03 Fakultät Chemie

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    Spectroscopic investigations of the magnetic anisotropy of lanthanide- and cobalt-based molecular nanomagnets
    (2016) Rechkemmer, Yvonne; Slageren, Joris van (Prof. Dr.)
    Single-molecule magnets are metal complexes exhibiting an energy barrier for spin reversal, leading to magnetic bistability and slow relaxation of the magnetization. Their potential for practical applications such as high-density magnetic data storage was recognized early on and with the goal of achieving high energy barriers, different kinds of single-molecule magnets have been synthesized. The quadratic dependence of the barrier height on the spin motivated chemists to synthesize metal complexes with very high total spins; however, with limited success. It was shown that high spins come along with low anisotropies and increased interest thus focused on the synthesis and investigation of (mononuclear) complexes of highly anisotropic metal centers, e.g. lanthanide or cobalt complexes. Although rather high energy barriers can be achieved in such systems, practical application remains problematic and has not been realized yet. Reasons are for example the lack of rational design criteria and the complex interplay of different magnetic relaxation pathways. The aim of this work was therefore the comprehensive magnetic and spectroscopic investigation of selected molecular lanthanide and cobalt compounds in order to obtain a deeper insight into the correlation of molecular and electronic structures as well as the corresponding magnetic properties. The applied spectroscopic methods included electron paramagnetic resonance spectroscopy, far-infrared spectroscopy and optical methods. Special emphasis was placed on magnetic circular dichroism (MCD) spectroscopy, which served as a main tool for electronic structure determination. However, since the MCD-spectrometer was not part of the available experimental equipment at the University of Stuttgart, its design, setup and characterization were the first part of this work. In the further course of this work MCD-spectroscopy was employed for the electronic structure determination of selected lanthanide and cobalt compounds. The studied lanthanide compounds were literature-known molecular tetra-carbonates of erbium (1-Er) and dysprosium (1-Dy). Detailed magnetometric studies showed that both 1-Er and 1-Dy are field-induced single-molecule magnets; however, 1-Er and 1-Dy show significant differences in their magnetic relaxation behavior. The magnetic studies were complemented by detailed spectroscopic investigations.The combination of far-infrared-, luminescence- and MCD-spectroscopy allowed for the experimental determination of 48 energy levels for 1-Er and 55 levels for 1-Dy, which built the foundation for the subsequent crystal field analysis and electronic structure determination. In addition, the results of EPR-spectroscopic studies were used for fine-tuning and verifying the respectively determined crystal field parameters. Calculating the magnetic dipole strengths for transitions between the relevant states led to a quantitative understanding of the magnetic relaxation pathways. Besides the investigation of lanthanide compounds, this thesis deals with two classes of cobalt complexes. The first class comprises mononuclear complexes in which one Co(II) ion is ligated by the nitrogen donors of two doubly deprotonated 1,2-bis(methanesulfonamido)-benzene-ligands. Rather acute N-Co-N bite angles indicate strong deviations from ideal tetrahedral symmetry. The static magnetic properties hint at very high energy barriers for spin reversal and with the help of far-infrared spectroscopy, largely negative axial zero-field splitting parameters were determined. The corresponding energy barriers belong to the highest ever reported for 3d-transition metal complexes and investigating the dynamic magnetic properties confirmed single-molecule magnet behavior. The unique magnetic properties were fully explained by analyzing spectroscopic results. The MCD-spectra showed intense signals that were assigned to spin-allowed d-d-transitions. Subsequent crystal field analysis revealed that the strong axial crystal field generated by the ligands leads to a large splitting of the electronic terms and thus in turn to a relatively small energy gap between the electronic ground state and the first excited state. The resulting increase in second-order spin-orbit coupling explains the high energy barriers observed in the studied complexes. The second class of cobalt compounds studied in this work included dimers of distorted octahedrally coordinated Co(II) ions bridged by symmetrical or asymmetrical quinone based bridging ligands. The main focus of investigation lay on the impact of the bridging ligand on the magnetic coupling between the cobalt centers. Thus, the magnetic properties of the complexes were studied with the help of static susceptibility and magnetization measurements and analyzed by means of different models. Depending on the bridging ligand, different signs for the exchange coupling constants were found. The varying signs can be explained by different relative contributions of possible exchange paths, influenced by the different substituents at the bridging ligands or slight geometry differences. The observations indicate that electron withdrawing substituents favor ferromagnetic couplings, which are preferred in the context of molecular magnetism. All in all, it can be concluded that this work provides a contribution to the deeper understanding of the features relevant for single-molecule magnets. The electronic structure determination for selected lanthanide and cobalt complexes applying advanced magnetometric and spectroscopic techniques not only led to an understanding of the static and dynamic magnetic properties but also allowed for the development of design criteria and new approaches for improved single-molecule magnets in the future.
