Patterns in and kinetics of phase separation in binary mixtures

This work focused mainly on two aspects of kinetics of phase separation in binary mixtures. In the first part, we studied the interplay of hydrodynamics and the phase separation of binary mixtures. A considerably flat container (a laterally extended geometry), at an aspect ratio of 14:1 (diameter: height) was chosen, so that any hydrodynamic instabilities, if they arise, could be tracked. Two binary mixtures were studied. One was a mixture of methanol and hexane, doped with 5% ethanol, which phase separated under cooling. The second was a mixture of butoxyethanol and water, doped with 2% decane, which phase separated under heating. The dopants were added to bring down the phase transition temperature around room temperature.rnrnAlthough much work has been done already on classical hydrodynamic instabilities, not much has been done in the understanding of the coupling between phase separation and hydrodynamic instabilities. This work aimed at understanding the influence of phase separation in initiating any hydrodynamic instability, and also vice versa. Another aim was to understand the influence of the applied temperature protocol on the emergence of patterns characteristic to hydrodynamic instabilities. rnrnOn slowly cooling the system continuously, at specific cooling rates, patterns were observed in the first mixture, at the start of phase separation. They resembled the patterns observed in classical Rayleigh-Bénard instability, which arises when a liquid continuously is heated from below. To suppress this classical convection, the cooling setup was tuned such that the lower side of the sample always remained cooler by a few millikelvins, relative to the top. We found that the nature of patterns changed with different cooling rates, with stable patterns appearing for a specific cooling rate (1K/h). On the basis of the cooling protocol, we estimated a modified Rayleigh number for our system. We found that the estimated modified Rayleigh number is near the critical value for instability, for cooling rates between 0.5K/h and 1K/h. This is consistent with our experimental findings. rnrnThe origin of the patterns, in spite of the lower side being relatively colder with respect to the top, points to two possible reasons. 1) During phase separation droplets of either phases are formed, which releases a latent heat. Our microcalorimetry measurements show that the rise in temperature during the first phase separation is in the order of 10-20millikelvins, which in some cases is enough to reverse the applied temperature bias. Thus phase separation in itself initiates a hydrodynamic instability. 2) The second reason comes from the cooling protocol itself. The sample was cooled from above and below. At sufficiently high cooling rates, there are situations where the interior of the sample is relatively hotter than both top and bottom of the sample. This is sufficient to create an instability within the cell. Our experiments at higher cooling rates (5K/h and above) show complex patterns, which hints that there is enough convection even before phase separation occurs. Infact, theoretical work done by Dr.Hayase show that patterns could arise in a system without latent heat, with symmetrical cooling from top and bottom. The simulations also show that the patterns do not span the entire height of the sample cell. This is again consistent with the cell sizes measured in our experiment.rnrnThe second mixture also showed patterns at specific heating rates, when it was continuously heated inducing phase separation. In this case though, the sample was turbid for a long time until patterns appeared. A meniscus was most probably formed before the patterns emerged. We attribute the reason of patterns in this case to Marangoni convection, which is present in systems with an interface, where local differences in surface tension give rise to an instability. Our estimates for the Rayleigh number also show a significantly lower number than that's required for RB-type instability.rnrnIn the first part of the work, therefore, we identify two different kinds of hydrodynamic instabilities in two different mixtures. Both are observed during, or after the first phase separation. Our patterns compare with the classical convection patterns, but here the origins are from phase separation and the cooling protocol.rnrnIn the second part of the work, we focused on the kinetics of phase separation in a polymer solution (polystyrene and methylcyclohexane), which is cooled continuously far down into the two phase region. Oscillations in turbidity, denoting material exchange between the phases are seen. Three processes contribute to the phase separation: Nucleation of droplets, their growth and coalescence, and their subsequent sedimentation. Experiments in low molecular binary mixtures had led to models of oscillation [43] which considered sedimentation time scales much faster than the time scales of nucleation and growth. The size and shape of the sample therefore did not matter in such situations. The oscillations in turbidity were volume-dominated. The present work aimed at understanding the influence of sedimentation time scales for polymer mixtures. Three heights of the sample with same composition were studied side by side. We found that periods increased with the sample height, thus showing that sedimentation time determines the period of oscillations in the polymer solutions. We experimented with different cooling rates and different compositions of the mixture, and we found that periods are still determined by the sample height, and therefore by sedimentation time. rnrnWe also see that turbidity emerges in two ways; either from the interface, or throughout the sample. We suggest that oscillations starting from the interface are due to satellite droplets that are formed on droplet coalescence at the interface. These satellite droplets are then advected to the top of the sample, and they grow, coalesce and sediment. This type of an oscillation wouldn't require the system to pass the energy barrier required for homogenous nucleation throughout the sample. This mechanism would work best in sample where the droplets could be effectively advected throughout the sample. In our experiments, we see more interface dominated oscillations in the smaller cells and lower cooling rates, where droplet advection is favourable. In larger samples and higher cooling rates, we mostly see that the whole sample becomes turbid homogenously, which requires the system to pass the energy barrier for homogenous nucleation.rnrnOscillations, in principle, occur since the system needs to pass an energy barrier for nucleation. The height of the barrier decreases with increasing supersaturation, which in turn is from the temperature ramp applied. This gives rise to a period where the system is clear, in between the turbid periods. At certain specific cooling rates, the system can follow a path such that the start of a turbid period coincides with the vanishing of the last turbid period, thus eliminating the clear periods. This means suppressions of oscillations altogether. In fact we experimentally present a case where, at a certain cooling rate, oscillations indeed vanish. rnrnThus we find through this work that the kinetics of phase separation in polymer solution is different from that of a low molecular system; sedimentation time scales become relevant, and therefore so does the shape and size of the sample. The role of interface in initiating turbid periods also become much more prominent in this system compared to that in low molecular mixtures.rnrnIn summary, some fundamental properties in the kinetics of phase separation in binary mixtures were studied. While the first part of the work described the close interplay of the first phase separation with hydrodynamic instabilities, the second part investigated the nature and determining factors of oscillations, when the system was cooled deep into the two phase region. Both cases show how the geometry of the cell can affect the kinetics of phase separation. This study leads to further fundamental understandings of the factors contributing to the kinetics of phase separation, and to the understandings of what can be controlled and tuned in practical cases. rn

