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Institute
- Theodor-Boveri-Institut für Biowissenschaften (124)
- Graduate School of Life Sciences (62)
- Universität - Fakultätsübergreifend (50)
- Physikalisches Institut (38)
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- Klinik und Poliklinik für Psychiatrie, Psychosomatik und Psychotherapie (26)
- Institut für Molekulare Infektionsbiologie (25)
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Sonstige beteiligte Institutionen
- Clinical Trial Center (CTC) / Zentrale für Klinische Studien Würzburg (ZKSW) (3)
- Röntgen Center for Complex Material Systems (RCCM), Am Hubland, 97074 W¨urzburg, Germany (2)
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ResearcherID
- I-5818-2014 (1)
Kardiomyopathien sind Erkrankungen des Herzmuskels, die mit einer kardialen Funktionsstörung einhergehen. Formen, die ohne erkennbare Ursache zu einer progredienten Dilatation und Reduktion der Kontraktilität des linken Ventrikels führen, werden als idiopathische dilatative Kardiomyopathie (DCM) bezeichnet. Sie ist der Hauptgrund für schwere Herzinsuffizienz und die damit assoziierten Einschränkungen der Lebensqualität bei jungen Erwachsenen. Neben der beeinträchtigten kardialen Funktion weisen diese Patienten oftmals auch Veränderungen im Bereich der humoralen und zellulären Immunität auf. Ein Teil der Patienten entwickelt Autoantikörper, die sich gegen den kardialen β1-adrenergen Rezeptor richten und ihn ähnlich wie der natürliche Ligand Adrenalin aktivieren. Hieraus resultiert eine chronische Überstimulation des Rezeptors, die über eine initiale Hypertrophie dann zu einer eingeschränkten Pumpfunktion führt.
Nachdem sich die Therapie der Antikörper-vermittelten Immunkardiomyopathie bisher auf die Behandlung der Herzinsuffizienz und die Kontrolle der Herz-insuffizienzsymptome beschränkt, könnten β1-ECII-homologe Peptide als Antikörper-Fänger bei Antikörper-positiven Patienten nun einen kausalen Therapieansatz darstellen. In diesem Zusammenhang wurden ein aus 25 Aminosäuren bestehendes zyklisches Peptid, eine aus 18 Aminosäuren bestehende Zyklopeptid-Mutante und ihre jeweiligen linearen Äquivalente im Rattenmodell auf Antikörper-neutralisierende Effekte und potentielle therapeutische Wirksamkeit getestet. Das Rattenmodell ist hierfür besonders geeignet, da die Aminosäuresequenz der funktionell wichtigen zweiten extrazellulären Domäne des β1-adrenergen Rezeptors (β1-ECII) bei Mensch und Ratte absolut identisch ist.
Auf immunologischer Ebene konnte der Titer der krankheitsinduzierenden β1-ECII-Antikörper bereits nach der ersten Applikation zyklischer Peptide relevant gesenkt werden und nahm im weiteren Verlauf der Behandlung kontinuierlich ab. Nach Zyklopeptidgabe kam es am Herzen zu einer Reduktion des linksventrikulären Durchmessers und zu einer fast vollständigen Normalisierung der anatomischen Proportionen. Auf die Morphologie der Myozyten selbst und auch den Kollagengehalt des Gewebes hatte die Zyklopeptidtherapie keinen wesentlichen Einfluss. Die funktionellen Eigenschaften des Herzens ließen sich durch die Neutralisation stimulatorischer β1-ECII-Antikörper mittels intravenöser Zyklopeptidapplikation deutlich verbessern: Die Verkürzungsfraktion des linken Ventrikels und der Herzindex als Parameter für die kardiale Leistungsfähigkeit konnten durch die Behandlung wieder weitgehend normalisiert werden.
Diese im Tiermodell erzielten Ergebnisse lassen einen therapeutischen Effekt der Zyklopeptide vermuten. Der Ansatz einer spezifisch gegen Antikörper gerichteten Therapie zur Behandlung von Patienten mit β1-Antikörper-positiver Herzinsuffizienz erscheint daher vielversprechend.
The discovery of the Giant Magneto Resistance (GMR) effect in 1988 by Albert Fert [Baib 88] and Peter Grünberg [Bina 89] led to a rapid development of the field of spintronics and progress in the information technology. Semiconductor based spintronics, which appeared later, offered a possibility to combine storage and processing in a single monolithic device. A direct result is reduced heat dissipation. The observation of the spin Seebeck effect by Ushida [Uchi 08] in 2008 launched an increased interest and encouraged research in the field of spin caloritronics. Spintronics is about the coupling of charge and spin transport. Spin caloritronics studies the interaction between heat and spin currents. In contrast to spintronics and its variety of applications, a particular spin-caloritronic device has not yet been demonstrated. However, many of the novel phenomena in spin caloritronics can be detected in most spintronic devices. Moreover, thermoelectric effects might have a significant influence on spintronic device operation. This will be of particular interest for this work. Additional knowledge on the principle of coupling between heat and spin currents uncovers an alternative way to control heat dissipation and promises new device functionalities.
This thesis aims to further extend the knowledge on thermoelectrics in materials with strong spin-orbit coupling, in this case the prototypical ferromagnetic semiconductor (Ga,Mn)As. The study is focused on the thermoelectric / thermomagnetic effects at the interface between a normal metal and the ferromagnetic (Ga,Mn)As. In such systems, the different interfaces provide a condition for minimal phonon drag contribution to the thermal effects. This suggests that only band contributions (a diffusion transport regime) to these effects will be measured.
Chapter 2 begins with an introduction on the properties of the studied material system, and basics on thermoelectrics and spin caloritronics. The characteristic anisotropies of the (Ga,Mn)As density of states (DOS) and the corresponding magnetic properties are described. The DOS and magnetic anisotropies have an impact on the transport prop- erties of the material and that results in effects like tunneling anisotropic magnetores- istance (TAMR) [Goul 04]. Some of these effects will be used later as a reference to the results from thermoelectric / thermomagnetic measurements. The Fingerprint tech- nique [Papp 07a] is also described. The method gives an opportunity to easily study the anisotropies of materials in different device geometries.
