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Rafts: Rafts sind spezialisierte Domänen biologischer Membranen, die sich durch ihre spezifische Lipid- und Proteinzusammensetzung auszeichnen (zur Übersicht siehe Simons und Toomre, 2000). Die am besten beschriebenen Rafts sind die Caveolae, doch es gibt noch weitere weniger gut charakterisierte Rafttypen. Rafts werden verschiedene zelluläre Funktionen zugeschrieben wie z.B. gerichteter Transport von Membranproteinen, Endozytose und Signaltransduktion. Diese Funktionen erfüllen sie vornehmlich, indem sie verschiedene Proteine und Lipide bedingt durch ihre biophysikalischen Eigenschaften selektiv aufnehmen oder ausschließen. Viele Raftproteine sind über gesättigte Acylketten, wie Myristat oder Palmitat, oder einen GPIAnker mit der Membran assoziiert. Transmembranproteine, wie z.B. der EGFRezeptor, können jedoch auch in Rafts angereichert sein. Besonders an der Plasmamembran dienen Rafts als Signaltransduktionszentren, indem sie beteiligte Rezeptoren und Signalmoleküle konzentrieren.
Reggie-Proteine: Bei der Suche nach Proteinen, die bei der Regeneration von verletzten Sehnerven von Fischen hochreguliert werden, wurden Reggie-1 und Reggie-2 entdeckt (Schulte et al., 1997). Gleichzeitig wurden diese Proteine bei der Suche nach neuen Raftproteinen gefunden und als Flotillin-1 (=Reggie-2) und Flotillin-2 (=Reggie-1) bezeichnet (Bickel et al., 1997). Reggie-1 und -2 haben ein Molekulargewicht von 47 kDa und sind auf Aminosäuren-Basis zu 44% identisch. Homologe zu Reggie-1 wurden bislang in Mensch, Maus, Ratte und Fisch, wie auch in D. melanogaster gefunden. Die evolutionäre Konservierung der Reggies ist, mit beispielsweise 80% zwischen Ratte und Goldfisch, sehr hoch und weist auf eine wichtige Funktion hin, die Sequenzkonservierung verlangt. Reggie-1 wird ubiquitär exprimiert, wogegen Reggie-2 ein weniger verbreitetes Expressionsmuster aufweist. Reggie-1 ist vornehmlich an der Plasmamembran und an Endosomen lokalisiert. Die subzelluläre Lokalisation von Reggie-2 hängt vom Zelltyp ab...
Aim of the present study was the characterization of the RORa receptor (Retinoidrelated Orphan Receptor a). RORa is a member of the nuclear receptor family and is involved into the differentiation of Purkinje cells, inflammation, arteriosclerosis, and bone mineralization. Nuclear receptors are transcription factors and mediate biological responses within target cells to outer signals such as lipophilic hormones. They are involved in development, growth, differentiation, proliferation, apoptosis, and maintenance of homeostasis. Ligand binding, posttranslational modifications, and cofactor recruitment control their activity. Nearly all nuclear receptors share a common modular structure with an Nterminal A/B region, a DNA-binding domain (DBD) that is composed of two zinc finger motifs, a hinge region, and a C-terminal ligand-binding domain (LBD). The RORs comprise the subtypes RORa, RORb, and RORg, which are encoded by different genes. All isoforms of the respective subtypes only differ in their A/B domain. This study focused mainly on the exploration of the gene structure, expression, and subcellular distribution of RORa...
The melibiose permease (MelB) of E.coli functions as a secondary-active symporter by using the electrochemical H+, Na+, or Li+ gradient to accumulate, e.g., melibiose [review in Pourcher et al. 1990a]. The global and primary objective of this thesis was to apply pre-steady state methods for the investigation of reaction rates of individual steps in the cycle of MelB. Especially the melibiose binding induced transition was investigated by the solid-supported membrane (SSM) technique [Seifert et al. 1993] in combination with a rapid solution exchange system [Pintchovius and Fendler 1999] and with the Stopped-flow technique [Roughton 1934]. To approach this goal, either wild-type or mutated MelB were purified and reconstituted into liposomes as described [Pourcher et al. 1995]. Although the orientation of the proteins is a critical factor for the activity of MelB, it was, so far, unknown. To determine the orientation of the proteins in the liposomes, single Cys mutants R139C and R141C [Abdel-Dayem et al. 2003] were selectively labeled with 3-(N-maleimidylpropionyl)biocytin (MPB) and analyzed by SDS-PAGE and Western Blot. The assay indicated that most of the proteins are inside-out (ISO) oriented permitting to relate the pre-steady state electrical and fluorescence signals to the reverse transport activity of MelB. The melibiose induced electrical signal was investigated in wild-type MelB with the SSM technique. The transporter was activated by a substrate concentration jump, and transient currents were measured. When the transporter was preincubated with Na+ at saturating concentrations, a charge translocation in the protein upon melibiose binding could still be observed. This result demonstrates that binding of the uncharged substrate melibiose triggers a charge displacement in the protein. Further analysis showed that the charge displacement is neither related to extra Na+ binding to the transporter, nor to the displacement of already bound Na+ within MelB. Electrogenic melibiose binding is explained by a conformational change with concomitant displacement of charged amino acid side chains and/or a reorientation of helix dipoles. A kinetic model is suggested, in which Na+ and melibiose binding are distinct electrogenic processes associated with approximately the same charge displacement. Melibiose binding is fast in the presence of Na+ (k > 50 s-1). Furthermore, two previously identified transport deficient mutants of loop 4-5, R141C and E142C [Abdel-Dayem et al. 2002, Séry 2002], were purified and extensively studied with the SSM. Whereas the electrical signals from control cysteine-less mutant showed a bi-exponential time course of decay, those from R141C or E142C consisted of only a single fast exponential component, and the slow decaying component associated with substrate translocation was missing. The electrical signals evoked by a melibiose concentration jump in the presence of Na+ were much smaller than the corresponding signals in C-less MelB. Furthermore, R141C lost the stimulating effect of melibiose on Na+ binding. Steady-state Trp fluorescence spectroscopy revealed impaired conformational changes after melibiose binding in the mutants and fluorescence resonance energy transfer (FRET) measurements indicated that the mutants still show cooperative modification of their sugar binding sites by Na+. These data suggest that loop 4-5 contributes to the coordinated interactions between the ion- and sugar binding site and participates in conformational changes after melibiose binding that are essential for the subsequent obligatory coupled translocation of substrates. By using the Stopped-flow technique, three different approaches were followed. First, the intrinsic Trp fluorescence of MelB, known to increase upon melibiose binding [Mus-Veteau et al. 1995], revealed a signal with a T 1 of ~15 ms in C-less. This time constant is of the same order of magnitude as that determined with the SSM method suggesting that Trp fluorescence and electrical signal are related processes. Conformation for this assumption came from the fact that the activation energies Ea for both processes are similar (around 45 KJ/mol). Second, by using the fluorescent sugar analog Dns2-S-Gal, which monitors events close to the sugar binding site [Maehrel et al. 1998], a signal with a T 1 of ~18 ms was recorded upon Na+ addition. Finally, the fluorescent dye MIANS was used to selectively label the single Cys mutant E365C of loop 10-11. Stopped-flow measurements revealed a melibiose-induced fluorescent signal with a T 1 of 45 ms. Since electrical measurements with the MIANS-labeled E365C excluded the possibility that the label is responsible for the slower kinetics, the conformational change detected by the MIANS fluorescence was assigned to a slow transition in the cycle of MelB after melibiose binding. Ea was determined to be 96 KJ/mol corroborating, thus, the hypothesis of a different process. In conclusion, it was possible to correlate the electrical and fluorescence signals to partial reactions of the transport cycle and to determine their rate constants. According to this new model, the melibiose-induced signal detected with the Trp and electrical measurements corresponds to a step preceding the carriers’ reorientation (3 <-> 3*, k ~ 65s-1), and the melibiose-induced signal detected with the MIANS fluorescence to the reorientation itself (3* <-> 4, k ~ 20s-1).
