abstract: Aluminum alloys are ubiquitously used in almost all structural applications due to their high strength-to-weight ratio. Their superior mechanical performance can be attributed to complex dispersions of nanoscale intermetallic particles that precipitate out from the alloy’s solid solution and offer resistance to deformation. Although they have been extensively investigated in the last century, the traditional approaches employed in the past haven’t rendered an authoritative microstructural understanding in such materials. The effect of the precipitates’ inherent complex morphology and their three-dimensional (3D) spatial distribution on evolution and deformation behavior have often been precluded. In this study, for the first time, synchrotron-based hard X-ray nano-tomography has been implemented in Al-Cu alloys to measure growth kinetics of different nanoscale phases in 3D and reveal mechanistic insights behind some of the observed novel phase transformation reactions occurring at high temperatures. The experimental results were reconciled with coarsening models from the LSW theory to an unprecedented extent, thereby establishing a new paradigm for thermodynamic analysis of precipitate assemblies. By using a unique correlative approach, a non-destructive means of estimating precipitation-strengthening in such alloys has been introduced. Limitations of using existing mechanical strengthening models in such alloys have been discussed and a means to quantify individual contributions from different strengthening mechanisms has been established. The current rapid pace of technological progress necessitates the demand for more resilient and high-performance alloys. To achieve this, a thorough understanding of the relationships between material properties and its structure is indispensable. To establish this correlation and achieve desired properties from structural alloys, microstructural response to mechanical stimuli needs to be understood in three-dimensions (3D). To that effect, in situ tests were conducted at the synchrotron (Advanced Photon Source) using Transmission X-Ray Microscopy as well as in a scanning electron microscope (SEM) to study real-time damage evolution in such alloys. Findings of precipitate size-dependent transition in deformation behavior from these tests have inspired a novel resilient aluminum alloy design. / Dissertation/Thesis / Doctoral Dissertation Materials Science and Engineering 2017

<p>  </p> <p>Atmospheric particles originate from all over the globe with wildly different sources such as sea spray aerosols of the ocean, mineral dust from deserts, biogenic emissions from forests, anthropogenic emissions of urban and industrial areas, volcanic eruptions, and many more. All of these particles can then be transported during which aging can occur where the external and internal chemical composition of particles and drastically be altered in which their physiochemical properties change or new particles as a whole are formed. Understanding what can cause this aging and correctly identifying how these particles change is vital for assessing climate in local areas. </p> <p>Chapter 3 focuses on dry intrusion (DI) and non-DI periods where vertical mixing of air occurs and allows for long range transport of particles. DI periods introduces populations of aged particles from far away sources into local regions. Identification and chemical characterization is performed for both of these periods to highlight the changes the DI period introduces in regards to particle morphology, chemical composition and lifetime. Analysis was performed via computer controlled scanning electron microscopy (CCSEM) for external information of the particles and scanning transmission x-ray microscopy (STXM) was used for internal information. The combination of these two techniques allows for a complete and thorough understanding of the particles during the two periods. </p> <p>Chapter 4 covers the first experiment done on a newly constructed cryogenic cooling cart which was created in the hopes to identify individual ice nucleating events of particles <em>in situ</em> when mimicking real world atmospheric conditions through temperature and humidity control. </p>