Chapter 3 continues with the experimental observation of the diffusion thermopower of (Ga,Mn)As / Si-doped GaAs tunnel junction. A device geometry for measuring the diffusion thermopower is proposed. It consists of a Si - doped GaAs heating channel with a Low Temperature (LT) GaAs / (Ga,Mn)As contact (junction) in the middle of the channel. A single Ti / Au contact is fabricated on the top of the junction. For transport characterization, the device is immersed in liquid He. A heating current technique is used to create a temperature difference by local heating of the electron system on the Si:GaAs side. An AC current at low frequency is sent through the channel and it heats the electron population in it, while the junction remains at liquid He temperature (experimentally con- firmed). A temperature difference arises between the heating channel and the (Ga,Mn)As contact. As a result, a thermal (Seebeck) voltage develops across the junction, which we call tunnelling anisotropic magneto thermopower (TAMT), similar to TAMR. TAMT is detected by means of a standard lock-in technique at double the heating current frequency (at 2f ). The Seebeck voltage is found to be linear with the temperature difference. That dependence suggests a diffusion transport regime. Lattice (phonon drag) contribution to the thermovoltage, which is usually highly nonlinear with temperature, is not observed.
The value of the Seebeck coefficient of the junction at 4.2 K is estimated to be 0.5 µV/K.
It is about three orders of magnitude smaller than the previously reported one [Pu 06]. Subsequently, the thermal voltage is studied in external magnetic fields. It is found that the thermopower is anisotropic with the magnetization direction. The anisotropy is explained with the anisotropies of the (Ga,Mn)As contact. Further, switching events are detected in the thermopower when the magnetic field is swept from negative to positive fields. The switchings remind of a spin valve signal and is similar to the results from previous experiments on spin injection using a (Ga,Mn)As contacts in a non-local detection scheme. That shows the importance of the thermoelectric effects and their possible contribution to the spin injection measurements. A polar plot of the collected switching fields for different magnetization angles reveals a biaxial anisotropy and resembles earlier TAMR measurements of (Ga,Mn)As tunnel junction. A simple cartoon model is introduced to describe and estimate the expected thermopower of the studied junction. The model yields a Fermi level inside of the (Ga,Mn)As valence band. Moreover, the model is found to be in good agreement with the experimental results.
The Nernst effect of a (Ga,Mn)As / GaAs tunnel junction is studied in Chapter 4. A modified device geometry is introduced for this purpose. Instead of a single contact on the top of the square junction, four small contacts are fabricated to detect the Nernst signal. A temperature difference is maintained by means of a heating current technique described in Chapter 3. A magnetic field is applied parallel to the device plane. A voltage drop across two opposite contacts is detected at 2f. It appears that a simple cosine function with a parameter the angle between the magnetization and the [100] crystal direction in the (Ga,Mn)As layer manages to describe this signal which is attributed to the anomalous Nernst effect (ANE) of the ferromagnetic contact. Its symmetry is different than the Seebeck effect of the junction. For the temperature range of the thermopower measurements the ANE coefficient has a linear dependence on the temperature difference (∆T). For higher ∆T, a nonlinear dependence is observed for the coefficient. The ANE coefficient is found to be several orders of magnitude smaller than any Nernst coefficient in the literature. Both the temperature difference and the size of the ANE coefficient require further studies and analysis. Switching events are present in the measured Nernst signal when the magnetic field is swept from positive to negative values. These switchings are related to the switching fields in the ferromagnetic (Ga,Mn)As. Usually, there are two states which are present in TAMR or AMR measurements - low and high resistance. Instead of that, the Nernst signal appears to have three states - high, middle and low thermomagnetic voltage. That behaviour is governed not only by the magnetization, but also by the characteristic of the Nernst geometry.
Chapter 5 summarizes the main observations of this thesis and contains ideas for future work and experiments.
Es werden Daten zur Entwicklung von 99 Kindern zwischen 13 und 36 Monaten, die in deutschen Kindertagesstätten betreut wurden, für die Bereiche Motorik, Sprache vorgestellt. Die Erhebung beruht auf dem Konzept des Pikler-Instituts in Budapest/Ungarn, mit dem die Entwicklung von mehreren tausend Kindern dokumentiert wurde. In den vorläufigen Schlussfolgerungen werden die aktuellen Diskussionen zur Tagesbetreuung von Kleinkindern berücksichtigt.
Der Wnt Signalweg spielt eine entscheidende Rolle in der Embryogenese durch Steuerung der Proliferation, Apoptose, Differenzierung und der Festlegung der Körperachsen im frühen Embryo. Eine Fehlregulation des Signalwegs durch Mutationen in einem der Proteine und Gene dieser hochkomplexen Signalkaskade kann fatale Folgen haben, und ist ein erster Schritt auf dem Weg der Krebsentstehung. Dabei spielt das Protein β-Catenin eine Schlüsselrolle im kanonischen Zweig des Wnt Signalwegs. Durch Steuerung seiner Konzentration im Zytoplasma wird die Expression seiner direkten Zielgene reguliert, da β-Catenin im aktiven Signalweg als Co-Transkriptionsfaktor agiert. Durch Sichtbarmachung dieses Proteins durch fluoreszierende Reportergenkonstrukte kann der Aktivitätsstatus des Wnt Signalwegs in der Zelle beobachtet werden. Das ermöglicht zum einen genaue Analysen des Signalwegs, wie zum Beispiel das Studium des Zusammenspiels mit anderen Signalwegen. Vor allem aber erlaubt es die gezielte Suche nach Wnt-Signalwegs-modulierenden Substanzen als potentielle Wirkstoffe in der Krebsmedikamentenentwicklung. In der vorliegenden Arbeit wurden mehrere Reportergenkonstrukte für die stabile Transfektion von Zelllinien entwickelt und hinsichtlich eines möglichen Einsatzes sowohl in der Forschung, als auch in Wirkstoffscreenings validiert. Dies umfasst sowohl mehrere Reporter mit β-Catenin als Fusionsprotein, als auch Wnt-Promoter-regulierte eGFP-Reporter, die den Akitvitätsstatus des Wnt-Signalwegs anzeigen. Mit Hilfe dieser Reporter konnten Untersuchungen zur Wirkung des Wnt-Signalwegs auf die Morphologie von transfizierten und nicht-transfizierten MDCK-Zellen durchgeführt werden. Überdies wurde ein promotorregulierter eGFP-Reporter konstruiert, mit welchem transfizierte Zellen mit aktiviertem Wnt-Signalweg aus einem Zellpool gefischt werden können. Diese Methode ist sowohl für den Einsatz in kultivierten Zelllinien, als auch in der Diagnostik nach der Transfektion primärer Zellen geeignet. Auf Grundlage der neuen Zelllinien wurde weiterhin ein neuer Screeningansatz für potentielle Wnt-Signalwegsinhibitoren entwickelt, der auf dem Ausbleichen der Fluoreszenz in einem Well einer Multiwell-Kulturplatte beruht.
