@phdthesis{Quast2017,
  author    = {Quast, Jan-Henrik},
  title     = {Influence of Hot Carriers on Spin Diffusion in Gallium Arsenide},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-147611},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2017},
  abstract  = {Since the late 20th century, spintroncis has become a very active field of research [ŽFS04]. The prospect of spin based information technology, featuring strongly decreased energy consumption and possibly quantum-computation capabilities, has fueled this interest. Standard materials, like bulk gallium arsenide (GaAs), have experienced new attention in this context by exhibiting extraordinarily long lifetimes for nonequilibrium spin information, which is an important requirement for efficient spin based information storage and transfer. Another important factor is the lengthscale over which spin information can be transported in a given material and the role of external influences. Both aspects have been studied experimentally with innovative optical methods since the late 1990s by the groups of D. D. AWSHALOM and S. A. CROOKER et al. [KA99, CS05, CFL+05]. Although the pioneering experimental approaches presented by these authors led to a variety of insights into spin propagation, some questions were raised as well. Most prominently, the classical Einstein relation, which connects the mobility and diffusivity of a given particle species, seemed to be violated for electron spins in a bulk semiconductor. In essence, nonequilibrium spins appeared to move (diffuse) faster than the electrons that actually carry the spin. However, this contradiction was masked by the fact, that the material of interest was n-type GaAs with a doping concentration directly at the transition between metallic and insulating behavior (MIT). In this regime, the electron mobility is difficult to determine experimentally. Consequently, it was not a priori obvious that the spin diffusion rates determined by the newly introduced optical methods were in contradiction with established electrical transport data. However, in an attempt to extend the available data of optical spin microscopy, another issue surfaced, concerning the mathematical drift-diffusion model that has been commonly used to evaluate lateral spin density measurements. Upon close investigation, this model appears to have a limited range of applicability, due to systematic discrepancies with the experimental data (chapter 4). These deviations are noticeable in original publications as well, and it is shown in the present work that they originate from the local heating of electrons in the process of optical spin pumping. Based on insights gained during the second half of the 20th century, it is recapitulated why conduction electrons are easily overheated at cryogenic temperatures. The main reason is the poor thermal coupling between electrons and the crystal lattice (chapter 3). Experiments in the present work showed that a significant thermal gradient exists in the conduction band under local optical excitation of electron-hole pairs. This information was used to develop a better mathematical model of spin diffusion, which allowed to derive the diffusivity of the undisturbed system, due to an effective consideration of electron overheating. In this way, spin diffusivities of n-GaAs were obtained as a function of temperature and doping density in the most interesting regime of the metal-insulator-transition. The experiments presented in this work were performed on a series of n-type bulk GaAs samples, which comprised the transition between metallic conductivity and electrical insulation at low temperatures. Local electron temperature gradients were measured by a hyperspectral photoluminescence imaging technique with subsequent evaluation of the electron-acceptor (e,A\$^0\$) line shape. The local density of nonequilibrium conduction electron spins was deduced from scanning magneto-optic Kerr effect microscopy. Numerical evaluations were performed using the finite elements method in combination with a least-squares fitting procedure. Chapter 1 provides an introduction to historical and recent research in the field of spintronics, as far as it is