<p>The Earth–atmosphere energy balance is dictated by incoming solar radiation and outgoing thermal radiation with greenhouse gases (GHG) and aerosols playing a major role in this effect. The atmospheric abundance and properties of airborne particles and gases lead to the redistribution of radiative energy, resulting in a warming or cooling effect. However, the extent of this effect remains to be insufficiently constrained. Improved quantification and characterization of GHG and aerosols are important requirements to inform current climate models. High-precision instrumentation and thoughtful experimental strategies are necessary to yield various analytical measurement datasets, despite complex meteorological and environmental conditions. This dissertation focuses on the assessment of CO₂and atmospheric particles from aircraft-based measurements enabling representative and spatially sampling of local regions of interest.</p> <p>Chapter 1 provides introductory discussion on the atmospheric implication of GHG and aerosols on the climate and related uncertainties. Chapter 2 summarizes the employed experimental techniques for quantification of GHG and characterization of atmospheric particles. We relied on an aircraft platform equipped with an air turbulence probe for 3D wind vector calculation and a high-precision cavity ring-down spectrometer for the quantification of ambient CO₂, CH₄, and H2O_<em>v</em>. Furthermore, the simultaneous composition and morphological information of aerosol samples were assessed using complementary chemical imaging techniques. Chemical composition of elements with Z > 23 was determined using computer-controlled scanning electron microscopy with energy dispersive X-ray spectroscopy (CCSEM/EDX). Scanning transmission X-ray microscopy coupled with near edge X-ray absorption fine structure spectroscopy (STXM/NEXAFS) was used to determined spatially resolved elemental specific molecular information present in atmospheric particles.</p> <p>Chapter 3 presents our study focused on the characterization of mixed mineral dust and biomass burning (BB) aerosols during an intensive burning event. We identified distinct particle types based on individual elemental contribution pre-, syn-, and post-burning event including highly carbonaceous (54–83%) particles, aged mineral dust (1–6%), and sulfur-containing particles (17–41%). X-ray spectromicroscopy techniques were used to characterize the internal chemical heterogeneity of individual BB particles and the morphology of soot inclusions, as well as changes in the particle organic volume fraction (OVF). An estimation method for particle component masses (i.e., organics, elemental carbon, and inorganics) inferred from STXM measurements was used to determine quantitative mixing state metrics based on entropy-derived diversity measures for particles acquired at different periods of the BB event. In general, there was a small difference in the particle-specific diversity among the samples (<em>D</em>_<em>α</em> = 1.3–1.8). However, the disparity from the bulk population diversity observed during the intense periods was found to have high values of <em>D</em>_<em>γ</em> = 2.5–2.9, while particles collected outside of the burning event displayed lower bulk diversity of <em>D</em>_<em>γ</em> = 1.5–2.0. Quantitative methods obtained from chemical imaging measurements presented here will serve to accurately characterize the evolution of mixed BB aerosols within urban environments.