In this work the synthesis of dendritic macromolecules and small redox cascades was reported and studies of their energy and electron transfer properties discussed.
The chromophores in the dendrimers and the redox cascades are linked via triazoles, which were built up by CuAAC. Thereby, a synthetic concept based on building blocks was implemented, which allowed the exchange of all basic components. Resulting structures include dendrimers composed exclusively of TAAs (G1–G3), dendrimers with an incorporated spirobifluorene core (spiro-G1 and spiro-G2) and the donor-acceptor dendrimer D-A-G1, in which the terminal groups are exchanged by NDIs.
Furthermore, a series of model compounds was synthesised in order to achieve a better understanding of the photophysical processes in the dendrimers.
A modification of the synthetic concept for dendrimers enabled the synthesis of a series of donor-acceptor triads (T-Me, T-Cl and T-CN) consisting of two TAA donors and one NDI acceptor unit. The intermediate TAA chromophore ensured a downhill redox gradient from the NDI to the terminal TAA, which was proved by cyclic voltammetry measurements. The redox potential of the intermediate TAA was adjusted by different redox determining substituents in the “free” p-position of the TAA. Additionally, two dyads (Da and Db) were synthesised which differ in the junction of the triazole to the TAA or the NDI, respectively. In these cascades a nodal-plane along the N-N-axes in the NDI and a large twist angle between the NDI and the N-aryl substituent guaranteed a small electronic coupling.
The photophysical investigations of the dendrimers focused on the homo-energy transfer properties in the TAA dendrimers G1–G3. Steady-state emission spectroscopy revealed that the emission takes place from a charge transfer state. The polar excited state resulted in a strong Stokes shift of the emission, which in turn led to a small spectral overlap integral between the absorption of the acceptor and the emission of the donor in the solvent relaxed state. According to the Förster theory, the overlap integral strongly determines the energy transfer rate. Fluorescence up-conversion measurements showed a strong and rapid initial fluorescence anisotropy decay and a much slower decrease on the longer time scale. The experiment revealed a fast energy transfer in the first 2 ps followed by a much slower energy hopping. Time resolved emission spectra (TRES) of the model compound M indicated a solvent relaxation on the same time scale as the fast energy transfer.
The Förster estimation of energy transfer rates in G1 explains fast energy transfer in the vibrotionally relaxed state before solvent relaxation starts. Thereby, the emission spectrum of G1 in cyclohexane served as the time zero spectrum. Thus, solvent relaxation and fast energy transfer compete in the first two ps after excitation and it is crucial to discriminate between energy transfer in the Franck-Condon and in the solvent relaxed state. Furthermore, this finding demonstrates that fast energy transfer occurs even in charge transfer systems where a large Stokes shift prevents an effective spectral overlap integral if there is a sufficient overlap integral in before solvent relaxation.
Energy transfer upon excitation was also observed in the spiro dendrimers spiro-G1 and spiro-G2 and identified by steady-state emission anisotropy measurements. It was assumed that the energy in spiro-G1 is completely distributed over the entire molecule while the energy in spiro-G2 is probably distributed over only one individual branch. This finding was based on a more polarised emission of spiro-G2 compared to spiro-G1. This issue has to be ascertained by e.g. time resolved emission anisotropy measurements in further energy transfer studies.
Concerning the electron transfer properties of TAA-triazole systems the radical cations of G1–G2, spiro-G1 and spiro-G2 and of the model compound M were investigated by steady-state absorption spectroscopy. Experiments showed that the triazole bridge exhibits small electronic communication between the adjacent chromophores but still possesses sufficient electronic coupling to allow an effective electron transfer from one chromophore to the other.
Due to the high density of chromophores, their D-A-D structure and their superficial centrosymmetry, the presented dendrimers are prospective candidates for two-photon absorption applications.
The dyads, triads and the donor-acceptor dendrimer D-A-G1 were investigated regarding their photoinduced electron transfer properties and the effects that dominate charge separation and charge recombination in these systems.
The steady-state absorption spectra of all cascades elucidated a superposition of the absorption characteristics of the individual subunits and spectra indicated that the chromophores do not interact in the electronic ground state.
Time resolved transient absorption spectroscopy of the cascades was performed in the fs- and ns-time regime in MeCN and toluene as solvent. Measurements revealed that upon with 28200 cm-1 (355) nm and 26300 cm-1 (380 nm), respectively, an electron is transferred from the TAA towards the NDI unit yielding a CS state. In the triads at first a CS1 state is populated, in which the NDI is reduced and the intermediate TAA1 is oxidised. Subsequently, an additional electron transfer from the terminal TAA2 to TAA1 led to the fully CS2 state. Fully CS states of the dyads and triads exhibit lifetimes in the ns-time regime. In contrast for Db in MeCN, a lifetime of 43 ps was observed for the CS state together with the population of a 3NDI state. The signals of the other CS states decay biexponentially, which is a result of the presence of the 1CS and the 3CS states. While magnetic field dependent measurements of Db did not show an effect due to the large singlet-triplet splitting, T-CN exhibited a strong magnetic field dependence which is an evidence for the 1CS/3CS assignment. Further analysis of the singlet-triplet dynamics are required and are currently in progress.
