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Nuclear matter, that takes the form of protons and neutrons under normal conditions, is subject to a phase transition at high temperatures and densities, liberating the quarks and gluons that are usually confined in nucleons and creating a medium of free partons: the Quark-Gluon-Plasma. It is generally believed that this state of matter can be created in relativistic collisions of heavy nuclei. The study of the medium created in these collisions is the subject of heavy-ion physics. One topic within this field are particles with high transverse momentum, that are created in initial hard collisions between partons of the incoming nuclei. The energetic partons lose energy due to interactions with the medium before they fragment into a jet of hadrons. Due to momentum conservation, these jets are usually created as back-to-back pairs, or less commonly as three-jet or photon-jet events, where a single jet is balanced by a hard photon. The energy loss can be measured using correlations between particles with high transverse momenta. A trigger particle is selected with very high transversemomentum and the distribution of the azimuthal angle of associated particles in the same event is studied, relative to the azimuth of the trigger particle.These azimuthal correlations show a peak for opening angles around 0 from particles selected from the same jet, and a second peak at opening angles around 180 degrees from back-to-back di-jets. Random combinations with the underlying event generate a flat background, extending over the full range of opening angles. The STAR experiment observed a modification of these correlations in central Au+Au collisions, where trigger particles with 4GeV < pT(trigger) < 6GeV and associated particles with 2GeV < pT(trigger) < 4GeV were selected. A strong suppression has been observed for away-side correlations in central Au+Au collisions, relative to p+p, d+Au and peripheral Au+Au data. This can be explained by assuming two partons going in opposite directions, where at least one has to travel a large distance through the medium, causing energy loss and effectively removing the event from the analysis. For near-side correlations, no significant modification has been observed, which can be explained by surface emission, assuming that the observed jets have travelled only a short distance in themedium, not leaving enough time for interactions with the medium. Both trigger- and associated particles in a correlation analysis with charged hadrons are subject to modifications due to the medium. This can be avoided by using photon-jet events instead of di-jets, because the photon does not interact with the medium and therefore provides the best available measure of the properties of the opposite jet in the presence of the underlying event. This thesis studies azimuthal correlations between regions of high energy deposition in the electro-magnetic calorimeter as trigger- and charged tracks as associated particles. The data sample had been enriched by online event selection, allowing for the selection of trigger particles with a transverse energy of more than 10GeV and associated particles with more than 2,3 or 4 GeV. The away-side yield per trigger particle is strongly suppressed like in correlations between charged particles. The near-side yield is also reduced by about a factor two, clearly different from charged correlations. The trigger particles are a mixture of photon pairs from the decays of neutral pions and single photons, mainly from photon-jet events, with small contributions from other hadron decays and fragmentation photons. Pythia simulations predict a ratio of neutral pions to prompt photons of 3.5:1 in p+p collisions with the same cuts as in the presented analysis. Single particle suppression further reduces this ratio in central Au_Au collisions, down to about 0.8:1, indicating that the majority of trigger particles in central Au+Au collisions are prompt photons. The increasing fraction of prompt photon triggers without an accompanying jet and therefore zero associated yield reduces the average yield per trigger particle. The magnitude of the observed effect agrees well with the expectation from Pythia simulations and the assumption of a single particle suppression by a factor 4-5. An analysis of away-side correlations is more difficult, because both photon-jet and di-jet events contribute. The aim is the separation of these two contributions. As a clear separation is not possible with the available dataset, a comparison with two different scenarios is given, where a surprisingly small suppression by only a factor of about 5 is favoured for both dijet- and photon-jet-correlations. A separate measurement of both contributions will be possible by a shower-shape analysis with the EM calorimeter or a comparison with charged correlations in the same kinematic region.
This thesis is concerned with the derivation of new methods for the analysis of nonstationary, cross correlated panels. The suggested procedures are carefully quantified by means of Monte Carlo experiments. Typical applications of the developed methods consist in multi-country studies, with several countries observed over a couple of decades. The empirical applications implemented here are the testing for trends in the investment share in European GDPs and the examination of OECD interest rates. In the first chapter, a panel test for the presence of a linear time trend is proposed. The test is applicable in cross-correlated, heterogeneous panels and it can also be used when the integration order of innovations is unknown, by means of subsampling. In the next chapter a cointegration test having asymptotic standard normal distributiun and not requiring exogeneity assumptions is derived. In panels exhibiting cross-correlation or cointegration, individual test statistics are asymptotically independent, which leads to a panel test statistic robust to dependence across units. The third chapter examines in an econometric context the simple idea of combining p-values from a series of statistical tests and improves its applicability in the presence of cross-correlation. The last chapter applies recent panel techniques to OECD long-term interest rates and differentials thereof, finding only rather week evidence in favor of stationarity when allowing for cross-correlation.
