@article{BhuvaneshMachatschekLysyakovaetal.2019,
  author    = {Bhuvanesh, Thanga and Machatschek, Rainhard Gabriel and Lysyakova, Liudmila and Kratz, Karl and Schulz, Burkhard and Ma, Nan and Lendlein, Andreas},
  title     = {Collagen type-IV Langmuir and Langmuir-Schafer layers as model biointerfaces to direct stem cell adhesion},
  series = {Biomedical materials : materials for tissue engineering and regenerative medicine},
  volume    = {14},
  journal   = {Biomedical materials : materials for tissue engineering and regenerative medicine},
  number    = {2},
  publisher = {Inst. of Physics Publ.},
  address   = {Bristol},
  issn      = {1748-6041},
  doi       = {10.1088/1748-605X/aaf464},
  pages     = {17},
  year      = {2019},
  abstract  = {In biomaterial development, the design of material surfaces that mimic the extra-cellular matrix (ECM) in order to achieve favorable cellular instruction is rather challenging. Collagen-type IV (Col-IV), the major scaffolding component of Basement Membranes (BM), a specialized ECM with multiple biological functions, has the propensity to form networks by self-assembly and supports adhesion of cells such as endothelial cells or stem cells. The preparation of biomimetic Col-IV network-like layers to direct cell responses is difficult. We hypothesize that the morphology of the layer, and especially the density of the available adhesion sites, regulates the cellular adhesion to the layer. The Langmuir monolayer technique allows for preparation of thin layers with precisely controlled packing density at the air-water (A-W) interface. Transferring these layers onto cell culture substrates using the Langmuir-Schafer (LS) technique should therefore provide a pathway for preparation of BM mimicking layers with controlled cell adherence properties. In situ characterization using ellipsometry and polarization modulation-infrared reflection absorption spectroscopy of Col-IV layer during compression at the A-W interface reveal that there is linear increase of surface molecule concentration with negligible orientational changes up to a surface pressure of 25 mN m(-1). Smooth and homogeneous Col-IV network-like layers are successfully transferred by LS method at 15 mN m(-1) onto poly(ethylene terephthalate) (PET), which is a common substrate for cell culture. In contrast, the organization of Col-IV on PET prepared by the traditionally employed solution deposition method results in rather inhomogeneous layers with the appearance of aggregates and multilayers. Progressive increase in the number of early adherent mesenchymal stem cells (MSCs) after 24 h by controlling the areal Col-IV density by LS transfer at 10, 15 and 20 mN m(-1) on PET is shown. The LS method offers the possibility to control protein characteristics on biomaterial surfaces such as molecular density and thereby, modulate cell responses.},
  language  = {en}
}
@phdthesis{Ulaganathan2016,
  author    = {Ulaganathan, Vamseekrishna},
  title     = {Molecular fundamentals of foam fractionation},
  url       = {http://nbn-resolving.de/urn:nbn:de:kobv:517-opus4-94263},
  school      = {Universit{\"a}t Potsdam},
  pages     = {ix, 136},
  year      = {2016},
  abstract  = {Foam fractionation of surfactant and protein solutions is a process dedicated to separate surface active molecules from each other due to their differences in surface activities. The process is based on forming bubbles in a certain mixed solution followed by detachment and rising of bubbles through a certain volume of this solution, and consequently on the formation of a foam layer on top of the solution column. Therefore, systematic analysis of this whole process comprises of at first investigations dedicated to the formation and growth of single bubbles in solutions, which is equivalent to the main principles of the well-known bubble pressure tensiometry. The second stage of the fractionation process includes the detachment of a single bubble from a pore or capillary tip and its rising in a respective aqueous solution. The third and final stage of the process is the formation and stabilization of the foam created by these bubbles, which contains the adsorption layers formed at the growing bubble surface, carried up and gets modified during the bubble rising and finally ends up as part of the foam layer. Bubble pressure tensiometry and bubble profile analysis tensiometry experiments were performed with protein solutions at different bulk concentrations, solution pH and ionic strength in order to describe the process of accumulation of protein and surfactant molecules at the bubble surface. The results obtained from the two complementary methods allow understanding the mechanism of adsorption, which is mainly governed by the diffusional transport of the adsorbing protein molecules to the bubble surface. This mechanism is the same as generally discussed for surfactant molecules. However, interesting peculiarities have been observed for protein adsorption kinetics at sufficiently short adsorption times. First of all, at short adsorption times the surface tension remains constant for a while before it decreases as expected due to the adsorption of proteins at the surface. This time interval