relevant for the understanding of the present work. Chapter 2 summarizes related physical concepts and experimental methods. Here, the main topics are semiconductor optics, relaxation of hot conduction electrons, and the dynamics of nonequilibrium electron spins in semiconductors. Chapter 3 discusses optical heating effects due to local laser excitation of electron-hole pairs. Experimental evaluations of the acceptor-bound-exciton triplet lines led to the conclusion that the crystal lattice is usually not overheated even at high excitation densities. Here, the heat is efficiently dissipated to the bath, due to the good thermal conductivity of the lattice. Furthermore, the heating of the lattice is inherently limited by the weak heat transfer from the electron system, which on the other hand is also the reason why conduction electrons are easily overheated at temperatures below ≈ 30 K. Spatio-spectral imaging of the electron-acceptor-luminescence line shape allowed to trace the thermal gradient within the conduction band under focused laser excitation. A heat-diffusion model was formulated, which reproduces the experimental electron-temperature trend nicely for low-doped GaAs samples of n- and p-type. For high-doped n-type GaAs samples, it could be shown that the lateral electron-temperature profile is well approximated by a Gaussian. This facilitated easy integration of hot electron influence into the mathematical model of spin diffusion. Chapter 4 deals with magneto-optical imaging of optically induced nonequilibrium conduction-electron spins in n-GaAs close to the MIT. First, the spectral dependence of the magneto-optic Kerr effect was examined in the vicinity of the fundamental band gap. Despite the marked differences among the investigated samples, the spectral shape of the Kerr rotation could be described in terms of a simple Lorentz-oscillator model in all cases. Based on this model, the linearity of the Kerr effect with respect to a nonequilibrium spin polarization is demonstrated, which is decisively important for further quantitative evaluations. Furthermore, chapter 4 presents an experimental survey of spin relaxation in n-GaAs at the MIT. Here, the dependence of the spin relaxation time on bath temperature and doping density was deduced from Hanle-MOKE measurements. While all observed trends agree with established literature, the presented results extend the current portfolio by adding a coherent set of data. Finally, diffusion of optically generated nonequilibrium conduction-electron spins was investigated by scanning MOKE microscopy. First, it is demonstrated that the standard diffusion model is inapplicable for data evaluation in certain situations. A systematic survey of the residual deviations between this model and the experimental data revealed that this situation unfortunately persisted in published works. Moreover, the temperature trend of the residual deviations suggests a close connection to the local overheating of conduction electrons. Consequently, a modified diffusion model was developed and evaluated, in order to compensate for the optical heating effect. From this model, much more reliable results were obtained, as compared to the standard diffusion model. Therefore, it was shown conclusively that the commonly reported anomalously large spin diffusivities were at least in parts caused by overheated conduction electrons. In addition to these new insights some experimental and technological enhancements were realized in the course of this work. First, the optical resolution of scanning MOKE microscopy was improved by implementing a novel scanning mechanism, which allows the application of a larger aperture objective than in the usual scheme. Secondly, imaging photoluminescence spectroscopy was employed for spatially resolved electron-temperature measurements. Here, two different implementations were developed: One for lattice-temperature measurements by acceptor-bound exciton luminescence and a second for conduction-electron temperature measurements via the analysis of the electron-acceptor luminescence line shape. It is shown in the present work that the originally stated anomalously high spin diffusivities were caused to a large extent by unwanted optical heating of the electron system. Although an efficient method was found to compensate for the influence of electron heating, it became also evident that the classical Einstein relation was nonetheless violated under the given experimental conditions. In this case however, it could be shown that this discrepancy did not originate from an experimental artifact, but was instead a manifestation of the fermionic nature of conduction electrons.},