</p> <p>Chapter 4 follows the investigation of the physicochemical properties of atmospheric particles collected onboard a research aircraft flown over the Azores using offline spectromicroscopy techniques. Particles were collected within the marine boundary layer (MBL) and free troposphere (FT) comparing samples after long-range atmospheric transport episodes facilitated by dry intrusion (DI) events. The quantification of the OVF of individual particles derived from X-ray spectromicroscopy, which relates to the multi-component internal composition of individual particles, showed a factor of 2.06±0.16 and 1.11±0.04 increase in the MBL and FT, respectively, among DI samples. We show that supplying particle OVF into the <em>κ</em>-Köhler equation can be used as a good approximation of field-measured <em>in situ</em> CCN concentrations. We also report changes in the <em>κ</em> values in the MBL from <em>κ</em>_{MBL, non-DI} = 0.48 to <em>κ</em>_{MBL, DI} = 0.41, while changes in the FT result in <em>κ</em>_{FT, non-D}_I = 0.36 to <em>κ</em>_{FT, DI} = 0.33, which is consistent with enhancements in OVF followed by the DI episodes. Our observations suggest that the entrainment of particles from long-range continental sources alters the mixing state population and CCN properties of aerosol in the region.</p> <p>Chapter 5 discusses the identification and characterization of fine-mode primary biogenic atmospheric particles (PBAP) from the harvesting of crops. Particle samples were analyzed using complementary chemical imaging techniques to apportion the particle-type population based on their size, morphology, and composition. The contribution of PBAP in the size range of 0.15−1.25 μm is estimated to be 10−12% of ∼39,000 analyzed particles. In addition, particle viscosity and phase state were inferred with X-ray spectromicroscopic analysis has shown that the fine-mode organic particles collected are viscous/semisolid (10²−10¹² Pa s) while the majority of PBAP fragments are solid (>10¹²Pa s). The observation of submicrometer, solid carbonaceous fragments of biogenic origin have implications for the regional CCN and ice nuclei budget. Therefore, the seasonal harvesting of crops may play an important, yet unrecognized, role in regional cloud formation and climate.</p> <p>Chapter 6  explores the measurements and quantification of latent heat, sensible heat, and CO₂ fluxes among different land covers in the surrounding area of urban regions using airborne flux techniques. Cities account for the majority of the global CO₂ emissions due to the consumption of energy, resources, infrastructure, and transportation demands. Accordingly, the accurate quantification of these emissions, with exceptional precision, is necessary so that progress towards emission reduction can be monitored. However, a major challenge in quantifying urban emission estimates arises from accurate background emission definitions and apportionment of emission sources in complex urban environments. Airborne eddy covariance measurements were performed to quantify the bidirectional exchange of latent heat, sensible heat, and CO₂ fluxes in the upwind region of Indianapolis within an active biosphere. Here, we observed differences in fluxes across different days and land covers (e.g., corn, soybean, and forests) allowing us to understand the impact of seasonal variability in urban emissions during the full growing season. These experiments illustrate the capability of a research aircraft to perform technically challenging near-direct measurements of atmosphere–surface exchange over local and regional scales.</p> <p>Chapter 7 presents a new method to spatially allocate airborne mass balance CO₂ emissions. We performed seven aircraft measurements downwind of New York City (NYC) quantifying CO₂ emissions during the non-growing seasons of 2018–2020. A series of prior inventories and footprint transport models were used to account for flux contribution outside the area of interest and attribute emission sources within policy-relevant boundaries of the five boroughs encompassing NYC and then employ the modeled enhancement fraction (Φ) to the bulk emission observations from the mass balance approach. Here, we calculated a campaign-averaged source apportioned mass balance CO₂ emission rate of 56±24 kmol/s. The performance and accuracy of this approach were evaluated against other published works including inventory scaling and inverse modeling, yielding a difference of 5.1% with respect to the average emission rate reported by the two complementary approaches. Utilizing the ensemble of emissions inventories and transport models, we also evaluated the overall sources of variability induced by the prior (1.7%), the transport (4.2%), and the daily variability (42.0%). This approach provides a solution to interpreting aircraft-based mass balance results in complex emission environments.