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Multiferroic materials, in which spontaneous orderings (especially magnetic and electrical, in some cases elastic) jointly exist and may mutually interact, are currently in the center of attention in many fields of research due to their high application potential. They are already used in many applications, as in various sensors, microwave filters or electro / magneto- mechanical manipulators and actuators. Nevertheless, many features of microstructure and moment arrangements are not yet fully explained and understood. The presented work is mostly experimental and focuses on the investigation of several promising multiferroic materials: Pb1 − xBax(Fe0.5Nb0.5)O3 (x = 0 - 1) and Pb(Fe0.5Sb0.5)O3 with a perovskite structure and labeled as multiferroics of the I. type according to the Khomsky classification, BaYFeO4, which belongs to the multiferroics of the II. Khomsky class, and LiFePO4, which is a potentially multiferroic substance containing Fe2+ and are used in electric accumulators at present. Mössbauer spectroscopy of the 57 Fe isotope was used as a key experimental method, which can provide new information about the local arrangement in the vicinity of resonantly absorbing nuclei in the investigated substances. Data evaluation and interpretation would not be possible without the using results...

Low Temperature Nuclear Orientation (LTNO) is an important technique in the study of nuclei far from stability. The theory of LTNO and its application to the measurement of static nuclear moments and other quantities of spectroscopic interest are reviewed. The off-line facility at Oxford was used to study the decay of ¹³³I→¹³³Xe and ¹³⁵I→¹³⁵Xe. ¹³³I having Z=53 and N=80 has three protons above the closed shell Z=50 and two neutrons holes in N=82 shell, while ¹³⁵I has fully closed neutron shell since it has N=82, and they are of considerable theoretical interest since a wide variety of the theoretical nuclear models may be used to describe the observed levels close to the stable double closed shell structure. Another aim is to search for the nuclear magnetic dipole moment of the ground state of ¹³⁵I. Nuclear orientation of ¹³³IFe and ¹³⁵IFe enabled the mixing ratios of several transitions in the decay scheme of ¹³³I and ¹³⁵I to be determined. From temperature dependence for ¹³⁵I, the nuclear magnetic moment of ¹³⁵I has been deduced. Also temperature dependence for ¹³³I, analysed using a simple model, gave value for the magnetic hyperfine field that differed from previous published values. The method of combining nuclear orientation with NMR has become a very popular technique in recent years for determining nuclear magnetic dipole moments very precisely. The purpose of the NMR/ON experiment was to measure the hyperfine field with greater precision and to get some idea of the proportion of nuclei subject to it. Light Eu and Sm nuclei have attracted attention as systems with the number of protons right below the Z=64 subshell gap and the number of neutrons approaching N=82 major shell closure. Odd-proton, odd-neutron and odd-odd nuclei near the A=140 region have been investigated in the framework of the particle-triaxial rotor model. Main attention has been paid to explanation of experimental magnetic dipole and electric quadrupole moments of ground and isomeric states. Model predictions for deformation parameters of ^136-142Sm even-even cores have been extracted.

The problem of the quadrupole interaction occurring in a vibrating-rotating C₃v symmetric top molecule has been studied in detail. The quadrupole interaction has been treated as another perturbation term to a general frequency expression accounting for the vibrating-rotating interaction of the molecule so that a complete frequency formula is obtained for both interactions, and from which hyperfine spectral components are predicted and measured. The hyperfine transitions in the ground, and v₈=1 and v₈=2 excited vibrational states of the ¹³C isotopes of methyl cyanide have been investigated in the frequency range 17-72 GHz, primarily in the low J transitions (0≤J≤3). The study of the ground state of isotope i3CH3i3CN, and the v₈=1, v₈=2 excited vibrational states for all the isotopes have been conducted here for the first time. A substantial perturbation has been discovered and discussed at the ΔJ=3→4 transitions within the Kl=1 sets in the v₈=1 mode for isotopes ¹³CH₃CN and CH₃¹³CN. A total of 716 hyperfine transitions have been assigned from measurements, only 7 of which have been measured previously. A total of 84 molecular constants have been reported; 70 of these constants are derived for the first time from microwave data.