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    Extension of a VCI program for the calculation of rovibrational intensities
    (2023) Tschöpe, Martin; Rauhut, Guntram (apl. Prof. Dr.)
    Die Identifizierung von Molekülen im interstellaren Medium, in zirkumstellaren Scheiben und in den Atmosphären kalter Exoplaneten ist eine große Herausforderung in der Astrophysik und basiert hauptsächlich auf hochgenauen Rotations- und Rotationsschwingungs-Referenzspektren. Eine Möglichkeit, diese Referenzspektren zu bestimmen, sind ab initio-Berechnungen, da sie eine effiziente Simulation eines breiten Bereichs von Bedingungen (einschließlich extrem niedriger Drücke und Temperaturen) ermöglichen. In dieser Arbeit wurde eine neue und besonders effiziente Implementierung der Rotationsschwingungskonfigurationswechselwirkungstheorie für die Berechnung von Infrarot-Rotationschwingungsspektren entwickelt, um die Berechnung dieser Referenzspektren zu ermöglichen. Der Ansatz basiert auf Normalkoordinaten und einer Mehrmodenentwicklung der mehrdimensionalen Potential- und Dipolmomentflächen sowie Schwingungs-Selbst-konsistentes-Feld-Verfahren und Schwingungskonfigurationswechselwirkungstheorie. Dabei wird ein direktes Produkt zwischen Schwingungsbasisfunktionen und Rotationsbasisfunktionen verwendet. So kann im Gegensatz zu der zuvor eingeführten Rotationskonfigurationswechselwirkungstheorie die Wechselwirkung zwischen Rotations- und Vibrationsbanden berücksichtigt werden. Dies geschieht mit hoher Genauigkeit, indem die Terme höherer Ordnung des inversen effektiven Trägheitsmomenttensors μ für den Rotationsterm und die Coriolis-Kopplung im Watson Hamiltonian berücksichtigt werden. Darüber hinaus werden eine neue Rotationsbasis namens Molekülspezifische Rotationsbasis (MSRB) und eine neue Art der Zuweisung von Rotationsschwingungsquantenzahlen eingeführt. Das Konvergenzverhalten verschiedener Entwicklungen für die Rotationsschwingungskonfigurationswechselwirkungstheorie (RVCI) zeigte sehr individuelle Effekte für die fünf untersuchten Parameter. Wenn die maximale Gesamtdrehimpulsquantenzahl Jmax oder die Größe der Schwingungsbasis nicht ausreichend konvergiert, treten besonders große Artefakte auf. Es werden effiziente Methoden zur Erkennung und Vermeidung dieser Probleme vorgestellt. Auch die Größe des Schwingungsbasissatzes ist ein entscheidender Parameter für die Konvergenz des Spektrums. Der beste Indikator für die Konvergenz bezüglich dieses Parameters und für die Stärke der Kopplung ist der spektrale Abstand zwischen den Schwingungsbanden. Für die beiden quasi-entarteten Schwingungsmoden von H2 CS ist die Coriolis-Kopplung nullter Ordnung sehr entscheidend, während die Terme erster Ordnung nur geringe Änderungen verursachen. Im Vergleich zu den Coriolis-Kopplungstermen erfordern die Rotationsterme eine um eine Ordnung höhere μ-Tensorentwicklung für die gleiche Genauigkeit. Die erste Ordnung führt für ganze Progressionen zu Energieverschiebungen von höchstens 5 cm-1 . Die durch die Terme der zweiten Ordnung hervorgerufenen Änderungen sind um mehr als eine Größenordnung geringer. Da das Fehlen von Kopplungstermen höherer Ordnung keine Artefakte im Spektrum verursacht, ist eine unzureichende Konvergenz in den resultierenden Spektren sehr schwierig zu erkennen. Die Berechnungen für die erste Veröffentlichung in dieser Dissertation beruhten auf einer Reihe von Näherungen, die im weiteren Verlauf dieser Arbeit entfernt werden konnten. Die meisten dieser Näherungen hatten kaum Auswirkungen auf die Spektren von Ketenimin, da sie bis 2900 cm-1 nur zu geringfügigen Änderungen des Spektrums führten. Oberhalb dieser Grenze zeigen jedoch die ν1 -Bande und die Kopplung zwischen ν8 + ν12 und ν11 , dass sich die Qualität der Quantenzahlzuordnung und die Konsistenz der Intensitäten in den letzten drei Jahren deutlich verbessert haben. Die neuen Berechnungen zeigen auch eine interessante turnaround Progression in diesem Bereich. Die Studie zur Linienverbreiterung unter Verwendung von Propynal als Anwendungsmolekül bestätigte die Annahme, dass