</p> <p>Chapter 8 concludes with a brief discussion of technological advances and research outlooks for X-ray spectromicroscopy analysis on atmospheric particles and the quantification of GHG. Opportunities for future applications and novel development of CCSEM/EDX and STXM/NEXAFS to substantially extend the instrument capabilities and improve our understanding of the physicochemical properties of individual atmospheric particles. Chapter 8 also discusses recent developments in satellite-based CO₂ monitoring to complement direct airborne observations. In recent years, significant progress has been made in satellite-based measurements of CO₂ to reveal the spatio-temporal variation in atmospheric CO₂ concentration. The column-averaged dry air CO₂ mole have reached an accuracy of ~1 ppm with a spatial resolution of less than 4 km. Furthermore, column-averaged retrievals can be used to detect and estimate the surface CO₂ fluxes in an active biosphere, quantify anthropogenic emissions over megacities, and monitor the transport of fossil fuel plumes across different continents and seasons.</p>

Obwohl wir sie oft nicht bewusst wahrnehmen, sind Nanopartikel heutzutage in den meisten Bereichen unseres Alltags präsent, unter anderem in Lebensmitteln und ihren Verpackungen, Medizin, Medikamenten, Kosmetik, Pigmenten und in elektronischen Geräten wie Computermonitoren. Ein Großteil dieser Partikel weist, beabsichtigt oder unbeabsichtigt, eine Kern-Schale Morphologie auf. Einfachheitshalber wird diese Morphologie eines Kern-Schale-Nanopartikels (CSNP) oft als ideal angenommen, d.h. als ein sphärischer Kern, der komplett von einer Schale homogener Dicke bedeckt ist, mit einer scharfen Grenzfläche zwischen Kern- und Schalenmaterial. Außerdem wird vielfach auch davon ausgegangen, alle Partikel der Probe hätten gleiche Schalendicken. Tatsächlich weichen die meisten realen CSNPs in verschiedenster Weise von diesem Idealmodell ab, mit oft drastischen Auswirkungen darauf, wie gut sie ihre Aufgabe in einer bestimmten Anwendung erfüllen. Das Thema dieser kumulativen Doktorarbeit ist die exakte Charakterisierung der wirklichen Morphologie von CSNPs mit modernen Röntgen-basierten Methoden, konkret Röntgen-Photoelektronen-Spektroskopie (XPS) und Raster-Transmissions-Röntgen-Mikroskopie (STXM). Der Fokus liegt insbesondere auf CSNPs, die von einer idealen Kern-Schale-Morphologie abweichen. Aufgrund der enormen Vielfalt an CSNPs, die sich in Material, Zusammensetzung und Form unterscheiden, kann eine Messmethode nicht völlig unverändert von einer Probe auf eine andere übertragen werden. Nichtsdestotrotz, da die als Teil dieser Doktorarbeit präsentierten Artikel eine deutlich ausführlichere Beschreibung der Experimente enthalten als vergleichbare Publikationen, stellen sie eine wichtige Anleitung für andere Wissenschaftler dafür dar, wie aussagekräftige Informationen über CSNPs durch Oberflächenanalytik erhalten werden können. / Even though we often do not knowingly recognize them, nanoparticles are present these days in most areas of our daily life, including food and its packaging, medicine, pharmaceuticals, cosmetics, pigments as well as electronic products, such as computer screens. The majority of these particles exhibits a core-shell morphology either intendedly or unintendedly. For the purpose of practicability, this core-shell nanoparticle (CSNP) morphology is often assumed to be ideal, namely a spherical core fully encapsulated by a shell of homogeneous thickness with a sharp interface between core and shell material. It is furthermore widely presumed that all nanoparticles in the sample possess the same shell thickness. As a matter of fact, most real CSNPs deviate in several ways from this ideal model with quite often severe impact on how efficiently they