Experimente zum radiativen Elektroneneinfang (REC, Radiative Electron Capture), der Zeitumkehrung der Photoionisation, wie er in Stößen hochgeladener, relativistischer Schwerionen mit leichten Gasatomen auftritt, ermöglicht einen einzigartigen Zugang zum Studium der Photonen-Materie-Wechselwirkung im Bereich extrem starker Coulombfeldern. So ist die REC-Strahlung im relativistischen Bereich zum einen geprägt durch das Auftreten von höheren elektrischen und magnetischen Multipolordnungen und zum anderen durch starke Retardierungseffekte. In Folge dessen wurde der REC-Prozeß in den vergangen Jahren sehr detailliert untersucht, wobei sich die experimentelle und theoretische Forschung auf die Emissionscharakteristik der REC-Photonen konzentrierte, wie z.B. auf Untersuchungen von Winkelverteilungen und Linienprofilen. Mittlerweile kann der REC-Prozeß als ein - selbst für die schwersten Ionen - wohlverstandener Effekt angesehen werden. Allerdings entzog sich den Experimenten bislang eine zur Beschreibung der Photonenmission wesentlich Größe, näamlich die Polarisation der Strahlung. Die lineare Polarisation der REC-Strahlung, wie sie in Stößen zwischen leichten Atomen und den schwersten, hochgeladenen Ionen vorhergesagt wird, war der Gegenstand der vorliegende Arbeit, in der es erstmals gelang, die diese für den konkreten Fall des Einfangs in die K-Schale von nackten Uranionen nachzuweisen und im Detail zu untersuchen. Die hierzu notwendigen experimentellen Untersuchungen erfolgten am Speicherring ESR der GSI-Darmstadt für das Stoßsystem U92+ -> N2 und für Projektilenergien, die im Bereich zwischen 98 und 400 MeV/u lagen. Besonders hervorzuheben ist der Einsatz eines segmentierten Germaniumdetektors, der speziell für den Nachweis linear polarisierter Strahlung im Energiebereich oberhalb 100 keV entwickelte wurde. Die lineare Polarisation der Strahlung wurde hierbei durch eine Analyse der Comptonstreuung innerhalb des Detektors gewonnen. Die durch eine präzise Analyse der Comptonstreuverteilungen gewonnenen Daten zeigen eine ausgeprägte lineare Polarisierung der REC-Strahlung in der Streuebene, die zudem eine starke Abhängigkeit als Funktion der Stoßenergie und des Beobachtungwinkels aufweist. Der detaillierte Vergleich mit nicht-relativistischen und relativistischen Vorhersagen ermöglichte darüberhinaus den Nachweis für das Auftreten starker relativistischer Effekte, die sich allerdings depolarisierend auswirken. Das Experiment wurde am internen Target des ESR-Speicherrings durchgeführt, wobei der Photonennachweis mittels mehrerer Ge(i)-Detektoren erfolgte, die die Ionen-Target-Wechselwirkungszone unter Beobachtungswinkeln zwischen nahe Null und 150 Grad einsahen. Alle Photonendetektoren wurden in Koinizidenz mit einem Teilchendetektor betrieben, um so die volle Charakteristik des REC-Prozesses zu erfassen, also den Einfang eines Targetelektrons in die nackten Uranionen (U92+) unter Emission eines Photons. Für den Polarisationsnachweis entscheidend war der Einsatz eines Germanium-Pixel-Detektors, der abwechselnd unter den Winkeln von 60 und 90 Grad betrieben wurde. Dieser Detektor verfügt über eine 4x4 Pixelmatrix (Pixelgröße: 7x7 mm), wobei die elektronische Information jedes Pixels (Energiesignale und schnelle Zeitsignale) separat registriert und aufgezeichnet wurde. Hierdurch war es möglich Ereignisse, die koinzident in zwei Pixeln erfolgten, zu detektieren und zu analysieren. Dies ist die eigentliche Voraussetzung für den Nachweis der linearen Polarisation bei hohen Photonenenergien, bei dem die Abhängigkeit des differenziellen Wirkungsquerschnitts für Comptonstreuung von der linearen Polarisation der einfallenden Photonen ausgenutzt wird (siehe Klein-Nishina Formel Eq. 2.7). Der Nachweis der Comptonstreuung erfolgt hierbei durch die Detektion des Compton-Rückstoßelektrons (deltaE) und des gestreuten Comptonphotons (hw'), die jeweils separat, aber koinzident in zwei unterschiedlichen Segmenten des Detektors nachgewiesen werden. Hier sei betont, dass für Germanium bereits ab Photonenenergien von ca. 160 keV die Absorption der Strahlung durch den Compton-Effekt über die Photoabsorption dominiert und somit das Ausnutzen des Compton-Effekts prinzipiell eine sehr effektive Technik ist. Der Auswertung der Datenfkam wesentlich zugute, dass der Germanium-Detektor über eine im Vergleich zu Szintillations- oder Gaszählern gute Energieauflösung von ca. 1.8 keV bei 122 keV verfügt. Somit kann durch Bilden der Summenenergie hw = hw' + deltaE für koinzidente Ereignisse die Energie des einfallenden Photons (hw) rekonstruieren werden und als zwingende Bedingung dafür herangezogen werden, dass es sich bei dem Ereignis im Detektor um ein Compton-Event gehandelt hat. Für den Fall linearer Polarisation ist eine wesentliche Aussage der Klein-Nishina-Formel, dass die maximale Intensität für die Compton gestreuten Photonen senkrecht zur Polarisationsebene zu erwarten ist. Tatsächlich zeigen bereits die während des Experiments aufgenommenen Rohdaten für den Fall der untersuchten REC-Strahlung, die durch den Einfang in die K-Schale des Projektils entsteht, dass es sich hierbei um eine stark polarisierte Strahlung handelt, wobei eine erhöhte Intensität für Comptonstreuung senkrecht zur Stoßebene (für den REC-Prozeß definiert durch die Ionenstrahlachse und den Impuls des REC-Photons) festgestellt wurde (vgl. Fig. 7.3). Zur genauen qualitativen Analyse der Meßdaten wurden alle möglichen Pixelkombinationen der (4x4) Detektorgeometrie ausgewertet, wobei jedoch koinzidente Ereignisse benachbarter Segmente ausgeschlossen wurden, um den hier vorhandenenen Einfluß elektronischer Übersprecher zu eliminieren. Zudem erfolgte die Analyse der Daten unter Berücksichtigung verschiedenster Effekte, die einen Einfluß auf die Nachweiseffizienzen für die Compton gestreuten Photonen haben könnten. An prominenter Stelle ist hier die Korrektur zu nennen, die durch die Detektordicke von 1,5 cm und der Pixelgröße von 7x7 cm2 hervorgerufen wird. Zu betonen ist hier, dass für die Auswertung nur relative Effizienzen eine Rolle spielen und so der Einfluß systematischer Fehler, hervorgerufen durch Effizienzkorrekturen, stark reduziert werden konnte (für eine so gewonnene, vollständige Compton-Streuverteilung sei auf Abbildung 9.1 verwiesen, in der die Intensitätsverteilung für Compton-Streuung dargestellt ist). Es sei auch hervorgehoben, dass der Nachweis der Polarisation durch Messungen von vollständigen Compton-Intensitätverteilung im Detektor erfolgte, was das hier diskutierte Experiment wesentlich von konventionellen Polarisationsexperimenten für harte Röntgen- und gamma-Strahlung unterscheidet. Üblicherweise wird in diesen Experimenten die Comptonstreuung ausschließlich in der Reaktionsebene und senkrecht dazu nachgewiesen. Generell weisen die in der vorliegenden Arbeit gewonnen Compton-Streuverteilungen für den K-REC-Prozeß ein ausgeprägtes Maxium senkrecht zur Reaktionsebene auf und bestätigen somit den bereits aus den Rohdaten abgeleiteten Befund, dass die Polarisationsebene der KREC Strahlung in der Reaktionsebene des Stosses liegt. In der Tat kann dieser Befund für alle Energien und Beobachtungswinkel bestätigt werden, die in dem hier diskutierten Experiment verwendet wurden. Hier sei zudem darauf hingewiesen, dass es durch die Erfassung der vollständigen Compton-Streuverteilung möglich war, die Orientierung der Polarisationsebene in Bezug auf die Stoßebene mit hoher Präzision zu erfassen. So konnte z.B. bei der Stossenergie von 400 MeV/u und dem Winkel von 90 Grad, die Orientierung der Comptonstreuverteilung in Bezug auf die Stoßebene zu ph=90 Grad bestimmt werden. Dieser Befund könnte für die Planung zukünftiger Experimente zum Nachweis polarisierter Ionenstrahlen entscheidend sein, da eine Abweichung von der ph = 90 Grad Symmetrie nur durch das Vorhandensein polarisierter Teilchen erklärt werden kann. Dieser Effekt, der in neuesten theoretischen Behandlungen im Detail untersucht wurde, stellt gleichsam einen neuen Zugang zur Bestimmung des Polarisationsgrads der Projektile dar. Hierdurch wird die Stärke der hier angewandten Technik verdeutlicht, die auf dem Einsatz eines ortsempfindlichen Germanium-Pixel- Detektors beruht. Die Bestimmung des genauen Polarisationsgrades für die K-REC-Strahlung erfolgte durch eine X2-Anpassung der Klein-Nishina-Formel an die experimentellen Daten. Die hieraus resultierenden Daten zeigen für alle Strahlenergien und Beobachtungsgwinkel eine starke Polarisation von etwa 80%, wobei die experimentelle Unsicherheit im 10% Bereich liegt. Letztere ist im wesentlichen auf die statistische Genauigkeit zurückzuführen. Die Daten wurden zudem eingehend mit theoretischen Vorhersagen verglichen. Die Theorie stützt sich auf eine vollständige relativistische Beschreibung des REC-Prozesses unter Verwendung exakter Wellenfunktionen für das Kontinuum und den 1s Zustand in wasserstoffartigem Uran. Typischer weise mußten bei den Rechnungen sowohl elektrische wie auch magnetische Multipolterme bis hin zu L=20 verwendet werden, um Konvergenz zu erreichen. Der Vergleich zeigt eine hervorragende Übereinstimmung zwischen Experiment und Theorie. Zudem verdeutlicht der Vergleich mit der ebenfalls diskutierten Vorhersage der nicht-relativistischen Dipolnäherung die Bedeutung relativistischer Effekte (vor allem das Auftreten höherer elektrischer und magnetischer Multipole), die für die Emission der REC-Strahlung bei hohen, relativistischen Energien und hohem Z charakteristisch sind. Offensichtlich wirken sich diese Effekte stark depolarisierend aus. Dass in der Tat eine Zunahme der depolarisierenden Effekte mit einer Zunahme der Strahlenergie verbunden ist, wird auch durch die Daten dokumentiert, die für den Beobachtungswinkel von 60 Grad als Funktion des Projektilenergie untersucht wurden. Die in der vorliegenden Arbeit gewonnenen Resultate für die Polarisation der REC-Strahlung ebenso wie die neuartige Experimenttechnik, die hierbei zum Einsatz kam, lassen für die nahe Zukunft eine Serie von weiteren Polarisations-Experimenten erwarten. Hierbei könnte der REC-Strahlung und deren Polarisation als Mittel zur Diagnostik und zum Nachweis des Polarisationsgrades gespeicherter Ionenstrahlen eine Schlüsselrolle zukommen. Als Detektorsysteme werden hierzu zwei-dimensionale Germanium- und Silizium-Streifen-Detektoren zum Einsatz kommen bzw. Kombinationen aus zweidimensionalen Silizium- und Germanium-Detektoren, sogenannte Compton-Teleskope. Diese Compton-Polarimeter, die gegenwärtig für neue Experimentvorhaben am ESR-Speicherring entwickelt werden, verfügen über eine wesentlich verbesserte Ortsauflösung (z.B. 1x1 mm2) und somit über eine wesentlich gesteigerte Nachweiseffizienz für die Comptonstreuung (ein bis zwei Größenordnungen). Hierdurch sollte es möglich sein, den für Polarisationexerperimente zugänglichen Energiebereich wesentlich auszudehnen, sodass selbst die charakteristische Strahlung der Schwerionen (ca. 50 bis 100 keV) für solche Experimente zugänglich wird.
