Simulation studies of correlation functions and relaxation in polymeric systems

We investigate the statics and dynamics of a glassy,non-entangled, short bead-spring polymer melt with moleculardynamics simulations. Temperature ranges from slightlyabove the mode-coupling critical temperature to the liquidregime where features of a glassy liquid are absent. Ouraim is to work out the polymer specific effects on therelaxation and particle correlation. We find the intra-chain static structure unaffected bytemperature, it depends only on the distance of monomersalong the backbone. In contrast, the distinct inter-chainstructure shows pronounced site-dependence effects at thelength-scales of the chain and the nearest neighbordistance. There, we also find the strongest temperaturedependence which drives the glass transition. Both the siteaveraged coupling of the monomer and center of mass (CM) andthe CM-CM coupling are weak and presumably not responsiblefor a peak in the coherent relaxation time at the chain'slength scale. Chains rather emerge as soft, easilyinterpenetrating objects. Three particle correlations arewell reproduced by the convolution approximation with theexception of model dependent deviations. In the spatially heterogeneous dynamics of our system weidentify highly mobile monomers which tend to follow eachother in one-dimensional paths forming ``strings''. Thesestrings have an exponential length distribution and aregenerally short compared to the chain length. Thus, arelaxation mechanism in which neighboring mobile monomersmove along the backbone of the chain seems unlikely.However, the correlation of bonded neighbors is enhanced. When liquids are confined between two surfaces in relativesliding motion kinetic friction is observed. We study ageneric model setup by molecular dynamics simulations for awide range of sliding speeds, temperatures, loads, andlubricant coverings for simple and molecular fluids. Instabilities in the particle trajectories are identified asthe origin of kinetic friction. They lead to high particlevelocities of fluid atoms which are gradually dissipatedresulting in a friction force. In commensurate systemsfluid atoms follow continuous trajectories for sub-monolayercoverings and consequently, friction vanishes at low slidingspeeds. For incommensurate systems the velocity probabilitydistribution exhibits approximately exponential tails. Weconnect this velocity distribution to the kinetic frictionforce which reaches a constant value at low sliding speeds. This approach agrees well with the friction obtaineddirectly from simulations and explains Amontons' law on themicroscopic level. Molecular bonds in commensurate systemslead to incommensurate behavior, but do not change thequalitative behavior of incommensurate systems. However,crossed chains form stable load bearing asperities whichstrongly increase friction.

The massless two-loop two-point function and zeta functions in counterterms of Feynman diagrams

The main part of this thesis describes a method of calculating the massless two-loop two-point function which allows expanding the integral up to an arbitrary order in the dimensional regularization parameter epsilon by rewriting it as a double Mellin-Barnes integral. Closing the contour and collecting the residues then transforms this integral into a form that enables us to utilize S. Weinzierl's computer library nestedsums. We could show that multiple zeta values and rational numbers are sufficient for expanding the massless two-loop two-point function to all orders in epsilon. We then use the Hopf algebra of Feynman diagrams and its antipode, to investigate the appearance of Riemann's zeta function in counterterms of Feynman diagrams in massless Yukawa theory and massless QED. The class of Feynman diagrams we consider consists of graphs built from primitive one-loop diagrams and the non-planar vertex correction, where the vertex corrections only depend on one external momentum. We showed the absence of powers of pi in the counterterms of the non-planar vertex correction and diagrams built by shuffling it with the one-loop vertex correction. We also found the invariance of some coefficients of zeta functions under a change of momentum flow through these vertex corrections.

Synthese, Evaluierung und 18 F-Markierung von neuen Liganden zur Visualisierung der Strychnin-insensitiven Bindungsstelle des NMDA-Rezeptors