perform in a specific application. The topic of this cumulative PhD thesis is the accurate characterization of the actual morphology of CSNPs by advanced X-ray analytical techniques, namely X-ray photoelectron spectroscopy (XPS) and scanning transmission X-ray microscopy (STXM). A special focus is on CSNPs which deviate from an ideal core-shell morphology. Due to the vast diversity of nanoparticles differing in material, composition and shape, a measurement procedure cannot unalteredly be transferred from one sample to another. Nevertheless, because the articles in this thesis present a greater depth of reporting on the experiments than comparable publications, they constitute an important guidance for other scientists on how to obtain meaningful information about CSNPs from surface analysis.

Das Schalten und das Auslesen der magnetischen Ausrichtung einzelner winziger magnetischer Informationsspeicher müssen zu wirklich nanoskopischer Dimension entwickelt werden, um mit der Miniaturisierung von modernen, nanoelektronischen Bauteilen Schritt zu halten. Daher sind neue Konzepte, den magnetischen Zustand von Nanostrukturen elektronisch gezielt zu beeinflussen, derzeitig im Mittelpunkt wissenschaftlicher Untersuchungen. Diese Arbeit befasst sich mit dem zuverlässigen Einstellen der Magnetisierung eines rein horizontal kontaktierten, nanoskopischen Magneten, in zwei stabile Zustände. Ein spinpolarisierter Strom wird bei Raumtemperatur in eine Leiterbahn unterhalb des magnetischen Nanopillars injiziert. Spindiffusion durch den Kontakt zwischen der Leiterbahn (Cu) und dem Pillar (CoFe) ruft eine Spin-Akkumulation im Nanopillar hervor, der durch den Spin Transfer Torque-Effekt (STT) vermittelt wird. Bei diesem Prozess verursachen die akkumulierten Elektronenspins ein auftretendes Netto-Moment, das senkrecht auf die Magnetisierungsorientierung des Nanopillars wirkt und so das Schalten ermöglicht. In den STT-induzierten Schaltexperimenten wird der magnetische Zustand des Nanopillars durch eine bildgebendes Messverfahren mittels Rasterröntgentransmissionsmikroskopie (STXM) erfasst. So konnte gezeigt werden, dass sich die Magnetisierung des Pillars auch gegen das Oersted-Feld des Schaltstroms reversibel schalten lässt. / “Changing and detecting the orientation of nanomagnetic structures, which can be used for durable information storage, needs to be developed towards true nanoscale dimensions for keeping up the miniaturization speed of modern nano electronic components. Therefore, new concepts for controlling the state of nano magnets are currently in the focus of research in the field of nanoelectronics. Here, we demonstrate reproducible switching of a purely metallic nanopillar placed on a lead that conducts a spin-polarized current at room temperature. Spin diffusion across the metal-metal (Cu to CoFe) interface between the pillar and the lead causes spin accumulation in the pillar, which may then be used to set the magnetic orientation of the pillar by means of Spin Transfer Torque (STT). In our experiments, the detection of the magnetic state of the nanopillar is performed by direct imaging via scanning transmission x-ray microscopy (STXM)” [1]. Therefore it could be demonstrated, to reversibly switch the nanopillar’s magnetic state even against the Oersted field which is induced by the switching current. Furthermore we could show, that magnetization switching is possible by a pure spin current that is diffusively transported beneath the nanopillar.