Charge recombination occurred in the Marcus inverted region for compounds solved in toluene and in the Marcus normal region for MeCN as solvent. However, a significant inverted region effect was observed only for Db. Triads are probably characterised by charge recombination rates in the inverted and in the normal region near to the vertex of the Marcus parabola. Hence the inverted region effect is not pronounced and the rate charge recombination rates are all in the same magnitude. However, compared to the charge recombination rate of Db the enlarged spatial distance between the terminal TAA and the NDI in the fully CS2 states in the triads resulted in reduced charge recombination rates by ca. one order of magnitude.
More important than a small charge recombination rate is an overall lifetime of the CS states and this lifetime can significantly be enhanced by the population of the 3CS state. The reported results reveal that a larger singlet-triplet splitting in the dyads led to a CS state lifetime in the us time regime while a lifetime in the ns-time regime was observed in cases of the triads. Moreover, the singlet-triplet splitting was found to be solvent dependent in the triads, which is a promising starting point for further investigations concerning singlet-triplet splitting.
The donor-acceptor dendrimer D-A-G1 showed similar characteristics to the dyads. The generation of a CS state is assumed due to a clear NDI radical anion band in the transient absorption spectrum. Noteworthy, the typical transient absorption band of the TAA radical cation is absent for D A-G1 in toluene. Bixon-Jortner analysis yielded a similar electronic coupling in D-A-G1 compared to the dyads. However, the charge recombination rate is smaller than of Db due to a more energetic CS state, which in the inverted region slows down charge recombination. In combination a singlet-triplet splitting similar to the dyads prolongs the CS state lifetime up to 14 us in diluted solution. Both effects result in an even better performance of D-A-G1 concerning energy conversion. D A-G1 is therefore a promising key structure for further studies on light harvesting applications. In a prospective study a second generation donor-acceptor dendrimer D-A-G2 might be an attractive structure accessible by “click reaction” of 13 and 8. D-A-G2 is expected to exhibit a downhill oriented gradient of CS states as assumed from the CV studies on G1–G3.
In this work the synthesis, the spectroscopic and electrochemical investigation as well as some applications of a broad diversity of indolenine squaraine dyes were presented. This diversity was based on two parent squaraine dyes, one standard trans-configured compound (M1) and one in which one central oxygen atom was replaced by a dicyanomethylene moiety (M2), which increased the acceptor strength and induced a cis-configuration. The variety of synthesised dyes included functionalised squaraine monomers, donor- and acceptor-substituted monomeric model squaraines, donor- and acceptor-squaraine copolymers, pure squaraine homopolymers, a squaraine-squaraine copolymer, as well as some conjugated cyclic oligomers.
In order to be able to synthesise all these different kinds of dyes, several bromine and boronic ester derivatives were synthesised, which enabled the use of the Suzuki cross coupling reaction, to generate model dyes and copolymers. In addition, the bromine derivatives were used to carry out the Yamamoto homocoupling reaction to the respective homopolymers and macrocycles.
The absorption maximum of unsubstituted reference dye M1 was found at ~ 15500 cm–1, while that of M2 was red-shifted to ~ 14300 cm–1 due to the increased acceptor strength of the central unit. The extinction coefficients were in the order of ~ 300000 M–1 cm–1 and ~ 200000 M–1 cm–1, respectively. It was found that the implementation of functional groups (M3–M9), additional electron donors (M10–M19) or acceptors (M20–M22) at the periphery lead to bathochromic shifts of the absorption depending on the strength of either - and/or -donating properties of the substituents.
For the bis- and triarylamine substituted dyes M10–M13 and the dibrominated dyes M5 and M7 the electronic structure of the mono- and diradical (di)cations was explored using the interplay of cyclic voltammetry, spectroelectrochemistry, and DFT calculations. It was demonstrated that the monoradical cations still show a cyanine-like character and are delocalised Robin-Day class III species due to the low redox potential of the squaraine bridge between the additional amine redox centres. To the best of my knowledge, this made M13+∙, with an N-N-distance of 26 bonds between the additional redox centres to the longest bis(triarylamine) radical cation that is completely delocalised. For the diradical dications, the situation was of larger complexity. The computed most stable energetic state of the dianisylamine-substituted dyes turned out to be a broken-symmetry state with almost equal contributions of an open-shell singlet and triplet state. In addition, it was shown that the HOMO–1→HOMO transition dominated the absorption spectra of the diradical dications where the trans-/cis-configuration of the squaraines had a direct impact due to symmetry reasons.
Based on the donor–squaraine model compounds M10–M19, a series of donor–squaraine copolymers was synthesised (P7–P12) in order to further red shift and broaden the low energy absorption band. However, these effects were only of marginal extent. Both the optical and the electrochemical derived band gaps were barely lowered compared to the respective monomeric model dyes. This was assigned to an increased squaraine-squaraine distance and resulting lower exciton coupling between the squaraine chromophores due to the bridging units. In addition, according to semiempirical calculations the bridges were twisted out of the squaraine plane what reduced conjugational effects between the chromophores. To sum up, the idea to insert additional electron rich bridging units in order to create copolymers with broad and red-shifted absorption did not fully work out for the presented systems.