The development of a drug product, beginning with the synthesis of the drug substance through approval for marketing, may take up to 15 years and a total amount of investment of up to half a billion Euro. After the discovery of a potential drug substance, many different investigations have to be performed: e.g. characterization of the physical-chemical properties, the pharmacological and toxicological profile and, especially relevant for this work, the development of the first dosage forms. After achieving these steps, first investigations in human studies can be carried out. After a positive assessment of the benefit to risk ratio, further investigations, such as food effects on the pharmacokinetics, multiple dosing studies and further studies on patients can be implemented. After successfully completing this second part the new drug product can be approved. With broader clinical experience it often becomes apparent that changes in relevant aspects of the formulation of the registered drug product e.g. excipients, concentration of the drug substance or excipient versus drug substance ratio, are necessary to optimise the therapy. This often leads to additional clinical investigations and a new registration, a procedure which is time and cost intensive. A possible way to reduce the financial and time investments, is to establish an appropriate in vivo- in vitro correlation (IVIVC). If it is possible to predict the in vivo performance of a drug product adequately with in vitro methods (dissolutions tests), it will no longer be necessary to perform additional clinical investigations. In this work, IVIVCs were investigated for three different drug substances and several different types of formulations.... ...Results of this work clearly show that successful IVIVCs can be achieved for the fasted state using biorelevant dissolution media. A prerequisite of achieving a good IVIVC is the availability of in vivo data of a reference product (i.v., oral solution or IR) tested within the same group of volunteers as the product of interest. Only with this procedure, one can obtain adequate IVIVCs for drug substances with high inter-individual variability of the plasma concentrations and with high first-pass metabolism. This work also shows that predictions of the in vivo behavior of a modified release dosage form after administration with a high fat meal are more difficult to obtain. This is mainly related to an absence of a medium, which could mimic the situation of the fed stomach adequately. Ensure plus®, which was chosen in this work, failed to simulate the fed stomach adequately in several cases; it suppressed the release of rosiglitazone from lipid formulations and led to rapid disruption of the HPMC-matrix of the 5-ISMN Geomatrix formulations. Future work should be directed towards optimization of the test media in the BioDis apparatus. This work clearly shows the inability of Ensure plus® to predict the in vivo performance of a drug under fed state conditions and indicates that alternative media must be developed. It is known that the pH of the stomach rises up to six after the intake of a meal. During the following hours the pH decreases until reaching the baseline value of approximately 1.8. One possibility of simulating the fed state stomach more precisely will be to divide the overall residence time into 4 different parts: 1. half a hour at pH 6 2. half a hour at pH 4 3. one hour at pH 3 4. two hours at pH 1.8 Another option is not only to modify the pH of the medium, but also to change its composition. During the decomposition of the food contents, the composition of the gastric juice changes, the ionic strength, the buffer capacity and the osmolarity rises, while the pH value decreases. A third possibility will be the addition of enzymes, mainly pepsin, lipases and amylases. Again, the quantity of the enzymes differs during the residence time of the food in the stomach. Highest quantities are expected in the first two hours after food intake and decreases in the remaining two hours. Another issue of this work was an assessment of the two dissolution apparatus, Paddle and BioDis. In general, the choice of the dissolution apparatus should be done primarily with respect to the solubility behavior of the drug substance. For high soluble drugs the USP apparatus II, Paddle, is sufficient (e.g. diltiazem or 5-ISMN). In cases of a poorly soluble drug (rosiglitazone), where the release strongly depends on the medium used, the USP apparatus III (BioDis) is favored, due to the advantage of simulating the GI-tract with a gradient of different dissolution media, each simulating one part of the GI-tract. In summary, the results of this work indicate that it is acurrently possible to predict fasted state behavior of a variety of controlled release products using in vitro tests. Prognoses was also made in terms of predicting food effects on the behavior of controlled release products, although it is clear that the media compositions will have to be revised to establish releiable predictive methods for the fed state.
Since its recognition as an endothelium-derived relaxing factor, the control and consequences of nitric oxide (NO) production have been investigated intensely. We know now that NO is not simply a vasodilator or regulator of smooth muscle tone but is a potent anti-platelet agent, neuromodulator and regulator of gene expression. NO is synthesized from the amino acid Larginine by a family of enzymes termed NO synthases (NOS). The ‘endothelial’ (eNOS or NOS III) and ‘neuronal’ (nNOS, NOS I or bNOS) NOS isoforms, which were named after the tissues in which they were first identified, are expressed constitutively and are generally regulated by Ca2+/calmodulin (CaM). Endothelium-derived NO is thought to be responsible for maintaining the vasculature in an anti-atherosclerotic state and a decrease in the bioavailability of NO (a state generally referred to as endothelial dysfunction) results in “proatherosclerotic” alterations in vascular gene expression. Recently it has become clear that the activity of eNOS is largely determined by its association with regulatory proteins as well as by the phosphorylation of the enzyme on serine, threonine and possibly tyrosine residues. Moreover, the enzyme can be “uncoupled” i.e. transformed from a NO generating to a superoxide (O2-)-generating enzyme, which would be expected to attenuate vasodilator responses and enhance vascular inflammation. The aim of this thesis was to study the consequences of phosphorylation on specific serine, threonine and tyrosine residues on the activity and intracellular localisation of eNOS and in particular to determine whether a phospho-switch for eNOS uncoupling exists. eNOS is phosphorylated under basal conditions and its serine phosphorylation can be enhanced following cell stimulation with hemodynamic stimuli such as cyclic stretch and fluid shear stress as well as by hormonal stimuli such as histamine and bradykinin. Our group has previously demonstrated the importance of Ser1177 in the activation of eNOS and here I set out to determine the relative importance of phosphorylation on Ser633 and Ser114. By generating point mutants in which serine was replaced by either alanine (nonphosphorylatable mutants) or aspartate (phosphomimetic mutants) it was observed that the activity of the S633D and S114A eNOS mutants exhibited an 2-fold increase over the activity of the wild-type enzyme or either of the S633/634A or S114D eNOS mutants as determined by monitoring the conversion of L-arginine to L-citrulline. eNOS is basally phosphorylated on Thr495 and stimulation of endothelial cells with Ca2+-elevating agonists generally results in the transient dephosphorylation of this residue. The latter is essential to allow the binding of calmodulin to the enzyme and is the actually initiating step in the generation of NO. Correspondingly, the T495A eNOS mutant can be activated at lower Ca2+ and calmodulin concentrations than the T495D mutant. However, some eNOS mutants (T494A/S1177D and T495A) showed an enhanced ability to generate O2- in a NOS inhibitor-sensitive manner suggesting that the phosphorylation of the enzyme may also play a role in the uncoupling process. To determine the physiological relevance of eNOS dephosphorylation on Thr495 we assessed the consequences of treating cells with oxidised low-density lipoprotein (ox-LDL) on eNOS phosphorylation as well as on the eNOS-dependent generation of NO and O2-. Oxidised LDL concentration- and time-dependently decreased phosphorylation of eNOS on Thr495 and led to a concomitant decrease in cellular levels of cyclic GMP and an enhanced production of O2 - compared to cells treated with native LDL. Alterations in the activity of protein kinase C (PKC) were related to the change in eNOS Thr495 phosphorylation. There was not only the basal activity of PKCα inhibited by ox-LDL but the PKC activator phorbol-12-myristate-13-acetate also failed to elicit the phosphorylation of Thr495 in ox-LDL-treated endothelial cells. The dephosphorylation of eNOS on Thr495 in response to the addition of ox-LDL was not associated with an increase in the binding of calmodulin to eNOS, an association usually necessary for the activation of eNOS. Moreover, following treatment with ox-LDL for 24 hours eNOS was no longer detected at the plasma membrane but was redistributed to the cytosol indicating that ox-LDL may disrupt the eNOS signalling complex or signalosome. To date the role played by the tyrosine phosphorylation of eNOS in the regulation of its activity or intracellular association is controversial. However, during the preparation of this thesis we have been able to demonstrate a link between the tyrosine phosphorylation of eNO and the activation of the tyrosine kinases Src and PYK2. The application of fluid shear stress to endothelial cells resulted in the activation of Src and PYK2 as well as in the association of PYK2 with eNOS. Co-expression of eNOS and PYK2 led to the putative identification of Tyr657 as a potential modulatory site. Mutating eNOS at Tyr657 to Asp or Glu resulted in the localisation of the mutant eNOS predominantly in the cytoskeleton and also in a complete inactivation of the enzyme. The Y657F mutants, on the other hand, did not demonstrate any marked alteration in the activity when compared with the wild-type eNOS. However, the In conclusion, the results describe in this thesis indicate that eNOS is regulated by phosphorylation at multiple sites. Depending on the phosphorylation site involved phosphorylation can inhibit or activate NO production or even uncouple the enzyme so that it generates O2-. While the phosphor-status of eNOS on Ser114 and Ser633 influenced NO release they did not contribute to O2 - production and the dephosphorylation of Thr495 seems sufficient to uncouple eNOS. Cell treatment with ox-LDL, which is known to increase eNOS-derived O2- output was correlated with a dephosphorylation of Thr495 as well as a decrease in the activity of the kinase that phosphorylates this site i.e., PKCα. The phosphorylation status of all the eNOS serine and threonine residues studied however did not influence the ability of the enzyme to dimerise, indicating that contrary to previously published reports the eNOS dimer is highly stable in endothelial cells. The tyrosine phosphorylation of eNOS was not initially expected to play a determinant role in the regulation but rather to facilitate the docking of associated regulatory proteins. However, Tyr657 seems to play a critical role in the generation of NO as its mutation resulted in the generation of a completely inactive enzyme as well as in an apparent intracellular mislocalisation of the protein. The physiological relevance of these findings remain to be further elucidated.