Amostras de dióxido de cério dopadas com La e Fe foram confeccionadas e caracterizadas por uma técnica nuclear baseada em interações hiperfinas conhecida como Correlação Angular Gama-Gama Perturbada (CAP). Como o composto em questão não é radioativo, foram utilizados núcleos radioativos como ponta de prova 111In 111Cd, que decaem através de uma cascata gama-gama 171-245 keV, com nível intermediário possui uma meia-vida de 84ns, spin 5/2- e um momento de quadrupolo elétrico Q= 0,83. Inicialmente uma metodologia para a produção das amostras precisou ser elaborada. As amostras de dióxido de cério e seus dopantes foram produzidas através do processo Sol-Gel, passando por uma calcinação e sinterização até a finalização da amostra. Sendo caracterizada por diversos tipos de técnicas (Difração de Raios-X e Microscopia Eletrônica de Varredura) culminando no estudo através da técnica CAP, para uma compreensão das interações quadrupolares elétricas das amostras e também a possibilidade da existência de comportamento magnético (assunto intensamente investigado dado o interesse na área da spintrônica). Os resultados encontrados foram analisados frente aos conhecimentos encontrados na literatura e as discussões foram feitas em função da variação do elemento dopante, tipos de tratamentos térmicos usados na sinterização e as diferentes temperaturas de medidas. Permitindo uma discussão e interpretação física dos resultados encontrados. / Samples of cerium dioxide doped with La and Fe were fabricated and characterized by a technique based on nuclear hyperfine interactions known as Perturbed Angular Gamma-Gamma Correlation (PAC). As the used compound is not radioactive and the PAC technique requires a radioactive decaying through a cascade gamma-gamma, a radioactive probe nuclei were used (111In 111Cd - 171-245 keV), with intermediate has a half-life of 84ns, spin 5/2- and a moment of electric quadrupole Q= 0,83. Initially a methodology for the production of the samples had to be prepared. The cerium dioxide and its dopants were produced by the Sol-Gel process, undergoing a calcining and sintering. The sample are characterized by various types of techniques (X-ray Diffraction and Scanning Electron Microscopy) succeeding study through hyperfine Interactions, with the PAC technique, to an understanding of the electric quadrupole inteirações samples and also the possibility of the existence of magnetic behavior (subject intensively investigated given the interest in the field of spintronics). The results were analyzed taking the knowledge found in the literature and discussions were made on the basis of the variation of the doping element, thermal treatments used in the sintering temperatures and the different measures. Allowing a discussion and physical interpretation of results.

O presente trabalho realiza a investigação dos parâmetros hiperfinos, incluindo a sua natureza dinâmica, em compostos ligantes em solução a temperatura ambiente (295 K) e resfriada (77K) através da espectroscopia de Correlação Angular γγ Perturbada (CAP). Para a realização das medidas experimentais, utilizou-se núcleos de prova radioativos de 111In111Cd, 181Hf181Ta e 111mCd111Cd, que decaem através de cascata gama. As amostras foram preparadas diluindo-se soluções com os núcleos radioativos em água, quando se investigou a interação do núcleo de prova com o ligante água; adicionando-se soluções com os núcleos radioativos em solução tampão, quando se investigou a interação do núcleo de prova com os íons ligantes provenientes do próprio tampão (CO32- e HCO31-) e com o OH1-; e adicionando-se soluções com os núcleos radioativos em soluções do ligante ácido etilenodiaminotetracético (EDTA), este em pH entre 4,0 e 5,0, (que corresponde ao pH da própria solução saturada do EDTA) e em solução tampão de pH entre 9 e 10. Assim foi possível investigar os efeitos gerados por cada um desses métodos de preparação de amostras nas medidas CAP. Finalmente foi feita uma análise comparativa para os vários métodos de inserção dos núcleos de prova na amostra, considerando-se aspectos químicos e nucleares. A inexistência de medidas para esse tipo de amostra, justifica a importância dos resultados obtidos. / In this study the hyperfine parameters, including the dynamical nature, Perturbed Angular Correlation (PAC) spectroscopy was used to measure the hyperfine parameters in molecules of ligand compounds in solutions. The measurements were carried out at 295 K and 77 K using 111In111Cd, 181Hf181Ta and 111mCd111Cd, as probe nuclei. Samples were prepared by adding a small volume of radioactive solution containing the probe nuclei in aqueous solution, buffer solution and ethylenediaminetetraacetic acid (EDTA) used as a ligand with pH 4.3 which correspond to the pH of the saturated EDTA solution and in buffer solution with pH between 9 and 10. The results made possible to understand the impact of each method for PAC measurements. Finally a comparative analysis for the several methods of inserting of the probe nuclei in the sample was made, considering chemical and nuclear aspects. The lack of measurements in this kind of samples justifies the importance of the obtained results.