The addition of strong electron accepting NDI units at the periphery resulted in M21, the most unique monomeric model squaraine in this work. The common picture of a sharp low energy squaraine absorption completely altered due to the addition of the NDIs and a rather broad and solvent dependent low energy absorption was found. Spectroelectrochemical experiments and semiempirical calculations showed that this band is a superposition of the common squaraine HOMO→LUMO transition and a partial squaraine→NDI charge transfer transition. The latter was lost upon oxidation of the squaraine and the absorption spectrum of the monocation of M21 was found to be nearly a 1:1 image of a pure squaraine monocation. Both the monomeric model M21 and the respective copolymer P13 showed low electrochemically obtained band gaps of 1.05–1.20 eV, which were the lowest of all squaraines in this work. For both dyes, transient absorption measurements in the fs-time regime revealed the ultrafast formation of a CS state via an intermediate CT state within a few ps. Besides, charge recombination to the ground state also occured within a few ps. In the polymer, there was barely any further energy or charge transfer within the excited state lifetime and therefore the CS state was confined on adjacent squaraine-NDI pairs and did not further travel along the polymer strand.
The Ni-mediated Yamamoto homocoupling reaction was applied for the synthesis of the homopolymers (P1–P5). In contrast to the donor–squaraine copolymers, those polymers revealed strongly red-shifted and broad absorption in the red to NIR region in addition to a sharp fluorescence. These features could be explained to originate mainly from the exciton coupling of localised excited states and the presence of different superstructures in solution. For the polymers P1 and P2, an elongated J-type polymer chain caused the strong lowest energy absorption band whereas a zig-zag type arrangement of the single chromophores lead to transitions into both low and high energy excited states of the excitonic manifold. For the polymers P3 and P4, several polymer fractions of different size were investigated. Here, also an elongated chain with J-type character induced the lowest energy absorption band whereas a helical H-type arrangement caused transitions to higher energies of the excitonic manifold. The fractions to which these structures were formed depended on the chain length and the solvent. In thin film measurements, it was shown that the initially in solution formed superstructures were partly retained in the thin film but could be altered by annealing procedures. A control of the superstructures should enable the controlled tuning of the optical properties. Despite the strong interaction of the chromophores in the excited state, the redox potentials of the homopolymers barely differed to those of the respective reference dyes, indicating negligible electronic interaction in the ground state.
In addition squaraine-squaraine copolymer P6, consisting of alternating parent dyes M1 and M2, was synthesised. Likewise to the homopolymers, a broad and red-shifted absorption was observed. This was explained by exciton coupling theory, which was extended to also suit alternating copolymers. In toluene, an extraordinary narrow and intense lowest energy absorption band was observed. This exchange narrowing might be a result of a highly ordered J-type structure of the polymer especially in this solvent because it was not found in others. The features of the polymer may be compared to typical J-aggregates formed from monomeric cyanine molecules for example and the polymer used as model for excitonic interactions in an alternating copolymer. Transient absorption measurements revealed a strong energy dependence of the decay traces of the copolymer, most strikingly at early decay times. This was assigned to the occurrence of multiple excitations of one polymer strand (due to the large extinction coefficients of the polymer) and resulting exciton-exciton annihilation. Due to the large exciton diffusion constants that were estimated, the static exciton-exciton annihilation was the rate limiting process of the decay, in contrast to other conjugated polymers, where in thin film measurements the decay was diffusion controlled.
To sum up, for the polymers consisting of exclusively squaraine chromophores, it was shown that the exciton coupling of single chromophores with strong transition dipole moments was a fruitful way to tune the absorption spectra.
As a side product of some of the polycondensation reactions, unprecedented cyclic conjugated oligomers such as the triarylamine-bridged dimer Dim1, the cyclic homotrimers Tri1–Tri3, and the tetramer Tet1 were obtained by recycling GPC in low yields. Especially the cyclic trimers showed unusual absorption and even more extraordinary fluorescence properties. They showed multiple fluorescence bands in the NIR that covered a range from ~ 8000–12500 cm–1 (800–1250 nm). First hints from theoretical calculations indicated that the trimer was not fully planar but comprised a mixture of both planar and bent single squaraine chromophores. However, final results of the calculations were still missing at the time of writing.
In the last part of this work, the application of some monomeric and polymeric squaraines in binary and ternary bulk heterojunction solar cells was demonstrated. Also the utilisation as a dopant in a polymer matrix in an OLED device was shown. The homopolymers P1–P4 were tested in the binary BHJ solar cells revealing poor performances and especially very low short circuit currents. The utilisation of the polymers P3 and P4 that carried the dicyanomethylene group resulted in higher open circuit voltages due to the lower LUMO energy levels but still an overall poor performance. Neither for the different alkyl chains nor for the size of the polymers was a trend observed. In the ternary BHJ solar cells, small amounts of either monomer M14 or polymers P1A, P4–1 or P13 were added to a P3HT/PCBM system in order to generate an additional pathway for charge or energy transfer that should result in a better device performance. However, for none of the tested squaraines, improved solar cells could be built. In similarity to the binary solar cells, the short circuit currents were lower compared to a P3HT/PCBM reference device. These low short circuit currents indicated that the morphology of the squaraine dyes was the major limitation in those devices. It is possible that the dimethyl groups at the indolenine hindered a favoured alignment of the compounds that would allow decent charge transport. In the squaraine doped OLED the squaraine M6 worked rather well as an NIR emitter. Already at low dye loads the fluorescence of the host polymer SY-PPV was completely quenchend and emission from the squaraine was observed. For electroluminescence measurements, a lower dye load (0.5 wt.%) compared to the photoluminescence measurements was sufficient, indicating that apart from FRET additional quenching mechanisms were at work in the electrically driven devices such as charge carrier dynamics.
Dockingbasierte Ansätze zählen zu den wichtigsten Komponenten im virtuellen Screening. Sie dienen der Vorhersage der Ligandposition und -konformation in der Bindetasche sowie der Abschätzung der Bindungsaffinität zum Protein. Bis heute stellt die korrekte Identifizierung proteingebundener Ligandkonformationen ein noch nicht vollständig gelöstes Problem für Scoringfunktionen dar. Der erste Teil der vorliegenden Arbeit ist daher der Entwicklung computergestützter Methoden zur Bewertung von Docking-Lösungen gewidmet.