Glutamat ist der wichtigste exzitatorische Neurotransmitter im Gehirn. Folglich spielen Glutamat-kontrollierte Rezeptorsysteme eine entscheidende Rolle in neurologischen Vorgängen, wie beispielsweise in Lern- und Gedächtnisprozessen. Gerade der NMDA-Rezeptor ist in eine Vielzahl solcher Vorgänge involviert und wird vor allem mit neurodegenerativen Erkrankungen wie Chorea Huntington, Morbus Alzheimer, Morbus Parkinson und zerebraler Ischämie in Verbindung gebracht. Folglich stellt die Visualisierung des NMDA-Rezeptorstatus eine Möglichkeit dar, den Verlauf solcher Prozesse zu untersuchen.rnDie Positronen-Emissions-Tomographie (PET) ist eine leistungsstarke Anwendung in der molekularen Bildgebung und erlaubt die in vivo-Visualisierung sowie Quantifizierung biochemischer Prozesse. Durch die Verwendung geeigneter Tracer können bestimmte pathologische und neurologische Abläufe beurteilt werden. rnZurzeit sind keine geeigneten PET-Tracer zur Untersuchung des NMDA-Rezeptors verfügbar. Bisher dargestellte PET-Liganden zeichneten sich durch nicht zufriedenstellende Affinitäten und Selektivitäten aus und führten meist auf Grund der hohen Lipophilie zu einem hohen Maß an unspezifischer Bindung. rnDie Strychnin-insensitive Glycinbindungsstelle des NMDA-Rezeptors stellt ein vielversprechendes Target dar, spezifische Liganden für diese Bindungsstelle zu synthetisieren. Hier zeichnen sich einige Verbindungsklassen durch exzellente Affinitäten und Selektivitäten sowie durch vielversprechende in vivo-Eigenschaften aus. rnAuf Grundlage dieser biologischen Daten wurden zwei Substanzen der 2-Indolcarbonsäure, nämlich die 4,6-Dichlor-3-(2-oxo-3-phenylimidazolidin-1-ylmethyl)-1H-indol-2-carbonsäure (MDJ-114) und die (E)-4,6-Dichlor-3-(2-phenylcarbamoylvinyl)-1H-indol-2-carbonsäure (GV150526), als Leitstruktur gewählt. Ferner wurde das 7-Chlor-4-hydroxy-3-(3-phenoxyphenyl)-1H-chinolin-2-on (L-701,324) aus der Substanzklasse der 4-Hydroxy-1H-chinolin-2-one als dritte Leitstruktur gewählt.rnFür diese Substanzen wurden 19F-markierte Analogverbindungen synthetisiert, um als inaktive Referenzverbindungen auf ihre Eignung überprüft zu werden. Hierzu wurde eine Fluorethoxygruppierung im terminalen Phenylring der entsprechenden Leitstruktur eingeführt. Durch Variation der Fluorethoxysubstitution in ortho-, meta- und para-Stellung, konnten die besten Affinitäten in einem kompetitiven Rezeptorbindungsassay durch Verdrängung von [3H]MDL-105,519 bestimmt werden. Als Maß für die Lipophilie wurden die entsprechenden log D-Werte über die HPLC-Methode bestimmt. Basierend auf den Ergebnissen der Evaluierung wurden zwei Derivate identifiziert, welche zur 18F-Markierung genutzt werden sollten (GV150526-Derivat 34: log D = 0,23 ± 0,03, IC50 = 0,20 ± 0,25 µM, Ki = 0,13 ± 0,16 µM; L701,324-Derivat 55: log D = - 0,25 ± 0,01, IC50 = 78 ± 37 µM, Ki = 51 ± 24 µM). Die 18F-Markierung erfolgte durch die Reaktion des entsprechenden Markierungsvorläufers mit dem Markierungssynthon 2-[18F]Fluorethyltosylat, welches durch die Umsetzung von Ethylenditosylat mit [18F]Fluorid hergestellt wurde. Die Radiosynthesen der beiden 18F-markierten Verbindungen [18F]34 (4,6-Dichlor-3-{2-[4-(2-[18F]fluorethoxy)-phenylcarbamoyl]-vinyl}-1H-indol-2-carbonsäure) und [18F]55 (7-Chlor-3-{3-[4-(2-[18F]fluorethoxy)-phenoxy]-phenyl}-4-hydroxy-1H-chinolin-2-on) wurden optimiert sowie semipräparative Abtrennverfahren entwickelt. Beide Tracer wurden auf ihre in vivo-Eignung im µPET-Experiment untersucht. Die Zeitaktivitätskurven lassen erkennen, dass beide Tracer entgegen der Erwartung nicht die Blut-Hirn-Schranke überwinden können. Für das GV150526-Derivat ([18F]34) wurden zusätzlich Autoradiographiestudien durchgeführt. Die erhaltenen Aufnahmen zeigten ein heterogenes Verteilungsmuster der Aktivitätsanreicherung. Ebenso wurde ein hohes Maß an unspezifischer Bindung beobachtet. Möglicherweise sind Cross-Affinitäten zu anderen Rezeptorsystemen oder der recht hohe lipophile Rest des Moleküls hierfür verantwortlich. Ein Grund für die unzureichende Hirngängigkeit der Radioliganden kann sich in der Carboxylatfunktion des GV150526-Derivats bzw. in der 4-Hydroxy-1H-chinolin-2-on-Einheit des L-701,324-Derivats wiederspiegeln. rnAuf Grundlage dieser Resultate können Versuche unternommen werden, für die Verbindungsklasse der 2-Indolcarbonsäuren entsprechende Ester als Prodrugs mit einer verbesserten Bioverfügbarkeit darzustellen. Ebenso können neue Strukturen als Grundlage für neue PET-Tracer untersucht werden.rnrn

3D-ultrastructure, functions and stress responses of rhogocytes from the freshwater gastropods Biomphalaria glabrata and Lymnaea stagnalis