is called induction time and it becomes shorter with increasing protein bulk concentration. Moreover, under special conditions, the surface tension does not stay constant but even increases over a certain period of time. This so-called negative surface pressure was observed for BCS and BLG and discussed for the first time in terms of changes in the surface conformation of the adsorbing protein molecules. Usually, a negative surface pressure would correspond to a negative adsorption, which is of course impossible for the studied protein solutions. The phenomenon, which amounts to some mN/m, was rather explained by simultaneous changes in the molar area required by the adsorbed proteins and the non-ideality of entropy of the interfacial layer. It is a transient phenomenon and exists only under dynamic conditions. The experiments dedicated to the local velocity of rising air bubbles in solutions were performed in a broad range of BLG concentration, pH and ionic strength. Additionally, rising bubble experiments were done for surfactant solutions in order to validate the functionality of the instrument. It turns out that the velocity of a rising bubble is much more sensitive to adsorbing molecules than classical dynamic surface tension measurements. At very low BLG or surfactant concentrations, for example, the measured local velocity profile of an air bubble is changing dramatically in time scales of seconds while dynamic surface tensions still do not show any measurable changes at this time scale. The solution's pH and ionic strength are important parameters that govern the measured rising velocity for protein solutions. A general theoretical description of rising bubbles in surfactant and protein solutions is not available at present due to the complex situation of the adsorption process at a bubble surface in a liquid flow field with simultaneous Marangoni effects. However, instead of modelling the complete velocity profile, new theoretical work has been started to evaluate the maximum values in the profile as characteristic parameter for dynamic adsorption layers at the bubble surface more quantitatively. The studies with protein-surfactant mixtures demonstrate in an impressive way that the complexes formed by the two compounds change the surface activity as compared to the original native protein molecules and therefore lead to a completely different retardation behavior of rising bubbles. Changes in the velocity profile can be interpreted qualitatively in terms of increased or decreased surface activity of the formed protein-surfactant complexes. It was also observed that the pH and ionic strength of a protein solution have strong effects on the surface activity of the protein molecules, which however, could be different on the rising bubble velocity and the equilibrium adsorption isotherms. These differences are not fully understood yet but give rise to discussions about the structure of protein adsorption layer under dynamic conditions or in the equilibrium state. The third main stage of the discussed process of fractionation is the formation and characterization of protein foams from BLG solutions at different pH and ionic strength. Of course a minimum BLG concentration is required to form foams. This minimum protein concentration is a function again of solution pH and ionic strength, i.e. of the surface activity of the protein molecules. Although at the isoelectric point, at about pH 5 for BLG, the hydrophobicity and hence the surface activity should be the highest, the concentration and ionic strength effects on the rising velocity profile as well as on the foamability and foam stability do not show a maximum. This is another remarkable argument for the fact that the interfacial structure and behavior of BLG layers under dynamic conditions and at equilibrium are rather different. These differences are probably caused by the time required for BLG molecules to adapt respective conformations once they are adsorbed at the surface. All bubble studies described in this work refer to stages of the foam fractionation process. Experiments with different systems, mainly surfactant and protein solutions, were performed in order to form foams and finally recover a solution representing the foamed material. As foam consists to a large extent of foam lamella - two adsorption layers with a liquid core - the concentration in a foamate taken from foaming experiments should be enriched in the stabilizing molecules. For determining the concentration of the foamate, again the very sensitive bubble rising velocity profile method was applied, which works for any type of surface active materials. This also includes technical surfactants or protein isolates for which an accurate composition is unknown.},
  language  = {en}
}
@phdthesis{Buller2013,
  author    = {Buller, Jens},
  title     = {Entwicklung neuer stimuli-sensitiver Hydrogelfilme als Plattform f{\"u}r die Biosensorik},
  url       = {http://nbn-resolving.de/urn:nbn:de:kobv:517-opus-66261},
  school      = {Universit{\"a}t Potsdam},
  year      = {2013},
