From discrete anions to extended solids: new uranium thiophosphates

Die wichtigste Klasse zeotyper Verbindungen sind die Thio- und Selenophosphate der Übergangsmetalle. Ziel dieser Dissertation war die Darstellung und Charakterisierung neuer Uranthiophosphate. Die dargestellten Verbindungen enthalten vierwertige Urankationen, die von acht Schwefelatomen koordiniert sind. Da die enthaltenen Thiophosphatanionen in den meisten Fällen als zweizähnige Liganden fungieren, entstehen dreidimensionale Netzwerke mit pseudotetraedrisch koordinierten Metallzentren. In der Verbindung U(P2S6)2 durchdringen sich drei identische diamantartige Netzwerke, wodurch optimale Raumerfüllung erreicht wird. Die Einführung von Alkalimetallkationen in das System führt zu einer Vielzahl neuer Verbindungen, deren Eigenschaften durch die Stöchiometrie der Edukte und durch die Kationenradien bestimmt werden. Beispielsweise enthält die Kristallstruktur von Na2U(PS4)2 zweidimensionale anionische [U(PS4)2]n-Schichten, während die analoge Verbindung CsLiU(PS4)2 eine poröse dreidimensionale Netzwerkstruktur besitzt. Der Vergleich der untersuchten quaternären und quinären Verbindungen zeigt, dass eine Korrelation zwischen dem Kationenradius und dem Durchmesser der Poren besteht. Dies lässt auf eine Templatfunktion der Alkalimetallkationen beim Aufbau der anionischen Teilstruktur schließen. Die neuen Verbindungen wurden aus reaktiven Polysulfidschmelzflüssen oder durch Auflösen amorpher Vorläufer in Alkalimetallchloridschmelzen synthetisiert. Die Kristallstrukturen wurden durch Einkristall-Röntgenmethoden bestimmt. Ein Vergleich der magnetischen Eigenschaften der Verbindungen beweist, dass in allen untersuchten Fällen U(IV) vorliegt. Die Substanzen zeigen paramagnetisches Verhalten, in UP2S7 und CsLiU(PS4)2 sind außerdem antiferromagnetische Wechselwirkungen zwischen benachbarten Uranatomen nachweisbar.

Automatisierte Flüssigchromatographie mit Säulenschaltung und Ultraviolettspektroskopie oder Massenspektrometrie für therapeutisches Drug Monitoring von Antipsychotika und Antidepressiva