Unlimited self-renewal is an absolute prerequisite for any malignancy, and is the ultimate arbiter of the continuous growth and metastasis of tumors. It has been suggested that the self-renewal properties of a tumor are exclusively contained within a small population, i.e., the so-called cancer stem cells. Enhanced self-renewal potential plays a pivotal role in the development of leukemia. My data have shown that APL associated translocation products PML/RARalpha and PLZF/RARalpha increased the replating efficiency of mouse lin-/Sca1+ hematopoietic stem cells (HSCs). This effect is partly mediated by induction of gamma–catenin which is an important mediator of the Wnt signaling pathway and has been shown to be up regulated by the AML associated translocation products(AATPs). Suppression of gamma–catenin by siRNA can abrogate the increased replating efficiency induced by AATPs. Transduction of gamma–catenin in lin-/Sca1+ HSCs led to increased replating efficiency and the expression of stem cell markers Sca1 and c-kit. Additionally it induced accelerated cell cycle progression of mouse bone marrow HSCs. Transduction/transplantation mouse models have shown that ectopic expression of gamma–catenin in HSCs led to acute myeloid leukemia without maturation. These data suggest important roles of Wnt signaling pathway in the leukemogenesis induced by PML/RARalpha, PLZF/RARalpha and AML1/ETO. In contrast to AATPs, CML and Ph+-ALL associated translocation products p185(BCR-ABL) and p210(BCR-ABL) did not affect the self-renewal potential of hematopoietic stem/progenitor cells. However my studies indicated that their reciprocal translocation products p40(ABL/BCR) and p96(ABL/BCR) actually increased the replating efficiency of hematopoietic stem/progenitor cells. The effect is stronger when induced by p96(ABL/BCR) than by p40(ABL/BCR). It is very intriguing that p96(ABL/BCR) can activate Wnt signaling and up regulate the expression of HoxB4. Transduction/transplantation mouse model has shown that p40(ABL/BCR) and p96(ABL/BCR) both have their own leukemogenic potential. Given the fact that leukemic stem cells maintain the growth of tumor and are the origin of relapse, the cure of leukemia is dependent on the eradication of the leukemic stem cell and abrogation of aberrantly regulated self-renewal capability. Both t-RA and As2O3 have been shown to induce complete remission in APL patients with PML/RARalpha translocation product. However, t-RA as a single agent achieves completeremission (CR) but not complete molecular remissions (CMR). Therefore, virtually all patients will experience a relapse within a few months. In contrast to t-RA, As2O3 as a single agent is able to induce CR as well as CMR followed by long-term relapse-free survival in about 50% of APL patients even if relapsed after treatment with t-RA-containing chemotherapy regimens. Nothing is known about the mechanisms leading to the complete different clinical outcomes by the two compounds although both have been shown to induce differentiation of blast cells, proliferation arrest, induction of apoptosis and degradation of PML/RARalpha. We investigated the effect of t-RA and arsenic on PML/RARalpha-expressing cell population with stem cell capacity derived from the APL cell line NB4 as well as Sca1+/lin- murine bone marrow cells. We found that t-RA did not reduce the replating efficiency in PML/RARalpha- and PLZF/RARalpha-infected Sca1+/lincells whereas it selected small compact colonies representing very early progenitor cells. T-RA was unable to reduce the capacity to form colony forming units-spleen (CFU-S) of Sca1+/lin-cells expressing PML/RARalpha, additionally t-RA did not impair the capability of engraftment of NB4 cells in NOD/SCID mouse. On the contrary to t-RA, As2O3 abolished the aberrant self-renewal potential of Sca1+/lin- cells expressing PML/RARalpha. As2O3 not only abolished the replating efficiency of PML/RARalpha positive cells but also completely abrogated the ability of PML/RARalpha-positive HSC to produce CFU-S in vivo. On the contrary to As2O3, t-RA increased the absolute cell number and the percentage of cells in the side population with respect to the whole cell population in NB4 cells. Taken together these data suggest that arsenic but not all-trans retinoic acid overcomes the aberrant stem cell capacity of PML/RARalpha positive leukemic stem cells. My data prove for the first time that there is a direct relationship between the capacity of compounds to effectively target the LSC and their capacity to eradicate the leukemia, and, thereby, to induce complete molecular remission and long-term relapse-free survival. Thus, in order to increase the curative potential of leukemia therapies, future studies need to include the effect of given compounds on the stem cell compartment to determine their ability to eradicate the LSC.
