Magnetic structures and magnetic phase transitions in the Mn-doped orthoferrite TbFeO3 studied by neutron powder diffraction

The magnetic structures and the magnetic phase transitions in the Mn-doped orthoferrite TbFeO3 studied using neutron powder diffraction are reported. Magnetic phase transitions are identified at T-N(Fe/Mn) approximate to 295K where a paramagnetic-to-antiferromagnetic transition occurs in the Fe/Mn sublattice, T-SR(Fe/Mn) approximate to 26K where a spin-reorientation transition occurs in the Fe/Mn sublattice and T-N(R) approximate to 2K where Tb-ordering starts to manifest. At 295 K, the magnetic structure of the Fe/Mn sublattice in TbFe0.5Mn0.5O3 belongs to the irreducible representation Gamma(4) (G(x)A(y)F(z) or Pb'n'm). A mixed-domain structure of (Gamma(1) + Gamma(4)) is found at 250K which remains stable down to the spin re-orientation transition at T-SR(Fe/Mn) approximate to 26K. Below 26K and above 250 K, the majority phase (>80%) is that of Gamma(4). Below 10K the high-temperature phase Gamma(4) remains stable till 2K. At 2 K, Tb develops a magnetic moment value of 0.6(2) mu(B)/f.u. and orders long-range in F-z compatible with the Gamma(4) representation. Our study confirms the magnetic phase transitions reported already in a single crystal of TbFe0.5Mn0.5O3 and, in addition, reveals the presence of mixed magnetic domains. The ratio of these magnetic domains as a function of temperature is estimated from Rietveld refinement of neutron diffraction data. Indications of short-range magnetic correlations are present in the low-Q region of the neutron diffraction patterns at T < T-SR(Fe/Mn). These results should motivate further experimental work devoted to measure electric polarization and magnetocapacitance of TbFe0.5Mn0.5O3. (C) 2016 AIP Publishing LLC.

Magnetic structures and magnetic phase transitions in the Mn-doped orthoferrite TbFeO3 studied by neutron powder diffraction

The magnetic structures and the magnetic phase transitions in the Mn-doped orthoferrite TbFeO3 studied using neutron powder diffraction are reported. Magnetic phase transitions are identified at T-N(Fe/Mn) approximate to 295K where a paramagnetic-to-antiferromagnetic transition occurs in the Fe/Mn sublattice, T-SR(Fe/Mn) approximate to 26K where a spin-reorientation transition occurs in the Fe/Mn sublattice and T-N(R) approximate to 2K where Tb-ordering starts to manifest. At 295 K, the magnetic structure of the Fe/Mn sublattice in TbFe0.5Mn0.5O3 belongs to the irreducible representation Gamma(4) (G(x)A(y)F(z) or Pb'n'm). A mixed-domain structure of (Gamma(1) + Gamma(4)) is found at 250K which remains stable down to the spin re-orientation transition at T-SR(Fe/Mn) approximate to 26K. Below 26K and above 250 K, the majority phase (>80%) is that of Gamma(4). Below 10K the high-temperature phase Gamma(4) remains stable till 2K. At 2 K, Tb develops a magnetic moment value of 0.6(2) mu(B)/f.u. and orders long-range in F-z compatible with the Gamma(4) representation. Our study confirms the magnetic phase transitions reported already in a single crystal of TbFe0.5Mn0.5O3 and, in addition, reveals the presence of mixed magnetic domains. The ratio of these magnetic domains as a function of temperature is estimated from Rietveld refinement of neutron diffraction data. Indications of short-range magnetic correlations are present in the low-Q region of the neutron diffraction patterns at T < T-SR(Fe/Mn). These results should motivate further experimental work devoted to measure electric polarization and magnetocapacitance of TbFe0.5Mn0.5O3. (C) 2016 AIP Publishing LLC.