Der Fokus eines ersten Teilprojektes lag auf der Berücksichtigung der Absättigung vergrabener Wasserstoffbrückenakzeptoren (HBA) und -donoren (HBD) bei der Bewertung von Docking-Lösungen. Nicht-abgesättigte vergrabene HBA und HBD stellen einen der Bindungsaffinität abträglichen Beitrag dar, der bis dato aufgrund fehlender Struktur- bzw. Affinitätsdaten in Scoringfunktionen vernachlässigt wird. Im Rahmen der vorliegenden Arbeit wurde auf der Basis einer detaillierten Untersuchung zur Häufigkeit vergrabener nicht-abgesättigter HBA und HBD in hochaufgelösten Protein-Ligand-Komplexen des Hartshorn-Datensatzes eine empirische Filterfunktion („vnaHB“-Filterfunktion) entwickelt, die unerwünschte Ligandbindeposen erkennt und von der Bewertung mittels Scoringfunktionen ausschließt. Der praktische Nutzen der empirischen Filterfunktion wurde für die Scoringfunktionen SFCscore und DSX anhand vorgenerierter Docking-Lösungen des Cheng-Datensatzes untersucht. Die Häufigkeitsuntersuchung zeigt, dass eine Absättigung vergrabener polarer Gruppen in Protein-Ligand-Komplexen für eine hochaffine Protein-Ligand-Bindung notwendig ist, da vergrabene nicht-abgesättigte HBA und HBD nur selten auftreten. Eine vollständige Absättigung durch entsprechende Proteinpartner wird für ca. 48 % der untersuchten Komplexe beobachtet, ca. 92 % weisen weniger als drei hauptsächlich schwache, nicht-abgesättigte HBA bzw. HBD (z. B. Etherfunktionen) auf. Unter Einbeziehung von Wassermolekülen in die Häufigkeitsanalyse sind sogar für ca. 61 % aller Komplexe alle wasserstoffbrückenbindenden Gruppen abgesättigt. Im Gegensatz zu DSX werden für SFCscore nach Anwendung der empirischen Filterfunktion erhöhte Erfolgsraten für das Auffinden einer kristallnahen Pose (≤ 2.0 Å Abweichung) unter den am besten bewerteten Docking-Posen erzielt. Für die beste SFCscore-Funktion (SFCscore::229m) werden Steigerungen dieses als „Docking Power“ bezeichneten Kriteriums für die Top-3-Posen (Erfolgsrate für die Identifizierung einer kristallnahen 2.0 Å Pose unter den besten drei Docking-Lösungen) von 63.1 % auf 64.2 % beobachtet.
In einem weiteren Teilprojekt wurden repulsive Protein-Ligand-Kontakte infolge sterischer Überlappungen der Bindungspartner bei der Bewertung von Docking-Lösungen berücksichtigt. Die adäquate Einbeziehung solcher repulsiver Kontakte im Scoring ist für die Identifizierung proteingebundener Ligandkonformationen entscheidend, jedoch aufgrund fehlender Affinitäts- bzw. Strukturdaten problematisch. Im Rahmen der vorliegenden Arbeit wurde auf der Basis des Lennard-Jones-Potentiales des AMBER-Kraftfeldes zunächst ein neuer Deskriptor zur Beschreibung repulsiver Kontakte („Clash“-Deskriptor) entwickelt und zur Untersuchung der Häufigkeit ungünstiger Protein-Ligand-Kontakte in hochaufgelösten Protein-Ligand-Komplexen des Hartshorn-Datensatzes herangezogen. Eine aus der Häufigkeitsverteilung abgeleitete empirische Filterfunktion („Clash“-Filterfunktion) wurde anschließend der Bewertung von Docking-Lösungen des Cheng-Datensatzes mittels der Scoringfunktionen SFCscore und DSX vorgeschaltet, um unerwünschte Ligandbindeposen auszuschließen. Die Häufigkeitsuntersuchung zeigt, dass vorwiegend schwache repulsive Kontakte in Protein-Ligand-Komplexen auftreten. So werden in 75 % der Komplexe des Hartshorn-Datensatzes abstoßende Potentiale unter 0.462 kcal/mol beobachtet. Zwar betragen die ungünstigen Beiträge pro Komplex für 50 % aller Strukturen ca. 0.8 kcal/mol bis 2.5 kcal/mol, jedoch können diese auf Ungenauigkeiten der Kristallstrukturen zurückzuführen sein bzw. durch günstige Protein-Ligand-Wechselwirkungen kompensiert werden. Die Anwendung der „Clash“-Filterfunktion zeigt signifikante Verbesserungen der Docking Power für SFCscore. Für die beste SFCscore-Funktion (SFCscore::frag) werden Steigerungen der Erfolgsraten für das Auffinden einer kristallnahen Pose unter den drei am besten bewerteten Docking-Lösungen von 61.4 % auf 86.9 % erzielt, was an die Docking Power der bis dato besten Scoringfunktionen aus der Literatur (z. B. DSX, GlideScore::SP) heranreicht (Docking Power (DSX): 92.6 %; Docking Power (GlideScore::SP): 86.9 %). Die „Clash“-Filterfunktion allein ist auch der Kombination der „Clash“- und der „vnaHB“-Filterfunktion überlegen.