A new technique for precision ion implantation has been developed. A scanning probe has been equipped with a small aperture and incorporated into an ion beamline, so that ions can be implanted through the aperture into a sample. By using a scanning probe the target can be imaged in a non-destructive way prior to implantation and the probe together with the aperture can be placed at the desired location with nanometer precision. In this work first results of a scanning probe integrated into an ion beamline are presented. A placement resolution of about 120 nm is reported. The final placement accuracy is determined by the size of the aperture hole and by the straggle of the implanted ion inside the target material. The limits of this technology are expected to be set by the latter, which is of the order of 10 nm for low energy ions. This research has been carried out in the context of a larger program concerned with the development of quantum computer test structures. For that the placement accuracy needs to be increased and a detector for single ion detection has to be integrated into the setup. Both issues are discussed in this thesis. To achieve single ion detection highly charged ions are used for the implantation, as in addition to their kinetic energy they also deposit their potential energy in the target material, therefore making detection easier. A special ion source for producing these highly charged ions was used and their creation and interactions with solids of are discussed in detail.
In the present work we applied the Optically read out PArticle track Chamber, OPAC, for the measurement of radial dose distributions, d(r), around tracks of heavy ions passing through the gas-filled sensitive volume of the chamber. The measured data were compared with d(r) functions derived from data calculated with the Monte Carlo particle transport code, TRAX – which is used for the heavy ion therapy planning at GSI. To measure this quantity we have used here an optically read out time projection chamber (OPAC) with a parallel-drift field and one or several electron and light amplification stages. The two dimensional projection of the three dimensional ionization pattern caused by the ionizing particle passing through the chamber is captured by an image intensified CCD camera. The work is motivated by the role the radial dose distribution plays in the estimation of the relative biological effectiveness (RBE) of heavy ions, e.g. in radiation therapy and in radiation protection. The most successful model for high-dose irradiation with ions (applicable e.g. for heavy ion therapy) is found to be the local effect model (LEM). The present work intends to deliver measured data for one of the basic physical parameters which serve as input for the application of the local effect model: the radial dose distribution, d(r). The first goal of our measurement program was the measurement of d(r) distributions around carbon ions of different energies from 400 MeV/u down to the Bragg peak regions. We found an excellent agreement between the measured and simulated distributions at all carbon energies for the r–range in which the measurements deliver useful results. The lower limit of this range is about 100 nm and the upper limit is 6000 nm at a resolution of down to 33 nm - if scaled to water density. Despite the simplifications in the TRAX code (e.g. binary encounter theory for the emission ionization electrons), the discrepancies between the simulated and measured d(r) distributions are found to be lower than the measurement uncertainties at most measured carbon ion energies in almost the whole observed r-range. Hence, within the limitations of our measurements we can conclude that the precision of TRAX is sufficient to simulate the d(r) distributions around carbon ions to serve as input parameter for therapy planning. However, this conclusion is only valid for larger radial distances (r >100 nm). For smaller radial distances the measured data are dominated by the diffusion. Apart from carbon ion tracks, tracks of very heavy ions (40Ar, 84Kr and 238U) were also measured with OPAC. The simulated d(r) values were typically slightly or significantly higher than the measured data in the 100 nm < r < 5000 nm region. The experience has shown: the heavier or the faster the ion, the higher the discrepancies. On the one hand, we found a surprisingly good agreement between measurements and simulations if the ions had energies of around 50 MeV/u (i.e. relatively low energy). On the other hand, at higher energies, simulated data underestimate the measured ones by up to a factor of two in the region of 100 nm < r < 1000 nm for 84Kr (E = 650 MeV/u) or in the region of 100 nm < r < 6000 nm for 238U (E = 1 GeV/u). A possible reason for these discrepancies is that the BEA model, used in TRAX for the production ionization electrons, is not adequate for very heavy projectiles. The energy values of the very heavy ions were selected with the aim of comparing the track structures - and namely the d(r) distributions - of ions with largely different atomic mass but similar LET values. From the Z-dependency of the stopping power we know that for heavier ions a higher specific ion energy (expressed in MeV/u) is required to provide the same LET. For example the common LET of 315 keV/micro-m was achieved at largely different specific energy levels of 4,4 MeV/u for 12C, 65 MeV/u for 40Ar and 650 MeV/u for 84Kr ions. The difference in the track structures was expected mainly due to the different ion velocities and thus e.g. different ranges of d-electrons. This expectation could be confirmed by the measurements. The reason why - in line with the simulations - no strong differences could be observed in the d(r) distributions of the argon and krypton ions is the relatively small difference in the velocities of the both ion types in conjunction with the limited range in r, where the data can be compared. In contrary, the d(r) function of the carbon ion shows a qualitatively different behavior than the heavier ions inside the observable radius-range - in agreement with the simulations.