Amblyopia is a developmental disorder of the visual system that leads to reduced vision in one or both eyes. People suffering from amblyopia show different perceptual deficits like reduced contrast sensitivity, reduced or no stereopsis, spatial uncertainty, and spatial and temporal distortions when viewing with the amblyopic eye. In the following thesis, different psychophysical methods are used to investigate anomalous perception of amblyopic participants in detail with the main focus on the perception of temporal instability. In the qualitative experimental paradigms it is shown that temporal instability is mainly perceived by strabismic and strabismic-anisometropic amblyopes. The temporal deficits occur only at spatial frequencies higher than 1.6 c/deg, and are perceived in addition to the spatial distortions. Illusory colours sometimes accompany the temporal distortions. There seems to be a relationship between crossed hand and eye dominance and the perception of temporal instability. In the quantitative experiments it is shown that temporal instability in amblyopic perception has a negative impact on the performance in psychophysical tasks. Amblyopes perceiving temporal instability show enhanced spatial uncertainty and spatial distortions for different types of stimulus presentation (auditive vs. visual) when compared to amblyopes without temporal instability. This might be due to deficits in auditive-visual mapping. These deficits in auditory-to-visual mapping suggest an impairment of the dorsal “where” pathway. Thus, it might be that amblyopes with temporal distortions have deficits in the dorsal pathway that come up in addition to the known deficits of the ventral “what” pathway and are related to the perception of temporal instability. The different results of the experiments found in this thesis seem to confirm this hypothesis. Studies using functional imaging techniques might be appropriate for a further investigation of amblyopic deficits involving the dorsal pathway.
The Kaon-Spectrometer (KaoS) at the heavy-ion synchrotron (SIS) at the Gesellschaft für Schwerionenforschung (GSI) in Darmstadt has been used to study production and propagation of K+ and K- mesons from Au+Au collisions at a kinetic beam energy of 1.5 AGeV. This energy for K+ mesons is close to the corresponding production threshold in binary nucleon-nucleon collisions and far below for K- mesons. The azimuthal angular distributions of particles as a function of the collision centrality and particle transverse momenta have been measured. The properties of strange mesons are expected to be modified by the in-medium meson-baryon potential. Theoretical calculations show that the superposition of the scalar and vector potentials leads to a small repulsive K+N and a strong attractive K-N potential. Additionally, the interaction of kaons and antikaons with nuclear matter is different. The strangeness conservation law inhibits the absorption probability of K+ mesons as they contain an s-quark. K- mesons, however, interact with nucleons via strangenessexchange (K- + N ->Y + pion, where Y = lambda, sigma). Moreover, the reverse process (pion + Y -> K- + N) is the dominant production mechanism of K- mesons at SIS energies. The azimuthal angular emission patterns of kaons are expected to be sensitive to the in-medium potentials. An enhanced out-of-plane emission of K+ mesons was observed in Au+Au reactions at 1.0 AGeV and 1.5 AGeV, and also in Ni+Ni at 1.93 AGeV. The out-of-plane emission of K+ mesons in Au+Au reactions at 1.0 AGeV was interpreted as a consequence of a repulsive K+N potential in the nuclear medium, however, recent transport calculations show that the emission patterns obtained in Au+Au at 1.5 AGeV and Ni+Ni at 1.93 AGeV are additionally influenced by the re-scattering of kaons. For K- mesons the calculations predict an almost isotropic emission pattern due to the attractive K-N potential which counteracts the absorption of K- mesons in the spectator fragments. In Ni+Ni collisions at 1.93 AGeV the azimuthal distribution of K- mesons has been found to be isotropic. In this case, however, the spectators are rather small and have large relative velocities. In addition, the delay of antikaon emission due to strangenessexchange reaction minimizes the interaction with the spectators. As a consequence the sensitivity of the K- meson emission pattern to the K-N in-medium potential is reduced. In Au+Au collisions we found a dependence of the K- meson azimuthal emission pattern on the transverse momentum. The antikaons registered with pt < 0.5 GeV/c are preferentially emitted in the reaction plane and the particles with pt > 0.5 GeV/c show strong out-of-plane enhancement. The emission patterns of K- can be explained in terms of two competing phenomena: one of them is indeed the influence of the attractive K-N potential, however, the second one originates from the strangeness-exchange process.