  subject      = {Galliumarsenid},
  language  = {en}
}
@unpublished{ArrowsmithBoehnkeBraunschweigetal.2017,
  author    = {Arrowsmith, Merle and B{\"o}hnke, Julian and Braunschweig, Holger and Deißenberger, Andrea and Dewhurst, Rian and Ewing, William and H{\"o}rl, Christian and Mies, Jan and Muessig, Jonas},
  title     = {Simple Solution-Phase Syntheses of Tetrahalodiboranes(4) and their Labile Dimethylsulfide Adducts},
  series = {Chemical Communications},
  volume    = {53},
  journal   = {Chemical Communications},
  doi       = {10.1039/C7CC03148C},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-149438},
  pages     = {8265-8267},
  year      = {2017},
  abstract  = {Convenient, solution-phase syntheses of tetrahalodiboranes(4) B\(_2\)F\(_4\), B\(_2\)Cl\(_4\) and B\(_2\)I\(_4\) are presented herein from common precursor B\(_2\)Br\(_4\). In addition, the dimethylsulfide adducts B\(_2\)Cl\(_4\)(SMe\(_2\))\(_2\) and B\(_2\)Br\(_4\)(SMe\(_2\))\(_2\) are conveniently prepared in one-step syntheses from the commercially-available starting material B\(_2\)(NMe\(_2\))\(_4\). The results provide simple access to the full range of tetrahalodiboranes(4) for the exploration of their untapped synthetic potential.},
  language  = {en}
}
@phdthesis{RietzlergebMathies2017,
  author    = {Rietzler [geb. Mathies], Antonia Theresa},
  title     = {Modulation des Arbeitsged{\"a}chtnisses durch transkranielle Gleichstromstimulation - eine Untersuchung mittels funktioneller Nah-Infrarot-Spektroskopie},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-151948},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2017},
  abstract  = {Die Transkranielle Gleichstromstimulation (tDCS) stellt ein Verfahren zur nicht-invasiven und schmerzfreien Stimulation des Gehirns dar. Ziel dabei ist es die kortikale Erregbarkeit zu modulieren, indem das Ruhemembranpotenzial der Nervenzellen verschoben wird. Anodale tDCS f{\"u}hrt dabei zu einer Depolarisierung des Membranpotenzials und somit zur Zunahme der neuronalen Aktivit{\"a}t. Kathodale tDCS hat durch die Hyperpolarisierung des Membranpotenzials eine Abnahme der neuronalen Aktivit{\"a}t zur Folge. Durch den exzitatorischen Effekt nach anodaler Stimulation und den inhibitorischen Effekt nach kathodaler Stimulation stellt die tDCS eine vielversprechende Option in der Therapie neurologischer oder neuropsychiatrischer Erkrankungen dar. In vorliegender Studie sollten die Auswirkungen der transkraniellen Gleichstromstimulation {\"u}ber dem linken dorsolateralen pr{\"a}frontalen Kortex (DLPFC) auf Arbeitsged{\"a}chtnisprozesse untersucht werden. Die Effekte der tDCS wurden an 56 gesunden Versuchspersonen getestet, die randomisiert drei Stimulationsgruppen zugeordnet wurden (anodale, kathodale und Sham-Stimulation). Stimuliert wurde mit 2 mA bei einer Elektrodengr{\"o}ße von 35 cm². Stimulationsort war dabei der linke DLPFC, die Referenzelektrode wurde {\"u}ber dem linken Mastoid platziert. W{\"a}hrend der Stimulation f{\"u}hrten die Versuchspersonen eine modifizierte N-Back-Aufgabe mit drei Bedingungen (0-Back, 1-Back und 2-Back) aus, um die Funktion des Arbeitsged{\"a}chtnisses hinsichtlich des Verhaltens erfassen zu k{\"o}nnen. Die Auswirkungen der tDCS auf die neuronale Aktivit{\"a}t wurden mittels funktioneller Nah-Infrarot-Spektroskopie (fNIRS) gemessen. Auf neuronaler Ebene erwarteten wir eine Zunahme der kortikalen Aktivit{\"a}t nach anodaler Stimulation innerhalb des linken DLPFC und gegenteilige Effekte nach kathodaler Stimulation. In vorliegender Untersuchung konnte lediglich eine Tendenz zu dieser Annahme beobachtet werden, eindeutige Signifikanzen blieben jedoch aus. Bei Betrachtung verschiedener Regions of Interest (ROIs) konnten nur