@article{SchmittKuperEliasetal.2014,
  author    = {Schmitt, Dominik R. and Kuper, Jochen and Elias, Agnes and Kisker, Caroline},
  title     = {The Structure of the TFIIH p34 Subunit Reveals a Von Willebrand Factor A Like Fold},
  series = {PLoS ONE},
  volume    = {9},
  journal   = {PLoS ONE},
  number    = {7},
  issn      = {1932-6203},
  doi       = {10.1371/journal.pone.0102389},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-119471},
  pages     = {e102389},
  year      = {2014},
  abstract  = {RNA polymerase II dependent transcription and nucleotide excision repair are mediated by a multifaceted interplay of subunits within the general transcription factor II H (TFIIH). A better understanding of the molecular structure of TFIIH is the key to unravel the mechanism of action of this versatile protein complex within these vital cellular processes. The importance of this complex becomes further evident in the context of severe diseases like xeroderma pigmentosum, Cockayne's syndrome and trichothiodystrophy, that arise from single point mutations in TFIIH subunits. Here we describe the structure of the p34 subunit of the TFIIH complex from the eukaryotic thermophilic fungus Chaetomium thermophilum. The structure revealed that p34 contains a von Willebrand Factor A (vWA) like domain, a fold which is generally known to be involved in protein-protein interactions. Within TFIIH p34 strongly interacts with p44, a positive regulator of the helicase XPD. Putative protein-protein interfaces are analyzed and possible binding sites for the p34-p44 interaction suggested.},
  language  = {en}
}
@phdthesis{Schmidt2015,
  author    = {Schmidt, Thomas Christian},
  title     = {Theoretical Investigations on the Interactions of Small Compounds with their Molecular Environments},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-127860},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2015},
  abstract  = {Im ersten Teil dieser Arbeit wird eine Kombination theoretischer Methoden f{\"u}r die strukturbasierte Entwicklung neuer Wirkstoffe pr{\"a}sentiert. Ausgehend von der Kristallstruktur eines kovalenten Komplexes einer Modellverbindung mit dem Zielprotein wurde mit Hilfe von quantenmechanischen und QM/MM Rechnungen die genaue Geometrie des vorausgehenden nicht-kovalenten Komplexes betimmt. Letztere ist der bestimmende Faktor f{\"u}r die Reaktivit{\"a}t des Inhibitors gegen{\"u}ber der katalytisch aktiven Aminos{\"a}ure und damit f{\"u}r die Ausbildung einer kovalenten Bindung. Aus diesem Grund wurde diese Geometrie auch f{\"u}r die Optimierung der Substitutionsmusters des Ihnibitors verwendet, um dessen Affinit{\"a}t zum Zielenzyme zu verbessern ohne dass dieser seine F{\"a}higkeit kovalent an das aktive Zentrum zu binden verliert. Die Optimierung des Substitutionsmuster wurde doch Methode des Molekularen Dockings unterst{\"u}tzt, das diese optimal dazu geeignet sind, Bindungsaffinit{\"a}ten vorherzusagen, die durch eine Modifikation der chemischen Struktur entstehen. Eine Auswahl der besten Strukturen wurde anschließend verwendet, um zu {\"u}berpr{\"u}fen, ob die ver{\"a}nderten Molek{\"u}le noch gen{\"u}gen Reaktivit{\"a}t gegen{\"u}ber dem Zielprotein aufweisen. Molek{\"u}ldynamik Simulationen der neuen Verbindungen haben jedoch gezeigt, dass die ver{\"a}nderten Verbindungen nur so and das Protein binden, dass die Bilung eine kovalenten Bindung zum Enzym nicht mehr m{\"o}glich ist. Daher wurden in einem weiteren Schritt die Modellverbindungen weiter modifiziert. Neben {\"A}nderungen im Substitutionsmuster wurde auch die chemische Struktur im Kern ver{\"a}ndert. Die Bindungsaffinit{\"a}ten wurde wieder mittels Docking {\"u}berpr{\"u}ft. F{\"u}r die besten Bindungsposen wurden wieder Simulationen zur Molek{\"u}ldynamik durchgef{\"u}hrt, wobei diesmal die Ausbildung einer kovalenten Bindung zum Enzyme m{\"o}glich erscheint. In einer abschließenden Serie von QM/MM Rechnungen unter Ber{\"u}cksichtigung verschiedener Protonierungszust{\"a}nde des Inhibitors und des Proteins konnten Reaktionspfade und zugeh{\"o}rige Reaktionsenergien bestimmt werden. Die Ergebnisse lassen darauf schließen, dass