Fluorescence correlation spectroscopy (FCS) analyzes the fluctuations in the fluorescence intensity, which is emitted from a tiny excition volume, to obtain information about the concentration, the mobility, and the molecular interactions of labeled molecules. The more advanced fluorescence cross-correlation spectroscopy (FCCS) increases the precision in the determination of fl ow velocities and binding constants compared to standard FCS. The miniaturization in biomedical and chemical engineering has been developing rapidly, propelled by the vision of a fully functional laboratory on a single chip and its use in human therapeutics, for example, as implanted drug delivery system. A key requirement to fulfill this vision is the ability to handle small fl uid volumes. Handling liquids using the electrohydrodynamical principle circumvents many of the disadvantages of other systems. The complex flow pattern in the active region of such a pump could not be resolved by common tracking techniques. In this thesis, two-focus FCCS (2f-FCCS) was used to map the flow pro file inside a micropump. The high precision of 2f-FCCS in the determination of fl ow measurements even with small fluorescent particles allowed the measurement of the flow velocities induced by electrohydrodynamic forces acting on the solvent, while excluding the effects of dielectrophoretic forces acting on larger particles. Analysis of the fl ow data indicates a fl ow pattern that consists of two vortices of different size and opposite direction of rotation. The flow pattern derived by 2f-FCCS explains the observed complex particle trajectories in the force field and the accumulation of particles in well-de fined regions above the microelectrode array. In the second part of this thesis, the mechanism of RNA interference (RNAi) was studied by dual-color FCCS in vivo. RNAi is an evolutionary conserved gene silencing mechanism, which uses short double-stranded RNA molecules, called short interfering RNAs (siRNAs), as effector molecules. Due to its speci city and simplicity, RNAi yields a great potential for a widespread therapeutic use. To broaden the therapeutic applications, the in vivo stability of siRNAs has to be improved by chemical modi cations, but some of these modi fications inhibit the gene silencing mechanism. The presented FCCS assays are very well suited to investigate the individual assembly steps of RNAi machinery with very high specifi city and sensitivity in real time and to study the cleavage activity of the activated RNAi machinery. A direct correlation between activity of the RNAi machinery and the results from the FCCS measurements could be shown. The in fluence of several chemical modi cations on the assembly and activity of the RNAi machinery was investigated with these assays. / Fluoreszenz-Korrelations-Spektroskopie (FCS) analysiert die Fluktuationen im Fluoreszenzsignal eines kleinen angeregten Volumens, um Informationen über die Konzentration, die Bewegung und die Interaktionen der markierten Moleküle zu erhalten. Die Fluoreszenz-Kreuzkorrelations-Spektroskopie (FCCS) erhöht die Genauigkeit bei der Messung von Fließgeschwindigkeiten und Bindungskonstanten im Vergleich zur Standard-FCS. Die Miniaturisierung der Biomedizin und Chemie hat sich rapide entwickelt, angetrieben von der Vision eines kompletten Labors auf einem Chip und dem Einsatz dieses in der medizinischen Therapie, zum Beispiel als implantierter Medikamentenspender. Ein Schlüsselelement zur Erfüllung dieser Vision ist der Transport von kleinsten Flüssigkeitsmengen in diesen miniaturisierten Systemen. Der Transport von Flüssigkeiten mittels des elektrohydrodynamischen Prinzips umgeht viele Nachteile von anderen Systemen, allerdings zeigt eine solche Pumpe ein kompliziertes Strömungsbild in der aktiven Region, welches sich mit herkömmlichen Methoden wie Teilchenverfolgung nicht vermessen ließ. Hier wurde Zwei-Fokus-FCCS (2f-FCCS) genutzt, um das Strömungsbild in der Pumpe zu vermessen. Die hohe Genauigkeit der 2f-FCCS bei der Bestimmung von Fließgeschwindigkeiten auch mit kleinen fluoreszierenden Teilchen ermöglichte die Messung der Fließgeschwindigkeiten, aufgrund der auf das Lösungsmittel wirkenden elektrohydrodynamischen Kräfte, unter Ausschluss der auf größere Teilchen wirkenden dielektrophoretischen Kräfte. Die Analyse der Daten ergab, dass das Strömungsbild aus zwei entgegengesetzt rotierenden unterschiedlich großen Wirbeln besteht. Dieses Strömungsbild erklärt die komplizierten Teilchenbewegungsbahnen und die Anreicherung der Teilchen in klar abgegrenzten Bereichen über den Mikroelektroden. Im zweiten Teil dieser Arbeit wurde der RNAi-Mechanismus in lebenden Zellen mittels Zwei-Farben-FCCS untersucht. RNA Interferenz (RNAi) ist ein evolutionär erhaltener Geninaktivierungsmechanismus, der kurze doppelsträngige RNA Moleküle, so genannte kurze interferierende RNAs (siRNAs), als Effektormoleküle nutzt. Die Spezifi tät und Einfachheit der RNAi hat ihr ein weites Feld in der medikamentösen Therapie geöffnet. Zur Erweiterung dieses Feldes ist es nötig die Stabilität der siRNAs im Körper mittels chemischer Modi fikationen zu erhöhen. Einige dieser Modifikationen hemmen aber den RNAi-Mechanismus. Die hier vorgestellten FCCS Experimente sind sehr gut geeignet, um die einzelnen Schritte des Zusammenbaus der RNAi Maschinerie mit hoher Empfi ndlichkeit und Spezi fität in Echtzeit zu untersuchen und die Aktivität der RNAi Maschinerie zu studieren. Es konnte ein Zusammenhang zwischen der Aktivität der RNAi Maschinerie und den Ergebnissen der FCCS Messungen hergestellt werden. Der Einfluss von verschiedenen chemischen Modikationen auf den Zusammenbau und die Aktivität der RNAi Maschinerie wurde mit diesen neuartigen Methoden untersucht.