signifikante Unterschiede zwischen der anodal und der kathodal stimulierten Gruppe nachgewiesen werden, was daf{\"u}r spricht, dass die Auswirkungen der tDCS zwar in die intendierte Richtung gehen, die Effekte aber nicht stark genug sind, um auch signifikante Unterschiede zur Kontrollgruppe nachweisen zu k{\"o}nnen. Somit m{\"u}ssen wir davon ausgehen, dass sich die Neurone des DLPFC nur schwach durch die transkranielle Stimulation beeinflussen lassen. Desweiteren wurden die Verhaltensdaten w{\"a}hrend der N-Back-Aufgabe untersucht. Angenommen wurde eine Verbesserung der Arbeitsged{\"a}chtnisleistung durch anodale Stimulation und eine Verschlechterung durch kathodale Stimulation. Hier zeigte sich allerdings, dass sich unsere drei Stimulationsgruppen weder in der Anzahl der Fehler, noch in der Anzahl der richtigen Antworten, der Anzahl der verpassten Antworten oder in der mittleren Reaktionszeit signifikant voneinander unterscheiden. Dies l{\"a}sst darauf schließen, dass die Stimulation des linken DLPFC keinen Einfluss auf das Verhalten w{\"a}hrend der Durchf{\"u}hrung der Arbeitsged{\"a}chtnisaufgabe hat und somit auch die Arbeitsged{\"a}chtnisleistung nicht beeinflusst wird. Obwohl die Ergebnisse unserer Studie durch fehlende Signifikanzen nicht hypothesenkonform sind, konnten wir zusammenfassend dennoch eine Tendenz zur anodal-exzitatorischen und kathodal-inhibitorischen Wirkung der tDCS beobachten. Die weitere Erforschung der Auswirkungen der tDCS auf das Arbeitsged{\"a}chtnis scheint also sehr vern{\"u}nftig, vor allem in Anbetracht der m{\"o}glichen Etablierung der tDCS als Therapieoption neuropsychiatrischer Erkrankungen. Weiterf{\"u}hrende Studien sollten die Wirksamkeit der tDCS weiter untersuchen und eine Optimierung der tDCS-induzierten Effekte {\"u}berpr{\"u}fen. Ansatzpunkte hierf{\"u}r w{\"a}ren beispielsweise die Durchf{\"u}hrung umfangreicherer Studien mit einem gr{\"o}ßeren Probandenkollektiv und ver{\"a}nderten Stimulationsparametern oder Studien, die die Auswirkungen der tDCS auf das Arbeitsged{\"a}chtnis auch bei psychiatrischen Patienten untersuchen.},
  subject      = {Arbeitsged{\"a}chtnis},
  language  = {de}
}
@phdthesis{Weirauch2017,
  author    = {Weirauch, Katja},
  title     = {Neue Herausforderungen an die professionellen Kompetenzen von Chemie-Lehrkr{\"a}ften durch die Implementation von Seminarf{\"a}chern},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-151330},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2017},
  abstract  = {Neuerungen in Bildungssystemen k{\"o}nnen nur erfolgreich sein, wenn sie planm{\"a}ßig implementiert werden. Maßgeblich ist hierf{\"u}r, dass die Lehrkr{\"a}fte {\"u}ber die entsprechenden professionellen Kompetenzen verf{\"u}gen. Die vorliegende Arbeit untersucht diesen Zusammenhang am Beispiel der Implementation von Seminarf{\"a}chern im bayerischem Gymnasium. Es wird identifiziert, welche neuen Herausforderungen Chemie-Lehrkr{\"a}fte mit Einf{\"u}hrung der Wissenschaftsprop{\"a}deutischen (W-) und Projekt-Seminare (P-) bew{\"a}ltigen m{\"u}ssen. Aus Interviews mit Lehrkr{\"a}ften wurden per qualitativer Inhaltsanalyse nach Mayring die Anforderungen an das Professionswissen der Lehrkr{\"a}fte identifiziert. F{\"u}r die W-Seminare konnte dargestellt werden, dass eine erfolgreiche Wissenschaftsprop{\"a}deutik h{\"a}ufig an fehlendem Fachwissen der Lehrkr{\"a}fte zu Nature of Science Inquiry (NOSI) scheiterte. Analog fehlte den Lehrkr{\"a}ften in den P-Seminaren Fachwissen zu Projektmanagement, sodass sie dies weder umsetzten, noch erfolgreich vermitteln konnten. Um die Lehrkr{\"a}fte bei der Bew{\"a}ltigung der Herausforderungen zu unterst{\"u}tzen, wurden vielf{\"a}ltige M{\"o}glichkeiten der Kooperation von Seminarf{\"a}chern mit der Universit{\"a}t als externem Partner erprobt. Methodenwerkzeuge f{\"u}r eine systematische Wissenschaftsprop{\"a}deutik wurden entwickelt und im Rahmen von Lehrerfortbildungen weitergegeben. Weiterhin wurde ein Lehr-Lern-Labor „Analyseverfahren der Chemie" f{\"u}r W-Seminare konzipiert und wiederholt erfolgreich durchgef{\"u}hrt. Damit wurden Erkenntnisse der empirischen Studie in nachweislich praxistaugliche Konzepte umgesetzt, die die erfolgreiche Implementation der Seminarf{\"a}cher unterst{\"u}tzen k{\"o}nnen.},
