Thesis (Ph.D.)--McMaster University, 2004. / Advisor: David Venus. Includes bibliographical references (leaves 138-144). Also available via World Wide Web.

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Orientador: Marcelo Knobel / Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Fisica Gleb Wataghin / Made available in DSpace on 2018-08-04T08:20:32Z (GMT). No. of bitstreams: 1 Duque_JoseGerivaldodosSantos_D.pdf: 2802085 bytes, checksum: 3e11d0645c4b8e47c4e251b671065013 (MD5) Previous issue date: 2005 / Resumo: Não informado / Abstract: Not informed. / Doutorado / Física da Matéria Condensada / Doutor em Ciências

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Ferromagnetic (FM) thin-film heterostructures provide opportunities to investigate GHz magnetic dynamics and emerging magnetoelectric devices based on dynamic phenomena. An intriguing direction for these studies is the control of the flow of pure (chargeless) spin current flow in different magnetic systems. In this thesis, we focus on the excitation of pure spin currents using ferromagnetic resonance (FMR), also known as spin pumping, and their transport characteristics in magnetic heterostructures based on Ni₈₁Fe₁₉ (Permalloy, or Py) under a variety of circumstances. In Chapter 2, we present measurements of the anisotropy of the spin pumping effect in the Pt/Py/Pt system via variable-frequency, swept-field FMR. We find a very small anisotropy of enhanced Gilbert damping with sign opposite to a recent theory's prediction from the Rashba effect at the FM/Pt interface. In Chapter 3, we present an experimental and theoretical study of spin dynamics in the antiferromagnetically coupled Py/Ru/Py system. We show that, contrary to the behavior of the uniform mode in a saturated single-layer FM, the symmetric mode in unsaturated synthetic antiferromagnet (SAF) has approximately constant FMR linewidth as a function of frequency. This behavior can be explained mostly semiclassically by our model. In Chapter 4, we present an investigation of interfacial Gilbert damping due to the spin pumping effect in Py/W heterostructures with enriched α phase or β phase W. The spin mixing conductances (SMC) for W at interfaces with Py are found to be significantly lower than those for similar heavy metals such as Pd and Pt, but comparable to those for Ta, and independent of enrichment in the β phase. The experimental results also indicate that W, no matter of which phase, is a good spin sink in Py/W heterostructures. In Chapter 5, we describe explorations of the spin pumping effect in antiferromagnetic insulator (AFI)-based heterostructures using variable-temperature, variable-frequency FMR. We find a spin-pumping-induced damping enhancement for Py/Cu/CoO, Py/Cu/CoO/Cu/Pt and Py/Cu/NiO/Cu/Pt. Broad peaks have been observed in FMR linewidth difference as a function of temperature for Py/Cu/NiO, normalized to the linewidth of the reference Py sample. Our results indicate that some effects previously attributed to spin current flow are better described by a defect-related mechanism. Chapter 6 summarizes the various findings of spin-pumping effects in ferromagnetic thin film heterostructures and possible future work.

Magnetic nanoparticles and molecules, in particular ferromagnetic noble metal nanoparticles, molecular magnet and single-molecule magnets (SMM), are perfect examples to investigate the role of quantum mechanics at the nanoscale. For example, SMMs are known to reverse their magnetization by quantum tunneling in the absence of thermal excitation and show a number of fundamental quantum mechanical manifestations, such as quantum interference effects. On the other hand, noble metal nanoparticles are found to behave ferromagnetically for diameters below a few nanometers. Some of these manifestations are still intriguing, and novel research approaches are necessary to advance towards a more complete understanding of these exciting nanoscale systems. In particular, the ability to study an isolated individual nanoscale system (i.e just one molecule or nanoparticle) is both challenging technologically and fundamentally essential. It is expected that accessing to the energy landscape of an isolated molecule/nanoparticle will allow unprecedented knowledge of the basic properties that are usually masked by collective phenomena when the systems are found in large ensembles or in their crystal form. Several approaches to this problem are currently under development by a number of research groups. For instance, some groups are developing deposition techniques to create patterned thin films of isolated magnetic nanoparticles and molecular magnets by means of optical lithography, low-energy laser ablation, or pulsed-laser evaporation or specific chemical functionalization of metallic surfaces with special molecular ligands. However, it is still a challenge to access the properties of an individual molecule or nanoparticle within a film or substrate. iv I have studied molecular nanomagnets and ferromagnetic noble metal nanoparticles by means of a novel experimental approach that mixes the chemical functionalization of nano-systems with the use of single-electron transistors (SETs). I have observed the Coulomb-blockade single-electron transport response through magnetic gold nanoparticles and single-molecule magnet. In particular, Coulomb-blockade response of a Mn4-based SET device recorded at 240 mK revealed the appearance of two diamonds (two charge states) with a clear switch between one and the other is indicative of a conformational switching of the molecule between two different states. The excitations inside the diamonds move with magnetic field. The curvature of the excitations and the fact of having them not going down to zero energy for zero magnetic field, indicated the presence of magnetic anisotropy (zero-field splitting) in the molecule. In addition, the high magnetic field slope of the excitations indicates that transitions between charge states differ by a net spin value equal to 9 (|∆S| = 9), as expected from the behavior of Mn4 molecules in their crystalline form. Anticrossings between different excitations are indicative of quantum superpositions of the molecular states, which are observed for the first time in transport measurements through and individual SMM.

<p>Predicting core losses in electromagnetic and electromechanical devices such as electric machines is crucial to avoid overheating or oversizing. This work focuses on predicting core loss under a dc bias condition which results in hysteresis loop distortion and an increase in the core loss. The interest in dc biased materials is to facilitate design of electric drive systems wherein the electric machine core is subject to a dc bias such as in homopolar machines. Owing to their simplicity and ease of use, Steinmetz-based models are considered in this work. Herein, four models based on Steinmetz Equations are studied and compared for dc offset sinusoidal field intensity waveforms. The model parameters are then characterized for a sample of M15 steel. Finally, the four models are compared with regards to their accuracy and performance under saturated conditions.</p>

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