CD137-selektierte leukämiereaktive T-Zellen gesunder Spender zur adoptiven Immuntherapie stammzelltransplantierter Leukämiepatienten = CD137-selected leukaemia-reactive T Cells from healthy donors for adoptive immunotherapy in stem-cell-transplanted leukaemia-patients

Bei stammzelltransplantierten Patienten, die ein Rezidiv ihrer Leukämie erleiden, kann eine Donor-Lymphozyten-Infusion (DLI) dauerhafte vollständige Leukämieremissionen induzieren. T-Zellen in der DLI vermitteln sowohl den potentiell kurativen Graft-versus-Leukaemia (GVL) Effekt, als auch die potentiell lebensbedrohliche Graft-versus-Host Disease (GVHD). Hingegen könnte die Infusion von leukämiereaktiven T-Zellen einen selektiven GVL Effekt und einen Langzeitschutz vor Rezidiven durch eine spezifisch gegen die Leukämie gerichtete Immunantwort und Immunität vermitteln. Unsere Arbeitsgruppe hat Protokolle zur in vitro Generierung leukämiereaktiver T-Zellen entwickelt, die hohe zytotoxische Aktivität gegen akute myeloische Leukämie-Blasten (AML) bei minimaler Reaktion auf mögliche GVHD Zielstrukturen zeigen. Für die klinische Anwendung sind diese Protokolle jedoch zu aufwändig, wobei vor allem eine erhebliche Verkürzung der Kulturzeit auf wenige Wochen erforderlich ist. Diese Verkürzung der in vitro Kulturzeit könnte das Wachstum von T-Zellen vom central memory oder frühen effector memory Phänotyp fördern, für die eine bessere in vivo Effektorfunktion und längere Persistenz im Rezipienten verglichen mit T-Zellen aus Langzeitkultur gezeigt werden konnte. Der Aktivierungsmarker und Kostimulations-Rezeptor CD137 kann zur Erkennung und Isolation antigenspezifischer T-Zellen genutzt werden, ohne dass dafür das von den T-Zellen erkannte Peptidepitop bekannt sein muss. Eine CD137-vermittelte Anreicherung mit Hilfe von clinical grade Materialien könnte verwendet werden, um DLI-Produkte mit leukämiespezifischen T-Zellen herzustellen, die sich sowohl durch eine effizientere T-Zell Generierung durch in vitro Selektion und Kostimulation, als auch durch eine verbesserte Spezifität des T-Zell-Produkts auszeichnen. Lymphozyten-Leukämie Cokulturen (mixed lymphocyte leukaemia cultures) wurden mit CD8 T-Zellen gesunder Spender und HLA-identischen oder einzel-HLA-mismatch AML-Blasten angesetzt und wöchentlich restimuliert. Nach zwei Wochen wurden die T-Zellen 12 Stunden nach Restimulation über den Marker CD137 positiv isoliert und anschließend separat weiterkultiviert. Die isolierten Fraktionen und unseparierten Kontrollen wurden im ELISPOT-Assay und im Chrom-Freisetzungstest an Tag 5 nach der Restimulation getestet. Es wurden keine konsistent nachweisbaren Vorteile im Hinblick auf Wachstum und Funktion der isolierten CD137-positiv Fraktion im Vergleich zur unseparierten Kontrolle gefunden. Verschiedene Isolationsmethoden, Patient-Spender-Systeme, Methoden zur Restimulation, Temperaturbedingungen, Zytokinkombinationen und Methoden der Zytokinzugabe sowie zusätzliche Feeder-Zellen oder AML-Blasten konnten Wachstum, funktionelle Daten und die deutlichen Zellverluste während der Isolation nicht entscheidend beeinflussen. Vitalfärbungen zeigten, dass aktivierungsinduzierter Zelltod CD137-positiver Zellen zu diesen Ergebnissen beitragen könnte. Im Gegensatz zur Stimulation mit AML-Blasten wurden erfolgreiche CD137-Anreicherungen für peptidstimulierte T-Zellen publiziert. Unterschiedliche CD137-Expressionskinetiken, aktivierungsinduzierter Zelltod und regulatorische T-Zellen sind mögliche Faktoren aufgrund derer die CD137-Anreicherung in diesem spezifischen Kontext ungeeinet sein könnte. Der stimulatorische Effekt eines CD137-Signals auf AML-reaktive CD8 T-Zellen wurde mit Hilfe von CD3/CD28 und CD3/CD28/CD137 Antikörper-beschichteten magnetischen beads untersucht. Für Nierenzellkarzinom-reaktive T-Zellen war die Stimulation mit CD3/CD28/CD137 beads genauso effektiv wie mit Tumorzellen und effektiver als mit CD3/CD28 beads. Beide Arten von beads waren für eine Stimulation während der ersten Wochen der Zellkultur geeignet, sodass ein zusätzliches CD137-Signal für die länger anhaltende Expansion tumorreaktiver T-Zellen zur klinischen Anwendung nützlich sein könnte. Die bead-Expansion veränderte die IFN-Sekretion im ELISPOT nicht, aber verursachte eine mäßige Verschlechterung der Zytotoxizität im Chrom-Freisetzungstest. Im Gegensatz dazu zeigten bei AML-reaktiven T-Zellen beide Arten von beads einen nicht apoptosevermittelten, dosisabhängigen zellschädigenden Effekt, der zu einer raschen Abnahme der Zellzahl in Kulturen mit beads führte. Unerwünschte Effekte auf die T-Zell-Funktionalität durch bead-Stimulation sind in der Literatur beschrieben, dennoch gibt es aktuell keine Veröffentlichungen, die eine fundierte Erklärung für den Effekt auf AML-reaktive T-Zellen bieten könnten. Abgesehen von Literaturdaten, die darauf hindeuten, dass CD137 ein vielversprechendes Kandidatenmolekül für die Anreicherung und Expansion von AML-reaktiven T-Zellen sein könnte, zeigen die eigenen Daten sowohl zur CD137-Isolation als auch zur bead-Stimulation, dass für diese spezielle Anwendung CD137 ein ungeeigneter Aktivierungsmarker und Kostimulations-Ligand ist.