  subject      = {Seminarfach},
  language  = {de}
}
@phdthesis{Wetter2017,
  author    = {Wetter, Christin},
  title     = {Das Erkennen des drohenden H{\"o}rverlustes nach Vestibularisschwannom-Operation},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-151569},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2017},
  abstract  = {Die Ableitung Akustisch evozierter Potentiale (AEP) durch intraoperatives Monitoring wird regelhaft bei der Operation von Vestibularisschwannomen mit dem Ziel des H{\"o}rerhaltes durchgef{\"u}hrt. Trotz AEP-Erhalt am Ende der Operation wurden F{\"a}lle mit postoperativer Taubheit beobachtet. Bisher ist es unklar, ob es sich um falsch positive AEP-Befunde oder F{\"a}lle von sekund{\"a}rer Taubheit handelt. Diese Pilotstudie, bei der zu definierten Zeitpunkten postoperativ AEP-Messungen durchgef{\"u}hrt wurden, zeigt erhebliche Ver{\"a}nderungen der AEP-Befunde im postoperativen Verlauf. Es fanden sich Patienten mit verbesserten AEP-Befunden, aber auch verschlechterten AEP bis zum vollst{\"a}ndigen Verlust aller AEP-Komponenten. Ob ein sekund{\"a}rer H{\"o}rverlust durch fr{\"u}hzeitiges Erkennen von AEP-Ver{\"a}nderungen verhindert werden kann, wird Inhalt von weiteren Studien sein.},
  subject      = {Kleinhirnbr{\"u}ckenwinkeltumor},
  language  = {de}
}
@phdthesis{Roeder2017,
  author    = {R{\"o}der, Anja M.},
  title     = {Excited-State Dynamics in Open-Shell Molecules},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-151738},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2017},
  abstract  = {In this thesis the excited-state dynamics of radicals and biradicals were characterized with femtosecond pump-probe spectroscopy. These open-shell molecules play important roles as combustion intermediates, in the formation of soot and polycyclic aromatic hydrocarbons, in atmospheric chemistry and in the formation of complex molecules in the interstellar medium and galactic clouds. In these processes molecules frequently occur in some excited state, excited either by thermal energy or radiation. Knowledge of the reactivity and dynamics of these excited states completes our understanding of these complex processes. These highly reactive molecules were produced via pyrolysis from suitable precursors and examined in a molecular beam under collision-free conditions. A first laser now excites the molecule, and a second laser ionizes it. Time-of-flight mass spectrometry allowed a first identification of the molecule, photoelectron spectroscopy a complete characterization of the molecule - under the condition that the mass spectrum was dominated by only one mass. The photoelectron spectrum was obtained via velocity-map imaging, providing an insight in the electronic states involved. Ion velocity map imaging allowed separation of signal from direct ionization of the radical in the molecular beam and dissociative photoionization of the precursor. During this thesis a modified pBasex algorithm was developed and implemented in python, providing an image inversion tool without interpolation of data points. Especially for noisy photoelectron images this new algorithm delivers better results. Some highlighted results: • The 2-methylallyl radical was excited in the ππ*-state with different internal energies using three different pump wavelengths (240.6 , 238.0 and 236.0 nm). Ionized with 800 nm multi-photon probe, the photoelectron spectra shows a s-Rydberg fingerprint spectrum, a highly positive photoelectron anisotropy of 1.5 and a bi-exponential decay ( τ1= 141\pm43 fs, τ2= 4.0\pm0.2 ps for 240.6 nm pump), where the second time-constant shortens for lower wavelengths. Field-induced surface hopping dynamics calculations confirm that the initially excited ππ*-state relaxes very fast to an s-Rydberg state (first experimentally observed time-constant), and then more slowly to the first excited state/ground state (second time-constant). With higher excitation energies the conical intersection between the s-Rydberg-state and the first excited state is reached faster, resulting in shorter life-times. • The benzyl radical was excited yith 265 nm and probed