Das Schalten und das Auslesen der magnetischen Ausrichtung einzelner winziger magnetischer Informationsspeicher müssen zu wirklich nanoskopischer Dimension entwickelt werden, um mit der Miniaturisierung von modernen, nanoelektronischen Bauteilen Schritt zu halten. Daher sind neue Konzepte, den magnetischen Zustand von Nanostrukturen elektronisch gezielt zu beeinflussen, derzeitig im Mittelpunkt wissenschaftlicher Untersuchungen. Diese Arbeit befasst sich mit dem zuverlässigen Einstellen der Magnetisierung eines rein horizontal kontaktierten, nanoskopischen Magneten, in zwei stabile Zustände. Ein spinpolarisierter Strom wird bei Raumtemperatur in eine Leiterbahn unterhalb des magnetischen Nanopillars injiziert. Spindiffusion durch den Kontakt zwischen der Leiterbahn (Cu) und dem Pillar (CoFe) ruft eine Spin-Akkumulation im Nanopillar hervor, der durch den Spin Transfer Torque-Effekt (STT) vermittelt wird. Bei diesem Prozess verursachen die akkumulierten Elektronenspins ein auftretendes Netto-Moment, das senkrecht auf die Magnetisierungsorientierung des Nanopillars wirkt und so das Schalten ermöglicht. In den STT-induzierten Schaltexperimenten wird der magnetische Zustand des Nanopillars durch eine bildgebendes Messverfahren mittels Rasterröntgentransmissionsmikroskopie (STXM) erfasst. So konnte gezeigt werden, dass sich die Magnetisierung des Pillars auch gegen das Oersted-Feld des Schaltstroms reversibel schalten lässt.:Kurzfassung v Abstract vi Danksagung xi 1 Einleitung 1 2 Grundlagen zu Spintronic 5 2.1 Elektronenspins als Grundlage für den Ferromagnetismus . . . . . . 6 2.2 Magnetowiderstandseffekte . . . . . . . . . . . . . . . . . . . . . . . 7 2.2.1 Anisotroper Magnetowiderstandseffekt (AMR) . . . . . . . . 8 2.2.2 Riesenmagnetowidersandseffekt (GMR) . . . . . . . . . . . . 10 2.2.3 Tunnelmagnetowiderstandeffekt (TMR) . . . . . . . . . . . 13 2.3 Spin–Transport . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15 2.3.1 Spinpolarisation . . . . . . . . . . . . . . . . . . . . . . . . . 17 2.3.2 Spin-Injektion und Spin-Akkumulation . . . . . . . . . . . . 17 2.3.3 Spinpolarisierter elektrischer Transport . . . . . . . . . . . . 20 2.4 Spin Transfer Torque (STT) . . . . . . . . . . . . . . . . . . . . . . 25 2.5 Geometrien für Spintronic–Bauelemente . . . . . . . . . . . . . . . 30 3 Probenkonzept und Fabrikationsmethoden 35 3.1 Probenkonzept . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 35 3.1.1 Anforderungen an die CIP–STT-Struktur . . . . . . . . . . . 37 3.1.2 Anforderungen an die ferromagnetischer Materialien . . . . . 38 3.2 Techniken der Probenfabrikation . . . . . . . . . . . . . . . . . . . . 40 3.2.1 Elektronenstrahllithografie (EBL) . . . . . . . . . . . . . . . 41 3.2.2 Positiv- und Negtivlack Prozess . . . . . . . . . . . . . . . . 41 3.2.3 Physikalisches Ätzen . . . . . . . . . . . . . . . . . . . . . . 43 3.3 Probenfabrikation . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43 4 Experimentelle Methoden 49 4.1 Transmissionsröntgenmikroskopie . . . . . . . . . . . . . . . . . . . 49 4.1.1 Rastertransmissionsröntgenmikroskopie (STXM) . . . . . . . 51 4.1.2 Kontrastmechanismen . . . . . . . . . . . . . . . . . . . . . 53 4.1.3 Röntgenmagnetischer zirkularer Dichroismus (XMCD) . . . 54 4.2 Magneto-optische Kerr–Effekt Mikroskopie . . . . . . . . . . . . . . 57 4.2.1 Kerr–Mikroskop . . . . . . . . . . . . . . . . . . . . . . . . . 58 4.2.2 Longitudinale Kerr–Geometrie . . . . . . . . . . . . . . . . . 58 5 STT–Experimente und Diskussion 61 5.1 Experimenteller Aufbau . . . . . . . . . . . . . . . . . . . . . . . . 62 5.2 Eigenschaften der magnetischen Bauelemente . . . . . . . . . . . . . 64 5.2.1 MOKE-Mikroskopie . . . . . . . . . . . . . . . . . . . . . . . 65 5.2.2 Mikromagnetische Simulation . . . . . . . . . . . . . . . . . 67 5.2.3 Analytische Berechnung zum Nanopillar . . . . . . . . . . . 70 5.2.4 Röntgentransmissionsmikroskopie . . . . . . . . . . . . . . . 72 5.3 Spin Transfer Torque-Schalten . . . . . . . . . . . . . . . . . . . . 74 5.3.1 STT-Schalten mit unterstützendem Magnetfeld . . . . . . . 74 5.3.2 STT-Schalten ohne unterstützendes Magnetfeld . . . . . . . 79 5.3.3 Betrachtung besonderer experimenteller Aspekte . . . . . . . 81 5.3.4 STT-Schalten ohne direkten Ladungstransport . . . . . . . . 89 5.3.5 Magnetisierungsumkehr durch Oersted-Feld . . . . . . . . . 