Plasmonic nanoparticles as sensors : a novel approach to quantify adsorption and diffusion kinetics

Biosensors find wide application in clinical diagnostics, bioprocess control and environmental monitoring. They should not only show high specificity and reproducibility but also a high sensitivity and stability of the signal. Therefore, I introduce a novel sensor technology based on plasmonic nanoparticles which overcomes both of these limitations. Plasmonic nanoparticles exhibit strong absorption and scattering in the visible and near-infrared spectral range. The plasmon resonance, the collective coherent oscillation mode of the conduction band electrons against the positively charged ionic lattice, is sensitive to the local environment of the particle. I monitor these changes in the resonance wavelength by a new dark-field spectroscopy technique. Due to a strong light source and a highly sensitive detector a temporal resolution in the microsecond regime is possible in combination with a high spectral stability. This opens a window to investigate dynamics on the molecular level and to gain knowledge about fundamental biological processes.rnFirst, I investigate adsorption at the non-equilibrium as well as at the equilibrium state. I show the temporal evolution of single adsorption events of fibrinogen on the surface of the sensor on a millisecond timescale. Fibrinogen is a blood plasma protein with a unique shape that plays a central role in blood coagulation and is always involved in cell-biomaterial interactions. Further, I monitor equilibrium coverage fluctuations of sodium dodecyl sulfate and demonstrate a new approach to quantify the characteristic rate constants which is independent of mass transfer interference and long term drifts of the measured signal. This method has been investigated theoretically by Monte-Carlo simulations but so far there has been no sensor technology with a sufficient signal-to-noise ratio.rnSecond, I apply plasmonic nanoparticles as sensors for the determination of diffusion coefficients. Thereby, the sensing volume of a single, immobilized nanorod is used as detection volume. When a diffusing particle enters the detection volume a shift in the resonance wavelength is introduced. As no labeling of the analyte is necessary the hydrodynamic radius and thus the diffusion properties are not altered and can be studied in their natural form. In comparison to the conventional Fluorescence Correlation Spectroscopy technique a volume reduction by a factor of 5000-10000 is reached.