No description available.

La toxine bactérienne de Shiga se lie au glycosphingolipide (GSL) globotriaosylcéramide (Gb3) afin d’entrer par endocytose dans les cellules en utilisant une voie dépendante et indépendante de la clathrine. Dans la voie indépendante de la clathrine, la toxine de Shiga réorganise les lipides de la membrane de façon à imposer une contrainte mécanique sur la bicouche, conduisant ainsi à la formation de pic d’invagination d'endocytose profonds et étroits. Mécaniquement ce phénomène n’est pas encore compris, notamment il reste énigmatique, comment se traduisent les propriétés géométriques de l’agrégation des glycosphingolipides GSLS et de la toxine. Dans mon travail de thèse, via l’utilisation de la sous-unité B de la toxine de Shiga (STxB) comme un modèle, différentes espèces moléculaires de son récepteur Gb3 ont été synthétisés avec des structures délibérément choisis. Les études réalisées par imagerie de haute résolution et par la modélisation informatique ont permis d’élucider les contraintes mécano-chimique sous-jacente conduisant à une réorganisation efficace qui a pour résultat l’agrégation de la toxine et la réorganisation des lipides. En combinant des expériences de simulation sur ordinateur de dynamique des particules dissipatives (DPD) et des expériences sur des modèles de membranes cellulaires, nous avons fourni la preuve de l’induction d’une force de fluctuation-membrane, de type « force de Casimir », conduisant à l'agrégation des molécules de toxines associées à la membrane à des échelles de longueur mésoscoiques. Nous avons observé et mesuré, en outre la condensation lipidique induite par la toxine, quantitativement sur des monocouches de Langmuir en utilisant la réflectivité des rayons X (XR) et par la mesure de la diffraction des rayons X par incidence rasante (GIXD), fournissant ainsi une preuve directe de l'hypothèse que la toxine a le potentiel de réduire de façon asymétrique la surface moléculaire sur la partie membranaire exoplasmique, ce qui conduit à une déformation locale de la membrane. Durant ma thèse, nos efforts ont été consacrés à la réalisation de nouveaux glycosphinolipides (GSL) comme outils chimiques à visée biologique. Par ailleurs, une nouvelle stratégie de reconstitution de GSL fonctionnels sur la membrane cellulaire, basée sur une réaction de ligation de type « click » entre un glycosyl-cyclooctyne et un azido-sphingosine a été étudiée. Les résultats obtenus sur les cellules se sont avérés beaucoup moins efficace que ceux in vitro. Une poursuite de l'optimisation de cette méthodologie est actuellement en cours. Une sonde fluorescente du glycosphinolipide Gb3, marquée à l’Alexa Fluor 568 lui-même lié par l'intermédiaire d'un bras PEG-α à la position de la chaîne acyle, a été synthétisée. Cette sonde se lie à la STxB sur couche mince de TLC, mais pas sur des membranes modèles. D'autres améliorations sont discutées. / Bacterial Shiga toxins bind to the glycosphingolipid (GSL) globotriaosylceramide (Gb3) to enter cells by clathrin-dependent and independent endocytosis. In the clathrin-independent pathway, Shiga toxin reorganizes membrane lipids in a way such as to impose mechanical strain onto the bilayer, thus leading to the formation of deep and narrow endocytic pits. Mechanistically how this occurs is not yet understood, and notably how the geometric properties of toxin-GSLs complexes translate into function has remained enigmatic. In my thesis work, using the B-subunit of Shiga toxin (STxB) as a model, different molecular species of its receptor Gb3 have been synthesized with deliberately chosen structures, coupled with high resolution imaging and computational modeling, to understand the underlying mechano-chemical