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Virulent Agrobacterium tumefaciens strains transfer and integrate a DNA region of the tumor-inducing (Ti) plasmid, the T-DNA, into the plant genome and thereby cause crown gall disease. The most essential genes required for crown gall development are the T-DNA-encoded oncogenes, IaaH (indole-3-acetamide hydrolase), IaaM (tryptophan monooxygenase) for auxin, and Ipt (isopentenyl transferase) for cytokinin biosynthesis. When these oncogenes are expressed in the host cell, the levels of auxin and cytokinin increase and cause cell proliferation. The aim of this study was to unravel the molecular mechanisms, which regulate expression of the agrobacterial oncogenes in plant cells. Transcripts of the three oncogenes were expressed in Arabidopsis thaliana crown galls induced by A. tumefaciens strain C58 and the intergenic regions (IGRs) between their coding sequences (CDS) were proven to have promoter activity in plant cells. These promoters possess eukaryotic sequence structures and contain cis-regulatory elements for the binding of plant transcription factors. The high-throughput protoplast transactivation (PTA) system was used and identified the Arabidopsis thaliana transcription factors WRKY18, WRKY40, WRKY60 and ARF5 to activate the Ipt oncogene promoter. No transcription factor promoted the activity of the IaaH and IaaM promoters, despite the fact that the sequences contained binding elements for type B ARR transcription factors. Likewise, the treatment of Arabidopsis mesophyll protoplasts with cytokinin (trans-zeatin) and auxin (1-NAA) exerted no positive effect on IaaH and IaaM promoter activity. In contrast, the Ipt promoter strongly responded to a treatment with auxin and only modestly to cytokinin. The three Arabidopsis WRKYs play a role in crown gall development as the wrky mutants developed smaller crown galls than wild-type plants. The WRKY40 and WRKY60 genes responded very quickly to pathogen infection, two and four hours post infection, respectively. Transcription of the WRKY18 gene was induced upon buffer infiltration, which implicates a response to wounding. The three WRKY proteins interacted with ARF5 and with each other in the plant nucleus, but only WRKY40 together with ARF5 increased activation of the Ipt promoter. Moreover, ARF5 activated the Ipt promoter in an auxin-dependent manner. The severe developmental phenotype of the arf5 mutant prevented studies on crown gall development, nevertheless, the reduced crown gall growth on the transport inhibitor response 1 (TIR1) tir1 mutant, lacking the auxin sensor, suggested that auxin signaling is required for optimal crown gall development. In conclusion, A. tumefaciens recruits the pathogen defense related WRKY40 pathway to activate Ipt expression in T-DNA-transformed plant cells. IaaH and IaaM gene expression seems not to be controlled by transcriptional activators, but the increasing auxin levels are signaled via ARF5. The auxin-depended activation of ARF5 boosts expression of the Ipt gene in combination with WRKY40 to increase cytokinin levels and induce crown gall development.
Post-translational histone modifications (PTMs) such as methylation of lysine residues influence chromatin structure and function. PTMs are involved in different cellular processes such as DNA replication, transcription and cell differentiation. Deregulations of PTM patterns are responsible for a variety of human diseases including acute leukemia. DOT1 enzymes are highly conserved histone methyltransferases that are responsible for methylation of lysine 79 on histone H3 (H3K79). Most eukaryotes contain one single DOT1 enzyme, whereas African trypanosomes have two homologues, DOT1A and DOT1B, which methylate H3K76 (H3K76 is homologous to H3K79 in other organisms). DOT1A is essential and mediates mono- and di-methylations, whereas DOT1B additionally catalyzes tri-methylation of H3K76. However, a mechanistic understanding how these different enzymatic activities are achieved is lacking. This thesis exploits the fact that trypanosomes possess two DOT1 enzymes with different catalytic properties to understand the molecular basis for the differential product-specificity of DOT1 enzymes. A trypanosomal nucleosome reconstitution system was established to analyze methyltransferase activity under defined in vitro conditions. Homology modeling allowed the identification of critical residues within and outside the catalytic center that modulate product-specificity. Exchange of these residues transferred the product-specificity from one enzyme to the other and revealed regulatory domains adjacent to the catalytic center. This work provides the first evidence that few specific residues in DOT1 enzymes are crucial to catalyze methyl-state-specific reactions. These results have also consequences for the functional understanding of homologous enzymes in other eukaryotes.
Several aspects of the control of large-scale systems communicating over digital channels are considered.
In particular, the issue of delay, quantization, and packet loss is addressed with the help of dynamic quantization.
New small-gain results suitable for networked control systems are introduced and it is shown that many of the known small-gain conditions are equivalent.
The issue of bandwidth limitations is addressed with the help of event-triggered control.
A novel approach termed parsimonious triggering is introduced, which helps to rule out the occurrence of an infinite number of triggering events within finite time.
Moreover, the feasibility of the presented approaches is demonstrated by numerical examples.
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.
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.
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.