eines der neu entwickelten Molek{\"u}le sowohl eine stark verbesserte Bindungsaffinit{\"a}t wie auch die M{\"o}glichkeit der kovalenten Bindung an Enzyme aufweist. Der zweite Teil der Arbeit konzentriert sich auf die Umgebungseinfl{\"u}sse auf die Elektronenverteilung eines Inhibitormodells. Als Grundlage dient ein vinylsulfon-basiertes Moek{\"u}l, f{\"u}r das eine experimentell bestimmte Kristallstruktur sowie ein theoretisch berechneter Protein Komplex verf{\"u}gbar sind. Ein Referendatensatz f{\"u}r diese Systeme wurde erstellt, indem der Konformationsraum des Inhibitors nach m{\"o}glichen Minimumsstrukturen abgesucht wurde, welche sp{\"a}ter mit den Geometrien des Molek{\"u}ls im Kristall und im Protein verglichen werden konnten. The Geometrie in der Kristallumgebung konnte direkt aus den experimentellen Daten {\"u}bernommen werden. Rechnungen zum nicht-kovalenten Protein Komplex hingegen haben gezeigt, dass f{\"u}r das Modellsystem mehrere Geometrien des Inhibiors sowie zwei Protonierungszust{\"a}nde f{\"u}r die katalytisch aktiven Aminos{\"a}uren m{\"o}glich sind. F{\"u}r die Analyse wurden daher alle m{\"o}glichen Proteinkomplexe mit der Kristallstruktur verglichen. Ebenso wurden Vergleiche mit der Geometrie des isolierten Molek{\"u}ls im Vakuum sowie der Geometrie in w{\"a}ssriger L{\"o}sung angestellt. F{\"u}r die Geometrie des Molek{\"u}ls an sich ergab sich eine gute {\"U}bereinstimmung f{\"u}r alle Modellsysteme, f{\"u}r die Wechselwirkungen mit der Umgebung jedoch nicht. Die Ausbildung von Dimeren in der Kristallumgebung hat einen stark stablisierenden Effekt und ist einer der Gr{\"u}nde, warum dieser Kristall so gut wie keine Fehlordungen aufweist. In den Proteinkomplexen hingegen ergibt sich eine Abstoßung zwischen dem Inhibitor und einer der katalytisch aktiven Aminos{\"a}uren. Als Ursache f{\"u}r diese Abstoßung konnte die Einf{\"u}hrung der Methylaminfunktion ausgemacht werden. Vermutlicherweise f{\"u}hrt diese strukturelle {\"A}nderung auch dazu, dass der Modellinhibitor nicht in der Lage ist, so wie die Leitstruktur K11777 an das aktive Zentrum des Enzyms zu binden.},
  subject      = {Theoretische Chemie},
  language  = {en}
}
@phdthesis{Roger2024,
  author    = {Roger, Chantal},
  title     = {Photophysics and Spin Chemistry of Triptycene Bridge Donor-Acceptor-Triads},
  doi       = {10.25972/OPUS-36303},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-363031},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2024},
  abstract  = {The goal of this thesis was to investigate the influence of rotational restriction between individual parts and of the varying electron density in the bridging unit of D B A systems on the exchange interaction 2J, and thus the electronic coupling between a donor state and an acceptor state. A better understanding of how to influence the underlaying spin dynamics in such donor acceptor systems can open up the door to new technologies, such as modern molecular electronics or optoelectronic devices. Therefore, three series of molecules consisting of a TAA electron donor, a TTC or ATC bridging unit and a PDI electron acceptor were studied. To investigate the influence of rotational restriction on 2J and the electronic coupling, a series of four rotationally hindered triads (chapter 6) was synthesised. The dihedral angle between the TAA and the TTC as well as between the TTC and the PDI was restricted by ortho methyl groups at the phenylene linkers of the connecting ends to the TTC bridge, producing a twist around the linking single bond which minimises the π overlap. The triads exhibit varying numbers of ortho methyl groups and therefore different degrees of rotational restriction. In order to shine light on the influence of varying electron density on 2J and the electronic coupling, a series of four substituted triptycene triads (chapter 7) was synthesised. The electron density in the TTC bridging unit was varied by electron donating and electron withdrawing groups in 12,13 position of the TTC bridging unit and thus varying its HOMO/LUMO energy. The last series of two anthracene bridge triads (chapter 8) connected both approaches by