento de 20-100 nm quanto nanobastões de FePt de 20-60 nm de comprimento, ambos com diâmetro de 2-3 nm. Todas as nanopartículas sintetizadas foram obtidas na fase cúbica de face centrada e o processo de tratamento térmico nas temperaturas de 450 oC e 560 oC levou a conversão para a fase tetragonal de face centrada, com custo da sinterização das nanopartículas. Os nanobastões, entretanto, apresentaram maior estabilidade térmica se comparado com o nanofio ramificado, obtendo propriedade ferromagnética na amostra. Alternativamente, têm sido obtidos satisfatoriamente nanobastões de platina para posterior recobrimento com ferro para a formação da liga FePt após o processo de recozimento. Na síntese de SmCo, foi estudada a formação da liga diretamente por via química através do uso de redutores comumente utilizandos em síntese de nanopartículas, porém foi possível observar apenas uma pequena quantidade da liga Sm2Co17 quando se utiliza o boroidreto de sódio. Isto se deve, principalmente, ao alto potencial de redução de Sm3+ e a sua instabilidade química. Entretanto, foram desenvolvidos métodos promissores para a obtenção de nanopartículas de CoO e SmCoO com tamanho e forma controlada. Além destes sistemas, tem sido obtidas diretamente através de síntese química nanopartículas de carbeto de cobalto com coercividade de até 2,3 kOe e magnetização de 45 emu/g, além de desenvolver um método geral de síntese de carbetos de outros metais. / SmCo, fct-FePt and CoC nanomaterials have been studied for application in magnetic recording and permanent magnets due to theirs high coercivity and magnetocrystalline anisotropy. One-dimensional FePt nanoparticles were proposed to improve the magnetic alignment of self-assembled system. In this work, the formation of FePt nanorods and nanowires was studied by using a small amount of carbon monoxide from the precursor pentacarbonyliron(0) and oleylamine. Both parameters of synthesis were studied and was verified that they influence the one-dimensional growth of FePt. In fact, branched FePt nanowires with 20 - 100 nm of length and nanorods with 20 - 60 nm were obtained, both with 2-3 nm of diameters. The FePt nanoparticles were obtained in face centered cubic phase and the transformation to face centered tetragonal phase was carry out in the temperatures of 450 oC and 560 oC, which led the formation of sintered nanoparticles. FePt nanorods have better thermal stability than nanowires according the results obtained. The platinum nanorods covered with iron oxide also were obtained to formation of FePt by thermal treatment. In concern of SmCo syntheses, the formation of SmCo phase directly by chemical synthesis was investigated by using some reduction agent, but was obtained a small amount of smco phase only if the sodium borohydrate was used in the synthesis. This could be occurred due to high reducing potential of Sm3+ and its chemical instability. However, some methods were obtained to obtain CoO and SmCoO nanoparticles with size and shape control. Furthermore, cobalt carbide nanoparticles were well obtained with coercivity of 2,3 kOe and magnetization of 45 emu/g, and a new general method to obtain metals carbides was developed.