with two wavelengths, 798 nm and 398 nm. Probed with 798 nm it shows a bi-exponential decay (\tau_{1}=84\pm5 fs, \tau_{2}=1.55\pm0.12 ps), whereas with 398 nm probe only the first time-constant is observed (\tau_{1}=89\pm5 fs). The photoelectron spectra with 798 nm probe is comparable to the spectrum with 398 nm probe during the first 60 fs, at longer times an additional band appears. This band is due to a [1+3']-process, whereas with 398 nm only signal from a [1+1']-process can be observed. Non-adiabatic dynamic on the fly calculations show that the initially excited, nearly degenerate ππ/p-Rydberg-states relax very fast (first time-constant) to an s-Rydberg state. This s-Rydberg state can no longer be ionized with 398 nm, but with 798 nm ionization via intermediate resonances is still possible. The s-Rydberg state then decays to the first excited state (second time-constant), which is long-lived. • Para-xylylene, excited with 266 nm into the S2-state and probed with 800 nm, shows a bi-exponential decay (\tau_{1}=38\pm7 fs, \tau_{2}=407\pm9 fs). The initially excited S2-state decays quickly to S1-state, which shows dissociative photoionization. The population of the S1-state is directly visible in the masses of the dissociative photoionization products, benzene and the para-xylylene -H. • Ortho-benzyne, produced via pyrolysis from benzocyclobutendione, was excited with 266 nm in the S2 state and probed with 800 nm. In its time-resolved mass spectra the dynamic of the ortho-benzyne signal was superposed with the dynamics from dissociative photoionization of the precursor and of the ortho-benzyne-dimer. With time-resolved ion imaging gated on the ortho-benzyne these processes could be seperated, showing that the S2-state of ortho-benzyne relaxes within 50 fs to the S1-state.},
  subject      = {Radikal <Chemie>},
  language  = {en}
}
@phdthesis{Gabor2017,
  author    = {Gabor, Sabine},
  title     = {Pr{\"a}klinische Evaluation von Aldosteronsynthaseinhibitoren als PET-Tracer f{\"u}r die Differentialdiagnostik des prim{\"a}ren Hyperaldosteronismus mit besonderem Fokus auf Cyanofluorphenylpyridinen und deren Derivate},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-137096},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2017},
  abstract  = {Zusammenfassend l{\"a}sst sich festhalten, dass in dieser Arbeit 15 neu entwickelte Substanzen zur selektiven und hochaffinen Blockade der Aldosteronsynthase untersucht werden konnten. Es wurden mehrere neue aufeinander aufbauende Testsysteme etabliert, um die neuen Substanzen auf ihre Selektivit{\"a}t und Affinit{\"a}t gegen{\"u}ber der Aldosteronsynthase zu untersuchen. Eine Testung der Inhibition der humanen Aldosteronsynthase und der 11β-Hydroxylase zuerst in getrennten Zellkulturans{\"a}tzen, die die humanen Enzyme stabil exprimieren, und anschließend in der NCI-h295 Zelllinie, die beide Enzyme und zus{\"a}tzlich die meisten anderen Enzyme der Steroidbiosynthese stabil exprimieren, ist eine gute Voraussetzung, um selektive und hochaffine Aldosteronsynthaseinhibitoren zu finden. Hier konnten sechs Inhibitoren ausgew{\"a}hlt werden, die hochaffin und selektiv an die Aldosteronsynthase binden und diese inhibieren. Die weitere Testung der [18F] markierten Substanzen zeigte f{\"u}r eine Substanz eine hochaffine und selektive Bindung an humanes adrenales Gewebe und keine unspezifische Bindung an andere humane Gewebe. Hier liegt die Voraussetzung vor, den Tracer weiteren in vivo Studien zuzuf{\"u}hren, um am humanisierten Mausmodell zu untersuchen, ob eine Bindung in vivo entsprechend den vielversprechenden Ergebnissen in vitro abl{\"a}uft. Auch die ex vivo Studie an Nebennieren einer gegen{\"u}ber der CYP11B2 humanisierten Maus bekr{\"a}ftigte diese Ergebnisse. Mit Hilfe dieser Untersuchungsmethoden lassen sich in Zukunft noch weiter entwickelte Substanzen umfangreich auf ihre Selektivit{\"a}t, Spezifit{\"a}t und Affinit{\"a}t testen. Dies dient als Grundlage f{\"u}r weitere Untersuchungen zur Entwicklung eines PET-Tracers f{\"u}r die Differentialdiagnostik bei prim{\"a}rem Hyperaldosteronismus. Eine Erkrankung, die h{\"a}ufiger ist als vermutet, und bei der die Differentialdiagnostik die entscheidende Voraussetzung f{\"u}r die Einleitung einer Therapie ist, die sich entweder operativ oder medikament{\"o}s darstellt. Bisherige differentialdiagnostische Vorgehensweisen beim prim{\"a}ren Hyperaldosteronismus bieten aktuell keine zufriedenstellenden Ergebnisse; dies kann sich mit der Einf{\"u}hrung eines neuen PET Tracers {\"a}ndern.},