constraints leading to efficient toxin clustering and lipids reorganization. By combining dissipative particle dynamics (DPD) computer simulation and experiments on cell and model membranes, we provided evidence that a membrane fluctuation-induced force, termed Casimir-like force, drives the aggregation of tightly membrane-associated toxin molecules at mesoscopic length scales. Furthermore, toxin-induced lipid condensation was observed and measured quantitatively on Langmuir monolayers using X-ray reflectivity (XR) and grazing incidence x-ray diffraction (GIXD), thereby providing direct evidence for the hypothesis that the toxin has the potential to asymmetrically reduce the molecular area of the exoplasmic membrane leaflet, leading to local membrane deformation. During my PhD, effort was also invested to develop new GSL tools applied to the biological setting. A novel strategy based on the Cu-free click reaction between glycosyl-cyclooctyne and azido-sphingosine was designed with the goal to functionally incorporate GSLs into cellular membranes. Following the synthesis work, click reactions have been performed in solution and on cells. Compared to the former, results on cells were far less efficient. Further optimization is currently ongoing. A fluorescently labeled Gb3 probe with Alexa Fluor 568 coupled via a PEG linker to the α-position of the acyl chain, was synthesized, to which STxB bound on TLCs, but not on model membranes. Further improvements are discussed.

The subject of this thesis is the generation of spatial temporal structures in living cells. Specifically, we studied the Min-system in the bacterium Escherichia coli. It consists of the MinC, the MinD, and the MinE proteins, which play an important role in the correct selection of the cell division site. The Min-proteins oscillate between the two cell poles and thereby prevent division at these locations. In this way, E. coli divides at the center, producing two daughter cells of equal size, providing them with the complete genetic patrimony. Our goal is to perform a quantitative study, both theoretical and experimental, in order to reveal the mechanism underlying the Min-oscillations. Experimentally, we characterize theMin-system, measuring the temporal period of the oscillations as a function of the cell length, the time-averaged protein distributions, and the in vivo Min-protein mobility by means of different fluorescence microscopy techniques. Theoretically, we discuss a deterministic description based on the exchange of Minproteins between the cytoplasm and the cytoplasmic membrane and on the aggregation current induced by the interaction between membrane-bound proteins. Oscillatory solutions appear via a dynamic instability of the homogenous protein distributions. Moreover, we perform stochastic simulations based on a microscopic description, whereby the probability for each event is calculated according to the corresponding probability in the master equation. Starting from this microscopic description, we derive Langevin equations for the fluctuating protein densities which correspond to the deterministic equations in the limit of vanishing noise. Stochastic simulations justify this deterministic model, showing that oscillations are resistant to the perturbations induced by the stochastic reactions and diffusion. Predictions and assumptions of our theoretical model are compatible with our experimental findings. Altogether, these results enable us to propose further experiments in order to quantitatively compare the different models proposed so far and to test our model with even higher precision. They also point to the necessity of performing such an analysis through single cell measurements.