Orientadores: Adelino de Aguiar Coelho, Lisandro Pavie Cardoso / Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Física Gleb Wataghin / Made available in DSpace on 2018-08-20T22:51:31Z (GMT). No. of bitstreams: 1 Tedesco_JulioCesarGuimaraes_D.pdf: 2714279 bytes, checksum: fa378b69872d0cd459b74a0b4da48885 (MD5) Previous issue date: 2012 / Resumo: Neste trabalho propomos o estudo de algumas propriedades magnéticas e do efeito magnetocalórico (EMC) de compostos da família TbxPr1-xAl2, onde x = 0,1; 0,2; 0,25; 0,3; 0,4; 0,5 e 0,75. É fato conhecido que dois elementos terras-raras se acoplam antiferromagneticamente quando inseridos em uma rede cristalina do tipo (R,R¿)Al2 se um deles é um elemento terra-rara leve o outro pesado. Desta forma, era esperado que as amostras desta série apresentassem um ordenamento ferrimagnético, o que foi confirmado pelos nossos dados. Comparamos nossos resultados com sistemas semelhantes e com eles fomos capazes de entender a origem de algumas características e aspectos físicos dos materiais, incluindo o EMC. Alguns compostos estudados aqui apresentaram o efeito magnetocalórico inverso, que acontece devido à competição entre as duas subredes magnéticas acopladas antiferromagneticamente. Observamos também os comportamentos da temperatura de transição magnética e dos parâmetros de rede em função da concentração de Tb, e verificamos o deslocamento dos picos do EMC associados à temperatura de transição (TC). Algumas propriedades importantes na aplicação destes materiais em refrigeração magnética foram levantadas e comparadas com a literatura. Verificamos que dois membros da série apresentaram o efeito de Exchange Bias (EB) e, em analogia com sistemas bicamadas FM-AFM em filmes finos, fomos capazes de entender e explicar este efeito. Acreditamos que o efeito de Exchange Bias está associado à forte anisotropia apresentada pelos compostos Tb0.3Pr0.7Al2 e Tb0.25Pr0.75Al2 que ocorre em temperaturas extremamente baixas e à magnetização dos elétrons polarizados de condução. Identificamos também as temperaturas de compensação (propriedades características deste tipo de sistema) nestes compostos / Abstract: In this work we studied some magnetic properties and the magnetocaloric effect (MCE) of the series of compounds TbxPr1-xAl2, where x = 0.1, 0.2, 0.25, 0.3, 0.4, 0.5 and 0.75. It is known from the literature that the moments of a light and a heavy rare earth are antiferromagnetically coupled when they are inserted in a crystal lattice and this was confirmed by our analysis of the experimental data. We compared our results with similar systems and we were able to understand the origin of some features and physical aspects of those materials, including the magnetocaloric effect (MCE). Some compounds show the inverse MCE, associated to the competition between the two magnetic sublattices antiferromagnetically coupled. We also observed the behavior of the magnetic transition temperature (TC) and lattice parameters as a function of the concentration ('x¿), with a corresponding MCE peak shift. Some important properties regarding the application of these materials in magnetic refrigeration are discussed. Two members of the family of compounds show a shifted hysteresis curve which was assigned to the Exchange Bias (EB) effect in analogy with FM-AFM bilayers systems in thin films. We believe that the EB effect is associated with strong unidirectional anisotropy of the magnetic sublattices appeared in Tb0.3Pr0.7Al2 and Tb0.25Pr0.75Al2, which occurs at low temperatures, and with the magnetization of the polarized conduction electrons. We also identified the compensation temperature (characteristic properties of this type of system) in these compounds / Doutorado / Física / Doutor em Ciências