93 6 Zusammenfassung und Ausblick 97 A STXM-Hysteresemessungen der Polarisatoren und Nanopillar 101 Literaturverzeichnis 105 / “Changing and detecting the orientation of nanomagnetic structures, which can be used for durable information storage, needs to be developed towards true nanoscale dimensions for keeping up the miniaturization speed of modern nano electronic components. Therefore, new concepts for controlling the state of nano magnets are currently in the focus of research in the field of nanoelectronics. Here, we demonstrate reproducible switching of a purely metallic nanopillar placed on a lead that conducts a spin-polarized current at room temperature. Spin diffusion across the metal-metal (Cu to CoFe) interface between the pillar and the lead causes spin accumulation in the pillar, which may then be used to set the magnetic orientation of the pillar by means of Spin Transfer Torque (STT). In our experiments, the detection of the magnetic state of the nanopillar is performed by direct imaging via scanning transmission x-ray microscopy (STXM)” [1]. Therefore it could be demonstrated, to reversibly switch the nanopillar’s magnetic state even against the Oersted field which is induced by the switching current. Furthermore we could show, that magnetization switching is possible by a pure spin current that is diffusively transported beneath the nanopillar.:Kurzfassung v Abstract vi Danksagung xi 1 Einleitung 1 2 Grundlagen zu Spintronic 5 2.1 Elektronenspins als Grundlage für den Ferromagnetismus . . . . . . 6 2.2 Magnetowiderstandseffekte . . . . . . . . . . . . . . . . . . . . . . . 7 2.2.1 Anisotroper Magnetowiderstandseffekt (AMR) . . . . . . . . 8 2.2.2 Riesenmagnetowidersandseffekt (GMR) . . . . . . . . . . . . 10 2.2.3 Tunnelmagnetowiderstandeffekt (TMR) . . . . . . . . . . . 13 2.3 Spin–Transport . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15 2.3.1 Spinpolarisation . . . . . . . . . . . . . . . . . . . . . . . . . 17 2.3.2 Spin-Injektion und Spin-Akkumulation . . . . . . . . . . . . 17 2.3.3 Spinpolarisierter elektrischer Transport . . . . . . . . . . . . 20 2.4 Spin Transfer Torque (STT) . . . . . . . . . . . . . . . . . . . . . . 25 2.5 Geometrien für Spintronic–Bauelemente . . . . . . . . . . . . . . . 30 3 Probenkonzept und Fabrikationsmethoden 35 3.1 Probenkonzept . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 35 3.1.1 Anforderungen an die CIP–STT-Struktur . . . . . . . . . . . 37 3.1.2 Anforderungen an die ferromagnetischer Materialien . . . . . 38 3.2 Techniken der Probenfabrikation . . . . . . . . . . . . . . . . . . . . 40 3.2.1 Elektronenstrahllithografie (EBL) . . . . . . . . . . . . . . . 41 3.2.2 Positiv- und Negtivlack Prozess . . . . . . . . . . . . . . . . 41 3.2.3 Physikalisches Ätzen . . . . . . . . . . . . . . . . . . . . . . 43 3.3 Probenfabrikation . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43 4 Experimentelle Methoden 49 4.1 Transmissionsröntgenmikroskopie . . . . . . . . . . . . . . . . . . . 49 4.1.1 Rastertransmissionsröntgenmikroskopie (STXM) . . . . . . . 51 4.1.2 Kontrastmechanismen . . . . . . . . . . . . . . . . . . . . . 53 4.1.3 Röntgenmagnetischer zirkularer Dichroismus (XMCD) . . . 54 4.2 Magneto-optische Kerr–Effekt Mikroskopie . . . . . . . . . . . . . . 57 4.2.1 Kerr–Mikroskop . . . . . . . . . . . . . . . . . . . . . . . . . 58 4.2.2 Longitudinale Kerr–Geometrie . . . . . . . . . . . . . . . . . 58 5 STT–Experimente und Diskussion 61 5.1 Experimenteller Aufbau . . . . . . . . . . . . . . . . . . . . . . . . 62 5.2 Eigenschaften der magnetischen Bauelemente . . . . . . . . . . . . . 64 5.2.1 MOKE-Mikroskopie . . . . . . . . . . . . . . . . . . . . . . . 65 5.2.2 Mikromagnetische Simulation . . . . . . . . . . . . . . . . . 67 5.2.3 Analytische Berechnung zum Nanopillar . . . . . . . . . . . 70 5.2.4 Röntgentransmissionsmikroskopie . . . . . . . . . . . . . . . 72 5.3 Spin Transfer Torque-Schalten . . . . . . . . . . . . . . . . . . . . 74 5.3.1 STT-Schalten mit unterstützendem Magnetfeld . . . . . . . 74 5.3.2 STT-Schalten ohne unterstützendes Magnetfeld . . . . . . . 79 5.3.3 Betrachtung besonderer experimenteller Aspekte . . . . . . . 81 5.3.4 STT-Schalten ohne direkten Ladungstransport . . . . . . . . 89 5.3.5 Magnetisierungsumkehr durch Oersted-Feld . . . . . . . . . 93 6 Zusammenfassung und Ausblick 97 A STXM-Hysteresemessungen der Polarisatoren und Nanopillar 101 Literaturverzeichnis 105