Therapeutisches Drug Monitoring (TDM) wird zur individuellen Dosiseinstellung genutzt, um die Effizienz der Medikamentenwirkung zu steigern und das Auftreten von Nebenwirkungen zu senken. Für das TDM von Antipsychotika und Antidepressiva besteht allerdings das Problem, dass es mehr als 50 Medikamente gibt. Ein TDM-Labor muss dementsprechend über 50 verschiedene Wirkstoffe und zusätzlich aktive Metaboliten messen. Mit der Flüssigchromatographie (LC oder HPLC) ist die Analyse vieler unterschiedlicher Medikamente möglich. LC mit Säulenschaltung erlaubt eine Automatisierung. Dabei wird Blutserum oder -plasma mit oder ohne vorherige Proteinfällung auf eine Vorsäule aufgetragen. Nach Auswaschen von störenden Matrixbestandteilen werden die Medikamente auf einer nachgeschalteten analytischen Säule getrennt und über Ultraviolettspektroskopie (UV) oder Massenspektrometrie (MS) detektiert. Ziel dieser Arbeit war es, LC-Methoden zu entwickeln, die die Messung möglichst vieler Antipsychotika und Antidepressiva erlaubt und die für die TDM-Routine geeignet ist. Eine mit C8-modifiziertem Kieselgel gefüllte Säule (20 µm 10x4.0 mm I.D.) erwies sich in Vorexperimenten als optimal geeignet bezüglich Extraktionsverhalten, Regenerierbarkeit und Stabilität. Mit einer ersten HPLC-UV-Methode mit Säulenschaltung konnten 20 verschiedene Psychopharmaka einschließlich ihrer Metabolite, also insgesamt 30 verschiedene Substanzen quantitativ erfasst werden. Die Analysenzeit betrug 30 Minuten. Die Vorsäule erlaubte 150 Injektionen, die analytische Säule konnte mit mehr als 300 Plasmainjektionen belastet werden. Abhängig vom Analyten, musste allerdings das Injektionsvolumen, die Flussrate oder die Detektionswellenlänge verändert werden. Die Methode war daher für eine Routineanwendung nur eingeschränkt geeignet. Mit einer zweiten HPLC-UV-Methode konnten 43 verschiedene Antipsychotika und Antidepressiva inklusive Metaboliten nachgewiesen werden. Nach Vorreinigung über C8-Material (10 µm, 10x4 mm I.D.) erfolgte die Trennung auf Hypersil ODS (5 µm Partikelgröße) in der analytischen Säule (250x4.6 mm I.D.) mit 37.5% Acetonitril im analytischen Eluenten. Die optimale Flussrate war 1.5 ml/min und die Detektionswellenlänge 254 nm. In einer Einzelprobe, konnten mit dieser Methode 7 bis 8 unterschiedliche Substanzen gemessen werden. Für die Antipsychotika Clozapin, Olanzapin, Perazin, Quetiapin und Ziprasidon wurde die Methode validiert. Der Variationskoeffizient (VK%) für die Impräzision lag zwischen 0.2 und 6.1%. Im erforderlichen Messbereich war die Methode linear (Korrelationskoeffizienten, R2 zwischen 0.9765 und 0.9816). Die absolute und analytische Wiederfindung lagen zwischen 98 und 118 %. Die für das TDM erforderlichen unteren Nachweisgrenzen wurden erreicht. Für Olanzapin betrug sie 5 ng/ml. Die Methode wurde an Patienten für das TDM getestet. Sie erwies sich für das TDM als sehr gut geeignet. Nach retrospektiver Auswertung von Patientendaten konnte erstmalig ein möglicher therapeutischer Bereich für Quetiapin (40-170 ng/ml) und Ziprasidon (40-130 ng/ml) formuliert werden. Mit einem Massenspektrometer als Detektor war die Messung von acht Neuroleptika und ihren Metaboliten möglich. 12 Substanzen konnten in einem Lauf bestimmt werden: Amisulprid, Clozapin, N-Desmethylclozapin, Clozapin-N-oxid, Haloperidol, Risperidon, 9-Hydroxyrisperidon, Olanzapin, Perazin, N-Desmethylperazin, Quetiapin und Ziprasidon. Nach Vorreinigung mit C8-Material (20 µm 10x4.0 mm I.D.) erfolgte die Trennung auf Synergi MAX-RP C12 (4 µm 150 x 4.6 mm). Die Validierung der HPLC-MS-Methode belegten einen linearen Zusammenhang zwischen Konzentration und Detektorsignal (R2= 0,9974 bis 0.9999). Die Impräzision lag zwischen 0.84 bis 9.78%. Die für das TDM erforderlichen unteren Nachweisgrenzen wurden erreicht. Es gab keine Hinweise auf das Auftreten von Ion Suppression durch Matrixbestandteile. Die absolute und analytische Wiederfindung lag zwischen 89 und 107 %. Es zeigte sich, dass die HPLC-MS-Methode ohne Modifikation erweitert werden kann und anscheinend mehr als 30 verschiedene Psychopharmaka erfasst werden können. Mit den entwickelten flüssigchromatographischen Methoden stehen neue Verfahren für das TDM von Antipsychotika und Antidepressiva zur Verfügung, die es erlauben, mit einer Methode verschiedene Psychopharmaka und ihre aktiven Metabolite zu messen. Damit kann die Behandlung psychiatrischer Patienten insbesondere mit Antipsychotika verbessert werden.

The collapse of linear polyelectrolyte chains in a poor solvent: When does a collapsing polyelectrolyte collect its counter ions?