Die vorliegende Arbeit beschäftigt sich mit der BFV-Reduktion von Hamiltonschen Systemen mit erstklassigen Zwangsbedingungen im Rahmen der klassischen Hamiltonschen Mechanik und im Rahmen der Deformationsquantisierung. Besondere Aufmerksamkeit wird dabei Zwangsbedingungen zuteil, die als Nullfaser singulärer äquivarianter Impulsabbildungen entstehen. Es ist schon länger bekannt, daß für Nullfasern regulärer äquivarianter Impulsabbildungen die in der theoretischen Physik gebräuchliche Methode der BFV-Reduktion zur Phasenraumreduktion nach Marsden/Weinstein äquivalent ist. In [24] konnte gezeigt werden, daß in dieser Situation die BFV-Reduktion sich auch im Rahmen der Deformationsquantisierung natürlich formulieren läßt und erfolgreich zur Konstruktion von Sternprodukten auf Marsden/Weinstein-Quotienten verwendet werden kann. Ein Hauptergebnis der vorliegenden Arbeit besteht in der Verallgemeinerung der Ergebnisse aus [24] auf den Fall singulärer Impulsabbildungen, deren Komponenten 1.) das Verschwindungsideal der Zwangsfläche erzeugen und 2.) einen vollständigen Durchschnitt bilden. Die Argumentation von [24] wird durch Gebrauch der Störungslemmata aus dem Anhang A.1 systematisiert und vereinfacht. Zum Existenzbeweis von stetigen Homotopien und stetiger Fortsetzungsabbildung für die Koszulauflösung werden der Zerfällungssatz und der Fortsetzungssatz von Bierstone und Schwarz [20] benutzt. Außerdem wird ein ’Jacobisches Kriterium’ für die Überprüfung von Bedingung 2.) angegeben. Basierend auf diesem Kriterium und Techniken aus [3] werden die Bedingungen 1.) und 2.) an einer Reihe von Beispielen getestet. Als Korollar erhält man den Beweis dafür, daß es symplektisch stratifizierte Räume gibt, die keine Orbifaltigkeiten sind und dennoch eine stetige Deformationsquantisierung zulassen. Ferner wird (ähnlich zu [92]) eine konzeptionielle Erklärung dafür gegeben, warum im Fall vollständiger Durchschnitte das Problem der Quantisierung der BRST-Ladung eine so einfache Lösung hat. Bildet die Impulsabbildung eine erstklassige Zwangsbedingung, ist aber kein vollständiger Durchschnitt, dann ist es im allgemeinen nicht bekannt, wie entsprechende Quantenreduktionsresultate zu erzielen sind. Ein Hauptaugenmerk der Untersuchung wird es deshalb sein, in dieser Situation die klassische BFV-Reduktion besser zu verstehen – natürlich in der Hoffnung, Grundlagen für eine etwaige (Deformations-)Quantisierung zu liefern. Wir werden feststellen, daß es zwei Gründe gibt, die Tate-Erzeuger (alias: Antigeister höheren Niveaus) notwendig machen: die Topologie der Zwangsfläche und die Singularitätentheorie der Impulsabbildung. Die Zahl der Tate-Erzeuger kann durch Übergang zu projektiven Tate-Erzeugern, also Vektorbündeln, verringert werden. Allerdings sorgt Halperins Starrheitssatz [57] dafür, daß im wesentlichen alle Fälle, für die die Zwangsfläche kein lokal vollständiger Durchschnitt ist, zu unendlich vielen Tate-Erzeugern führen. Erzeugen die Komponenten einer Impulsabbildung einer linearen symplektischen Gruppenwirkung das Verschwindungsideal der Zwangsfläche, so kann man eine lokal endliche Tate-Auflösung finden. Diese besitzt nach dem Fortsetzungssatz und dem Zerfällungssatz von Bierstone und Schwarz stetige, kontrahierende Homotopien. Ausgehend von einer solchen Tate-Auflösung konstruieren wir, die klassische BFV-Konstruktion für vollständige Durchschnitte verallgemeinernd, eine graduierte superkommutative Algebra. Wir können zeigen, daß diese graduierte Algebra auch im Vektorbündelfall eine graduierte Poissonklammer besitzt, die sogenannte Rothstein-Poissonklammer. Die Existenz einer solchen Poissonklammer war bereits von Rothstein [87] für die einfachere Situation einer symplektischen Supermannigfaltigkeit bewiesen worden. Darüberhinaus werden wir sehen, daß es auch im Vektorbündelfall eine BRST-Ladung gibt. Diese sieht im Fall von Impulsabbildungen etwas einfacher aus als für allgemeine erstklassige Zwangsbedingungen. Insgesamt wird also die klassische BFV-Konstruktion [95] auf den Fall projektiver Tate-Erzeuger verallgemeinert, und als eine Homotopieäquivalenz in der additiven Kategorie der Fréchet-Räume interpretiert.