Soluble guanylyl cyclase (sGC) is a cytosolic enzyme producing the intracellular messenger cyclic guanosine monophosphate (cGMP) on activation with nitric oxide (NO) which leads to the activation of GMP dependent protein kinases and to vasodilation. NO signaling may be affected by altered expression of sGC subunits, as has been shown in different pathological and physiological conditions and developmental stages. The molecular mechanisms underlying altered sGC expression in these and other conditions have not yet been revealed. Gene expression can also be regulated at the level of mRNA through alterations in translational efficiency and in mRNA stability. HuR (Human R) is a ubiquitously expressed member of the embryonic lethal abnormal vision (ELAV) family of RNA-binding proteins. Among other RNAs, there has been recent evidence that the expression of sGC is subject to post-transcriptional regulation by HuR. It has been shown that chronic hypertension induces changes in HuR expression and activity, which account for decreased sGC expression and activity in the aorta of hypertensive rats. This thesis should study was performed in an effort to provide some insight to the transcriptional and post-transcriptional regulation of sGC expression in a mammal, the rat. We investigated rat sGC alpha-1 transcriptional regulation in rat lung fibroblast (RLF-6) cells. The 3000bp 5' upstream region of the alpha-1 sGC gene was isolated and analyzed for promoter activity by using luciferase reporter constructs- Alpha3000 (with -2794 bp), Alpha1100 (-1092 bp), Alpha350 (-346 bp) and Alpha200 (-200 bp). The promoter activity was the highest in the 200bp construct (about 6-fold higher than Alpha3000) suggesting that this fragment contains all the crucial elements necessary to support basal transcription of the alpha-1 sGC gene. Analysis of the 200 bp of the 5’ UTR of the alpha-1 gene was performed using the MATINSPECTOR V2.2 software for putative transcription factors. The constructs containing the deleted sites for NFY and Sp1 showed a significant decrease in constitutive promoter activity by almost 80% and 60% respectively, implying that these transcription factors are crucial elements in the basal expression of the of sGC alpha-1 subunit. Treatment of RLF-6 cells with genistein 50 microM and mithramycinA 100 nM, known to inhibit the NFY and Sp1 binding to DNA respectively, reflected the same effects. Furthermore the cGMP content of the cells was significantly reduced by both inhibitors, almost completely by genistein, and by about 40 % by mithramycinA. Electrophoretic mobility-shift assay (EMSA) clearly showed the formation of multiple complexes with the biotinylated ODN (decoy oligodeoxynucleotide) probes for NFY and Sp1 when incubated with RLF-6 nuclear extract. A “supershift” observed in the presence of antibodies to the individual transcription factors confirmed that these factors were present in the shifted band, indeed. NFY and Sp1 are instrumental in several physiological and pathophysiological effects mediated by several growth factors in smooth muscle cells. Thus the regulation of the promoter, in response to serum, was also analysed. 10% foetal calf serum led to decreased alpha-1 sGC level as shown by western blots performed with rat aorta. Decreased sGC alpha-1 mRNA expression was observed in RLF-6 cells and cultured rat aortic smooth muscle cells incubated with FCS for 24 hours. This decrease was reflected in the promoter activity in RLF-6 cells using both Alpha3000 and Alpha200 constructs confirming that the regulation took place at promoter level. EMSA performed with nuclear extracts from FCS treated RLF-6 cells led to diminished binding to NFY, but to an enhanced binding to Sp1 site. We concluded that the factors Sp1 and NFY (the sites overlapping) compete for binding, and in the presence of FCS, it is Sp1 that binds stronger, and hence results in diminishing promoter activity. In order to delineate the post-transcriptional regulation of sGC alpha-1 subunit, studies were performed to demonstrate the regulation of expression of the mRNA stabilizing protein HuR. It has been observed that exposure of isolated rat aortic segments to the activator of adenylyl cyclase, forskolin, strongly reduced sGC alpha-1/beta-1 and HuR protein and mRNA expression in a time-dependent and actinomycin D-sensitive fashion. Transcription factor decoy approach proved that the cAMP-induced down-regulation of HuR is mediated by the activation of AP-1. It has been established that HuR stabilises the sGC alpha-1 and beta-1 mRNA. However the pathway underlying this regulation remains unknown. In order to identify the mechanism of this regulation, we looked for HuR interacting proteins employing the yeast two hybrid assay. The enzyme of the polyamine catabolic pathway spermidine/spermine N1-acetyltransferase (SSAT) was found to interact with the hinge region of HuR. This interaction was confirmed by performing immunoprecipitation and GST-pulldown experiments. A direct effect of these proteins on each other’s biological activity was not visible as tested through the SSAT activity assay and HuR gel shift. It might be possible that SSAT-mediated modulation of local polyamine concentrations enhances/reduces HuR activity and sGC expression to affect cell proliferation. In summary, this study represents an analysis of the rat sGC alpha-1 promoter regulation in rat fibroblast cells and identifies NFY and Sp1 as important factors in sGC alpha-1 expression. It also gives first evidence of sGC regulation at the transcriptional level in response to an external stimulus, and proposes the possible mechanism. It also identifies SSAT as a HuR interacting protein. These might have implications in the various pathophysiological conditions where sGC plays an important role.
The generation of O2- by NADPH oxidaes was mainly attributed to immune cells that kill invading bacteria or cancer cells. But importantly, in the past several years, several homologs of the catalytic subunit gp91phox (Nox2) of the phagocytic NADPH oxidase have been identified in non-immune cells and tissues. Superoxide production derived from NADPH oxidaes has been shown to play a role not only in host defense but also in defined signaling cascades mediating growth and apoptosis. The aim of this work was to study the expression and the regulation of the”new” Nox isoforms in rat renal mesangial cells (MC). In particular the following results were achieved. 1) mRNA’s for both Nox1 and Nox4 were detected by RT-PCR. 2) Nox1 mRNA levels were increased upon exposure to basic fibroblast growth factor (bFGF), platelet-derived growth factor (PDGF) and fetal calf serum (FCS) in a time- and dose-dependent manner. Exposure of MC to bFGF and FCS increased also basal production of reactive oxygen species (ROS) by MC. By contrast, Nox4 mRNA levels were not significantly affected by bFGF treatment, but were markedly down-regulated by PDGF and FCS. 3) To study the regulation of Nox1 on the protein level, an anti-Nox1 antibody was generated and characterized using affinity chromatography. Up-regulation of Nox1 expression by growth factors was confirmed also on the protein level. 4) Based on the already known cDNA sequence for Nox1, the transcriptional start site was determined by the “gene RACE” technique. 2547 bp of the genomic sequence of the 5´-flanking region of the Nox1 gene were cloned and sequenced using the „Genome-Walking“ method. To study the regulation of Nox1 transcription functional Nox1 promoter/luciferase fusions were be established. MC were transiently transfected with different promoter/luciferase constructs and stimulated with growth factors. By measuring luciferase activity it was determined that growth factors induced the Nox1 transcription and that the Nox1 core promoter is sufficient for the activation. 5) By measurement of superoxide radicals and analysis of Nox1 mRNA expression by quantitative RT-PCR (TaqMan) as well as protein level by Western blotting it could be shown that treatment of MC with NO donors inhibited the expression of Nox1 in a time- and dose-dependent manner. Moreover, using activators and inhibitors of the soluble guanylyl cyclase (sGC) it could be shown, that the activation of sGC mediates the effect of NO on Nox1 expression. However, NO had no inhibitory effect on Nox1 promoter activity. Experiments with the inhibitor of transcription, actinomycin D, suggest that NO-mediated regulation of Nox1 is triggered probably via post-transcriptional mechanisms. Nox4 is regulated on the mRNA levels in a similar manner as Nox1. 6) To analyze the sub-cellular localization of the Nox isoforms, coding sequences for Nox1 and Nox4 were fused together with green fluorescent protein into the pEGFP-N1 demonstrated that both isoforms are localized predominantly in the plasma membrane, but also in the perinuclear region and cytoplasm. However, the localization of Nox1 in the plasma membrane was more pronounced. 7) In addition to Nox1 and Nox4, mRNA of the newly identified NOXA1 that is a homolog of the p67phox subunit of NADPH oxidase was detected in MC by RT-PCR.
Studies in particular of the last decade showed that active neurogenesis continuously takes place in the subventricular zone (SVZ) of the lateral ventricles of the adult rodent brain. Neurogenesis in the SVZ leads to migration of neuroblasts within the rostral migratory stream (RMS) and mature neuron formation mainly in the olfactory bulb (OB). According to present understanding, glial cells with astrocytic properties represent the actual adult neural stem cells. The cell types representing the various cellular transition states leading to the formation of mature neurons as well as the mechanisms controlling adult neurogenesis and neuroblast migration are poorly understood. A previous study from this laboratory demonstrated that the ATP-hydrolyzing enzyme nucleoside triphosphate diphosphohydrolase 2 (NTPDase2) is associated with type B cells, the presumptive neural stem cells. NTPDase2 is a protein of the plasma membrane with its catalytic site facing the extracellular space. It hydrolyzes extracellular nucleoside triphosphates to their respective nucleoside diphosphates. This raises the possibility that the signaling pathway via extracellular nucleotides is involved in the control of adult neurogenesis. Neurons as well as glial cells express several subtypes of receptors (P2 receptors) that are responsive to the nucleotides ATP, ADP, UTP, or UDP. P2X receptors are ATP-gated Na+, K+ and Ca2+ permeable ion channels, P2Y receptors are coupled to trimeric G-proteins. In order to probe for a functional role of nucleotides in adult neurogenesis, the present study referred to an in vitro system (neurospheres). Neurospheres produced from isolates of the mouse SVZ and cultured in the presence of EGF and bFGF expressed the neural stem cell marker nestin and also GFAP, S100β, NTPDase2 and tissue non-specific alkaline phosphatase. Neurospheres generated from the cells of the subventricular zone were multipotenital. This was revealed by immunostaining of differentiated cells with markers for astrocytes, neurons and oligodendrocytes. The presence of ecto-nucleotidase was verified by analyzing the free phosphate released from nucleotides. The tissue non-specific form of alkaline phosphatase was the predominant enzyme. Both NTPDase2 and TNAP could be identified by immunocytochemistry and Western blotting. Hydrolysis was not observed for p-nitrophenyl thymidine monophosphate, a substrate of members of the ectonucleotide pyrophosphatase/phosphodiesterase family (NPP1 to NPP3). Since ecto-nucleotidases control the availability of extracellular nucleotide agonists, neurospheres were studied for the potential expression and functional role of nucleotide receptors. Neurospheres responded to extracellular nucleotides with a transient rise in Ca2+ (ATP = ADP > UTP). The rise in Ca2+ was due to P2Y receptors. The Ca2+ response was unaltered in the absence of extracellular Ca2+ and strongly reduced by thapsigargin, a blocker of internal Ca2+ stores. The P2Y1 antagonist MRS2179 strongly reduced the ATP- or ADP-induced increase in Ca2+, suggesting the involvement of a P2Y1 receptor. In addition, suramin and PPADS, non-selective antagonists for P2 receptors, inhibited most of the Ca2+ response. The agonistic activity of UTP and the lack of response to UDP implied the additional presence of a P2Y2 and/or a P2Y4 receptors and the absence of a functional P2Y6 receptor. RT-PCR experiments demonstrated that neurospheres expressed P2Y1 and P2Y2 receptors but not P2Y4 receptor. That the majority of the Ca2+ response to ATP was mediated via P2Y1 receptors was also confirmed by analysis of P2Y1 knockout mice and by application of the P2Y1 receptor-specific antagonist MRS2179. In addition, agonists of P2Y1 and P2Y2 receptors and low concentrations of adenosine augmented cell proliferation inspite of the presence of mitogenic growth factors. Neurosphere cell proliferation was attenuated after application of MRS2179 and in neurospheres from P2Y1 receptor knockout mice. These results infer a nucleotide receptor-mediated synergism that augments growth factor-mediated cell proliferation. Taken together these results suggest that P2Y-mediated nucleotidergic signalling is involved in neurosphere function and possibly also in adult neurogenesis in situ.