The collapse of linear polyelectrolyte chains in a poor solvent: When does a collapsing polyelectrolyte collect its counter ions? The collapse of polyions in a poor solvent is a complex system and is an active research subject in the theoretical polyelectrolyte community. The complexity is due to the subtle interplay between hydrophobic effects, electrostatic interactions, entropy elasticity, intrinsic excluded volume as well as specific counter-ion and co-ion properties. Long range Coulomb forces can obscure single molecule properties. The here presented approach is to use just a small amount of screening salt in combination with a very high sample dilution in order to screen intermolecular interaction whereas keeping intramolecular interaction as much as possible (polyelectrolyte concentration cp ≤ 12 mg/L, salt concentration; Cs = 10^-5 mol/L). This is so far not described in literature. During collapse, the polyion is subject to a drastic change in size along with strong reduction of free counterions in solution. Therefore light scattering was utilized to obtain the size of the polyion whereas a conductivity setup was developed to monitor the proceeding of counterion collection by the polyion. Partially quaternized PVP’s below and above the Manning limit were investigated and compared to the collapse of their uncharged precursor. The collapses were induced by an isorefractive solvent/non-solvent mixture consisting of 1-propanol and 2-pentanone, with nearly constant dielectric constant. The solvent quality for the uncharged polyion could be quantified which, for the first time, allowed the experimental investigation of the effect of electrostatic interaction prior and during polyion collapse. Given that the Manning parameter M for QPVP4.3 is as low as lB / c = 0.6 (lB the Bjerrum length and c the mean contour distance between two charges), no counterion binding should occur. However the Walden product reduces with first addition of non solvent and accelerates when the structural collapse sets in. Since the dielectric constant of the solvent remains virtually constant during the chain collapse, the counterion binding is entirely caused by the reduction in the polyion chain dimension. The collapse is shifted to lower wns with higher degrees of quaternization as the samples QPVP20 and QPVP35 show (M = 2.8 respectively 4.9). The combination of light scattering and conductivity measurement revealed for the first time that polyion chains already collect their counter ions well above the theta-dimension when the dimensions start to shrink. Due to only small amounts of screening salt, strong electrostatic interactions bias dynamic as well as static light scattering measurements. An extended Zimm formula was derived to account for this interaction and to obtain the real chain dimensions. The effective degree of dissociation g could be obtained semi quantitatively using this extrapolated static in combination with conductivity measurements. One can conclude the expansion factor a and the effective degree of ionization of the polyion to be mutually dependent. In the good solvent regime g of QPVP4.3, QPVP20 and QPVP35 exhibited a decreasing value in the order 1 > g4.3 > g20 > g35. The low values of g for QPVP20 and QPVP35 are assumed to be responsible for the prior collapse of the higher quaternized samples. Collapse theory predicts dipole-dipole attraction to increase accordingly and even predicts a collapse in the good solvent regime. This could be exactly observed for the QPVP35 sample. The experimental results were compared to a newly developed theory of uniform spherical collapse induced by concomitant counterion binding developed by M. Muthukumar and A. Kundagrami. The theory agrees qualitatively with the location of the phase boundary as well as the trend of an increasing expansion with an increase of the degree of quaternization. However experimental determined g for the samples QPVP4.3, QPVP20 and QPVP35 decreases linearly with the degree of quaternization whereas this theory predicts an almost constant value.

Feasibility studies of the pp pi 0 e + e - electromagnetic channel at PANDA

Among all possible realizations of quark and antiquark assembly, the nucleon (the proton and the neutron) is the most stable of all hadrons and consequently has been the subject of intensive studies. Mass, shape, radius and more complex representations of its internal structure are measured since several decades using different probes. The proton (spin 1/2) is described by the electric GE and magnetic GM form factors which characterise its internal structure. The simplest way to measure the proton form factors consists in measuring the angular distribution of the electron-proton elastic scattering accessing the so-called Space-Like region where q2 < 0. Using the crossed channel antiproton proton <--> e+e-, one accesses another kinematical region, the so-called Time-Like region where q2 > 0. However, due to the antiproton proton <--> e+e- threshold q2th, only the kinematical domain q2 > q2th > 0 is available. To access the unphysical region, one may use the antiproton proton --> pi0 e+ e- reaction where the pi0 takes away a part of the system energy allowing q2 to be varied between q2th and almost 0. This thesis aims to show the feasibility of such measurements with the PANDA detector which will be installed on the new high intensity antiproton ring at the FAIR facility at Darmstadt. To describe the antiproton proton --> pi0 e+ e- reaction, a Lagrangian based approach is developed. The 5-fold differential cross section is determined and related to linear combinations of hadronic tensors. Under the assumption of one nucleon exchange, the hadronic tensors are expressed in terms of the 2 complex proton electromagnetic form factors. An extraction method which provides an access to the proton electromagnetic form factor ratio R = |GE|/|GM| and for the first time in an unpolarized experiment to the cosine of the phase difference is developed. Such measurements have never been performed in the unphysical region up to now. Extended simulations were performed to show how the ratio R and the cosine can be extracted from the positron angular distribution. Furthermore, a model is developed for the antiproton proton --> pi0 pi+ pi- background reaction considered as the most dangerous one. The background to signal cross section ratio was estimated under different cut combinations of the particle identification information from the different detectors and of the kinematic fits. The background contribution can be reduced to the percent level or even less. The corresponding signal efficiency ranges from a few % to 30%. The precision on the determination of the ratio R and of the cosine is determined using the expected counting rates via Monte Carlo method. A part of this thesis is also dedicated to more technical work with the study of the prototype of the electromagnetic calorimeter and the determination of its resolution.

