@phdthesis{Saretia2021,
  author    = {Saretia, Shivam},
  title     = {Modulating ultrathin films of semi-crystalline oligomers by Langmuir technique},
  doi       = {10.25932/publishup-54210},
  url       = {http://nbn-resolving.de/urn:nbn:de:kobv:517-opus4-542108},
  school      = {Universit{\"a}t Potsdam},
  pages     = {XIII, 109},
  year      = {2021},
  abstract  = {Polymeric films and coatings derived from semi-crystalline oligomers are of relevance for medical and pharmaceutical applications. In this context, the material surface is of particular importance, as it mediates the interaction with the biological system. Two dimensional (2D) systems and ultrathin films are used to model this interface. However, conventional techniques for their preparation, such as spin coating or dip coating, have disadvantages, since the morphology and chain packing of the generated films can only be controlled to a limited extent and adsorption on the substrate used affects the behavior of the films. Detaching and transferring the films prepared by such techniques requires additional sacrificial or supporting layers, and free-standing or self supporting domains are usually of very limited lateral extension. The aim of this thesis is to study and modulate crystallization, melting, degradation and chemical reactions in ultrathin films of oligo(ε-caprolactone)s (OCL)s with different end-groups under ambient conditions. Here, oligomeric ultrathin films are assembled at the air-water interface using the Langmuir technique. The water surface allows lateral movement and aggregation of the oligomers, which, unlike solid substrates, enables dynamic physical and chemical interaction of the molecules. Parameters like surface pressure (π), temperature and mean molecular area (MMA) allow controlled assembly and manipulation of oligomer molecules when using the Langmuir technique. The π-MMA isotherms, Brewster angle microscopy (BAM), and interfacial infrared spectroscopy assist in detecting morphological and physicochemical changes in the film. Ultrathin films can be easily transferred to the solid silicon surface via Langmuir Schaefer (LS) method (horizontal substrate dipping). Here, the films transferred on silicon are investigated using atomic force microscopy (AFM) and optical microscopy and are compared to the films on the water surface. The semi-crystalline morphology (lamellar thicknesses, crystal number densities, and lateral crystal dimensions) is tuned by the chemical structure of the OCL end-groups (hydroxy or methacrylate) and by the crystallization temperature (Tc; 12 or 21 °C) or MMAs. Compression to lower MMA of ~2 {\AA}2, results in the formation of a highly crystalline film, which consists of tightly packed single crystals. Preparation of tightly packed single crystals on a cm2 scale is not possible by conventional techniques. Upon transfer to a solid surface, these films retain their crystalline morphology whereas amorphous films undergo dewetting. The melting temperature (Tm) of OCL single crystals at the water and the solid surface is found proportional to the inverse crystal thickness and is generally lower than the Tm of bulk PCL. The impact of OCL end-groups on melting behavior is most noticeable at the air-solid interface, where the methacrylate end-capped OCL (OCDME) melted at lower temperatures than the hydroxy end-capped OCL (OCDOL). When comparing the underlying substrate, melting/recrystallization of OCL ultrathin films is possible at lower temperatures at the air water interface than at the air-solid interface, where recrystallization is not visible. Recrystallization at the air-water interface usually occurs at a higher temperature than the initial Tc. Controlled degradation is crucial for the predictable performance of degradable polymeric biomaterials. Degradation of ultrathin films is carried out under acidic (pH ~ 1) or enzymatic catalysis (lipase from Pseudomonas cepcia) on the water surface or on a silicon surface as transferred films. A high crystallinity strongly reduces the hydrolytic but not the enzymatic degradation rate. As an influence of end-groups, the methacrylate end-capped linear oligomer, OCDME (~85 ± 2 \% end-group functionalization) hydrolytically degrades faster than the hydroxy end capped linear oligomer, OCDOL (~95 ± 3 \% end-group functionalization) at different temperatures. Differences in the acceleration of hydrolytic degradation of semi-crystalline films were observed upon complete melting, partial melting of the crystals, or by heating to temperatures close to Tm. Therefore, films of densely packed single crystals are suitable as barrier layers with thermally switchable degradation rates. Chemical modification in ultrathin films is an intricate process applicable to connect functionalized molecules, impart stability or create stimuli-sensitive cross-links. The reaction of end-groups is explored for transferred single crystals on a solid surface or amorphous monolayer at the air-water interface. Bulky methacrylate end-groups are expelled to the crystal surface during chain-folded crystallization. The density of end-groups is inversely proportional to molecular weight and hence very pronounced for oligomers. The methacrylate end-groups at the crystal surface, which are present at high concentration, can be used for further chemical functionalization. This is demonstrated by fluorescence microscopy after reaction with fluorescein dimethacrylate. The thermoswitching behavior (melting and recrystallization) of fluorescein functionalized single crystals shows the temperature-dependent distribution of the chemically linked fluorescein moieties, which are accumulated on the surfaces of crystals, and homogeneously dispersed when the crystals are molten. In amorphous monolayers at the air-water interface, reversible cross-linking of hydroxy-terminated oligo(ε-caprolactone) monolayers using dialdehyde (glyoxal) lead to the formation of 2D networks. Pronounced contraction in the area occurred for 2D OCL films in dependence of surface pressure and time indicating the reaction progress. Cross linking inhibited crystallization and retarded enzymatic degradation of the OCL film. Altering the subphase pH to ~2 led to cleavage of the covalent acetal cross-links. Besides as model systems, these reversibly cross-linked films are applicable for drug delivery systems or cell substrates modulating adhesion at biointerfaces.},