O presente trabalho realiza a investigação dos parâmetros hiperfinos, incluindo a sua natureza dinâmica, em compostos ligantes em solução a temperatura ambiente (295 K) e resfriada (77K) através da espectroscopia de Correlação Angular γγ Perturbada (CAP). Para a realização das medidas experimentais, utilizou-se núcleos de prova radioativos de 111In111Cd, 181Hf181Ta e 111mCd111Cd, que decaem através de cascata gama. As amostras foram preparadas diluindo-se soluções com os núcleos radioativos em água, quando se investigou a interação do núcleo de prova com o ligante água; adicionando-se soluções com os núcleos radioativos em solução tampão, quando se investigou a interação do núcleo de prova com os íons ligantes provenientes do próprio tampão (CO32- e HCO31-) e com o OH1-; e adicionando-se soluções com os núcleos radioativos em soluções do ligante ácido etilenodiaminotetracético (EDTA), este em pH entre 4,0 e 5,0, (que corresponde ao pH da própria solução saturada do EDTA) e em solução tampão de pH entre 9 e 10. Assim foi possível investigar os efeitos gerados por cada um desses métodos de preparação de amostras nas medidas CAP. Finalmente foi feita uma análise comparativa para os vários métodos de inserção dos núcleos de prova na amostra, considerando-se aspectos químicos e nucleares. A inexistência de medidas para esse tipo de amostra, justifica a importância dos resultados obtidos. / In this study the hyperfine parameters, including the dynamical nature, Perturbed Angular Correlation (PAC) spectroscopy was used to measure the hyperfine parameters in molecules of ligand compounds in solutions. The measurements were carried out at 295 K and 77 K using 111In111Cd, 181Hf181Ta and 111mCd111Cd, as probe nuclei. Samples were prepared by adding a small volume of radioactive solution containing the probe nuclei in aqueous solution, buffer solution and ethylenediaminetetraacetic acid (EDTA) used as a ligand with pH 4.3 which correspond to the pH of the saturated EDTA solution and in buffer solution with pH between 9 and 10. The results made possible to understand the impact of each method for PAC measurements. Finally a comparative analysis for the several methods of inserting of the probe nuclei in the sample was made, considering chemical and nuclear aspects. The lack of measurements in this kind of samples justifies the importance of the obtained results.

Neste trabalho foi realizado um estudo sistemático, das interações hiperfinas (campo hiperfino magnético e campo hiperfino elétrico), nos compostos do tipo RMn2Si2 e RMn2Ge2 (onde R = La, Nd, Pr), sendo que, para a amostra de La foi estudada a série LaMn2(Si(1-x)Gex)2 (onde x = 0, 0.2, 0.4, 0.6, 0.8, 1), por meio da técnica de correlação angular gama-gama perturbada (CAP), utilizando os núcleos de prova 111In(111Cd) e 140La(140Ce). Além disso, foram realizadas medições para a caracterização estrutural utilizando a técnica de difração de raios X, para a caracterização magnética, a nível macroscópico, através de medições de magnetização, caracterização nuclear utilizando a técnica de espectrometria da radiação gama e um estudo complementar por cálculos de primeiros princípios somente para as amostras de LaMn2Ge2 e LaMn2Si2. A maior contribuição para o comportamento magnético nesses compostos tem origem no ordenamento magnético da sub rede do Mn, que aparece em temperaturas relativamente altas, da ordem de 480 K, sendo que, esses compostos possuem um ordenamento antiferromagnético e próximo a temperatura ambiente passam a possuir um ordenamento ferromagnético. Além disso, para o caso especifico dos compostos PrMn2Ge2 e NdMn2Ge2, abaixo de 40K é observado, também, o ordenamento ferromagnético dos spins da sub rede da terra rara. O