Global modeling of pollutant transport and deposition from anthropogenic emission hot spots on global scale

Urban centers significantly contribute to anthropogenic air pollution, although they cover only a minor fraction of the Earth's land surface. Since the worldwide degree of urbanization is steadily increasing, the anthropogenic contribution to air pollution from urban centers is expected to become more substantial in future air quality assessments. The main objective of this thesis was to obtain a more profound insight in the dispersion and the deposition of aerosol particles from 46 individual major population centers (MPCs) as well as the regional and global influence on the atmospheric distribution of several aerosol types. For the first time, this was assessed in one model framework, for which the global model EMAC was applied with different representations of aerosol particles. First, in an approach with passive tracers and a setup in which the results depend only on the source location and the size and the solubility of the tracers, several metrics and a regional climate classification were used to quantify the major outflow pathways, both vertically and horizontally, and to compare the balance between pollution export away from and pollution build-up around the source points. Then in a more comprehensive approach, the anthropogenic emissions of key trace species were changed at the MPC locations to determine the cumulative impact of the MPC emissions on the atmospheric aerosol burdens of black carbon, particulate organic matter, sulfate, and nitrate. Ten different mono-modal passive aerosol tracers were continuously released at the same constant rate at each emission point. The results clearly showed that on average about five times more mass is advected quasi-horizontally at low levels than exported into the upper troposphere. The strength of the low-level export is mainly determined by the location of the source, while the vertical transport is mainly governed by the lifting potential and the solubility of the tracers. Similar to insoluble gas phase tracers, the low-level export of aerosol tracers is strongest at middle and high latitudes, while the regions of strongest vertical export differ between aerosol (temperate winter dry) and gas phase (tropics) tracers. The emitted mass fraction that is kept around MPCs is largest in regions where aerosol tracers have short lifetimes; this mass is also critical for assessing the impact on humans. However, the number of people who live in a strongly polluted region around urban centers depends more on the population density than on the size of the area which is affected by strong air pollution. Another major result was that fine aerosol particles (diameters smaller than 2.5 micrometer) from MPCs undergo substantial long-range transport, with about half of the emitted mass being deposited beyond 1000 km away from the source. In contrast to this diluted remote deposition, there are areas around the MPCs which experience high deposition rates, especially in regions which are frequently affected by heavy precipitation or are situated in poorly ventilated locations. Moreover, most MPC aerosol emissions are removed over land surfaces. In particular, forests experience more deposition from MPC pollutants than other land ecosystems. In addition, it was found that the generic treatment of aerosols has no substantial influence on the major conclusions drawn in this thesis. Moreover, in the more comprehensive approach, it was found that emissions of black carbon, particulate organic matter, sulfur dioxide, and nitrogen oxides from MPCs influence the atmospheric burden of various aerosol types very differently, with impacts generally being larger for secondary species, sulfate and nitrate, than for primary species, black carbon and particulate organic matter. While the changes in the burdens of sulfate, black carbon, and particulate organic matter show an almost linear response for changes in the emission strength, the formation of nitrate was found to be contingent upon many more factors, e.g., the abundance of sulfuric acid, than only upon the strength of the nitrogen oxide emissions. The generic tracer experiments were further extended to conduct the first risk assessment to obtain the cumulative risk of contamination from multiple nuclear reactor accidents on the global scale. For this, many factors had to be taken into account: the probability of major accidents, the cumulative deposition field of the radionuclide cesium-137, and a threshold value that defines contamination. By collecting the necessary data and after accounting for uncertainties, it was found that the risk is highest in western Europe, the eastern US, and in Japan, where on average contamination by major accidents is expected about every 50 years.