The Na+/proline transporter of E. Coli (PutP) is responsible for the uptake of proline which is subsequently used not only as a carbon and nitrogen source and a constituent of proteins but also as a particularly effective osmoprotectant. However, for a long time there was little known about the single steps in the reaction cycle of this transporter and only few details about its structure-function relationship are available. Aim of the present work was to achieve a deeper understanding about the kinetic properties of the Na+/proline transporter and to get insights into the structure-function relationship of the substrate binding. To answer these questions different techniques were used. By using the novel SSM technique combining the preparation of PutP proteoliposomes it was possible to demonstrate for the first time the electrogenic substrate binding to PutP transporter. Due to rapid solution exchange measurements on the SSM it was additionally possible to obtain time resolved information about the kinetic details of the cytoplasmic substrate binding sites which were not available by previous steady state and equilibrium binding measurements. Pre-steady-state charge translocation was observed after rapid addition of one or both of the cosubstrates Na+ and/or proline to the PutP-WT proteoliposomes adsorbed on the SSM. Thereby it was possible to link the observed electrical signals with the binding activity of PutP. The observed Na+ and/or proline induced charge displacement were assigned to an electrogenic Na+ and/or proline binding process at the cytoplasmic face of the enzyme with a rate constant of k > 50 s-1 proceeding the rate limiting step of the reaction cycle. Furthermore, based on the kinetic analysis of the electrical signals obtained from the measurements of PutP on SSM, the following characteristics of the substrates binding in PutP were deduced: (1) both Na+ and proline can bind individually to the transporter. Under physiological conditions, an ordered binding mechanism prevails; while at sufficiently high concentrations, each substrate can bind in the absence of the other; (2) substrate binding is electrogenic not only for Na+, but also for the uncharged cosubstrate proline. The charge displacement associated with Na+ binding and proline binding is of comparable size and independent of the presence of the respective cosubstrate. In addition, it was concluded that Na+ accesses its binding site through a high-field access channel resulting in a charge translocation, whereas the binding of the electroneutral proline induces a conformation alteration involving the displacement of charged amino acid residue(s) of the protein; (3) Na+ and proline binding sites interact cooperatively with each other by increasing the affinity and/or the speed of binding of the respective cosubstrate; (4) proline binding proceeds in a two step process: low affinity (~ 0.9 mM) electroneutral substrate binding followed by a nearly irreversible electrogenic conformational transition; (5) membrane impermeable PCMBS inhibits both Na+ and proline binding to the inside-out orientated PutP transporter, indicating that rather than selectively blocking a specific binding site, PCMBS probably locks the enzyme in an inactive state. The possible targets for this SH-reagent are cysteines 281 and 344 located close to the cytoplasmic surface of the protein. Beyond it, transient electrical currents of PutP were also observed on the BLM after rapid addition of proline in the presence of Na+. This was possible by combining the conventional BLM technique with high-speed flash-photolysis of caged-proline. Indeed the signals on the BLM indicate the detection of a different underlying reaction process in comparison to the data achieved by the SSM technique. This has paved the way for supplemental information about the reaction cycle since it was possible to assign the flash-photolysis BLM signals to the proline binding step followed by the internalization of Na+ and proline into the liposome. Thereby it was found, that the presence of Na+ is indispensable and the time constant for the process is ~ 63 ms. Moreover, structure-function information about the Na+ and proline binding sites of PutP was obtained by investigating the functionally important amino acid residues Asp55, Gly63 and Asp187 with site-directed mutagenesis and the combined SSM technique. One finding is that the mutated proteins PutP-D55C and PutP-G63C showed no activity on the SSM. Therefore, it can be assumed that either both Asp55 and Gly63 are crucial for the structure of PutP protein, or they are located at or close to the Na+ and proline binding sites. Furthermore, the results obtained from PutP-D187N and PutP-D187C mutants on SSM suggest that Asp187 of PutP is likely to be involved in the Na+ binding at the cytoplasmic side of the backward running carrier. Taken together the results of the present work have substantially broadened the known picture of the Na+/proline transporter PutP thereby several steps of the reaction cycle were elucidated, and moreover, valuable insights into the structure-function relationship of the transporter have become available.
The technique of site-specific fluorescence labelling with Tetramethylrhodaminemaleimide (TMRM) in combination with two electrode voltage-clamp technique (TEVC), an approach that has been named voltage clamp fluorometry (VCF), has been used in this work to study the Na,K-ATPase. The TMRM dye has the ability to attach covalently to cysteine residues and it responds to changes in the hydrophobicity of its local environment. We exploited this property using a construct of the Na-pump in which the native, extracellularly accessible cysteines were removed and cysteine residues were introduced by site-directed mutagenesis in specific positions of the Na-pump. In this way it was possible to detect site-specific conformational rearrangements of the Na-pump in a time-resolved fashion within a native membrane environment. In particular this technique allows to resolve reactions with low electrogenicity that cannot be satisfactorily analyzed with purely electrophysiological techniques and to identify the conformations of the enzyme under specific ionic composition of the measuring buffers. We used VCF to study the influence that several cations like Na+, K+, NMG+, TEA+ and BTEA+ exert on the distribution of the Na,K-ATPase between several enzymatic intermediates and on some of the reactions related to cation transport. To this end we utilized the mutants N790C in the loop M5-M6 and the mutant E307C, T309C, L311C and E312C in the loop M3-M4. From the correspondence of the fluorescence changes with the activation and inhibition of pumping current, by K+ and ouabain respectively, and from the fact that in Na+/Na+ exchange conditions the voltage distribution of charge movement and fluorescence changes evoked by voltage jumps are in reasonable agreement we conclude that through the fluorescence signals measured from these mutants, we can indeed monitor conformational changes linked to transport activity of the enzyme. For the mutants N790 and L311, it was found that the Na+ dependence of the amplitude and kinetics of the fluorescence signal associated with the E1P-E2P transition is in agreement with the prediction of an access channel model describing the regulation of the access of extracellular Na+ to its binding site. In particular for the mutants E307 and T309 it was found that in Na+/Na+ exchange conditions, the conformational change tracked by the fluorescence was much slower than the charge relaxation at hyperpolarized potentials while the kinetics was very similar at depolarized potentials. This implies that at hyperpolarized potentials the conformational change connected to the E1P-E2P transition does not give a large contribution to the electrogenicity of the process which is also consistent with the access channel model. On the mutant N790C it was found that the external pH does not seem to have any effect on the E1P-E2P equilibrium even if it seems to modulate the fluorescence quantum yield of the dye. Fluorescence quenching experiments with iodide and D2O indicate that at hyperpolarized potentials the local environment of the mutant N790C, experiences a small change in the accessibility to water without major changes in the local electrostatic field ...
Sodium proton antiporters are ubiquitous membrane proteins found in the cytoplasmic and organelle membranes of cells of many different origins, including plants, animals and microorganisms. They are involved in cell energetics, and play primary roles in the homeostasis of intracellular pH, cellular Na+ content and cell volume. Adaptation to high salinity and/or extreme pH in plants and bacteria or in human heart muscles requires the action of such Na+/H+ antiporters. NhaA is the essential Na+/H+ antiporter for pH and Na+ homeostasis (at alkaline pH) in Escherichia coli and many other enterobacteria. NhaA is an electrogenic Na+/H+ antiporter that exchanges 2H+ for 1Na+ (or Li+). NhaA shares with many other prokaryotic and eukaryotic antiporters a very strong dependence on pH. In order to achieve three-dimensional structure of NhaA, the previously described NhaA protein preparation was modified: (i) the wild type bacterial strain (TA16) used for homologous over-expression of NhaA was replaced with a delta nhaA strain (RK20). As a result, the purity and homogeneity of the sample was significantly improved; (ii) the previously two-step purification procedure was shortened to a single step affinity chromatography purification; (iii) a wide-range screening of crystallisation conditions, more than 20,000, was performed; (iv) a Seleno-L-methionine (SeMet) NhaA derivative was produced in order to solve the phases during structure determination. In parallel, attempts of production and crystallisation of co-complexes composed of NhaA and antibody fragments have been made. Four different monoclonal antibodies were available against NhaA. Selected antibody fragments were produced and the stability of the complex analysed. Here, the crystal structure of the pH down-regulated secondary transporter NhaA of Escherichia coli is presented at 3.45 Å resolution. A negatively charged ion funnel opens to the cytoplasm and ends in the middle of the membrane at the putative ion-binding site. There, a unique assembly of two pairs of short helices connected by crossed, extended chains creates a balanced electrostatic environment. A possible mechanism is proposed: the binding of charged substrates causes electric imbalance inducing movements, which allow for a rapid alternating access mechanism. This ion exchange machinery is regulated by a conformational change elicited by a pH signal perceived at the cytoplasmic funnel entry. The structure represents a novel fold that provides two major insights: it reveals the structural basis for the mechanism of Na+/H+ exchange and its unique regulation by pH in NhaA and in many other similar antiporters. Furthermore, it is also important for the understanding of the architecture of membrane proteins in general. However, although many aspects of the ion-translocation mechanism and pH regulation are clarified by the NhaA structure, higher resolution structures with Li+ or Na+ bound are required for understanding the ligand binding and the translocation mechanism at the atomic level. The alkaline pH-induced conformation is essential to further understand the pH-control and proton access to the binding site.