Magnetic structures and magnetic phase transitions in the Mn-doped orthoferrite TbFeO3 studied by neutron powder diffraction

The magnetic structures and the magnetic phase transitions in the Mn-doped orthoferrite TbFeO3 studied using neutron powder diffraction are reported. Magnetic phase transitions are identified at T-N(Fe/Mn) approximate to 295K where a paramagnetic-to-antiferromagnetic transition occurs in the Fe/Mn sublattice, T-SR(Fe/Mn) approximate to 26K where a spin-reorientation transition occurs in the Fe/Mn sublattice and T-N(R) approximate to 2K where Tb-ordering starts to manifest. At 295 K, the magnetic structure of the Fe/Mn sublattice in TbFe0.5Mn0.5O3 belongs to the irreducible representation Gamma(4) (G(x)A(y)F(z) or Pb'n'm). A mixed-domain structure of (Gamma(1) + Gamma(4)) is found at 250K which remains stable down to the spin re-orientation transition at T-SR(Fe/Mn) approximate to 26K. Below 26K and above 250 K, the majority phase (>80%) is that of Gamma(4). Below 10K the high-temperature phase Gamma(4) remains stable till 2K. At 2 K, Tb develops a magnetic moment value of 0.6(2) mu(B)/f.u. and orders long-range in F-z compatible with the Gamma(4) representation. Our study confirms the magnetic phase transitions reported already in a single crystal of TbFe0.5Mn0.5O3 and, in addition, reveals the presence of mixed magnetic domains. The ratio of these magnetic domains as a function of temperature is estimated from Rietveld refinement of neutron diffraction data. Indications of short-range magnetic correlations are present in the low-Q region of the neutron diffraction patterns at T < T-SR(Fe/Mn). These results should motivate further experimental work devoted to measure electric polarization and magnetocapacitance of TbFe0.5Mn0.5O3. (C) 2016 AIP Publishing LLC.

Magnetic structures and magnetic phase transitions in the Mn-doped orthoferrite TbFeO3 studied by neutron powder diffraction

The magnetic structures and the magnetic phase transitions in the Mn-doped orthoferrite TbFeO3 studied using neutron powder diffraction are reported. Magnetic phase transitions are identified at T-N(Fe/Mn) approximate to 295K where a paramagnetic-to-antiferromagnetic transition occurs in the Fe/Mn sublattice, T-SR(Fe/Mn) approximate to 26K where a spin-reorientation transition occurs in the Fe/Mn sublattice and T-N(R) approximate to 2K where Tb-ordering starts to manifest. At 295 K, the magnetic structure of the Fe/Mn sublattice in TbFe0.5Mn0.5O3 belongs to the irreducible representation Gamma(4) (G(x)A(y)F(z) or Pb'n'm). A mixed-domain structure of (Gamma(1) + Gamma(4)) is found at 250K which remains stable down to the spin re-orientation transition at T-SR(Fe/Mn) approximate to 26K. Below 26K and above 250 K, the majority phase (>80%) is that of Gamma(4). Below 10K the high-temperature phase Gamma(4) remains stable till 2K. At 2 K, Tb develops a magnetic moment value of 0.6(2) mu(B)/f.u. and orders long-range in F-z compatible with the Gamma(4) representation. Our study confirms the magnetic phase transitions reported already in a single crystal of TbFe0.5Mn0.5O3 and, in addition, reveals the presence of mixed magnetic domains. The ratio of these magnetic domains as a function of temperature is estimated from Rietveld refinement of neutron diffraction data. Indications of short-range magnetic correlations are present in the low-Q region of the neutron diffraction patterns at T < T-SR(Fe/Mn). These results should motivate further experimental work devoted to measure electric polarization and magnetocapacitance of TbFe0.5Mn0.5O3. (C) 2016 AIP Publishing LLC.

Generalized Maugis-Dugdale Model of an Elastic Cylinder in Non-Slipping Adhesive Contact with a Stretched Substrate

We have recently developed a generalized JKR model for non-slipping adhesive contact between an elastic cylinder and a stretched substrate where both tangential and normal tractions are transmitted across the contact interface. Here we extend this model to a generalized Maugis-Dugdale model by adopting a Dugdale-type adhesive interaction law to eliminate the stress singularity near the edge of the contact zone. The non-slipping Maugis-Dugdale model is expected to have a broader range of validity in comparison with the non-slipping JKR model. The solution shares a number of common features with experimentally observed behaviors of cell reorientation on a cyclically stretched substrate.