Rhogocytes, also termed ‘pore cells’, exist free in the hemolymph or embedded in the connective tissue of different body parts of molluscs, notably gastropods. These unique cells can be round, elongated or irregularly shaped, and up to 30 μm in diameter. Their hallmark is the so-called slit apparatus: i.e. pocket-like invaginations of the plasma membrane creating extracellular lacunae, bridged by cytoplasmic bars. These bars form distinctive slits of ca. 20 nm width. A slit diaphragm composed of proteins establishes a molecular sieve with holes of 20 x 20 nm. Different functions have been assigned to this special molluscan cell type, notably biosynthesis of the hemolymph respiratory protein hemocyanin. It has further been proposed, but not proven, that in the case of red-blooded snail species rhogocytes might synthesize the hemoglobin. However, the secretion pathway of these hemolymph proteins, and the functional role of the enigmatic slit apparatus remained unclear. Additionally proposed functions of rhogocytes, such as heavy metal detoxification or hemolymph protein degradation, are also not well studied. This work provides more detailed electron microscopical, histological and immunobiochemical information on the structure and function of rhogocytes of the freshwater snails Biomphalaria glabrata and Lymnaea stagnalis. By in situ hybridization on mantle tissues, it proves that B. glabrata rhogocytes synthesize hemoglobin and L. stagnalis rhogocytes synthesize hemocyanin. Hemocyanin is present, in endoplasmic reticulum lacunae and in vesicles, as individual molecules or pseudo-crystalline arrays. The first 3D reconstructions of rhogocytes are provided by means of electron tomography and show unprecedented details of the slit apparatus. A highly dense material in the cytoplasmic bars close to the diaphragmatic slits was shown, by immunogold labeling, to contain actin. By immunofluorescence microscopy, the protein nephrin was localized at the periphery of rhogocytes. The presence of both proteins in the slit apparatus supports the previous hypothesis, hitherto solely based on similarities of the ultrastructure, that the molluscan rhogocytes are phylogenetically related to mammalian podocytes and insect nephrocytes. A possible secretion pathway of respiratory proteins that includes a transfer mechanism of vesicles through the diaphragmatic slits is proposed and discussed. We also studied, by electron microscopy, the reaction of rhogocytes in situ to two forms of animal stress: deprivation of food and cadmium contamination of the tank water. Significant cellular reactions to both stressors were observed and documented. Notably, the slit apparatus surface and the number of electron-dense cytoplasmic vesicles increased in response to cadmium stress. Food deprivation led to an increase in hemocyanin production. These observations are also discussed in the framework of using such animals as potential environmental biomarkers.

Hadronic correlation functions with quark-disconnected contributions in lattice QCD

One of the fundamental interactions in the Standard Model of particle physicsrnis the strong force, which can be formulated as a non-abelian gauge theoryrncalled Quantum Chromodynamics (QCD). rnIn the low-energy regime, where the QCD coupling becomes strong and quarksrnand gluons are confined to hadrons, a perturbativernexpansion in the coupling constant is not possible.rnHowever, the introduction of a four-dimensional Euclidean space-timernlattice allows for an textit{ab initio} treatment of QCD and provides arnpowerful tool to study the low-energy dynamics of hadrons.rnSome hadronic matrix elements of interest receive contributionsrnfrom diagrams including quark-disconnected loops, i.e. disconnected quarkrnlines from one lattice point back to the same point. The calculation of suchrnquark loops is computationally very demanding, because it requires knowledge ofrnthe all-to-all propagator. In this thesis we use stochastic sources and arnhopping parameter expansion to estimate such propagators.rnWe apply this technique to study two problems which relay crucially on therncalculation of quark-disconnected diagrams, namely the scalar form factor ofrnthe pion and the hadronic vacuum polarization contribution to the anomalousrnmagnet moment of the muon.rnThe scalar form factor of the pion describes the coupling of a charged pion torna scalar particle. We calculate the connected and the disconnected contributionrnto the scalar form factor for three different momentum transfers. The scalarrnradius of the pion is extracted from the momentum dependence of the form factor.rnThe use ofrnseveral different pion masses and lattice spacings allows for an extrapolationrnto the physical point. The chiral extrapolation is done using chiralrnperturbation theory ($chi$PT). We find that our pion mass dependence of thernscalar radius is consistent with $chi$PT at next-to-leading order.rnAdditionally, we are able to extract the low energy constant $ell_4$ from thernextrapolation, and ourrnresult is in agreement with results from other lattice determinations.rnFurthermore, our result for the scalar pion radius at the physical point isrnconsistent with a value that was extracted from $pipi$-scattering data. rnThe hadronic vacuum polarization (HVP) is the leading-order hadronicrncontribution to the anomalous magnetic moment $a_mu$ of the muon. The HVP canrnbe estimated from the correlation of two vector currents in the time-momentumrnrepresentation. We explicitly calculate the corresponding disconnectedrncontribution to the vector correlator. We find that the disconnectedrncontribution is consistent with zero within its statistical errors. This resultrncan be converted into an upper limit for the maximum contribution of therndisconnected diagram to $a_mu$ by using the expected time-dependence of therncorrelator and comparing it to the corresponding connected contribution. Wernfind the disconnected contribution to be smaller than $approx5%$ of thernconnected one. This value can be used as an estimate for a systematic errorrnthat arises from neglecting the disconnected contribution.rn