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First milestone of this Ph.D. thesis was the successful extension of conventional NTA/His-tag technique to self-assembling, multivalent chelator thiols for high-affinity recognition as well as stable and uniform immobilization of His-tagged proteins on chip surfaces. Bis-NTA was linked via an oligoethylene glycol to alkyl thiols by an efficient modular synthesis strategy yielding a novel, multivalent compound for formation of mixed SAMs with anti-adsorptive matrix thiols on gold. Multivalent chelator chips allow a specific, high-affinity, reversible, long-term immobilization of His-tagged proteins. In AFM studies reversibility of the specific protein immobilization process was visualized at single molecule level. The entire control over the orientation of the immobilized protein promotes this chip surface to an optimal platform for studies focusing on research targets at single molecule level and nanobiotechnology. Based on the constructed protein chip platform above and a novel AFM mode (contact oscillation mode, COM) – developed during the current Ph.D. work – protein nanolithography under physiological conditions enabling fabrication of active biomolecular patterns in countless variety has been established. Reversible COM-mediated nanostructuring is exceptionally suitable for multiplexed patterning of protein assemblies in situ. The first selfassembled protein layer acts as a biocompatible and ductile patterning material. Immobilized proteins can be replaced by the AFM tip applying COM, and the generated structures can be erased and refilled with different proteins, which are immobilized in a uniform and functional manner. Multi-protein arrays can be systematically fabricated by iterative erase-and-write processes, and employed for protein-protein interaction analysis. Fabrication of two-dimensionally arranged nanocatalytic centres with biological activity will establish a versatile tool for nanobiotechnology. As an alternative chip fabrication approach, the combined application of methodologies from surface chemistry, semiconductor technology, and chemical biology demonstrated successfully how pre-patterned templates for micro- and nanoarrays for protein chips are fabricated. The surface physical, as well the biophysical experiments, proved the functionality of this technology. The promises of such process technology are fast and economic fabrication of ready-to-use nanostructured biochips at industrial scale. Membrane proteins are complicated in handling and hence require sophisticated solutions for chip technological application. A silicon-on-insulator (SOI) chip substrate with microcavities and nanopores was employed for first technological investigation to construct a protein chip suitable for membrane proteins. The formation of an artificial lipid bilayer using vesicle fusion on oxidized SOI cavity substrates was verified by CLSM. Future AFM experiments will give further insights into the chip architecture and topography. This will provide last evidence of the sealing of the cavity by the lipid bilayer. Transmembrane proteins will be employed for reconstitution experiments on this membrane protein chip platform. Highly integrated microdevices will find application in basic biomedical and pharmaceutical research, whereas robust and portable point-of-care devices will be used in clinical settings.
An application of EPR spectroscopy that is becoming increasingly important is the measurement of distances between electron spins. Several EPR methods have been developed for this purpose, all based on measuring the dipolar coupling between two spins. Due to the specific nature of the sample, we applied dipolar relaxation enhancement measurements to study the geometry of a protein-protein complex. The paramagnetic centers in question had EPR spectra that were too broad and had such short relaxation time that they could not be studied using the more straightforward PELDOR technique. EPR spectral resolution can be increased appreciably by measuring at a frequency higher than conventional X-band (9 GHz) frequency. The spectra of many paramagnetic species can only be resolved at frequencies higher than 90 GHz. For accurate measurement of the orientation of the vector between two dipolar coupled spins with respect to the g-tensors of the spins, high spectral resolution is required. We therefore performed our EPR measurements at G-band (180 GHz) frequency. Dipolar relaxation measurements were applied to study the complex that is formed by the two electron-transfer proteins cytochrome c and cytochrome c oxidase (CcO) from the soil bacterium Paracoccus denitrificans. We were able to detect dipolar relaxation enhancement due to complex formation of soluble subunit II of P.d. CcO (CcOII) with two substrate cytochromes, which was practically absent in a mixture of CcOII with the negative control protein cytochrome c1. This complex formation was characterized by a pronounced temperature dependence that could be simulated using a home-written computer program. The G-band EPR measurements could not be simulated with a single complex geometry. This provided evidence for the hypothesis that electron-transfer protein complexes are short-lived and highly dynamic; they do not seem to form one specific electron-transfer conformation, but rather move around on each other’s binding surfaces and transfer an electron as soon as the distance between donor and acceptor is short enough. As a test of our simulation program, we also applied dipolar relaxation measurements to specially synthesized organic molecules that contained a nitroxide radical and a metal center. The transverse relaxation of Cu2+-OEP-TPA was compared to the relaxation of Ni2+-OEP-TPA at temperatures between 20 and 120 K. In this temperature range, the nitroxide relaxation was enhanced due to the presence of Cu2+, but not by Ni2+. Similarly, relaxation enhancement was found in the nitroxide-Mn2+ pair in Mn2+-terpyridine-TPA with respect to the terpyridine-TPA ligand. Due to the fast T2 relaxation of the nitroxide radical at high temperatures, the measurements were all performed in the low-temperature regime where the T1 relaxation rate of the metal ion was smaller than the dipolar coupling frequency. In this region, no structural information about the molecule can be deduced, since the dipolar relaxation enhancement is only determined by the T1 of the metal ion. The dipolar relaxation measurements we performed at high field indicated a difference in relaxation times between X-band and G-band frequencies. Extensive T1 - measurements of different paramagnetic centers (CuA, Cu2+) confirmed a strong dependence of T1 on magnetic field in the temperature range where the direct process is the dominating T1 relaxation process. This dependence is very strong (factor of 103 with respect to X-band), but does not follow the B04 dependence predicted in literature. The T1 relaxation of low-spin iron in cytochrome c at high magnetic field, estimated from dipolar relaxation data, is also in agreement with a larger contribution by the direct process (factor of 104). Dipolar relaxation enhancement was found to be a technique that is useful for measuring distances between paramagnetic centers, but only for systems where several important conditions are met, such as: the system exists in one certain static geometry, and the relaxation rate of the fast-relaxing spin is faster than the dipolar coupling frequency within the accessible temperature range. Additionally, it is a great advantage for the analysis of dipolar relaxation data if the procedure of dividing the relaxation trace of the dipolar-coupled slow-relaxing spin by the relaxation trace of the slow-relaxing spin in absence of dipolar coupling can be applied. Another useful application of dipolar relaxation enhancement measurements is the measurement of T1 relaxation of extremely fast-relaxing spins, or spins that are otherwise difficult to detect.