Phase transitions in planar magnetic nanostructures

Using numerical micromagnetics we have studied the ground state magnetization distribution of square planar ferromagnetic elements ("nanostructures"). As the element size is reduced from 250 to 2 nm at constant thickness (2-35 nm), we find that the magnetization distribution undergoes up to three phase transitions involving as many as three different near single domain states. One of these phase transitions is analogous to the reorientation phase transition observed in continuous ultrathin magnetic films. © 1998 American Institute of Physics.

细胞黏附的力学建模及其力敏感性的机理研究

细胞黏附在机体的生理和病理过程中起着重要的作用。作为细胞内、外信息交流和传递的通道，细胞黏附斑具有独特的力敏感性。实验表明，在力的作用下，黏附斑不仅可以生长、成熟和破坏，而且还能感知外部环境的力学性质，如基底硬度、硬度梯度和形貌等等。细胞黏附如何响应不同的力学刺激，物理机理是什么，如何定量描述这些物理机理？这些问题是细胞生物学和细胞力学中的重要问题。本论文通过在分子和亚细胞尺度上的力学建模研究了黏附斑的力敏感性机理，主要包括以下几方面的内容： (1) 发展了一个非线性的撕裂模型，研究了细胞黏附的稳定性和边缘依赖性。通过引入黏附分子键的非线性本构关系，并考虑黏附分子键的多种分布形式，我们发现黏附分子键的非线性效应对维持细胞黏附的稳定性起着至关重要的作用。黏附分子键的非线性力学性质使黏附分子键可以同时承载，降低了细胞对黏附分子键分布的依赖性，大大提高了细胞的黏附强度。本文的预测结果与实验结果一致。 (2) 建立了细胞黏附的细观力学模型，研究了在力作用下黏附斑生长和失稳的分子机理。在细观力学模型中，引入了“整联蛋白的聚集”和“整联蛋白-配体的反应”两个分子作用机理，并用两个化学反应来描述。通过基于Monte Carlo思想的Gillespie算法模拟了细胞黏附在不同载荷下的响应。我们发现黏附斑只能在一定范围的张力下生长，在这个范围内整联蛋白的聚集机制占主导。而当张力大于某个临界值时，黏附斑将失稳并导致破坏，这时整联蛋白-配体分子键的解离机制占主导。因此，黏附斑对作用力的不同响应，是不同分子作用机制在力作用下相互消长的结果。同时我们还建立了一个唯象的热力学模型中，验证了我们的细观力学模型。 (3) 基于细胞黏附的细观力学模型，研究了周期性载荷下细胞的重排和转向机理。在细观力学模型中，通过黏附块(adhesion plaque)，将整联蛋白-配体分子键和细胞骨架联系起来。基于Monte Calro模拟，我们发现存在一个载荷临界值，当外载大于临界值时，细胞将进行重排。细胞重排的原因是在周期性载荷下黏附斑的失稳。通过引入整联蛋白-配体成键的化学反应动力学和应力纤维的粘弹性性质，解释了细胞黏附稳定性的频率依赖性。本文预测的细胞转向临界载荷和重排方向，与实验结果一致。

Atomistic Simulation On Size-Dependent Yield Strength And Defects Evolution Of Metal Nanowires

A simple derivation based on continuum mechanics is given, which shows the surface stress is critical for yield strength at ultra-small scales. Molecular dynamics (MD) simulations with modified embedded atom method (MEAM) are employed to investigate the mechanical behaviors of single-crystalline metal nanowires under tensile loading. The calculated yield strengths increasing with the decrease of the cross-sectional area of the nanowires are in accordance with the theoretical prediction. Reorientation induced by stacking faults is observed at the nanowire edge. In addition. the mechanism of yielding is discussed in details based on the snapshots of defects evolution. The nanowires in different crystallographic orientations behave differently in stretching deformation. This study on the plastic properties of metal nanowires will be helpful to further understanding of the mechanical properties of nanomaterials. (C) 2009 Elsevier B.V. All rights reserved.