für Moleküle mit 6 - 10 Atomen keine Notwendigkeit besteht, beyond Voigt-Profile zu verwenden, wie sie für kleine Moleküle (N2 , H2 O, CH4, NH3 , etc.) benutzt werden. Der Grund dafür ist, dass die höhere Masse und der größere Trägheitstensor zu einer hohen Schwingungszustandsdichte führen, wodurch die genaue Form des Verbreiterungsprofil weniger relevant wird. Am Ende dieser Arbeit werden verschiedene Laufzeitoptimierungen analysiert. Die Parallelisierung zeigt eine nahezu perfekte Skalierung in der Anzahl der CPU-Kerne für die Vorberechnungen der Schwingungsintegrale und für die Intensitätsberechnung. Darüber hinaus sparen die Vorberechnungen der Schwingungsintegrale etwa einen Faktor von 8 an Gesamtrechenzeit ein. Die Kontraktion der MSRB-Koeffizienten mit den RVCI-Koeffizienten führt zu einer Gesamtrechenzeitreduktion von 50% für H2CS und 97% für Ketenimin. Die derzeitige Implementierung der RVCI-Theorie in MOLPRO ist in der Lage, Infrarot- und Raman-Spektren für bis zu 10 Atome, von T = 0 K bis zu Raumtemperatur und über einen weiten Spektralbereich zu berechnen. Die Kombination all dieser Eigenschaften erfordert jedoch große Rechenressourcen. Im Ausblick wird daher eine Liste von Optimierungen zur Steigerung der Recheneffizienz vorgestellt. Darüber hinaus wird eine Reihe von möglichen zusätzlichen Funktionalitäten und Methoden zur Erhöhung der Robustheit des Programms aufgelistet.
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    Novel X-ray lenses for direct and coherent imaging
    (2019) Sanli, Umut Tunca; Schütz, Gisela (Prof. Dr.)
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    Chirality effects in thermotropic and lyotropic nematic liquid crystals under confined geometries
    (2019) Dietrich, Clarissa; Giesselmann, Frank (Prof. Dr.)
    Chirality is a phenomenon in nature that appears across all disciplines of natural science, from biology to mathematics. The spontaneous formation of chiral structures in a system of achiral components is known as spontaneous mirror symmetry breaking and is by itself of fundamental interest leading also towards the question of the origin of homochirality in nature in general. In this work, we show that by means of the topology imposed by the confining geometry and by interfacial boundary conditions - in combination with the physical properties of a liquid crystal - spontaneous mirror symmetry broken structures can be obtained. They are analyzed, inter alia, with respect to the types of geometrical confinements used, e.g. how the confinement amplifies, induces, and influences the detection of chirality effects in order to facilitate the measurement of tiny amounts of chiral additives qualitatively and quantitatively.
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    Micellar lyotropic gels : the interplay between gel network and liquid-crystalline order
    (2021) Dieterich, Sonja; Gießelmann, Frank (Prof. Dr.)
    Surfactant based lyotropic liquid-crystalline (LLC) gels in the sense that genuine micellar LLC phases are immobilized by an interpenetrating gel network were practically unknown until 2016. This “blind spot” in the landscape of anisotropic gels has now been filled to a certain extent by the results of this dissertation. Following the rational design strategy to gel surfactant based LLC phases with the help of low molecular mass gelators (LMWGs), not only lamellar and hexagonal LLC gels, but also the very first example of micellar nematic gels were obtained. Furthermore, this work has led to first important insights into how the self assembly of the gel is directed and how the gel network and the LLC phase mutually influence each other in terms of structure and morphology
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    Chiral metamaterials
    (2016) Eslami, Sahand; Fischer, Peer (Prof. Dr.)
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    Ion beam lithographic and multilayer fresnel zone plates for soft and hard X-rays: nanofabrication and characterization
    (2015) Keskinbora, Kahraman; Schütz, Gisela (Prof. Dr.)