Die vorliegende Arbeit behandelt die Entwicklung und Überprüfung von Modellen zur Berechnung von Schwingungspektren von Peptiden und Proteinen. Solche Modelle verbinden die Konformationsstruktur eines Moleküls mit seinen Schwingungseigenschaften und sind demzufolge wichtig für die Interpretation der Schwingungspektren. Die im Rahmen dieser Arbeit durchgeführte theoretische Erforschung dieses Gebietes beschränkt sich auf die Betrachtung der Amide-I-Moden, welche aufgrund ihrer physikalischen Eigenschaften sich zur Untersuchung der Peptidkonformationen eignen. Die Arbeit kann prinzipiell in zwei Teile separiert werden. In dem ersten Teil werden Fragen betrachtet, die mit der Entwicklung des Schwingungshamiltonian verbunden sind. Im zweiten Teil wurden die erhaltenen Hamiltonian für die Berechnung der Schwingungspektren verwendet. Bei der Berechnung der Schwingungspektren wurden verschiedene spektroskopische Näherungen verwendet und erforscht. Die Entwicklung des Schwingungshamiltonian beinhaltet zwei Aufgaben. Die ab initio Parametrisierung des Schwingungshamiltonian von Dipeptiden, sowie die Analyse der Entwicklungsmethoden für Schwingungshamiltonian von Polypeptiden. Die Entwicklungsmethoden stützen sich auf ab initio berecheten Schwingungseigenschaften von Dipeptiden und/oder elektrostatische Modelle. Die ab initio Parametrisierung basiert auf einer Geometrieoptimierung und anschließender Berechnung von Normalmoden. Hierbei wurde die Abhängigkeit der Ergebnisse vom theoretischen Niveau und dem verwendeten Basissatz untersucht. Die Transformation der errechneten Normalmoden lieferte die Schwingungseigenschaften der lokale Amide-I-Mode. Die Lokalisierung der Normalmode folgt diversen Kriterien. Sie ist von der Wahl der Lokalmoden und somit implizit auch von der Art der Geometrieoptimierung abhängig. Mit dieser Arbeit konnte die Abhängigkeit der Ergebnisse von der Parameterwahl weitgehend aufgeklärt und eine für das Amide-I-System geeignet Parametrisierung gefunden werden. Im nächsten Arbeitsschritt wurde die Abhängigkeit der Amide-I-Schwingungseigenschaften von den Peptidseitenketten und terminalen Gruppen untersucht. Desweiteren wurden Methoden zur Formulierung der Hamiltonian für Polypeptide konzeptionell entwickelt. Diese Untersuchung ist außerordentlich wichtig, da direkte quantenmechanische Berechnungen von Polypeptiden zu zeitaufwendig sind. Solche Methoden beruhen auf dem sogenannten “Building-Block”-Ansatz und verschiedenen elektrostatischen Modellen. In dieser Arbeit wurden sowohl die einzelnen Methoden als auch ihre Kombination für die Entwicklung des Hamiltonians verwendet. Zur Abschätzung der Genauigkeit der verwendeten Methoden wurden Vergleichsrechnungen durchgeführt. Im zweiten Teil dieser Arbeit wurden die erhaltenen Schwingungshamiltonian zur Berechnung von Schwingungsspektren diverser gelöster Peptide angewandt. In diesem Zusammenhang konnte die Genauigkeit unterschiedlicher spektroskopischer Approximationen überprüft werden. Auf Grundlage der erhaltenen Ergebnisse können wir sagen, dass eine angemessene Beschreibung der konformationellen Verteilung und eine korrekte Berechnung des dynamischen Absorptionsspektrum gewährleistet ist. Was noch fehlt, ist ein hinreichend genaues quantenchemisches Modell für die Schwingungsfrequenzen eines gelösten Peptids. Diese Aufgabe stellt zur Zeit ein aktives Forschungsgebiet dar. Zuletzt wurde das Schwingungsspektrum eines sogenanten “Photoschaltbaren”-Peptids simuliert. Mit Hilfe des dafür aufgestellten Hamiltonians ist man in der Lage spektroskopische Beobachtungen auf Konformationsänderungen direkt zu übertragen.