  subject      = {Aldosteronsynthaseinhibitor},
  language  = {de}
}
@phdthesis{Rueth2017,
  author    = {R{\"u}th, Sebastian},
  title     = {Monetary Policy, Housing Market Dynamics, and the Propagation of Shocks},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-137221},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2017},
  abstract  = {This dissertation studies the interrelations between housing markets and monetary policy from three different perspectives. First, it identifies housing finance specific shocks and analyzes their impact on the broader economy and, most importantly, the systematic monetary policy reaction to such mortgage sector disturbances. Second, it investigates the implications of the institutional arrangement of a currency union for the potential buildup of a housing bubble in a member country of the monetary union by, inter alia, fostering border-crossing capital flows and ultimately residential investment activity. This dissertation, third, quantifies the effects of autonomous monetary policy shifts on the macroeconomy and, in particular, on housing markets by conditioning on financial sector conditions. From a methodological perspective, the dissertation draws on time-series econometrics like vector autoregressions (VARs) or local projections models.},
  subject      = {Geldpolitik},
  language  = {en}
}
@phdthesis{Juergens2017,
  author    = {J{\"u}rgens, Stefan},
  title     = {Correlated Topological Materials},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-152202},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2017},
  abstract  = {The topic of this PhD thesis is the combination of topologically non-trivial phases with correlation effects stemming from Coulomb interaction between the electrons in a condensed matter system. Emphasis is put on both emerging benefits as well as hindrances, e.g. concerning the topological protection in the presence of strong interactions. The physics related to topological effects is established in Sec. 2. Based on the topological band theory, we introduce topological materials including Chern insulators, topological insulators in two and three dimensions as well as Weyl semimetals. Formalisms for a controlled treatment of Coulomb correlations are presented in Sec. 3, starting with the topological field theory. The Random Phase Approximation is introduced as a perturbative approach, while in the strongly interacting limit the theory of quantum Hall ferromagnetism applies. Interactions in one dimension are special, and are treated through the Luttinger liquid description. The section ends with an overview of the expected benefits offered by the combination of topology and interactions, see Sec. 3.3. These ideas are then elaborated in the research part. In Chap. II, we consider weakly interacting 2D topological insulators, described by the Bernevig-Hughes-Zhang model. This is applicable, e.g., to quantum well structures made of HgTe/CdTe or InAs/GaSb. The bulk band structure is here a mixture stemming from linear Dirac and quadratic Schr{\"o}dinger fermions. We study the low-energy excitations in Random Phase Approximation, where a new interband plasmon emerges due to the combined Dirac and Schr{\"o}dinger physics, which is absent in the separate limits. Already present in the undoped limit, one finds it also at finite doping, where it competes with the usual intraband plasmon. The broken particle-hole symmetry in HgTe quantum wells allows for an effective separation of the two in the excitation spectrum for experimentally accessible parameters, in the right range for Raman or electron loss spectroscopy. The interacting bulk excitation spectrum shows here clear differences between the topologically trivial and topologically non-trivial regime. An even stronger signal in experiments is expected from the optical conductivity of the