    X-ray microscopy has become an important analytical characterization method for a plethora of applications in materials science, physics, chemistry and biology, thanks to the emergence of modern synchrotron radiation facilities. These facilities enable high brilliance, energy tunable, variable polarization X-rays which gives access to mass density, elemental, chemical, electronic and magnetic properties of materials. In the soft X-ray energies nearly all elements can be probed by spectromicroscopic methods. Another important property of synchrotron radiation is the time structure in the ns to ps range, which can be utilized for sophisticated time resolution studies. These opportunities can be combined with high spatial resolution which is determined by the focusing method and the optic. Focusing of X-rays has historically been a difficult task due to strong absorption and weak phase shift of X-rays within matter. The required phase shift of X-rays, which depends on the real part of the complex refractive index, differs from 1 (the vacuum refractive index) only on the order of 10^-2 to 10^-6 and conventional lenses do not work. One very successful X-ray optic is the Fresnel Zone Plate (FZP), a diffractive optic that act as a lens under certain conditions and can focus X-rays to nanometer sized spots. The resolution of the FZP depends on the width of the outermost zone and is highly correlated with the smallest feature that can be fabricated. Conventionally, the e-beam lithography (EBL) is used for production FZPs which could resolve up to 10 nm structures with serious limitations. One difficulty of EBL is its ever increasing complexity for many-step fabrication of smaller features or intricate geometries. Therefore, EBL is mostly constrained to planar, binary geometries with moderate efficiencies strongly decreasing with energy and not effective for hard X-rays. Special 3D geometries in the form of kinoform lenses can theoretically have 100 % focusing efficiencies. Attempts to approximate these geometries via EBL increased the number of process steps even further. The smallest FZP feature size even for low aspect ratios achievable via EBL is fundamentally limited due to the proximity effect which is the interaction and spread of electrons within the resist material. We addressed these issues by focusing our research on alternative FZP fabrication techniques as high-speed ion beam lithography (IBL), and gray scale ion lithography to realize efficient kinoforms. Another approach towards full-material multilayer FZPs with infinite aspect ratio was based on atomic layer deposition (ALD) with subsequent ion beam slicing. Each of these three methods targets specific challenges faced by the e-beam lithography based FZP fabrication techniques. All the fabricated FZPs were tested for their resolution and efficiency performances at a state of the art scanning transmission X-ray microscope at BESSY for soft X-rays and/or at optical test stations at ESRF and PETRA III for hard X-rays. Using IBL the rapid preparation of a 110 nm thick Au FZP with 50 µm diameter and 50 nm ∆r in less than 13 minutes is demonstrated. Employed for X-ray microscopy, the FZP clearly resolved 28.5 nm features with a cut-off of 24.3 nm at ~1120 eV. Additional process improvements were made towards smaller zones with higher zone quality. They allowed the preparation of a FZP with 30 nm outermost half-period remarkably, in about 8 min. This FZP was shown to clearly resolve 21 nm features on a multilayer test object with large room for improvement. This high through-put FZP production route is of special interest not only concerning the low cost and easy availability. A large array of these optical components is attractive, for experiments such as one-shot ultra-high brilliance FEL investigations due to the radiation damage or for instance for coded-aperture arrays for high-angle resolving X-ray astronomy. Towards fabrication of kinoforms for high efficiency X-ray focusing, we have performed various materials optimization studies in order to achieve a high surface quality optic. After various trials the materials were finally optimized and the fabricated lenses achieved more than 14 % absolute diffraction efficiency that is almost 90 % compared to the theoretical prediction. This confirms how closely we were able to replicate the ideal three dimensional surface relief structure for the first time. It was possible to carry out imaging with these lenses with half-pitch resolutions down to 60 nm. The kinoform lenses were tested at the soft X-ray range where a significant absorption is present in materials. These results also potentially pave the way for very high efficiency hard X-ray focusing which can in principle be utilized in laboratory based X-ray sources, X-ray astronomy and the new rising field of X-ray ptychography. To fabricate high resolution ML-FZPs, Al2O3/Ta2O5multilayers, deposited on a smooth glass optical fiber via atomic layer deposition using non-dedicated instruments were carefully cut-out, sliced and polished to a high quality surface finish using focused ion beams. Following the transfer of the slice to a TEM grid as holder the slices were polished to a high surface finish quality, also via a focused ion beam. Fabricated ML-FZPs were synchrotron tested using an in-house constructed 2-axis tilt stage specially designed for aligning ML-FZP with respect to the X-ray optical axis. The results showed that it was possible to resolve 21 nm features in direct imaging at 1200 eV and sub-30 nm focusing at 8 keV. This is the highest demonstrated resolving power for a multilayer type FZP, to date to the best of our knowledge. Results exhibit the potential for high-resolution hard X-ray focusing where this type of optics are especially efficient. For ultra-high resolution hard and soft X-ray imaging, with potentially achievable ∆r of a few nm is well below what can be achieved through any lithography method available today.