Stabilizing to disruptive transition of focal adhesion response to mechanical forces

Strong mechanical forces can, obviously, disrupt cell-cell and cell-matrix adhesions, e.g., cyclic uniaxial stretch induces instability of cell adhesion, which then causes the reorientation of cells away from the stretching direction. However, recent experiments also demonstrated the existence of force dependent adhesion growth (rather than dissociation). To provide a quantitative explanation for the two seemingly contradictory phenomena, a microscopic model that includes both integrin-integrin interaction and integrin-ligand interaction is developed at molecular level by treating the focal adhesion as an adhesion cluster. The integrin clustering dynamics and integrin-ligand binding dynamics are then simulated within one unified theoretical frame with Monte Carlo simulation. We find that the focal adhesion will grow when the traction force is higher than a relative small threshold value, and the growth is dominated by the reduction of local chemical potential energy by the traction force. In contrast, the focal adhesion will rupture when the traction force exceeds a second threshold value, and the rupture is dominated by the breaking of integrin-ligand bonds. Consistent with the experiments, these results suggest a force map for various responses of cell adhesion to different scales of mechanical force. PMID: 20542514

Estudo do efeito magnetocalórico em sistemas magnéticos com terras raras

O efeito magnetocalórico, base da refrigeração magnética, é caracterizado por duas quantidades: a variação isotérmica da entropia (ΔST) e a variação adiabática da temperatura (ΔTS); que são obtidas sob variações na intensidade de um campo magnético aplicado. Em sistemas que apresentam anisotropia magnética, pode‐se definir o efeito magnetocalórico anisotrópico, o qual, por definição, é calculado sob variações na direção de aplicação de um campo magnético cuja intensidade mantém‐se fixa, e é caracterizado por duas quantidades: a variação anisotrópico‐isotérmica da entropia (ΔSan) e a variação anisotrópico‐adiabática da temperatura (ΔTan). O efeito magnetocalórico e o efeito magnetocalórico anisotrópico foram estudados nos compostos intermetálicos formados por terras e outros materiais não magnéticos: RNi2, RNi5, RZn e Gd1‐nPrnAl2. Os cálculos foram feitos partindo de hamiltonianos modelo que incluem as interações de troca, Zeeman, de campo cristalino e quadrupolar.

As transformações no ensino na saúde: um estudo sobre a extensão universitária e sua relação com a formação do profissional de saúde para o SUS

HENRIQUES, Regina Lúcia Monteiro.2011. 182 f. Tese (Doutorado em Saúde Coletiva) Instituto de Medicina Social, Universidade do Estado do Rio de Janeiro, Rio de Janeiro, 2011. Este estudo trata dos processos de mudança na formação em saúde, especialmente das questões político estruturais da articulação do ensino e da extensão para a construção de estratégias de transformação dos cursos da área da saúde. Tem por objetivos analisar as perspectiva dos sujeitos envolvidos na transformação curricular no que diz respeito à articulação entre práticas de ensino, extensão universitária e saúde, a constituição de novos cenários de prática e sua relação com a extensão universitária, assim como examinar os sentidos atribuídos pelos sujeitos aos processos políticos internos e externos às instituições de ensino. Parte-se da compreensão de que há em andamento um grande movimento de lutas pela mudança na formação em saúde e de algumas das ideias que têm sido discutidas e difundidas na defesa da reorientação da formação em saúde baseada em princípios e diretrizes consoantes com a política de saúde e com a defesa de direitos de cidadania. Baseia-se em concepções de espaço cotidiano das instituições de formação superior em saúde e dos serviços de saúde e outros cenários de prática. Reflete sobre a responsabilidade política das instituições formadoras e da extensão universitária como lugar de tornar públicas as posições e valores defendidos para as práticas do cuidado e da relação social e política da universidade. Para a operacionalização do estudo, foram escolhidas duas instituições universitárias que se apresentaram e que foram selecionadas no programa do Pro-Saúde. Foram realizadas entrevistas com roteiro semi-estruturado com protagonistas de processos de mudança na formação nestas instituições, em três profissões da área da saúde, enfermagem, medicina e odontologia. Fez-se analise hermenêutica a partir dos sentidos que foram atribuídos a estas experiências concretas pelos atores que as empreenderam. Definiu-se três categorias de análise, a dimensão das políticas governamentais de incentivo a mudanças na formação em saúde e os efeitos das mesmas para as instituições de ensino; a ampliação de cenários de prática, as estratégias de aproximação entre os mundos do ensino e do trabalho e se significaram novas práticas de cuidado; relação existente entre os processos de transformação curricular e a extensão universitária. A extensão vem adquirindo protagonismo na construção de dispositivos de enfrentamento e superação das dificuldades e resistências nos processos de transformação curricular, além de criar com relativa liberdade novas possibilidades espaciais e conceituais para o cuidado em saúde, porém pelos próprios sentidos que assume desde a invisibilidade até a redenção da universidade sua baixa institucionalidade e reflexão impede que sua potencialidade seja tomada como aliada nestes processos de modo mais sistemático e impactante.