  language  = {en}
}
@phdthesis{Richter2007,
  author    = {Richter, Andreas},
  title     = {Structure formation and fractionation in systems of colloidal rods},
  url       = {http://nbn-resolving.de/urn:nbn:de:kobv:517-opus-13090},
  school      = {Universit{\"a}t Potsdam},
  year      = {2007},
  abstract  = {Nowadays, colloidal rods can be synthesized in large amounts. The rods are typically cylindrically and their length ranges from several nanometers to a few micrometers. In solution, systems of colloidal rodlike molecules or aggregates can form liquid-crystalline phases with long-range orientational and spatial order. In the present work, we investigate structure formation and fractionation in systems of rodlike colloids with the help of Monte Carlo simulations in the NPT ensemble. Repulsive interactions can successfully be mimicked by the hard rod model, which has been studied extensively in the past. In many cases, attractive interactions like van der Waals or depletion forces cannot be neglected, however. In the first part of this work, the phase behavior of monodisperse attractive rods is characterized for different interaction strengths. Phase diagrams as a function of rod length and pressure are presented. Most systems of synthesized mesoscopic rods have a polydisperse length distribution as a consequence of the longitudinal growth process of the rods. For many technical and research applications, a rather small polydispersity is desired in order to have well defined material properties. The polydispersity can be reduced by a spatial demixing (fractionation) of long and short rods. Fractionation and structure formation is studied in a tridisperse and a polydisperse bulk suspension of rods. We observe that the resulting structures depend distinctly on the interaction strength. The fractionation in the system is strongly enhanced with increasing interaction strength. Suspensions are typically confined in a container. We also examine the influence of adjacent substrates in systems of tridisperse and polydisperse rod suspensions. Three different substrate types are studied in detail: a planar wall, a corrugated substrate, and a substrate with rectangular cavities. We analyze the fluid structure close to the substrate and substrate controlled fractionation. The spatial arrangement of long and short rods in front of the substrate depends sensitively on the substrate structure and the pressure. Rods with a predefined length are segregated at substrates with rectangular cavities.},
  language  = {en}
}
@phdthesis{Bischofs2004,
  author    = {Bischofs, Ilka Bettina},
  title     = {Elastic interactions of cellular force patterns},
  url       = {http://nbn-resolving.de/urn:nbn:de:kobv:517-0001767},
  school      = {Universit{\"a}t Potsdam},
  year      = {2004},
  abstract  = {Gewebezellen sammeln st{\"a}ndig Informationen {\"u}ber die mechanischen Eigenschaften ihrer Umgebung, indem sie aktiv an dieser ziehen. Diese Kr{\"a}fte werden an Zell-Matrix-Kontakten {\"u}bertragen, die als Mechanosensoren fungieren. J{\"u}ngste Experimente mit Zellen auf elastischen Substraten zeigen, dass Zellen sehr empfindlich auf Ver{\"a}nderungen der effektiven Steifigkeit ihrer Umgebung reagieren, die zu einer Reorganisation des Zytoskeletts f{\"u}hren k{\"o}nnen. In dieser Arbeit wird ein theoretisches Model entwickelt, um die Selbstorganisation von Zellen in weichen Materialien vorherzusagen. Obwohl das Zellverhalten durch komplexe regulatorische Vorg{\"a}nge in der Zelle gesteuert wird, scheint die typische Antwort von Zellen auf mechanische Reize eine einfache Pr{\"a}ferenz f{\"u}r große effektive Steifigkeit der Umgebung zu sein, m{\"o}glicherweise weil in einer steiferen Umgebung Kr{\"a}fte an den Kontakten effektiver aufgebaut werden k{\"o}nnen. Der Begriff Steifigkeit umfasst dabei sowohl Effekte, die durch gr{\"o}ßere H{\"a}rte als auch durch elastische Verzerrungsfelder in der Umgebung verursacht werden. Diese Beobachtung kann man als ein Extremalprinzip in der Elastizit{\"a}tstheorie formulieren. Indem man das zellul{\"a}re Kraftmuster spezifiziert, mit dem Zellen mit ihrer Umgebung wechselwirken, und die Umgebung selbst als linear elastisches Material modelliert, kann damit die optimale Orientierung und Position von Zellen vorhergesagt werden. Es werden mehrere praktisch relevante Beispiele f{\"u}r Zellorganisation theoretisch betrachtet: Zellen in externen Spannungsfeldern und Zellen in der N{\"a}he von Grenzfl{\"a}chen f{\"u}r verschiedene Geometrien und Randbedingungen des elastischen Mediums. Daf{\"u}r werden die entsprechenden elastischen Randwertprobleme in Vollraum, Halbraum und Kugel exakt gel{\"o}st. Die Vorhersagen des Models stimmen hervorragend mit experimentellen Befunden f{\"u}r Fibroblastzellen {\"u}berein, sowohl auf elastischen Substraten als auch in physiologischen Hydrogelen. Mechanisch aktive Zellen wie Fibroblasten k{\"o}nnen auch elastisch miteinander wechselwirken. Es werden daher optimale Strukturen als Funktion von Materialeigenschaften und Zelldichte bzw. der Geometrie der Zellpositionen berechnet. Schließlich wird mit Hilfe von Monte Carlo Simulationen der Einfluss stochastischer St{\"o}rungen auf die Strukturbildung untersucht. Das vorliegende Model tr{\"a}gt nicht nur zu einem besseren Verst{\"a}ndnis von vielen physiologischen Situationen bei, sondern k{\"o}nnte in Zukunft auch f{\"u}r biomedizinische Anwendungen benutzt werden, um zum Beispiel Protokolle f{\"u}r k{\"u}nstliche Gewebe im Bezug auf Substratgeometrie, Randbedingungen, Materialeigenschaften oder Zelldichte zu optimieren.},
  language  = {en}
}