In this thesis, I study the phase diagram of dense, locally neutral three-flavor quark matter as a function of the strange quark mass, the quark chemical potential, and the temperature, employing a general nine-parameter ansatz for the gap matrix. At zero temperature and small values of the strange quark mass, the ground state of quark matter corresponds to the color–flavor-locked (CFL) phase. At some critical value of the strange quark mass, this is replaced by the recently proposed gapless CFL (gCFL) phase. I also find several other phases, for instance, a metallic CFL (mCFL) phase, a so-called uSC phase where all colors of up quarks are paired, as well as the standard two-flavor color-superconducting (2SC) phase and the gapless 2SC (g2SC) phase. I also study the phase diagram of dense, locally neutral three-flavor quark matter within the framework of a Nambu–Jona-Lasinio (NJL) model. In the analysis, dynamically generated quark masses are taken into account self-consistently. The phase diagram in the plane of temperature and quark chemical potential is presented. The results for two qualitatively different regimes, intermediate and strong diquark coupling strength, are presented. It is shown that the role of gapless phases diminishes with increasing diquark coupling strength. In addition, I study the effect of neutrino trapping on the phase diagram of dense, locally neutral three-flavor quark matter within the same NJL model. The phase diagrams in the plane of temperature and quark chemical potential, as well as in the plane of temperature and leptonnumber chemical potential are presented. I show that neutrino trapping favors two-flavor color superconductivity and disfavors the color–flavor-locked phase at intermediate densities of matter. At the same time, the location of the critical line separating the two-flavor color-superconducting phase and the normal phase of quark matter is little affected by the presence of neutrinos. The implications of these results for the evolution of protoneutron stars are briefly discussed.
Eine große Zahl natürlicher sekundärer Metabolite sind kleine und strukturell oft sehr verschiedene Polypeptide und Polyketide. Diese bioaktiven Substanzen haben im allgemeinen ein breit aufgestelltes therapeutisches Potential und werden von verschiedenen bakteriellen Stämmen und Pilzen biosynthetisiert. Sie sind sowohl biologisch, als auch therapeutisch wichtig als Cytostatika, Immunsuppressiva und Antibiotika mit einem sehr großen antibakteriellen und antiviralen Potential. Diese oft äußerst komplexen Polypeptide und Polyketide werden von modular aufgebauten Megaenzymen in mehrstufigen Mechanismen synthetisiert. Für die Synthese dieser Peptide sind sehr große Proteincluster verantwortlich, die meistens aus einer begrenzten Anzahl sehr großer, Multidomänen umfassenden, Superenzyme aufgebaut werden. Diese Proteincluster mit einem Molekulargewicht bis in den Bereich von MegaDalton werden als nicht-ribosomale Peptidsynthetasen (NRPS) und Polyketidsynthetasen (PKS) bezeichnet. Die NRPS Systeme zeichnen sich dadurch aus, daß für die biosynthetisierten Polypeptide keine Information in Form von Nukleinsäuren wie DNA oder RNA kodiert (Walsh, C.T., 2004; Sieber & Marahiel, 2005). Für die Synthese der Polypeptide ist eine Aktivierung der einzelnen Bausteine, der Aminosäuren, durch Amino-acyl-adenylierung notwendig. Im Anschluß an die Aktivierung, wird die aktivierte Aminosäure über einen Thioester gebunden weitertransportiert. Die Thioesterbildung erfolgt an Cysteaminthiolgruppen intrinsischer 4’-Phosphopantethein-kofaktoren. Eine Modul einer NRPS stellt eine geschlossene Einheit zum Einbau einer Aminosäure mit einer hohen Spezifität für das Substrat und die biosynthetische Reaktion dar. Diese Module sind aus Domänen aufgebaut, die definierte Funktionen haben und mittels flexibler Linker miteinander verbunden sind. Die