Ein weiterer Schwerpunkt der vorliegenden Arbeit wurde auf die Einbeziehung von Decoy-Daten (Struktur- und Affinitätsdaten schwach affiner und inaktiver Liganden) im Zuge der Entwicklung computergestützter Methoden zur Bewertung von Docking-Lösungen gelegt. Dadurch soll eine adäquate Berücksichtigung ungünstiger Beiträge zur Bindungsaffinität ermöglicht werden, die für die Richtigkeit und Zuverlässigkeit ermittelter Vorhersagen essentiell ist. In der vorliegenden Arbeit wurden binäre Klassifizierungsmodelle zur Bewertung von Docking-Lösungen entwickelt, die die Einbeziehung von Decoy-Daten ohne die Verfügbarkeit von Affinitätsdaten erlauben. Der Random-Forest-Algorithmus (RF), SFCscore-Deskriptoren, der neu entwickelte „Clash“-Deskriptor, und die Decoy-Datensätze von Cheng und Huang (Trainingsdaten) bilden die Grundlage des leistungsfähigsten Klassifizierungsmodells. Der praktische Nutzen des „besten“ RF-Modells wurde nach Kombination mit der Scoringfunktion DSX anhand der Docking Power für das Auffinden einer kristallnahen Pose auf Rang 1 am unabhängigen Cheng-/Huang- (Komplexe, die nicht in den Trainingsdaten enthalten sind) und CSAR-2012-Testdatensatz untersucht. Gegenüber einer alleinigen Anwendung von DSX werden an beiden Testdatensätzen weitere Verbesserungen der Docking Power erzielt (Cheng-/Huang-Testdatensatz: DSX 84.24 %, RF 87.27 %; CSAR-2012-Testdatensatz: DSX 87.93 %, RF 91.38 %). Das „beste“ Modell zeichnet sich durch die zuverlässige Vorhersage richtig-positiver Docking-Lösungen für einige wenige Komplexe aus, für die DSX keine kristallnahe Ligandkonformation identifizieren kann. Ein visueller Vergleich der jeweils am besten bewerteten RF- und DSX-Pose für diese Komplexe zeigt Vorteile des RF-Modells hinsichtlich der Erkennung für die Protein-Ligand-Bindung essentieller Wechselwirkungen. Die Untersuchung der Bedeutung einzelner SFCscore-Deskriptoren für die Klassifizierung von Docking-Lösungen sowie die Analyse der Misserfolge nach Anwendung des Modells geben wertvolle Hinweise zur weiteren Optimierung der bestehenden Methode. Hinsichtlich der zu bewertenden Eigenschaften ausgeglichenere Trainingsdaten, Weiterentwicklungen bestehender SFCscore-Deskriptoren sowie die Implementierung neuer Deskriptoren zur Beschreibung bis dato nicht-berücksichtigter Beiträge zur Bindungsaffinität stellen Ansatzpunkte zur Verbesserung dar.
Der zweite Teil der vorliegenden Arbeit umfasst die Anwendung dockingbasierter Methoden im Rahmen der Entwicklung neuer Inhibitoren des „Macrophage Infectivity Potentiator“-(MIP)-Proteins von Legionella pneumophila und Burkholderia pseudomallei.
Das MIP-Protein von Legionella pneumophila stellt einen wichtigen Virulenzfaktor und daher ein attraktives Zielprotein für die Therapie der Legionellose dar. Im Rahmen der vorliegenden Arbeit erfolgten systematische Optimierungen des Pipecolinsäure-Sulfonamides 1, des bis dato besten niedermolekularen MIP-Inhibitors (IC50 (1): 9 ± 0.7 µM). Nach Hot-Spot-Analysen der Bindetasche wurden Docking-Studien zur Auswahl aussichtsreicher Kandidaten für die Synthese und Testung auf MIP-Inhibition durchgeführt. Die Ergebnisse der Hot-Spot-Analysen zeigen günstige Wechselwirkungsbereiche für Donorgruppen und hydrophobe Substituenten in meta-Position sowie Akzeptorgruppen in para-Position des Benzylringes von 1 auf. Die Einführung einer Nitrofunktion in para-Position des Benzylringes von 1 (2h) resultiert in einer erhöhten MIP-Inhibition (IC50 (2h): 5 ± 1.5 µM), was wahrscheinlich auf die Ausbildung einer zusätzlichen Wasserstoffbrücke zu Gly116 zurückzuführen ist. Selektivitätsverbesserungen gegenüber dem strukturverwandten humanen FKBP12-Protein werden insbesondere für das para-Aminoderivat von 1 (2n) erzielt (Selektivitätsindex (1): 45, Selektivitätsindex (2n): 4.2; mit Selektivitätsindex = IC50 (MIP)/IC50 (FKBP12)). Der Ersatz des hydrophoben Trimethoxyphenylrestes von 1 durch einen Pyridinring (2s) führt zu einer verbesserten Löslichkeit bei vergleichbarer MIP-Inhibition.
Das MIP-Protein von Burkholderia pseudomallei spielt eine wichtige Rolle in der Pathogenese der Melioidose und stellt daher ein attraktives Zielprotein für die Entwicklung neuer Arzneistoffe dar. In der vorliegenden Arbeit erfolgten Optimierungen des bis dato besten niedermolekularen MIP-Inhibitors 1. Ausgehend von einem Strukturvergleich von Burkholderia pseudomallei MIP mit Legionella pneumophila MIP und einer Hot-Spot-Analyse der Burkholderia pseudomallei MIP-Bindetasche wurden Docking-Studien zur Auswahl aussichtsreicher Kandidaten für die Synthese und Testung auf MIP-Inhibition durchgeführt. Der Strukturvergleich zeigt eine hohe Homologie beider Bindetaschen. Größere konformelle Änderungen werden lediglich für den von Ala94, Gly95, Val97 und Ile98 geformten Bindetaschenbereich beobachtet, was unterschiedliche Optimierungsstrategien für 1 erforderlich macht. Günstige Wechselwirkungsbereiche der Burkholderia pseudomallei MIP-Bindetasche finden sich einerseits für Donorgruppen oder hydrophobe Substituenten in para-Position des Benzylringes (Region A) von 1, andererseits für Akzeptor- bzw. Donorgruppen in para- bzw. meta-/para-Position des Trimethoxyphenylringes (Region B). Anhand von Docking-Studien konnten sowohl für Variationen in Region A als auch in Region B aussichtsreiche Kandidaten identifiziert werden. Initiale MIP-Inhibitionsmessungen der bis dato synthetisierten Derivate deuten auf erhöhte Hemmungen im Vergleich zu 1 hin. Der Ersatz des hydrophoben Trimethoxyphenylrestes von 1 durch einen Pyridinring führt auch hier zu vergleichbarer MIP-Inhibition bei verbesserter Löslichkeit. Derzeit sind weitere Synthesen und Testungen aussichtsreicher Liganden durch die Kooperationspartner geplant. Die Ergebnisse der Inhibitionsmessungen sollen deren Nutzen als MIP-Inhibitoren aufzeigen und wertvolle Informationen für weitere Zyklen des strukturbasierten Wirkstoffdesigns liefern.