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    Structural and electronic properties of nickelate heterostructures
    (2016) Wrobel, Friederike; Keimer, Bernhard (Prof. Dr.)
    The fabrication of thin films and multilayers has led to the discovery of novel functional properties which are widely used in electronic devices nowadays. The limit of such a material design is atomic layer-by-layer deposition which was made possible through shuttered molecular beam epitaxy (MBE) growth. In the course of this thesis project a newly developed oxide MBE system was used to grow two different types of nickelate heterostructures, namely superlattices (SLs) consisting of metallic and paramagnetic LaNiO3 sandwiched between a large band-gap insulator and a combination of lanthanum nickelate and cuprate layers into a single hybrid structure. The former type was intensively studied in the last years and a transition to a weakly insulating, antiferromagnetically ordered state was observed in samples where the LaNiO3 thickness had been reduced to only two unit cells. So far little was known about the influence of the growth method on the defects in the samples and consequently on their physical properties. The use of oxide MBE enabled us to improve the overall sample quality of nickelate SLs and to design a novel material. We first optimized the growth of LaNiO3 and thoroughly analyzed the heterostructures by synchrotron-based x-ray diffraction, transmission electron microscopy, and temperature-dependent electrical resistivity. Furthermore we conducted in-depth studies, including x-ray absorption and magneto-transport measurements. The knowledge gained thereby was used grow new, layered nickelate-cuprate hybrid structures with novel electronic and magnetic properties.
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    Monodisperse highly ordered and polydisperse biobased solid foams
    (2018) Andrieux, Sébastien; Stubenrauch, Cosima (Prof. Dr.)
    The aim of this work was the synthesis of monodisperse highly ordered biobased polymer foams and a comparison with their polydisperse counterparts. We used the biobased and biodegradable polymer chitosan, which we cross-linked with genipin. The polymer foams were synthesised via foam templating, i.e. via a liquid foam whose continuous phase contains a polymer and can be solidified. In order to obtain monodisperse highly ordered polymer foams, one first has to generate monodisperse highly ordered liquid foam templates. We did so by using microfluidics, which allows to produce monodisperse liquid foams with bubble sizes from 200 µm to 800 µm and polydispersities below 5%. The monodisperse foams were collected outside of the microfluidic channels and left to self-order under the influence of gravity and confinement. We studied the kinetics of the cross-linking reaction to find the optimal storage conditions during cross-linking. Once cross-linked we freeze-dried the gelled foams to obtain solid chitosan foams. We compared the morphological properties of the solid foams with those of the liquid templates in order to test the efficiency of the developed templating route. We observed how modifying the cross-linking and drying conditions can strongly affect the morphology of the solid foams. The main issue was to maintain the key properties of the liquid foam template throughout the solidification process, namely the bubble size distribution, the structural order and the density. We then compared the synthesised monodisperse polymer foams with their polydisperse counterparts. Although easy foaming methods exist for the generation of polydisperse foams, they do not allow the control over the polydispersity. We thus used microfluidics to generate liquid chitosan foams with tunable polydispersities from below 5% up to 26%. Microfluidics allows to match the average bubble size and density of the polydisperse liquid chitosan foam with those of the monodisperse counterpart. After solidifying the liquid templates we obtained solid foams with controlled polydispersities and studied the in uence of the polydispersity on the mechanical properties. However, we observed that not the polydispersity but the foam density was the main parameter at play. Moreover, the solid chitosan foams had weak mechanical properties with elastic moduli below 100 kPa. To overcome this issue, we incorporated cellulose nanofibres to the original chitosan solution and followed the developed route for foam templating. We had to adapt the microfluidic parameters to account for the viscosity changes brought about by the nanofibres. However, we managed to produce monodisperse liquid foams having the same bubble size, i.e. ~300 µm, but different amounts of cellulose nanofibres. The cellulose content had a strong influence on the solid foam morphology in general and on the pore connectivity in particular.