A prática educativa como expressão da prática profissional no contexto da equipe de saúde da família no município do Rio de Janeiro

Este estudo teve como objeto as práticas educativas em saúde desenvolvidas no Programa de Saúde da Família (PSF), no Município do Rio de Janeiro. O objetivo geral foi a compreensão das práticas educativas realizadas pelos profissionais que atuam no PSF. O interesse se deu pelo fato de reconhecer o PSF como espaço privilegiado no desenvolvimento de práticas educativas voltadas para a conscientização popular, nos aspectos sociais, políticos e da saúde, pelas suas características de atuação em território definido, e na lógica de vigilância à saúde. Ressalta-se a importância da Educação em Saúde como estratégia de intervenção por uma sociedade mais saudável. Trata-se de pesquisa qualitativa descritiva, realizada entre 2007 e 2008. A análise dos dados foi orientada pelo método de Análise de Conteúdo. Os dados foram coletados através de entrevista semi-estruturada, com cinco equipes de saúde da família, totalizando vinte profissionais. Na análise foram identificadas quatro categorias: organização do processo de trabalho, papel do profissional na equipe, organização da prática educativa e fatores que interferem na realização das práticas educativas. Na análise verificou-se que os profissionais enfrentam dificuldades no planejamento das práticas educativas, relacionadas, principalmente, à falta de capacitação pedagógica e à dificuldade de organização do processo de trabalho, centrado no modelo biomédico. Os agentes comunitários se destacam na realização das atividades, com o apoio da equipe, principalmente da enfermeira. Os temas são escolhidos, prioritariamente, a partir da identificação das necessidades de saúde dos usuários pelos profissionais. Verifica-se que há dificuldade na definição dos objetivos das práticas educativas. Predomina o formato de grupos, voltados para a promoção da saúde, mas também com enfoque preventivista. Verifica-se a presença de práticas com outras formas de relação entre profissionais e usuários, num exercício de cidadania para a qualidade de vida. A avaliação é realizada informalmente, entre os profissionais e, geralmente, se detém à quantidade de usuários participantes, ou na constatação de mudança de comportamento do usuário. Os fatores que interferem dizem respeito às relações estabelecidas entre os profissionais, e entre estes e os usuários. A violência associada ao narcotráfico surge como fator que prejudica a atividade no território. As capacitações em prática educativa também são mencionadas. Verifica-se que a forma de organização do processo de trabalho influencia fortemente, visto que a realização das práticas educativas depende diretamente da dinâmica dada ao trabalho, e do espaço destinado para essa atividade na divisão do trabalho. As questões relacionadas à infra-estrutura são relatadas, principalmente, no que diz respeito à escassez de material, recursos financeiros, e espaço físico inadequado. Percebe-se que a falta da sistematização da prática educativa parece comprometer as transformações necessárias para o seu aprimoramento e reflete a falta de compreensão dos profissionais sobre a importância do processo educativo para a saúde e como instrumento de transformação social e política dos sujeitos. Percebe-se, ainda, a necessidade de investimentos para a qualificação do profissional do PSF, não somente em relação às práticas educativas, mas também para que seja possível operar as mudanças necessárias para a reorientação do modelo de atenção à saúde proposto pelo PSF.