  abstract  = {Diese Arbeit befasst sich mit der Synthese und der Charakterisierung von thermoresponsiven Polymeren und ihrer Immobilisierung auf festen Oberfl{\"a}chen als nanoskalige d{\"u}nne Schichten. Dabei wurden thermoresponsive Polymere vom Typ der unteren kritischen Entmischungstemperatur (engl.: lower critical solution temperature, LCST) verwendet. Sie sind bei niedrigeren Temperaturen im L{\"o}sungsmittel gut und nach Erw{\"a}rmen oberhalb einer bestimmten kritischen Temperatur nicht mehr l{\"o}slich; d. h. sie weisen bei einer bestimmten Temperatur einen Phasen{\"u}bergang auf. Als Basismaterial wurden verschiedene thermoresponsive und biokompatible Polymere basierend auf Diethylenglykolmethylethermethacrylat (MEO2MA) und Oligo(ethylenglykol)methylethermethacrylat (OEGMA475, Mn = 475 g/ mol) {\"u}ber frei radikalische Copolymerisation synthetisiert. Der thermoresponsive Phasen{\"u}bergang der Copolymere wurde in w{\"a}ssriger L{\"o}sung und in gequollenen vernetzten d{\"u}nnen Schichten beobachtet. Außerdem wurde untersucht, inwiefern eine selektive Proteinbindung an geeignete funktionalisierte Copolymere die Phasen{\"u}bergangstemperatur beeinflusst. Die thermoresponsiven Copolymere wurden {\"u}ber photovernetzbare Gruppen auf festen Oberfl{\"a}chen immobilisiert. Die n{\"o}tigen lichtempfindlichen Vernetzereinheiten wurden mittels des polymerisierbaren Benzophenonderivates 2 (4 Benzoylphenoxy)ethylmethacrylat (BPEM) in das Copolymer integriert. D{\"u}nne Filme der Copolymere mit ca. 100 nm Schichtdicke wurden {\"u}ber Rotationsbeschichtung auf Siliziumwafer aufgeschleudert und anschließend durch Bestrahlung mit UV Licht vernetzt und auf der Oberfl{\"a}che immobilisiert. Die Filme sind stabiler je gr{\"o}ßer der Vernetzeranteil und je gr{\"o}ßer die Molmasse der Copolymere ist. Bei einem Waschprozess nach der Vernetzung wird beispielsweise aus einem Film mit moderater Molmasse und geringem Vernetzeranteil mehr unvernetztes Copolymer ausgewaschen als bei einem h{\"o}hermolekularen Copolymer mit hohem Vernetzeranteil. Die Quellbarkeit der Polymerschichten wurde mit Ellipsometrie untersucht. Sie ist gr{\"o}ßer je geringer der Vernetzeranteil in den Copolymeren ist. Schichten aus thermoresponsiven OEG Copolymeren zeigen einen Volumenphasen{\"u}bergang vom Typ der LCST. Der thermoresponsive Kollaps der Schichten ist komplett reversibel, die Kollapstemperatur kann {\"u}ber die Zusammensetzung der Copolymere eingestellt werden. F{\"u}r einen Vergleich dieser Eigenschaften mit dem gut charakterisierten und derzeit wohl am h{\"a}ufigsten untersuchten thermoresponsiven Polymer Poly(N-isopropylacrylamid) (PNIPAM) wurden zus{\"a}tzlich photovernetzte Schichten aus PNIPAM hergestellt und ebenfalls ellipsometrisch vermessen. Im Vergleich zu PNIPAM verl{\"a}uft der Phasen{\"u}bergang der Schichten aus den Copolymeren mit Oligo(ethylenglykol)-seitenketten (OEG Copolymere) {\"u}ber einen gr{\"o}ßeren Temperaturbereich. Mit Licht einer Wellenl{\"a}nge > 300 nm wurden die photosensitiven Benzophenongruppen selektiv angeregt. Bei der Verwendung kleinerer Wellenl{\"a}ngen vernetzten die Copolymerschichten auch ohne die Anwesenheit der lichtempfindlichen Benzophenongruppen. Dieser Effekt ließ sich zur kontrollierten Immobilisierung und Vernetzung der OEG Copolymere einsetzen. Als weitere Methode zur Immobilisierung der Copolymere wurde die Anbindung {\"u}ber Amidbindungen untersucht. Dazu wurden OEG Copolymere mit dem carboxylgruppenhaltigen 2 Succinyloxyethylmethacrylat (MES) auf mit 3 Aminopropyldimethylethoxysilan (APDMSi) silanisierte Siliziumwafer rotationsbeschichtet, und mit dem oligomeren α, ω Diamin Jeffamin® ED 900 vernetzt. Die Vernetzungsreaktion erfolgte ohne weitere Zus{\"a}tze durch Erhitzen der Proben. Die Hydrogelschichten waren anschließend stabil und zeigten neben thermoresponsivem auch pH responsives Verhalten. Um zu untersuchen, ob die Phasen{\"u}bergangstemperatur durch eine Proteinbindung beeinflusst werden kann, wurde ein polymerisierbares Biotinderivat 2 Biotinyl-aminoethylmethacrylat (BAEMA) in das thermoresponsive Copolymer eingebaut. Der Einfluss des biotinbindenen Proteins Avidin auf das thermoresponsive Verhalten des Copolymers in L{\"o}sung wurde untersucht. Die spezifische Bindung von Avidin an das biotinylierte Copolymer verschob die {\"U}bergangstemperatur deutlich zu h{\"o}heren Temperaturen. Kontrollversuche zeigten, dass dieses Verhalten auf eine selektive Proteinbindung zur{\"u}ckzuf{\"u}hren ist. Thermoresponsive OEG Copolymere mit photovernetzbaren Gruppen aus BPEM und Biotingruppen aus BAEMA wurden {\"u}ber Rotationsbeschichtung auf Gold- und auf Siliziumoberfl{\"a}chen aufgetragen und durch UV Strahlung vernetzt. Die spezifische Bindung von Avidin an die Copolymerschicht wurde mit Oberfl{\"a}chenplasmonenresonanz und Ellipsometrie untersucht. Die Bindungskapazit{\"a}t der Schichten war umso gr{\"o}ßer, je kleiner der Vernetzeranteil, d. h. je gr{\"o}ßer die Maschenweite des Netzwerkes war. Die Quellbarkeit der Schichten wurde durch die Avidinbindung erh{\"o}ht. Bei hochgequollenen Systemen verursachte eine Mehrfachbindung des tetravalenten Avidins allerdings eine zus{\"a}tzliche Quervernetzung des Polymernetzwerkes. Dieser Effekt wirkt der erh{\"o}hten Quellbarkeit durch die Avidinbindung entgegen und l{\"a}sst die Polymernetzwerke schrumpfen.},
  language  = {de}
}