Les alliages Fe-Si sont connus pour combiner d’excellentes propriétés magnétiques avec de bonnes propriétés électriques (forte résistivité électrique). Dans ce contexte nous avons recherché à élaborer des matériaux à forte teneur en Si, souvent difficiles à obtenir et mettre en forme industriellement. Des alliages magnétiques doux de type Fe-Si avec une teneur élevée en Si (4,5%, 6,5%, 10% et 15% massique) ont été obtenus avec succès à l’état nanocristallin par broyage mécanique et recuit. La formation des alliages a été étudiée par diffraction X, spectroscopie Mössbauer et analyses thermomagnétiques. La stabilité thermique de la poudre a été analysée par DSC. Des mesures d’aimantation ont été réalisées pour caractériser les performances magnétiques. La durée de broyage nécessaire pour la formation de l’alliage a été déterminée pour chaque teneur en Si. Pour les faibles temps de broyage, le recuit conduit à la formation du composé Fe3Si. Après la formation de l’alliage par le broyage mécanique, l’effet du recuit est seulement de réduire les tensions internes du second ordre, induites dans la poudre par le broyage. L’addition de Si conduit à la diminution de la température de Curie de 770 °C pour le Fe pur, à 725 °C pour une teneur de 4,5% massique de Si et à 550 °C pour 15% massique de Si. Pour les temps faibles de broyage, l’écart entre l’aimantation de la poudre avant et après recuit est dû à la formation du composé Fe3Si pendant le recuit, lequel a une aimantation plus faible que la solution solide de Feα(Si). Pour les longs temps de broyage, le recuit à 400 °C pour 4 heures n’a pas d’effet sur la valeur de l’aimantation à saturation. En augmentant la teneur en Si, l’aimantation à saturation de l’alliage Fe-Si décroit.Les alliages Ni3Fe (aussi connus comme Permalloys) présentent de meilleures propriétés magnétiques, mais ils ont une résistivité inférieure à celles des Fe-Si. Une voie attractive semble la combinaison des propriétés des 2 classes de matériaux doux en formant un composite. Les alliages Fe-Si précédemment obtenus ont été utilisés pour l’élaboration des poudres composites de type Permalloy/Fe-Si par la mécanosynthèse. Le broyage mécanique conduit à la formation des particules composites avec un aspect stratifié. Quatre heures de broyage de l’alliage Fe-Si avec du Ni3Fe ne conduisent pas à la formation des nouvelles phases, mais la formation d’un alliage ternaire Ni-Fe-Si résulte d’un recuit ultérieur à 900 °C. L’aimantation à saturation du composite augmente avec la croissance de la teneur le d’alliage Fe-Si, mais le temps de broyage ne semble avoir aucun effet sur cela.Une étude préliminaire a été réalisée sur l’élaboration des compacts composites de type Ni3Fe/Fe-Si par frittage flash, dans le but de préserver l’état nanocristallin par de basses températures de frittage. L’influence de la température de frittage et de la durée de maintien sur la structure, et les propriétés physiques des compacts est discutée. Des températures allant jusqu'à 750 °C pour une durée de maintien minimale ou un palier de 2 minutes maximum à 700 °C ne conduisent pas à la diffusion des éléments des alliages. L'augmentation de la température ou de la durée de frittage conduit à des cristallites plus grandes, mais qui restent dans le domaine nano pour les températures étudiées. La densité des compactes augmente avec la température et le palier. En outre, la résistivité diminue en augmentant ces 2 paramètres. L'effet de la teneur en Fe-Si est de diminuer la densité et en même temps d'augmenter la résistivité des compacts. La perméabilité magnétique est réduite avec l'augmentation de la température et de la durée de frittage, ainsi que lors de la diminution du contenu de Ni3Fe. Une température élevée et un long temps de maintien à la température de frittage conduisent à l’augmentation des pertes magnétiques. Le champ coercitif est également influencé par les paramètres de frittage, via l'effet qu'ils ont sur la taille des cristallites. / Fe-Si alloys are known for combining excellent magnetic properties with good electric characteristics (high resistivity). In this context we sought to develop materials with a relatively high Si content, often difficult to obtain and shape industrially.In this thesis, soft magnetic Fe-Si alloys with high Si content (4.5, 6.5, 10 and 15 wt. %) were successfully obtained in nanocrystalline state by mechanical alloying and annealing. The formation of the alloy was studied by X-ray and neutron diffraction, Mossbauer spectroscopy and thermomagnetic analysis. DSC technique was used in order to study the powder’s thermal stability. Magnetisation measurements were also made in order to characterise their magnetic performances. The milling duration necessary for the formation of the alloy was determined for each Si content. For low milling times, annealing leads to the formation of the Fe3Si compound. Once the alloy is formed by mechanical milling, the effect of the annealing is only to reduce the second order stress induced in the powder by the milling process. Si addition leads to the decrease of the alloy’s Curie temperature from 770 °C for pure Fe to 725 °C for a 4.5 wt. % Si and down to 550 °C if the Si content increases to 15 wt. %. For low milling times, a gap between the magnetisation of the as-milled alloy and of the milled and subsequently annealed one is due to the formation of the Fe3Si compound during annealing which has a lower magnetisation than that of the αFe (Si) solid solution. For longer milling durations, annealing at 400 °C for 4 hours has no effect on the saturation magnetisation value. By increasing the Si content, the Fe-Si alloy’s saturation magnetisation decreases.Fe-Ni alloys whose composition is close to Ni3Fe (commonly known as Permalloys) have better magnetic properties, but a resistivity well inferior to that of Fe-Si alloys. Therefore, a combination of the properties of these 2 alloy classes of soft magnetic materials into a composite seems to be an attractive route. The previously obtained Fe-Si alloys were used for the preparation of Permalloy/Fe-Si composite powders by mechanical milling. Milling leads to the formation of composite powder particles with a stratified aspect. Milling of the Fe-Si and Ni3Fe alloys for 4 hours does not lead to the formation of new phases, but a subsequent annealing at 900 °C results in the formation of a Ni-Fe-Si alloy. Saturation magnetisation of the composite increases with increasing of the Fe-Si content, but milling duration seems to have no effect on it.A preliminary study was made on the elaboration of Ni3Fe/Fe-Si composite compacts obtained by spark plasma sintering, aiming to preserve the nanocrystalline state by lower sintering temperatures. The influence of the sintering temperature and temperature holding duration on the structure, density, resistivity and magnetic properties of the compacts is discussed. Temperatures of up to 750 °C for minimal holding duration or a maintain at the temperature of 700 °C for a duration of up to 2 minutes does not lead to a diffusion of the alloys’ elements. Increasing of the sintering temperature or duration leads to larger crystallite sizes, but they remain in the nano domain for the studied temperatures. The compacts’ density increases with temperature and sintering duration. Resistivity, on the other hand decreases when increasing the aforementioned parameters. The effect of the Fe-Si content is to decrease the density and at the same time increase the compacts’ resistivity. Magnetic permeability is reduced with increasing sintering temperature and duration, as well as when decreasing of the Ni3Fe content. High temperature and long maintaining duration leads to an increase of magnetic losses. Coercive field is also influenced by sintering parameters by the effect they have on the crystallite size.