restricting the rotation with ortho methyl groups and simultaneously by varying the bridge energies. In order to obtain the electronic properties, steady state absorption and emission spectra of all triads were investigated (chapter 4). Here, all triads show spectral features associated with the separate absorption bands of TAA and the PDI moiety. The reduced QYs, compared to the unsubstituted PDI acceptor, indicate a non radiative quenching mechanism in all triads. The CV data (chapter 5) were used to calculate the energies of possible CSSs and those results were used to assign the CR dynamics into the different Marcus regions. fs TA measurements reveal that all triads form a CSS upon excitation of the PDI moiety. The lifetimes of the involved states and the rate constants were determined by global exponential fits and global target analysis. The CR dynamics upon depopulation of the CSSs were investigated using external magnetic field dependent ns TA spectroscopy. The ns TA maps show that all triads recombine via CRT pathway populating the local 3PDI state in toluene and provided the respective lifetimes. The approximate QYs of triplet formation were determined using actinometry. The magnetic field dependent ns TA data reveal the exchange interaction 2J between singlet and triplet CSS for each triad. Those magnetic field dependent ns TA data in toluene were furthermore treated using a quantum mechanical simulation (done by U.E. Steiner) to extract the rate constants kT and kS for CRT and CRS, respectively. However, the error margins of kS were rather wide. Finally, the electronic couplings between the donor and the acceptor states were obtained by combining the aforementioned experimental results of the rate constants and applying the Bixon Jortner theoretical description of diabatic ET and Andersons perturbative theory of the exchange coupling. Therefore, the experimentally determined values of 2J and the calculated values of kCS and kT were used. The rate constant kS was calculated based on the electronic coupling V1CSS 1S0. The rotationally hindered triads (chapter 6) show a strong influence of the degree of rotational restriction on the lifetimes and rate constants of the CS processes. The rate constants of CS are increasing with increasing rotational freedom. The magnetic field dependent decay data show that the exchange interactions increase with increasing rotational freedom. Based on the CR dynamics, the calculated electronic couplings of the ET processes reflect the same trend along the series. Here, only singlet couplings turned out to be strongly influenced while the triplet couplings are not. Therefore, this series shows that the ET dynamics of donor acceptor systems can strongly be influenced by restricting the rotational freedom. In the substituted triptycene triads (chapter 7), decreasing electron density in the bridging unit causes a decrease of the CS rate constants. The magnetic field dependent decay data show that with decreasing electron density in the bridge the exchange interaction decreases. The CR dynamics-based rate constants and the electronic couplings follow the same trend as the exchange interaction. This series shows that varying the HOMO/LUMO levels of the connecting bridge between donor and acceptor strongly influences the ET processes. In the anthracene bridge triads (chapter 8), the CS process is slow in both triads. The CR was fast in the anthracene triad and is slowed down in the methoxy substituted anthracene bridge triad. The increase of the exchange interaction with increasing electron density in the bridge was more pronounced than in the substituted triptycene triads. Thus, the variation of electron density in the bridge strongly influences the ET processes even though the rotation is restricted. In this thesis, it was shown that the influence of the rotational hindrance as well as the electron density in a connecting bridge have strong influence on all ET processes and the electronic coupling in donor acceptor systems. These approaches can therefore be used to modify magnetic properties of new materials.},
  subject      = {Rotation},
  language  = {en}
}