Domänen werden nach ihrer Funktion unterschieden. Die Acyl-adenylierung oder Aktivierung eines Substrates, beispielsweise einer Aminosäure, erfolgt durch die A-Domänen. Die Peptidyl- oder Acyltransportfunktion der aktivierten Substrate wird durch Thioester-domänen (T-Domäne), auch PCP (peptidyl carrier domain) genannt, bewältigt. Die Biosynthese der Kopplungsreaktion, beispielsweise die Ausbildung der Peptidbindung in NRPS Systemen, erfolgt an den Kondensations-Domänen (C-Domäne). Für die Substratspezifität eines Synthesemoduls sind die A-Domänen verantwortlich, welche die Aktivierung eines Substrat durch ATP-Hydrolyse ermöglichen. In NRPS Systemen sind auch Zyklisierungsreaktionen, durchgeführt von Cyclase-Domänen (Cy-Domänen), L/D-Epimerase-funktionen (E-Domänen) und N-Methylierungen (M-Domänen) beschrieben. So wird in Tyrocidin A an zwei Positionen spezifisch Phenylalanin in die D-Form epimerisiert und anschließend in der Peptidbiosynthese verwendet. Die Interaktion und Erkennung zwischen den multi-modularen Superenzymen, zum korrekten Aufbau der kompletten Synthetase, wurden in letzter Zeit Kommunikations-Domänen (COM-Domänen) beschrieben. Wie die aufgebaute Synthetase die korrekte Sequenz der biosynthetischen Reaktionsschritte sicherstellt ist nicht bekannt. Die enorme Diversität biosynthetischer Reaktionen in NRPS Systemen und die hohe Substratvielfalt in den verschiedensten Synthetasen unterschiedlicher Stämme eröffnet ein weites Feld für mögliche Neukombinationen von Modulen und Modifikationen von Produkten, um neue bioaktive Polypeptide mit antibiotischen Eigenschaften durch die Gestaltung neuer biosynthetischer Reaktionswege zu erhalten. Die Biosyntheseprodukte der NRPS und PKS Systeme lassen sich Gruppen kategorisieren wie Peptidantibiotika, beispielsweise beta-Lactame und makrozyklischer Polypeptide. Weitere Gruppen sind die makrozyklischen Lactone, beispielsweise Polyene und Makrolide, aromatische Verbindungen, wie Chloramphenicol, und Chinone (Tetracyclin). Die näher diskutierten Beispiele sind die antibakteriellen Polypeptide Surfactin und Tyrocidin A. Surfactin ist ein antibakteriell wirkendes makrozyklisches Lipoheptapeptid, welches von Bacillus subtilis synthetisiert wird und ein enormes antivirales Potential besitzt. Tyrocidin A ist ein antibakteriell wirkendes makrozyklisches Decapeptid und wird von Bacillus brevis und Brevisbacillus parabrevis synthetisiert. Zusätzlich werden viele bakterielle Toxine ebenfalls durch solche Systeme multi-modularer Synthetasen erzeugt. Ein Beispiel ist das Polyketid Vibriobactin, das Toxin des humanpathogenen Bakterium Vibrio cholerae. Ein zunehmendes Problem der wachsenden Weltbevölkerung moderner Gesellschaften und in den Entwicklungsländern ist die wachsende Zahl multiresistenter Bakterienstämme. Die starke Progression in der Entwicklung von Resistenzen gegen Antibiotika ist auch Gegenstand des aktuellen WHO-Reports (2006). Alarmierend ist die beschleunigte Resistenzentwicklung gegen die sogenannten Reserveantibiotika Vancomycin und Ceftazidim. Ein umfangreicheres Verständnis der Interaktion zwischen Domänen in einem Modul und zwischen Modulen eines NRPS Systems ist Grundlage für die Neukombination unterschiedlicher Module zur erfolgreichen Gestaltung neuer Biosynthesen. Da die meisten dieser Biosynthesen oder die Synthese alternativer Substanzen nicht in der Organischen Chemie zu realisieren sind oder die Produkte zu teuer wären, um diese in großen Mengen zu erzeugen, muß das Ziel sein die NRPS und PKS Systeme in ihrem modularen Aufbau und ihre Interaktion zu verstehen, um alternative Antibiotika biosynthetisch herzustellen. Peptidyl Carrier Proteine (PCPs) sind kleine zentrale Transport-Domänen, integriert in den Modulen nicht-ribosomaler Peptidsynthetasen (NRPSs). PCPs tragen kovalent über eine Phosphoesterbindung einen aus dem Protein herausragenden 4’-phosphopantetheinyl (4’-PP) Kofaktor. Der 4’-PP Kofaktor ist an der Seitenkette eines hochkonservierten Serins gebunden, welche ein zentraler Bestandteil der Phosphopantethein-Erkennungs-Sequenz ist. Die Erkennungssequenz ist homolog in vielen Proteinen mit ähnlicher Funktion, inklusive Acyl Carrier Proteinen (ACPs) der Fettsäuresynthetasen (FAS) und der Polyketidsynthetasen (PKS). Die Thiolgruppe des 4’-PP Kofaktors dient zum aktiven Transport der Substrate und der Intermediate der NRPS Systeme. Die generelle Organisation und die Kontrolle der exakt aufeinander folgenden Reaktionsschritte in der Peptidsynthetase, ist die entscheidende Frage für die Funktion des Proteinclusters (assembly line mechanism). In Modulen der NRPS Systeme folgen die PCP-Domänen C-terminal auf die Adenylierungsdomänen (A-Domäne). Die Aufgabe der A-Domänen ist die Selektion and die Aktivierung einer spezifischen Aminosäure für die „assembly line“. Die eigentliche Bildung der Peptidbindung erfolgt an der Kondensations-Domäne (C-Domäne). Der Transfer der Peptidintermediate und der aktivierten Aminosäuren zwischen A-Domänen und C-Domänen ist Aufgabe der PCPs. Um diese Funktion erfüllen zu können, ist eine große Bewegung in PCPs, bzw. des 4’-PP Kofaktors notwendig, welche als „swinging arm model“ (Weber et al., 2001) beschrieben wurde. Die PCPs koordinieren damit die Peptidbiosynthese während sie mit diversen Domänen der Synthetasen spezifisch wechselwirken müssen. Die molekularen Mechanismen des Transportes wurden bisher allerdings nicht untersucht. Eine Dynamik der Transport-Domänen wurde bereits postuliert (Kim & Prestegard, 1989; Andrec et al., 1995), konnte bisher aber nicht gezeigt werden (Weber et al., 2001). Interessanterweise zeigt sowohl apo-PCP (ohne den kovalent gebundenen 4’-PP Kofaktor) also auch holo-PCP langsamen chemischen Austausch, der als jeweils zwei stabile Konformationen beschrieben werden konnte. Diese jeweils zwei stabilen Zustände, welche sich im Austausch befinden, wurden als A und A*, für apo-PCP, und entsprechend H und H* für holo-PCP bezeichnet. Während der A- und der H-Zustand sich sowohl voneinander als auch von den entsprechenden A* und H*-Zuständen unterscheiden und spezifisch für die apo- und die holo-Form von PCP sind, ist die kalkulierte Struktur vom A*-Zustand größten Teils identisch mit der des H*-Zustandes. Die erhaltenen NMR-Strukturen des A-Zustandes, des H-Zustandes und des gemeinsamen A/H-Zustandes beschreiben in ihrer Gesamtheit ein neues Modell für ein allosterie-kontrolliertes System dualer konformationeller Zwei-Zustands-Dynamik. Zu dem beobachteten konformationellen Austausch der PCP-Domäne, konnte die Bewegung des 4’-PP Kofaktors koordiniert werden. Die Bewegung des 4’-PP Kofaktors in Verbindung mit dem konformationellen Austausch der PCP-Domäne charakterisiert die Interaktion mit katalytischen Domänen eines NRPS Moduls. Des weiteren konnte mit Hilfe des Modells die Wechselwirkung mit externen Interaktionspartnern, wie der Thioesterase II und der 4’-PP Transferase, untersucht werden. Die externe Thioesterase II der Surfactin-Synthetase (SrfTEII) von Bacillus subtilis ist ein separat expremiertes 28 KDa Protein. Sie gehört zur Familie der alpha/beta-Hydrolasen und ist verantwortlich für die Regenerierung falsch beladener 4’- PP Kofaktoren der Peptidyl Carrier Domänen. Die SrfTEII wurde mittels Lösungs-NMR untersucht, die Resonanzen wurden zugeordnet, erste strukturelle Modelle konnte berechnet werden und das Interaktionsverhalten mit verschiedenen modifizierten Kofaktoren und PCPs wurde analysiert. Die Spezifität der Substraterkennung durch die SrfTEII kann beschrieben werden. Interessanterweise zeigt auch die SrfTEII Doppelpeaks für einzelne Aminosäuren, diese können als Indikator für eine spezifische Substraterkennung durch das Enzym verwendet werden und helfen den funktionellen Unterschied zwischen der SrfTEI-Domäne und SrfTEII zu verstehen.