No description available.

Les effets de transfert de spin sont devenus un sujet de recherche majeur ces quinze dernières années. Cependant, un manque de vérifications expérimentales pour beaucoup de modèles décrivant les effets de transfert de spin peut être constaté. Ceci est surtout lié à un manque de systèmes magnétiques modèles permettant un contrôle précis des paramètres pertinents utilisés dans les modèles théoriques. Dans ce travail deux systèmes magnétiques à aimantation perpendiculaire ont été analysés : les alliages amorphes de Co1-xTbx élaborés par pulvérisation cathodique et les super-réseaux [Co/Ni](111) élaborés par épitaxie par jets moléculaires. L'anisotropie et l'aimantation, qui sont des paramètres pertinents dans beaucoup de modèles sur le transfert de spin, sont variables dans une large gamme. L'origine de cette anisotropie est discutée. La structure des domaines magnétiques est analysée et les résultats des mesures de transport sont interprétés. Pour les super-réseaux [Co/Ni](111) une forte polarisation en spin au niveau de Fermi est démontrée grâce à des expériences de photo émission résolue en spin et un coefficient d'amortissement intrinsèque [alpha] très faible est trouvé. Il est conclu que les alliages amorphes de Co1-xTbx et les super-réseaux [Co/Ni](111) sont des systèmes modèles pour le transfert de spin. / Spin transfer torque effects have become a research subject of high interest during the last 15 years. However, in order to probe the fundamental physics of spin transfer torque model systems are needed. For a model system it must be as simple as possible to tune the significant parameters (magnetic and structural). In this work we analyze the suitability of two materials for this need. The studied materials are amorphous Co1-xTbx alloys elaborated by sputtering and MBE grown [Co/Ni](111) superlattices. Both systems show perpendicular magnetic anisotropy (PMA), which provides a uniaxial anisotropy to the system. This anisotropy and the magnetization, which are significant parameters for many models on spin transfer torque, can be tuned in a large range of values. The origin of this PMA is discussed. The domain structure is analyzed and transport measurements are interpreted. In addition we show a strong spin polarization of the electrons close to the Fermi level by doing photoemission experiments. A small intrinsic Gilbert damping parameter [alpha] is found by FMR spectroscopy. We conclude that both materials are good candidates to be used as model systems for spin transfer torque

No description available.

In the foundation of this work is the issue for production of non-magnetic materials with predetermined weak magnetic properties. Preferable solution is to dope these materials with ferromagnetic impurities in low concentrations. One of the efficient ways to obtain such materials is the use of powder metallurgy which gives an opportunity to produce complex powder compositions with variety of components in precisely specified concentrations.

The main objective of this thesis was to bring the first experimental evidence about the spin-Hall magnetoresistance (SMR) in the Terahertz (THz) spectral range. The time-domain THz spectroscopy (TDTS) was chosen as the main method, and we presented a new experimental scheme, which allows us to observe SMR or magnetoresistive effects with similar symmetry at a wide range of THz frequencies very efficiently. We focused on the study of SMR in the bilayers consisting of either a prototypical ferrimagnetic isolator or of heavy metal (FI/HM) and metallic stacks of ferromagnetic CoFeB and heavy metal Pt layer (FM/HM). While SMR shows a rapid decrease already at the lowest THz frequencies (< 1 THz) in the FI/HM structures, the SMR in FM/HM bilayers persists above 30 THz. These observations are then explained by a different mechanism of SMR. The second part of the thesis is devoted to the construction of the new TDTS setup and an easy-to-use model of the THz setup using the Gaussian description of THz radiation. The simulated results have been compared to corresponding experimental measurements using a spintronic THz emitter (STE). The last part of the thesis describes the emission of intensive THz pulses from large-area STE.