núcleo de prova 111In(111Cd) foi utilizado para medir, tanto as interações de quadrupolo elétrico, como de dipolo magnético na rede do Mn (interação matrizmatriz). Esses resultados evidenciaram a transição de fase magnética (antiferromagnética para ferromagnética), sendo que, o campo hiperfino magnético, para as duas fases magnéticas, segue o comportamento da função de Brillouin. Já o núcleo de prova 140La(140Ce) permitiu medir a interação de dipolo magnético, tanto originada pela rede do Mn, como pela rede da terra rara. Mas, nesse caso, pode ser verificado somente o campo hiperfino magnético da fase ferromagnética da rede do Mn. Para a análise dos resultados PAC levou-se em conta uma interação matriz-impureza, pois o íon Ce3+ possui um elétron 4f desemparelhado, que pode contribuir para o campo hiperfino total. O composto LaMn2Si2 apresentou o comportamento do campo hiperfino magnético com a temperatura que segue o comportamento da função de Brillouin. Já os compostos LaMn2Ge2, PrMn2Ge2 e NdMn2Ge2 apresentaram um comportamento anômalo ao da função de Brillouin. Esse comportamento pode ser associado a uma forte hibridização da banda 4f do Ce com a banda 3d do Mn, tal conclusão foi reforçada pelos resultados do DOS (densidade de estados), resultados dos cálculos de primeiros princípios, dos compostos LaMn2Si2 e LaMn2Ge2. / This thesis reports a systematic study of the hyperfine interactions (magnetic hyperfine field and electric field gradient) in the RMn2Si2 and RMn2Ge2 ( R = La, Nd, Pr) compounds as well as in LaMn2(Si(1-x)Gex)2 (where x = 0, 0.2, 0.4, 0.6, 0.8, 1) mixed compounds. The hyperfine interactions were measured through Perturbed Angular Correlation Gamma-Gamma Spectroscopy technique using 111In(111Cd) and 140La(140Ce) as probe nuclei. Structural, magnetic and chemical analysis characterization were carried out by X-ray diffraction, magnetization measurements and gamma radiation spectrometry, respectively. An additional study by first-principles calculations for LaMn2Ge2 e LaMn2Si2 samples were also performed. The magnetic behavior in these compounds is mainly associated with the ordering of the magnetic moments of Mn sublattice, which appears at high temperature around 480 K. All studied compounds undergo a transition from antiferromagnetic to ferromagnetic ordering around room temperature. Specifically for PrMn2Ge2 and NdMn2Ge2 compounds, an additional ferromagnetic ordering due to the polarization of Pr or Nd magnetic moments is also observed below 40 K. 111In(111Cd) probe nuclei were used to measure the temperature dependence of the electric quadrupole and the dipole magnetic interactions at the Mn sublattice (matrix-matrix interaction). The results show the magnetic transition (antiferromagnetic to ferromagnetic phase), where the magnetic hyperfine field associated to both magnetic phases follows the Brillouin function. For the 140La(140Ce) probe nuclei, only dipole magnetic interaction measurements in the ferromagnetic phase were possible, also caused by the Mn sublattice and, for R = Pr, Nd, by the rare earth sublattice. The analysis of results considers a matrix-impurity interaction because the Ce3+ has an unpaired 4f electron, which can contribute to the total hyperfine field. The compound LaMn2Si2 presents a behavior for the temperature dependence of the magnetic hyperfine field that could be fitted by a Brillouin function. On the other hand, LaMn2Ge2, PrMn2Ge2 and NdMn2Ge2 compounds showed an anomalous Brillouin function behavior. This behavior can be associated with a strong hybridization Ce 4f band with the Mn 3d band. Such conclusion was reinforced by the DOS (density of stats), first-principles calculations, results to LaMn2Si2 and LaMn2Ge2.