The transport of optically excited states, called excitons, as well as their conversion into charges define the two major steps allowing for the operation of organic photovoltaic (OPV) devices. Hence, a deep understanding of these processes, the involved mechanisms as well as possible loss channels is crucial for further improving the efficiency of organic solar cells. For studying the aforementioned processes spectroscopic methods like absorption and emission measurements are useful tools. As many of the processes take place on a sub-nanosecond (ns) timescale ultrafast spectroscopic methods are required. Due to this reason two experiments based on a femtosecond laser system were built and employed in this work, namely picosecond (ps) time-resolved photoluminescence (PL) and transient absorption (TA) spectroscopy.
By analyzing the PL decay dynamics in the prototypical organic semiconductor rubrene, the feasibility of a new approach for improving the efficiency of organic solar cells by harvesting triplet excitons generated by singlet fission was examined. Singlet fission describes a process where two triplet excitons are generated via a photoexcited singlet exciton precursor state if the energy of the two triplets is comparable with the energy of the singlet. For this purpose the influence of characteristic length scales on the exciton dynamics in different rubrene morphologies exhibiting an increasing degree of confinement was analyzed. The results show that the quenching at interfacial states efficiently suppresses the desired fission process if these states are reached by excitons during migration. Since interfacial states are expected to play a significant role in thin film solar cells and are easily accessible for the migrating excitons, the results have to be considered for triplet-based OPV.
While the aforementioned approach is only investigated for model systems so far, the efficiency of disordered organic bulk heterojunction (BHJ) solar cells could be significantly enhanced in the last couple of years by employing new and more complex copolymer donor materials. However, little is known about the photophysics and in particular the excitation dynamics of these systems. By carrying out a systematic optical study on the prominent copolymer PCDTBT and its building blocks we were able to identify the nature of the two characteristic absorption bands and the coupling mechanism between these levels. The latter mechanism is based on an intrachain partial charge transfer between two functional subunits and our time-resolved measurements indicate that this coupling governs the photophysical properties of solar cells based on these copolymers. The efficient coupling of functional subunits can be seen as a key aspect that guarantees for the success of the copolymer approach.
Another important issue concerns the optimization of the morphology of BHJ solar cells. It arises from the discrepancy between the exciton diffusion length \mbox{($\approx$ 10 nm)} and the absorption length of solar irradiation ($\approx$ 100 nm). Due to this reason, even for devices based on new copolymer materials, processing parameters affecting the morphology like annealing or employing processing additives are of major importance. In our combined optical, electrical and morphological study for solar cells based on the high-efficient copolymer PBDTTT-C we find a direct correlation between additive content and intermixing of the active layer. The observed maximum in device efficiency can be attributed to a morphology guaranteeing for an optimized balance between charge generation and transport. Our results highlight the importance of understanding the influence of processing parameters on the morphology of the BHJ and thus on the efficiency of the device.
Ziel dieser Studie war es, mögliche Veränderungen des psychischen Befindens sowie Ausprägungen der Persönlichkeitsdimensionen Extraversion und Neurotizismus im Verlauf der Übungen der Progressiven Muskelrelaxation zu untersuchen. Weiterhin sollte der Einfluss der Persönlichkeitsmerkmale auf die Veränderung des Befindens überprüft werden.
Im theoretischen Teil der Arbeit wurde die Entstehung und Wirkungsweise der PR, Eysencks Theorien und die bisherige Literatur zum Thema dargestellt. Zum Einen konnte festgesellt werden, dass die PR als Teil unterschiedlicher Therapieintervention Einfluss auf das Befinden und die Persönlichkeitsmerkmale hat. Zum Anderen wurde deutlich, dass die Wirkung der PR auf das psychische Befinden und Persönlichkeitsausprägung durch verschiedene, sich gegenseitig bedingende Faktoren, beeinflusst wird. Folgende Hypothesen wurden aufgestellt:
Im Verlauf eines Kurses der PR verbessert sich das psychische Befinden. Zugleich nimmt der Neurotizismuswert ab und der Extraversionswert zu. Außerdem hängt das Ausmaß der Veränderung des psychischen Befindens mit der Persönlichkeits-ausprägung zu Beginn der Durchführung der PR zusammen. Introvertierte und emotional Labile sollen deutlicher von der Wirkung der PR profitieren als Extrovertierte und emotional Stabile.
93 Probanden füllten zu vier Messzeitpunkten vor, während und nach der PR Fragebögen (Eysenck-Persönlichkeits-Inventar, Form A und Eigenschaftswörterliste, Normalform) aus.
Die Ergebnisse zeigen keine Veränderung des Extraversionswertes, wohingegen es nach Beendigung der Übungen zu einer signifikanten Besserung der emotionalen Stabilität kam, was sich in einer Verringerung des Neurotizismuswertes äußerte. Es konnte während und nach Durchführung der PR eine signifikante Verringerung des negativen und Zunahme des positiven Befindens festgestellt werden. Eine Abhängigkeit der Veränderung des Befindens von den Persönlichkeitsdimensionen ließ sich nicht nachweisen. Die Annahme, dass vor allem emotional Labile und Introvertierte eine Verbesserung des Befindens zeigen, ließ sich nicht bestätigen.
Unter Beachtung, dass die tatsächlich involvierten Daten etwa der Hälfte der insgesamt an der Studie teilgenommenen Probanden entsprechen sowie unter Berücksichtigung des Studiendesigns (Ein-Gruppen-Prä-Post-Studie ohne Kontrollgruppe), kann man abschließend formulieren, dass die PR zur Verbesserung der Stimmungslage und Erlangung einer psychischen Stabilität beiträgt, unabhängig von der Ausprägung des Extraversions- und Neurotizismusgrades.