I. Electron spin relaxation studies of manganese(II) complexes in acetonitrile. II. Nuclear spin relaxation studies of bromine in tetrabromomanganese(II) in acetonitrile

Magnetic resonance techniques have given us a powerful means for investigating dynamical processes in gases, liquids and solids. Dynamical effects manifest themselves in both resonance line shifts and linewidths, and, accordingly, require detailed analyses to extract desired information. The success of a magnetic resonance experiment depends critically on relaxation mechanisms to maintain thermal equilibrium between spin states. Consequently, there must be an interaction between the excited spin states and their immediate molecular environment which promote changes in spin orientation while excess magnetic energy is coupled into other degrees of freedom by non-radiative processes. This is well known as spin-lattice relaxation. Certain dynamical processes cause fluctuations in the spin state energy levels leading to spin-spin relaxation and, here again, the environment at the molecular level plays a significant role in the magnitude of interaction. Relatively few electron spin relaxation studies of solutions have been conducted and the present work is addressed toward the extension of our knowledge in this area and the retrieval of dynamical information from line shape analyses on a time scale comparable to diffusion controlled phenomena.

Specifically, the electron spin relaxation of three Mn⁺²3d⁵ complexes, Mn(CH₃CN)₆⁺², MnCl₄^-2 in acetonitrile has been studied in considerable detail. The effective spin Hamiltonian constants were carefully evaluated under a wide range of experimental conditions. Resonance widths of these Mn⁺² complexes were studied in the presence of various excess ligand ions and as a function of concentration, viscosity, temperature and frequency (X-band, ~9.5 Ԍ Hz and K-band, ~35 Ԍ Hz).

A number of interesting conclusions were drawn from these studies. For the Et₄NCl-₄^-2 system several relaxation mechanisms leading to resonance broadening were observed. One source appears to arise through spin-orbit interactions caused by modulation of the ligand field resulting from transient distortions of the complex imparted by solvent fluctuations in the immediate surroundings of the paramagnetic ion. An additional spin relaxation was assigned to the formation of ion pairs [Et₄N⁺…MnCl₄^-2] and it was possible to estimate the dissociation constant for this specie in acetonitrile.

The Bu₄NBr-MnBr₄^-2 study was considerably more interesting. As in the former case, solvent fluctuations and ion-pairing of the paramagnetic complex [Bu₄N⁺…MnBr₄^-2] provide significant relaxation for the electronic spin system. Most interesting, without doubt, is the onset of a new relaxation mechanism leading to resonance broadening which is best interpreted as chemical exchange. Thus, assuming that resonance widths were simply governed by electron spin state lifetimes, we were able to extract dynamical information from an interaction in which the initial and final states are the same

MnBr₄^-2 + Br^- = MnBr₄^-2 + Br^-.

The bimolecular rate constants were obtained at six different temperatures and their magnitudes suggested that the exchange is probably diffusion controlled with essentially a zero energy of activation. The most important source of spin relaxation in this system stems directly from dipolar interactions between the manganese 3d⁵ electrons. Moreover, the dipolar broadening is strongly frequency dependent indicating a deviation between the transverse and longitudinal relaxation times. We are led to the conclusion that the 3d⁵ spin states of ion-paired MnBr₄^-2 are significantly correlated so that dynamical processes are also entering the picture. It was possible to estimate the correlation time, ^Td, characterizing this dynamical process.