In this thesis, we opened the door towards a novel estimation theory for homogeneous vectors and have taken several steps into this new and uncharted territory. Present state of the art for homogeneous estimation problems treats such vectors p 2 Pn as unit vectors embedded in Rn+1 and approximates the unit hypersphere by a tangent plane (which is a n-dimensional real space, thus having the same number of degrees of freedom as Pn). This approach allows to use known and established methods from real space (e.g. the variational approach which leads to the FNS algorithm), but it only works well for small errors and has several drawbacks: • The unit sphere is a two-sheeted covering space of the projective space. Embedding approaches cannot model this fact and therefore can cause a degradation of estimation quality. • Linearization breaks down if distributions are not highly concentrated (e.g. if data configurations approach degenerate situations). • While estimation in tangential planes is possible with little error, the characterization of uncertainties with covariance matrices is much more problematic. Covariance matrices are not suited for modelling axial uncertainties if distributions are not concentrated. Therefore, we linked approaches from directional statistics and estimation theory together. (Homogeneous) TLS estimation could be identified as central model for homogeneous estimation and links to axial statistics were established. In the first chapters, a unified estimation theory for the point data and axial data was developed. In contrast to present approaches, we identified axial data as a specific data model (and not just as directional data with symmetric probability density function); this led to the development of novel terms like axial mean vectors, axial variances and axial expectation values. Like a tunnel which is constructed from both ends simultaneously, we also drilled from the parameter estimation side towards directional/axial statistics in the second part. The presentation of parameter estimation given in this thesis deviates strongly from all known textbooks by presenting homogeneous estimation problems as a distinguished class of problems which calls for different estimation tools. Using the results from the first part, the TLS solution can be interpreted as the weighted anti-mean vector of an axial sample. This link allows to use our results from axial statistics; for instance, the certainty of the anti-mode (i.e. of the TLS solution!) can be described with a weighted Bingham distribution (see (3.91)). While present approaches are only interested in the eigenvector of the some matrix, we can now exploit the whole mean scatter matrix to describe TLS solution and its certainty. Algorithms like FNS, HEIV or renormalization were presented in a common context and linked to each other. One central result is that all iterative homogeneous estimation algorithms essentially minimize a series of evolving Rayleigh coefficients which corresponds to a series of (converging?) cost functions. Statistical optimization is only possible if we clearly identify every step as what it exactly is. For instance, the vague statement “solving Xp ... 0” means nothing but setting ˆp := arg minp pTXp pT p . We identified the most complex scenario for which closed form optimal solutions are possible (in terms of axial statistics: the type-I matrix weighted model). The IETLS approach which is developed in this thesis then solves general type-II matrix weighted problems with an iterative solution of a series of type-I matrix weighted problems. This approach also allows to built converging schemes including robust and/or constrained estimation – in contrast to other approaches which can have severe convergence problems even without such extensions if error levels are not low. Chapter 6 then is another big step forward. We presented the theoretical background of homogeneous estimation by introducing novel concepts like singular vector unbiasedness of random matrices and solved the problem of optimal estimation for correlated data. For instance, these results could be used for better estimation of local image orientation / optical flow (see section 7.2). At the end of this thesis, simulations and experiments for a few computer vision applications were presented; besides orientation estimation, especially the results for robust and constrained estimation for fundamental matrices is impressive. The novel algorithms are applicable for a lot of other applications not presented here, for instance camera calibration, factorization algorithm formulti-view structure from motion, or conic fitting. The fact that this work paved the way for a lot of further research is certainly a good sign.
The N-terminal domain (matrix protein or MA) of a retroviral Gag polyprotein precursor plays a critical role in several stages of the retrovirus life cycle. MA is involved in the effective membrane targeting, assembly and release of the immature viral particles from the infected cell. In order to understand the structural basis of these functions, the full length MA from Moloney Murine Leukemia Virus (MoMuLV) was purified and the solution structure of the MA MoMuLV was determined by means of heteronuclear high-resolution NMR spectroscopy and compared with that of the X-ray diffraction analysis as well as with the structures of several MA proteins from geterologous viruses. Structural features were also obtained from CD spectroscopy, dynamic light scattering, sedimentation velocity, differential scanning calorimetry and other methods. It was found that the MA MoMuLV globular core (residues 8-98) is comprised of 7 well-defined helices (five alpha-helices and two 310 helices), with the general fold typical for MA proteins from other retroviral species. The N-terminus (residues Met1-Leu7) and the C-terminal proline-rich part (residues Pro103-Tyr131) are not structured in solution. Although MA MoMuLV has a low sequence identity compared with other matrix proteins for which the three-dimensional structure is known, it was shown that its overall topology and pattern of secondary structural units is similar to other retroviral matrix proteins. The monomeric state is observed for the correctly folded MA MoMuLV in a variety of external conditions and protein concentrations, indicating that virion assembly starts with the plasma membrane targeting of the nascent Gag precursor. The denaturation of MA MoMuLV is irreversible and is connected with protein aggregation. For Moloney Murine Leukemia Virus (MoMuLV) a proteolytic processing of the R-peptide (last 16 amino acids from the C-terminus of the Envelope protein (Env)) has been described as a second mode of fusion and activation preceding the receptor contact between the viral particle and the cellular membrane. An interaction between the R-peptide and MA MoMuLV has been proposed, since the R-peptide and MA are localized at the inner part of the membrane. Therefore the interaction between 15N labelled purified MA MoMuLV and synthesized R-peptide has been investigated using high-resolution NMR. It was found that in water solution MA MoMuLV and R-peptide do not form a tight complex, but in a mature virion in the presence of membranes or other protein factors it might be possible. In the case of HIV-1 the cytoplasmic part (EnvC) of the Env protein is much longer than in other retroviruses and again as for MoMuLV little is known about the interaction between EnvC and HIV MA. Hence, the full length HIV MA, and the last 150 amino acids from HIV Env have been subcloned with suitable expression vectors, purified and analysed by native gel electrophoresis, a pull down assay and by high resolution NMR for the purpose to detect the complex formation of EnvC and HIV MA. Finally, after all those experiments, it was found that a stable complex is not formed, but a weak interaction between the two proteins can not be excluded.
I derive a general effective theory for hot and/or dense quark matter. After introducing general projection operators for hard and soft quark and gluon degrees of freedom, I explicitly compute the functional integral for the hard quark and gluon modes in the QCD partition function. Upon appropriate choices for the projection operators one recovers various well-known effective theories such as the Hard Thermal Loop/ Hard Dense Loop Effective Theories as well as the High Density Effective Theory by Hong and Schaefer. I then apply the effective theory to cold and dense quark matter and show how it can be utilized to simplify the weak-coupling solution of the color-superconducting gap equation. In general, one considers as relevant quark degrees of freedom those within a thin layer of width 2 Lambda_q around the Fermi surface and as relevant gluon degrees of freedom those with 3-momenta less than Lambda_gl. It turns out that it is necessary to choose Lambda_q << Lambda_gl, i.e., scattering of quarks along the Fermi surface is the dominant process. Moreover, this special choice of the two cutoff parameters Lambda_q and Lambda_gl facilitates the power-counting of the numerous contributions in the gap-equation. In addition, it is demonstrated that both the energy and the momentum dependence of the gap function has to be treated self-consistently in order to determine the imaginary part of the gap function. For quarks close to the Fermi surface the imaginary part is calculated explicitly and shown to be of sub-subleading order in the gap equation.
