Open Access

Es wurde eine Methode zur Herstellung ultradünner Filme aus Metall bzw. metallischen Verbindungen (Legierungen) etabliert. Die Struktur und die physikalischen Eigenschaften der Filme wurden untersucht. Die entwickelte Präparationsmethode beruht auf induzierter Filmkontraktion nach erzwungener Benetzung (iFCaFW). Die Filme bestehen aus ultradünnen vertikal heterostrukturierten Multischichten (2D-VHML), sie entstehen durch den Beschichtungsvorgang und bestehen aus jeweils einer nm-dicken metallischen Schicht (M) eingebettet zwischen zwei Metall(hydr)oxidschichten (MOxHy) im nm- bis sub-nm Bereich. Dieser vertikal heterostrukturierte Aufbau wurde bei allen untersuchten Filmmaterialien beobachtet. Alle in dieser Arbeit vorgestellten Schichtsysteme wurden unter atmosphärischem Druck hergestellt. Es konnten Substrate aus Silicium und Muskovit sowie aus Borosilikat- und Kalk-Natron-Glas (Objektträger) beschichtet werden. Jede, aus flüssigem Metall bzw. flüssiger Legierung hergestellte Schicht verfügt über eine feste (Hydr)oxidschicht an der Luftgrenzfläche. Diese feste (Hydr)oxidschicht fungiert als Substrat für die nächste darüber aufgebrachte Schicht aus flüssigem Metall bzw. flüssiger Legierung. Somit entstehen vertikal heterostrukturierte Multischichten durch identische Wiederholung des Beschichtungsvorgangs. Dies ist eine innovative und vergleichsweise umweltfreundliche Methode, um transparente, elektrisch leitfähige und lateral homogene nm-dünne ein- oder mehrschichtige Metallfilme herzustellen. Verwendet wurden Metalle mit sehr niedriger Schmelztemperatur (kleiner als 300 °C), wie Bismut, Gallium, Indium, Zinn und ihre Legierungen. Die hohe Oberflächenspannung der geschmolzenen Metalle und Legierungen sowie die Adhäsion mit der die (Hydr)oxidhaut dieser Metalle und Legierungen auf verschiedenen Substraten haftet ermöglicht die Beschichtungsmethode.

This work study a monolayer of branched poly(ethyleneimine (PEI) adsorbed onto oppositely charged surfaces with iron chelates or iron ions in the absorption solution. The conformation of adsorbed PEI is explored in the dependence of the composition of the adsorption solution by measuring the surface forces using atomic force microscopy (AFM) with the colloidal probe (CP) at different ionic strengths (INaCl) in surrounding aqueous solution. The surface coverage of these layers is investigated using X-ray reflectivity. PEI solutions show different pH values with iron chelates (pH = 3), iron ions (pH = 4.67) or pure water (pH = 9.3) at room temperature. Low surface coverage of PEI at pH = 3 adjusted by monovalent ions was also observed. However, adsorbing PEI with iron ions or iron chelates and washing with pure water shifts the pH, leading to an adsorbed PEI layer with high coverage. In our observation, the influence of iron ions and iron chelates on the surface coverage of PEI film is stronger than the pH effect. PEI adsorbed from a pure water solution shows flat conformation. Surface force measurements with CP show that PEI adsorbed from solutions containing iron chelates or iron ions cause almost identical steric forces. The thickness of the brush L is determined as a function of the ionic INaCl in the measuring solution. It scales as a polyelectrolyte brush. The maximum number density of gold nanoparticles (AuNPs) adsorbed onto the PEI brushes was identical and larger than on flatly adsorbed PEI. On the PEI layer with the larger surface coverage, the AuNPs aggregate; on the PEI layer with the lower surface coverage they do not aggregate. Taken together, these results contribute to understanding the mechanisms determining surface coverage and conformation of PEI and demonstrate the possibility of controlling surface properties, which is highly desirable for potential future applications. In this thesis, we also investigate the top layer (PSS and PDADMA) of polyelectrolyte multilayer (PEM) films. PEM films were prepared by sequential adsorption of oppositely charged PEs on solid substrates. PEM films consist of polydiallyldimethylammonium (PDADMA) as polycation and the polystyrene sulfonate (PSS) as polyanion. PDADMA has a smaller linear charge density than PSS. For this system, two different growth regimes are known: parabolic and linear. I studied the top layer (PSS and PDADMA) conformation of PEM films and how the structure of this top layer is affected by increasing the number of PDADMA/PSS layer pairs N and the addition of salt to the surrounding solution. The INaCl was changed during the force-distance measurements. PSS terminated films always show electrostatic forces at INaCl < 0.1 M and flat conformation. The surface charge density is always negative at INaCl < 0.1 M. The surface charge of the PSS top layer starts to turn from negative to positive at N ≥ 14. At N between 13 and 15, adsorbed PSS cannot compensate all the excess PDADMA charge. This leads to an accumulation of the positive extrinsic sites within the PSS terminated film beyond a specific N. At INaCl ≈ 0.1 M, an exponential decaying force was measured. This is an indication of unusual long-ranged hydration force (decay length λ-1 ≈ 0.2-0.5 nm), and PSS terminated film shows zwitterionic or neutral surface. At INaCl > 0.1 M, a non-electrostatic action occurs and the PSS terminated film reswells in solution. PDADMA terminated surface consisting of few layers show a flat conformation and the electrostatic forces were measured. For N ≥ 9 and INaCl ≤ 0.1 M, steric forces were measured. The force-distance profiles are well-explained by Alexander and de Gennes theory. PDADMA chains show a maximum L that is around 40-45 % of the contour length. For INaCl ≈ 0.1 M, and N > 9, a flat, neutral or zwitterionic surface is found (λ-1 ≈ 0.3-0.9 nm). For N = 9 and INaCl > 0.1 M, a strong screening of electrostatic interaction and attractive forces are observed. For N > 9 and INaCl > 0.1 M, the ion adsorption into the PE chains leads to an increase in the monomer size and as a result, the L increases and PDADMA brushes reswell again into the solution. These data show that by varying N and INaCl, different surface forces can be obtained: Electrostatic forces (flat chains) both positive and negative, steric forces (brush), hydration force (flat, neutral or zwitterionic surface), and effects not yet explained (reswelling brush).