No presente trabalho, a técnica de Espectroscopia de Correlação Angular Perturbada (CAP) foi usada para medir a interação de quadrupolo elétrico em amostras de DNA de diferentes linhagens de camundongos (A/J, C57BL/6, B6AF1, BXA1 e BXA2), amostras de antiimunoglobulinas pertencentes as subclasses (IgG1, IgG2a e IgG2b) e de porções ativas de imunoglobulinas fracionadas ou inteiras, correspondentes a parte diversificada da imunoglobulina, responsável pelo padrão de resposta imunológica apresentado pelos organismos. Também foram realizadas medidas da interação de quadrupolo elétrico em amostras de bases nitrogenadas do DNA (adenina, citosina, guanina e timina). As medidas CAP foram realizadas utilizando os núcleos de prova 111In111Cd; 111mCd111Cd; 111Ag111Cd; e 181Hf181Ta, nas temperaturas ambiente e do nitrogênio líquido para investigar as interações dinâmicas e estáticas, respectivamente. As biomoléculas foram marcadas por meio direto, onde os átomos dos núcleos de prova devem se ligar a um determinado sítio da biomolécula. Os materiais biológicos e os núcleos de prova foram escolhidos com o objetivo de verificar, em todos os seus aspectos, a possibilidade de aplicação da espectroscopia de CAP na investigação dos parâmetros hiperfinos em um núcleo de prova de um átomo metálico ligado às biomoléculas (incluindo o uso de diferentes núcleos de prova, resultantes do decaimento do núcleo pai de quatro diferentes metais) e estudar, por meio dos parâmetros hiperfinos medidos, o comportamento dessas diferentes moléculas. Os resultados obtidos mostram as diferenças entre a interação das biomoléculas estudadas com os núcleos de prova Estas diferenças foram observadas por meio de variações nos parâmetros hiperfinos medidos, que depende do tipo de molécula, mostrando que o núcleo de prova em alguns casos ligou-se as moléculas e em outros não houve esta ligação. / In the present work perturbed angular correlation (PAC) spectroscopy was used to measured electric quadrupole interactions in DNA biomolecules of different mice lineages (A/J, C57BL/6, B6AF1, BXA1 e BXA2), samples of different isotypes of immunoglobulin G (IgG1, IgG2a e IgG2b) and active portions of complete and fragmented immunoglobulin responsible by the immune response. Electric quadrupole interactions were also measured in DNA nitrogenous bases (adenine, cytosine, guanine, thymine). PAC measurements were performed using 111In111Cd; 111mCd111Cd; 111Ag111Cd; e 181Hf181Ta as probe nuclei, and carried out at room temperature and liquid nitrogen temperature, in order to investigate dynamic and static hyperfine interactions, respectively. The biomolecule samples were directly marked with the radioactive parent nuclei, whose atom link to a certain site in the biomolecules. The biological materials as well as the probe nuclei were chosen to investigate the possibility to use PAC spectroscopy to measure hyperfine parameters at nuclei from metallic elements bound to biomolecules (including the use of different probe nuclei produced in the decay of parent nuclei of four different metals) and also to study the behavior of different biomolecules by means of the measured hyperfine parameters. Results show differences in the hyperfine interactions of probe nuclei bound to the studied biomolecules. Such differences were observed by variations in the hyperfine parameters, which depend on the type of biomolecule and the results also show that the probe nuclei atom bound to the molecule in some cases and in others do not.

In the present work we performed electronic structure calculations within the Kohn-Sham scheme of the density functional theory (DFT). We studied two molecules with potential applications in life sciences and medicine: ferrioxamine B and 5,10,15,20-tetrakis(1-methyl-4-pyridyl)-21H,23H (TMPyP) porphyrin. We used different methods and different exchange and correlation functionals, analyzing optical and vibrational properties and hyperfine interactions. In the case of ferrioxamine B, results in the crystalline phase (molecular crystal), and gas phase were compared with experimental results obtained using Mössbauer spectroscopy from the literature. We analyzed hyperfine parameters such as the electric quadrupole splitting, asymmetry parameter, hyperfine field and isomer shift. In the case of TMPyP porphyrin we analyzed vibrational properties in the gas phase and optical properties. For the electronic absorption, solvent effects and electronic charges states were analyzed. / In the present work we performed electronic structure calculations within the Kohn-Sham scheme of the density functional theory (DFT). We studied two molecules with potential applications in life sciences and medicine: ferrioxamine B and 5,10,15,20-tetrakis(1-methyl-4-pyridyl)-21H,23H (TMPyP) porphyrin. We used different methods and different exchange and correlation functionals, analyzing optical and vibrational properties and hyperfine interactions. In the case of ferrioxamine B, results in the crystalline phase (molecular crystal), and gas phase were compared with experimental results obtained using Mössbauer spectroscopy from the literature. We analyzed hyperfine parameters such as the electric quadrupole splitting, asymmetry parameter, hyperfine field and isomer shift. In the case of TMPyP porphyrin we analyzed vibrational properties in the gas phase and optical properties. For the electronic absorption, solvent effects and electronic charges states were analyzed.