Customer channel migration
(2006)
Customer Channel Migration deals with the active management of a customer's channel usage behavior with the aim to increase her profitability and lifetime. Hence, the dissertation answers two distict questions: on one hand, it investigates the impact of channel use on a customer's profitability and lifetime. On the other hand, it is researched how a customer's channel usage behavior can be influenced and managed. The cumulative dissertation consists of five articles: the first article describes the matching method and its application to marketing problems. The matching method is necessary to estimate the unbiased impact of channel use on a customer's profitability and lifetime. The second article describes the application of the matching method in order to determine the monetary implications of using the internet in the financial services industry. The third article investigates the impact of the internet use on a customer's lifetime. The forth and the fifth article of the dissertation both investigate the management of a customer's channel usage behavior. The forth article designs a scale to measure a customer's perceived channel value. The fifth article builds upon these findings and develops a model which explains a customer's channel usage behavior. Based on these insights this article derives some managerial implications on how to manage customers between different channels.
In the first part of the present work (Chapter 3), EPR spectroscopy at different microwave frequencies, namely at 9 GHz (X-band), 34 GHz (Q-band) and 180 GHz (G-band), was employed to resolve the g-values and the HFCs of a putative radical intermediate involved in the reduction of benzoyl-CoA catalyzed by benzoyl-CoA reductase. In particular, the effect of 33S-labeling on the EPR line shape was studied at X- and Q-band frequencies in order to gain further evidence for a sulfur centered radical proposed to be the electron donor in the reduction or the aromatic ring of BCoA [I]. The spectral components observed at X-, Q- and G-band were overall consistent and showed at least three overlapping EPR signals. The signal postulated to be due to a disulfide radical anion showed no resolved g-values and a relaxation behaviour faster than expected for such a radical species. These observations together with the simulations suggest that the signal could arise from a radical exchange coupled to an [4Fe-4S] cluster located nearby. In the future, pulsed EPR and ENDOR spectroscopy on the 57Fe-labeled enzyme could help to solve this question. The potential of high-field ENDOR in combination with 13C- and 31P-labeling for investigating the structure at the active site in proteins could be verified in the studies of the ligation sphere of the cofactor Mn2+ in Ras as reported in Chapter 4 [2]. Therein, high-field ENDOR performed at 94 GHz (W-band) was used to detect the hyperfine interactions between the electron spin mainly located on the metal ion and the phosphorous nuclei of the bound GDP and GppNHp as well as the carbon nuclei of bound amino acids in the wild-type Ras protein and its oncogenic mutant G12V. These studies aimed at searching for an additional free phosphate ion or amino acid ligand bound to the metal center in the wild type GDP-bound protein with respect to its oncogenic mutant. Rom the 13C- and 31P-ENDOR spectra, the hyperfine couplings of directly bound amino acids and the bound nucleotides were compatible with the hyperfine couplings obtained from DFT calculations based on the crystal structure data. No differences in the 13C- and 31P-ENDOR spectra could be found for the wild-type GDP-bound protein in comparison to its oncogenic mutant in frozen solution. Therefore, no evidence for binding of an additional free phosphate ion or amino acid ligand in the wild-type GDP-bound protein was found. The distances between the detected nuclei and the meta1 ion were in agreement with the ones extracted from crystal structures reported in the literature. Future 35C1-ENDOR studies could clarify whether a chloride ion from the buffer solution could be the ligand replacing one water molecule in the wild type GDP-bound Ras. In Chapter 5, the implementation of a high-field ENDOR setup into a homebuilt pulsed EPR spectrometer operating at 180 GHz is reported and its performance for 1H-ENDOR demonstrated on the model system BDPA. Mims and Davies ENDOR spectra were also obtained for Ras(wt).Mn2+.DP. The increased nuclear Zeeman resolution at 180 GHz may be further exploited in the future by extending the setup for studying hyperfine couplings of low-y nuclei such as 33S, 15N , 17O or 2H. In the present work, the advantages of performing EPR and ENDOR experiments at high fields and frequencies could be nicely demonstrated with the 94 GHz ENDOR studies of Ras. Furthermore, the complementing information obtained at X- and Q-band frequencies in the multifrequency EPR studies on BCR demonstrated that the analysis of EPR spectra can be greatly facilitated by simulating the spectra measured at different MW frequencies with the same set of parameters consistent with a proposed radical. Overall, it could be shown that the use of different experimental techniques at multiple fields and frequencies renders EPR spectroscopy a powerfull tool for structural studies in biological systems.