The thioredoxin (Trx) family of proteins comprises many key enzymes in redox signaling, that catalyzes specific reversible redox reactions, e.g. dithiol-disulfide exchange reactions, (de-)glutathionylation, trans-nitrosylation, or peroxide reduction. With the analysis of a large number of proteins, as well as a certain redox couple in [article 1] and [article 4], we demonstrated that electrostatic complementarity is the major distinguishing feature that controls the specific interactions of Trxs with their target proteins. The primary aim of this work was to determine the importance of this specific interaction and the prediction, modulation, and engineering of functional redox interactions of Trx family proteins. To understand the role of electrostatic complementarity for the mammalian Trx1-TrxR complex, we generated more than 20 hTrx1 mutants and systematically engineered the electrostatic potential within and outside the contact area with TrxR [article 1]. The effects of these specific alterations distributed all over the protein surface were analyzed by enzyme kinetics, differential scanning fluorimetry (DSF), circular dichroism (CD) spectroscopy, and MD simulations. Trx family proteins have a broad and very distinct substrate specificity, which is a prerequisite for redox switching. In [article 4], we comprehensively compared the classification of various redoxins from all kingdoms of life based on their similarity in amino acid sequence, tertiary structure, and electrostatic properties. These similarities were then correlated to the existence of common interaction partners. Our analyses confirmed that the primary and tertiary structure similarities do not correlate to the target specificity of the proteins as thiol-disulfide oxidoreductases. However, we demonstrated that the electrostatic properties of the protein from both Trx or Grx subfamilies is the major determinant for their target specificity. Although structurally very similar, CxxC/S-type or class I Grxs act as oxidoreductases and CGFS-type or class II Grxs act as FeS cluster transferases. In [article 3], we re-investigated the structural differences between the two main classes of Grxs to solve the mystery of the missing FeS transferase activity of the CxxC/S-type and the lack of oxidoreductase activity of the CGFS-type Grxs. The presence of a distinct loop structure adjacent to the active site is the major determinant of the Grx function. We confirmed that the function of Grxs can be switched from oxidoreductase to FeS cluster transferase by construction of a CxxC/S-type Grx with a CGFS-type Grx loop and vice versa. Results of several in vitro and in vivo assays together with the detailed structural analyses indicate that not a radically different substrate specificity accounts for the lack of activity, but rather slightly different modes of GSH binding, which is an essential nucleophile required in redox and iron homeostasis. Various processes within the cell depend on GSH, including redox reactions, reversible posttranslational modifications, and iron metabolim. GSH is not only important in the export of FeS precursors from mitochondria, but it is also an essential cofactor for cluster binding in iron sulfur Grxs. In [article 2], we discussed the role of GSH and iron sulfur Grxs in iron metabolism, the physiological role of CGFS-type Grx interactions with BolA- like proteins, and the cluster transfer between Grxs and recipient proteins. The first well characterized physiological function of a Grx-BolA hetero complex is presented with the Grx3/4-Fra2-mediated regulation of iron homeostasis in yeast. In synopsis, the results presented and discussed in these articles and the manuscript support the concept of electrostatic properties as the main determinant in substrate specificity towards functional predictions in Trx family proteins. The mathematical model presented here showed significantly accuracy and precision in function prediction. We are aware that our findings are focused on Trx family proteins as a particular family of proteins, but by using a machine learning strategy this mathematical model is being trained with numerous different protein models for better efficacy and accuracy, that may lead to new insights also in the specific interactions of other protein families. The new concept for the substrate specificity determinant doesn’t eliminate previously described aspects for molecular recognition, instead it reveals a deeper understanding of the protein-protein interaction. The 3D structural elements of a protein play a significant role in the specificity and function. We have been able to activate an inactive protein by replacing defined structural elements. Elimination of the loop structure from CGFS-type Grx5 transformed it from an FeS transferase into an oxidoreductase and the activity was further increased by modification of the active site. We believe that the present findings may be useful to investigate proteins in great detail regarding their function based on structure and electrostatic properties. Understanding the nature of the specific interactions may enable us to specifically modify the signal transduction pathways.