system. It thus offers a quantitative way to identify the topological phase of 2D topological insulators from a bulk measurement. In Chap. III, we study a strongly interacting system, forming an ordered, quantum Hall ferromagnetic state. The latter can arise also in weakly interacting materials with an applied strong magnetic field. Here, electrons form flat Landau levels, quenching the kinetic energy such that Coulomb interaction can be dominant. These systems define the class of quantum Hall topological insulators: topologically non-trivial states at finite magnetic field, where the counter-propagating edge states are protected by a symmetry (spatial or spin) other than time-reversal. Possible material realizations are 2D topological insulators like HgTe heterostructures and graphene. In our analysis, we focus on the vicinity of the topological phase transition, where the system is in a strongly interacting quantum Hall ferromagnetic state. The bulk and edge physics can be described by a nonlinear \sigma-model for the collective order parameter of the ordered state. We find that an emerging, continuous U(1) symmetry offers topological protection. If this U(1) symmetry is preserved, the topologically non-trivial phase persists in the presence of interactions, and we find a helical Luttinger liquid at the edge. The latter is highly tunable by the magnetic field, where the effective interaction strength varies from weakly interacting at zero field, K \approx 1, to diverging interaction strength at the phase transition, K -> 0. In the last Chap. IV, we investigate whether a Weyl semimetal and a 3D topological insulator phase can exist together at the same time, with a combined, hybrid surface state at the joint boundaries. An overlap between the two can be realized by Coulomb interaction or a spatial band overlap of the two systems. A tunnel coupling approach allows us to derive the hybrid surface state Hamiltonian analytically, enabling a detailed study of its dispersion relation. For spin-symmetric coupling, new Dirac nodes emerge out of the combination of a single Dirac node and a Fermi arc. Breaking the spin symmetry through the coupling, the dispersion relation is gapped and the former Dirac node gets spin-polarized. We propose experimental realizations of the hybrid physics, including compressively strained HgTe as well as heterostructures of topological insulator and Weyl semimetal materials, connected to each other, e.g., by Coulomb interaction.},
  subject      = {Topologie},
  language  = {en}
}
@phdthesis{Carinci2017,
  author    = {Carinci, Flavio},
  title     = {Quantitative Characterization of Lung Tissue Using Proton MRI},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-151189},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2017},
  abstract  = {The focus of the work concerned the development of a series of MRI techniques that were specifically designed and optimized to obtain quantitative and spatially resolved information about characteristic parameters of the lung. Three image acquisition techniques were developed. Each of them allows to quantify a different parameter of relevant diagnostic interest for the lung, as further described below: 1) The blood volume fraction, which represents the amount of lung water in the intravascular compartment expressed as a fraction of the total lung water. This parameter is related to lung perfusion. 2) The magnetization relaxation time T\(_2\) und T� *\(_2\) , which represents the component of T\(_2\) associated with the diffusion of water molecules through the internal magnetic field gradients of the lung. Because the amplitude of these internal gradients is related to the alveolar size, T\(_2\) und T� *\(_2\) can be used to obtain information about the microstructure of the lung. 3) The broadening of the NMR spectral line of the lung. This parameter depends on lung inflation and on the concentration of oxygen in the alveoli. For this reason, the spectral line broadening can be regarded as a fingerprint for lung inflation; furthermore, in combination with oxygen enhancement, it provides a measure for lung ventilation.},
  subject      = {Kernspintomografie},
  language  = {en}
}