G protein-coupled receptors (GPCRs) play regulatory roles in many different physiological processes and they represent one of the most important class of drug targets. However, due to the lack of three-dimensional structures, structure based drug design has not been possible. The major bottleneck in getting three-dimensional crystal structure of GPCRs is to obtain milligram quantities of pure, homogenous and stable protein. Therefore, during my Ph.D. thesis, I focused on expression, characterization and isolation of three GPCRs namely human bradykinin receptor subtype 2 (B2R), human angiotensin II receptor subtype 1 (AT1aR), and human neuromedin U receptor subtype 2 (NmU2R). These receptors were heterologously produced in three different expression systems (i.e. Pichia pastoris, insect cells and mammalian cells), biochemically characterized and subsequently solubilized and purified for structural studies The human bradykinin receptor subtype 2 (B2R) is constitutively expressed in a variety of cells, including endothelial cells, vascular smooth muscle cells and cardiomyocytes. Activation of B2R is important in pathogenesis of inflammation, pain, tissue injury and cardioprotective mechanisms. During this study, recombinant B2R was produced in methylotrophic yeast Pichia pastoris (3.5 pmol/mg), insect cells (10 pmol/mg) and mammalian cells (60 pmol/mg). The recombinant receptor was characterized in terms of [3H] bradykinin binding, G protein coupling, localization, and glycosylation. Subsequently, it was solubilized and purified using affinity chromatography. Homogeneity and stability of purified B2R was monitored by gel filtration analysis. Milligram amounts of pure and stable receptor were obtained from BHK cells and Sf9 cells, which were used for three-dimensional crystallization attempts. The second receptor, which I worked on, is human angiotensin II receptor subtype 1 (AT1aR). AT1aR is distributed in smooth muscle cells, liver, kidney, heart, lung and testis. Activation of AT1aR is implicated in the regulation of blood pressure, hypertension and cardiovascular diseases. Recombinant AT1aR was produced at high levels in Pichia pastoris (167 pmol/mg), while at moderate levels in insect cells (29 pmol/mg) and mammalian cells (32 pmol/mg). The recombinant receptor was characterized in terms of [3H] angiotensin II binding, localization, and glycosylation. Subsequently, the receptor was solubilized and purified using affinity chromatography. Homogeneity and stability of purified AT1aR was monitored by gel filtration analysis. Milligram amounts of pure and stable receptor were obtained from Pichia pastoris, which were used for threedimensional crystallization attempts. In addition to B2R and AT1aR, I also attempted to produce and isolate the human neuromedin U receptor subtype 2 (NmU2R), which was deorphanized recently. It is found in highest abundance in the central nervous system, particularly the medulla oblongata, spinal cord and thalamus. The distribution of this receptor suggests its regulatory role in sensory transmission and modulation. During this study, recombinant NmU2R was produced in Pichia pastoris (6 pmol/mg) and BHK cells (9 pmol/mg). Recombinant receptor was characterized with regard to [125I] NmU binding, localization and glycosylation. Subsequently, the receptor was solubilized and purified using affinity chromatography. Due to its low expression level, further expression optimization is required in order to obtain milligram amounts for structural studies. The long-term goal of this study was to obtain three-dimensional crystal structure of recombinant GPCRs. However, 3-dimensional crystallization of human recombinant membrane proteins still remains a difficult task. On the other hand, recent advances in the solid-state NMR spectroscopy offer ample opportunities to study receptor-ligand systems, provided milligram quantities of purified receptor are available. Therefore, in parallel to 3-dimensional crystallization trials, purified B2R was also used for solid-state NMR analysis in order to investigate the receptor bound conformation of bradykinin. Preliminary results are promising and indicate significant structural changes in bradykinin upon binding to B2R. Further experiments are ongoing and will hopefully result in the structure of receptor bound bradykinin. One of the challenges in GPCR crystallization is the small hydrophilic surface area that is available to make crystal contacts. One possibility to overcome this problem can be the reconstitution of a GPCR complex with an interacting protein for cocrystallization. For this purpose, I coexpressed B2R and AT1aR, which form a stable heterodimer complex, in BHK cells. I could successfully isolate the heterodimer complex by using two-step affinity purification. Unfortunately, this complex was not stable over time and disassociates within three days of purification. However, during coexpression of B2R and AT1aR in BHK cells, I observed that B2R was localized in the plasma membrane in coexpressing cells while it was retained intracellularly when expressed alone. This coexpression of AT1aR with B2R resulted in a four-fold increase in [3H] bradykinin binding sites on the cell surface. In addition, these two receptors were cointernalized in response to their individual specific ligands. Interestingly, colocalization of B2R and AT1aR was also found in human foreskin fibroblasts (which endogenously express both receptors), in line with the possibility that heterodimerization may be required for surface localization of B2R in native tissues as well. This is the first report where surface localization of a peptide GPCR is triggered by a distantly related peptide GPCR. These data support the hypothesis that heterodimerization may be a prerequisite for cell surface localization of some GPCRs. A second approach that I followed to stabilize the purified B2R was to reconstitute the B2R-β-arrestin complex. β-arrestin is a cytosolic protein that participates in agonist mediated desensitization of GPCRs and therefore dampens the cellular responses initiated by the activation of GPCRs. I tried to reconstitute B2R-β-arrestin complex in vitro by mixing purified B2R and purified β-arrestin. But, no interaction of these two proteins was observed in the pull-down assays. However, a C-terminal mutant of B2R (where a part of the C-terminus of the B2R is exchanged with that of the vasopressin receptor) was found to interact with β-arrestin in vitro as revealed by pull-down assays. In conclusion, this work establishes the production, characterization and isolation of three recombinant human GPCRs. Recombinant receptors were produced in milligram amounts and therefore, pave the way for structural analysis. The heterodimer complex of B2R-AT1aR and B2R-β-arrestin complex can be of great help during crystallization. In addition, it was also found for the first time that the surface localization of a peptide GPCR can be triggered by heterodimerization with a distantly related peptide GPCR.
In the classical Dirac equation with strong potentials, called overcritical, a bound state reaches the negative continuum. In QED the presence of a static overcritical external electric field leads to a charged vacuum and indicates spontaneous particle creation when the overcritical field is switched on. The goal of this work is to clarify whether this effect exists, i.e. if it can be uniquely defined and proved, in time-dependent physical processes. Starting from a fundamental level of the theory we check all mathematical and interpretational steps from the algebra of fields to the very effect. In the first, theoretical part of this thesis we introduce the mathematical formulation of the classical and quantized Dirac theory with their most important results. Using this language we define rigorously the notion of spontaneous particle creation in overcritical fields. First, we give a rigorous definition of resonances as poles of the resolvent or the Green's function and show how eigenvalues become resonances under Hamiltonian perturbations. In particular, we consider essential for overcritical potentials perturbation of eigenvalues at the edge of the continuous spectrum. Next, we gather various adiabatic theorems and discuss well-posedness of the scattering in the adiabatic limit. Then, we construct Fock space representations of the field algebra, study their equivalence and give a unitary implementer of all Bogoliubov transformations induced by unitary transformations of the one-particle Hilbert space as well as by the projector (or vacuum vector) changes as long as they lead to unitarily equivalent Fock representations. We implement in Fock space self-adjoint and unitary operators from the one-particle space, discussing the charge, energy, evolution and scattering operators. Then we introduce the notion of particles and several particle interpretations for time-dependent processes with a different Fock space at every instant of time. We study how the charge, energy and number of particles change in consequence of a change of representation or in implemented evolution or scattering processes, what is especially interesting in presence of overcritical potentials. Using this language we define rigorously the notion of spontaneous particle creation. Then we look for physical processes which show the effect of vacuum decay and spontaneous particle creation exclusively due to the overcriticality of the potential. We consider several processes with static as well as suddenly switched on (and off) static overcritical potentials and conclude that they are unsatisfactory for observation of the spontaneous particle creation. Next, we consider properties of general time-dependent scattering processes with continuous switch on (and off) of an overcritical potential and show that they also fail to produce stable signatures of the particle creation due to overcriticality. Further, we study and successfully define the spontaneous particle creation in adiabatic processes, where the spontaneous antiparticle is created as a result of a resonance (wave packet) decay in the negative continuum. Unfortunately, they lead to physically questionable pair production as the adiabatic limit is approached. Finally, we consider extension of these ideas to non-adiabatic processes involving overcritical potentials and argue that they are the best candidate for showing the spontaneous pair creation in physical processes. Demanding creation of the spontaneous antiparticle in the state corresponding to the overcritical resonance rather quick than slow processes should be considered, with a possibly long frozen overcritical period. In the second part of this thesis we concentrate on a class of spherically symmetric square well potentials with a time-dependent depth. First, we solve the Dirac equation and analyze the structure and behaviour of bound states and appearance of overcriticality. Then, by analytic continuation we find and discuss the behaviour of resonances in overcritical potentials. Next, we derive and solve numerically (introducing a non-uniform continuum discretization for a consistent treatment of narrow peaks) a system of differential equations (coupled channel equations) to calculate particle and antiparticle production spectra for various time-dependent processes including sudden, quick, slow switch on and off of a sub- and overcritical potentials. We discuss in detail how and under which conditions an overcritical resonance decays during the evolution giving rise to the spontaneous production of an antiparticle. We compare the antiparticle production spectrum with the shape of the resonance in the overcritical potential. We study processes, where the overcritical potentials are switched on at different speed and are possibly frozen in the overcritical phase. We prove, in agreement with conclusions of the theoretical part, that the peak (wave packet) in the negative continuum representing a dived bound state partially follows the moving resonance and partially decays at every stage of its evolution. This continuous decay is more intensive in slow processes, while in quick processes the wave packet more precisely follows the resonance. In the adiabatic limit, the whole decay occurs already at the edge of the continuum, resulting in production of antiparticles with vanishing momentum. In contrast, in quick switch on processes with delay in the overcritical phase, the spectrum of the created antiparticles agrees best with the shape of the resonance. Finally, we address the question how much information about the time-dependent potential can be reconstructed from the scattering data, represented by the particle production spectrum. We propose a simple approximation method (master equation) basing on an exponential, decoherent decay of time-dependent resonances for prediction of particle creation spectra and obtain a good agreement with the results of full numerical calculations. Additionally, we discuss various sources of errors introduced by the numerical discretization, find estimations for them and prove convergence of the numerical schemes.