A new method, probability distribution of diffusivities (time scaled square displacements between succeeding video frames), was developed to analyze single molecule tracking (SMT) experiments. This method was then applied to SMT experiments on ultrathin liquid tetrakis(2-ethylhexoxy)silane (TEHOS) films on Si wafer with 100 nm thermally grown oxide, and on thin semectic liquid crystal films. Spatial maps of diffusivities from SMT experiments on 220 nm thick semectic liquid crystal films reveal structure related dynamics. The SMT experiments on ultrathin TEHOS films were complemented by fluorescence correlation spectroscopy (FCS). The observed strongly heterogeneous single molecule dynamics within those films can be explained by a three-layer model consisting of (i) dye molecules adsorbed to the substrate, (ii) slowly diffusing molecules in the laterally heterogeneous near-surface region of 1 - 2 molecular diameters, and (iii) freely diffusing dye molecules in the upper region of the film. FCS and SMT experiments reveal a strong influence of substrate heterogeneity on SM dynamics. Thereby chemisorption to substrate surface silanols plays an important role. Vertical mean first passage times (mfpt) in those films are below 1 µs. This appears as fast component in FCS autocorrelation curves, which further contain a contribution from lateral diffusion and from adsorption events. Therefore, the FCS curves are approximated by a tri-component function, which contains an exponential term related to the mfpt, the correlation function for translational diffusion and a stretched exponential term for the broad distribution of adsorption events. Lateral diffusion coefficients obtained by FCS on 10 nm thick TEHOS films, thereby, are effective diffusion coefficients from dye transients in the focal area. They strongly depend on the substrate heterogeneity. Variation of the frame times for the acquisition of SMT experiments in steps of 20 ms from 20 ms to 200 ms revealed a strong dependence of the corresponding probability distributions of diffusivities on time, in particular in the range between 20 ms and 100 ms. This points to average dwell times of the dye molecules in at least one type of the heterogeneous regions (e.g. on and above silanol clusters) in the range of few tens of milliseconds. Furthermore, time series of SM spectra from Nile Red in 25 nm thick poly-n-alkyl-methacrylate (PnAMA) films were studied. In analogy to translational diffusion, spectral diffusion (shifts in energetic positions of SM spectra) can be studied by probability distributions of spectral diffusivities, i.e. time scaled square energetic displacements. Simulations were run and analyzed to study contributions from noise and fitting uncertainty to spectral diffusion. Furthermore the effect of spectral jumps during acquisition of a SM spectrum was investigated. Probability distributions of spectral diffusivites of Nile Red probing vitreous PnAMA films reveal a two-level system. In contrast, such probability distributions obtained from Nile Red within a 25 nm thick poly-n-butylmethacrylate film around glass transition and in the melt state, display larger spectral jumps. Moreover, for longer alkyl side chains a solvent shift to higher energies is observed, which supports the idea of nanophase separation within those polymers.

A new method, probability distribution of diffusivities (time scaled square displacements between succeeding video frames), was developed to analyze single molecule tracking (SMT) experiments. This method was then applied to SMT experiments on ultrathin liquid tetrakis(2-ethylhexoxy)silane (TEHOS) films on Si wafer with 100 nm thermally grown oxide, and on thin semectic liquid crystal films. Spatial maps of diffusivities from SMT experiments on 220 nm thick semectic liquid crystal films reveal structure related dynamics. The SMT experiments on ultrathin TEHOS films were complemented by fluorescence correlation spectroscopy (FCS). The observed strongly heterogeneous single molecule dynamics within those films can be explained by a three-layer model consisting of (i) dye molecules adsorbed to the substrate, (ii) slowly diffusing molecules in the laterally heterogeneous near-surface region of 1 - 2 molecular diameters, and (iii) freely diffusing dye molecules in the upper region of the film. FCS and SMT experiments reveal a strong influence of substrate heterogeneity on SM dynamics. Thereby chemisorption to substrate surface silanols plays an important role. Vertical mean first passage times (mfpt) in those films are below 1 µs. This appears as fast component in FCS autocorrelation curves, which further contain a contribution from lateral diffusion and from adsorption events. Therefore, the FCS curves are approximated by a tri-component function, which contains an exponential term related to the mfpt, the correlation function for translational diffusion and a stretched exponential term for the broad distribution of adsorption events. Lateral diffusion coefficients obtained by FCS on 10 nm thick TEHOS films, thereby, are effective diffusion coefficients from dye transients in the focal area. They strongly depend on the substrate heterogeneity. Variation of the frame times for the acquisition of SMT experiments in steps of 20 ms from 20 ms to 200 ms revealed a strong dependence of the corresponding probability distributions of diffusivities on time, in particular in the range between 20 ms and 100 ms. This points to average dwell times of the dye molecules in at least one type of the heterogeneous regions (e.g. on and above silanol clusters) in the range of few tens of milliseconds. Furthermore, time series of SM spectra from Nile Red in 25 nm thick poly-n-alkyl-methacrylate (PnAMA) films were studied. In analogy to translational diffusion, spectral diffusion (shifts in energetic positions of SM spectra) can be studied by probability distributions of spectral diffusivities, i.e. time scaled square energetic displacements. Simulations were run and analyzed to study contributions from noise and fitting uncertainty to spectral diffusion. Furthermore the effect of spectral jumps during acquisition of a SM spectrum was investigated. Probability distributions of spectral diffusivites of Nile Red probing vitreous PnAMA films reveal a two-level system. In contrast, such probability distributions obtained from Nile Red within a 25 nm thick poly-n-butylmethacrylate film around glass transition and in the melt state, display larger spectral jumps. Moreover, for longer alkyl side chains a solvent shift to higher energies is observed, which supports the idea of nanophase separation within those polymers.