In Part II we study nuclear magnetic relaxation of bromine ions in the MnBr4-2-Bu4NBr-acetonitrile system. Essentially we monitor the 79Br and 81Br linewidths in response to the [MnBr4-2]/[Br-] ratio with the express purpose of supporting our contention that exchange is occurring between "free" bromine ions in the solvent and bromine in the first coordination sphere of the paramagnetic anion. The complexity of the system elicited a two-part study: (1) the linewidth behavior of Bu4NBr in anhydrous CH3CN in the absence of MnBr4-2 and (2) in the presence of MnBr4-2. It was concluded in study (1) that dynamical association, Bu4NBr k1= Bu4N+ + Br-, was modulating field-gradient interactions at frequencies high enough to provide an estimation of the unimolecular rate constant, k1. A comparison of the two isotopic bromine linewidth-mole fraction results led to the conclusion that quadrupole interactions provided the dominant relaxation mechanism. In study (2) the "residual" bromine linewidths for both 79Br and 81Br are clearly controlled by quadrupole interactions which appear to be modulated by very rapid dynamical processes other than molecular reorientation. We conclude that the "residual" linewidth has its origin in chemical exchange and that bromine nuclei exchange rapidly between a "free" solvated ion and the paramagnetic complex, MnBr4-2.

I. Nuclear spin-internal-rotation-coupling. II. Fluorine spin-rotation interaction and magnetic shielding in fluorobenzene

Part I.

The interaction of a nuclear magnetic moment situated on an internal top with the magnetic fields produced by the internal as well as overall molecular rotation has been derived following the method of Van Vleck for the spin-rotation interaction in rigid molecules. It is shown that the Hamiltonian for this problem may be written

H_SR = Ῑ · M · Ĵ + Ῑ · M” · Ĵ”

Where the first term is the ordinary spin-rotation interaction and the second term arises from the spin-internal-rotation coupling.

The F¹⁹ nuclear spin-lattice relaxation time (T₁) of benzotrifluoride and several chemically substituted benzotrifluorides, have been measured both neat and in solution, at room temperature by pulsed nuclear magnetic resonance. From these experimental results it is concluded that in benzotrifluoride the internal rotation is crucial to the spin relaxation of the fluorines and that the dominant relaxation mechanism is the fluctuating spin-internal-rotation interaction.

Part II.

The radiofrequency spectrum corresponding to the reorientation of the F¹⁹ nuclear moment in flurobenzene has been studied by the molecular beam magnetic resonance method. A molecular beam apparatus with an electron bombardment detector was used in the experiments. The F¹⁹ resonance is a composite spectrum with contributions from many rotational states and is not resolved. A detailed analysis of the resonance line shape and width by the method of moments led to the following diagonal components of the fluorine spin-rotational tensor in the principal inertial axis system of the molecule:

F/Caa = -1.0 ± 0.5 kHz

F/Cbb = -2.7 ± 0.2 kHz

F/Ccc = -1.9 ± 0.1 kHz

From these interaction constants, the paramagnetic contribution to the F¹⁹ nuclear shielding in C₆H₅F was determined to be -284 ± ppm. It was further concluded that the F¹⁹ nucleus in this molecule is more shielded when the applied magnetic field is directed along the C-F bond axis. The anisotropy of the magnetic shielding tensor, σ_” - σ_⊥, is +160 ± 30 ppm.

A Continuum Model for Slip-Twinning Interactions in Magnesium and Magnesium Alloys

Due to their high specific strength and low density, magnesium and magnesium-based alloys have gained great technological importance in recent years. However, their underlying hexagonal crystal structure furnishes Mg and its alloys with a complex mechanical behavior because of their comparably smaller number of energetically favorable slip systems. Besides the commonly studied slip mechanism, another way to accomplish general deformation is through the additional mechanism of deformation-induced twinning. The main aim of this thesis research is to develop an efficient continuum model to understand and ultimately predict the material response resulting from the interaction between these two mechanisms.

The constitutive model we present is based on variational constitutive updates of plastic slips and twin volume fractions and accounts for the related lattice reorientation mechanisms. The model is applied to single- and polycrystalline pure magnesium. We outline the finite-deformation plasticity model combining basal, pyramidal, and prismatic dislocation activity as well as a convexification based approach for deformation twinning. A comparison with experimental data from single-crystal tension-compression experiments validates the model and serves for parameter identification. The extension to polycrystals via both Taylor-type modeling and finite element simulations shows a characteristic stress-strain response that agrees well with experimental observations for polycrystalline magnesium. The presented continuum model does not aim to represent the full details of individual twin-dislocation interactions, yet it is sufficiently efficient to allow for finite element simulations while qualitatively capturing the underlying microstructural deformation mechanisms.