Bacterial mastitis is caused by invasion of the udder, bacterial multiplication and induction of
inflammatory responses in the bovine mammary gland. Disease severity and the cause of disease are
influenced by environmental factors, the cow’s immune response as well as bacterial traits. Escherichia coli (E. coli) is one of the main causes of acute bovine mastitis, but although pathogenic E. coli strains can be classified into different pathotypes, E. coli causing mastitis cannot unambiguously be distinguished from commensal E. coli nor has a common set of virulence factors
been described for mastitis isolates. This project focussed on the characterization of virulence-
associated traits of E. coli mastitis isolates in comprehensive analyses under conditions either
mimicking initial pathogenesis or conditions that E. coli mastitis isolates should encounter while entering the udder. Virulence-associated traits as well as fitness traits of selected bovine mastitis or faecal E. coli strains were identified and analyzed in comparative phenotypic assays. Raw milk whey was introduced to
test bacterial fitness in native mammary secretion known to confer antimicrobial effects.
Accordingly, E. coli isolates from bovine faeces represented a heterogeneous group of which some
isolates showed reduced ability to survive in milk whey whereas others phenotypically resembled
mastitis isolates that represented a homogeneous group in that they showed similar survival and
growth characteristics in milk whey. In contrast, mastitis isolates did not exhibit such a uniform phenotype when challenged with iron shortage, lactose as sole carbon source and lingual
antimicrobial peptide (LAP) as a main defensin of milk. Reduced bacterial fitness could be related to LAP suggesting that bacterial adaptation to an intramammary lifestyle requires resistance to host
defensins present in mammary secretions, at least LAP.
E. coli strain 1303 and ECC-1470 lack particular virulence genes associated to mastitis isolates. To find out whether differences in gene expression may contribute to the ability of E. coli variants to cause mastitis, the transcriptome of E. coli model mastitis isolates 1303 and ECC-1470 were analyzed to
identify candidate genes involved in bacterium-host interaction, fitness or even pathogenicity during bovine mastitis.
DNA microarray analysis was employed to assess the transcriptional response of E. coli 1303 and
ECC-1470 upon cocultivation with MAC-T immortalized bovine mammary gland epithelial cells to
identify candidate genes involved in bacterium-host interaction. Additionally, the cell adhesion and invasion ability of E. coli strain 1303 and ECC-1470 was investigated. The transcriptonal response to the presence of host cells rather suggested competition for nutrients and oxygen between E. coli and MAC-T cells than marked signs of adhesion and invasion. Accordingly, mostly fitness traits that may also contribute to efficient colonization of the E. coli primary habitat, the gut, have been utilized by the mastitis isolates under these conditions. In this study, RNA-Seq was employed to assess the bacterial transcriptional response to milk whey.
According to our transcriptome data, the lack of positively deregulated and also of true virulence-associated determinants in both of the mastitis isolates indicated that E. coli might have adapted by other means to the udder (or at least mammary secretion) as an inflammatory site. We identified traits that promote bacterial growth and survival in milk whey. The ability to utilize citrate promotes fitness and survival of E. coli that are thriving in mammary secretions. According to our results, lactoferrin has only weak impact on E. coli in mammary secretions. At the same time bacterial determinants involved in iron assimilation were negatively regulated, suggesting that, at least during the first hours, iron assimilation is not a challenge to E. coli colonizing the mammary gland. It has been hypothesized that cellular iron stores cause temporary independency to extracellular accessible iron. According to our transcriptome data, this hypothesis was supported and places iron uptake
systems beyond the speculative importance that has been suggested before, at least during early
phases of infection. It has also been shown that the ability to resist extracytoplasmic stress, by oxidative conditions as well as host defensins, is of substantial importance for bacterial survival in mammary secretions.
In summary, the presented thesis addresses important aspects of host-pathogen interaction and
bacterial conversion to hostile conditions during colonization of the mastitis inflammatory site, the mammary gland.
More warning Advanced Driver Assistance Systems (ADAS) will be integrated into the European vehicles in the coming years, due to the ongoing progress on the way to automated driving and Euro NCAP requirements. Furthermore, upcoming technologies like Car-2-X will extend the sensory horizon of ADAS and enable the possibility to warn drivers earlier against various hazards than today. Regarding this progress, increasing numbers of different ADAS warnings will be communicated to the driver. In this context, an important question is how multiple ADAS warnings can be integrated into the Human Machine Interface (HMI) of vehicles and which warning elements are needed to ensure warning acceptance, efficiency and understandability seen from the driver’s point of view.
Two driving simulator studies were conducted and the effects of specific warning elements examined to develop a concept for the integration of upcoming warning ADAS, which focuses on early collision warnings. The implemented early warnings were defined with a warning onset of approximately two seconds before the last possible warning onset. Main questions were whether and how drivers profit from warning direction cues and/or warning object cues for their response to a hazard, and how these cues affect the acceptance of an integrated warning ADAS approach. Furthermore, it was analyzed whether a generalized warning can be used for a cluster of different ADAS concerning the group “warning of collisions”. Therefore critical scenarios in rural and urban surroundings were evaluated, including frontal and lateral (intersections) scenarios. Unnecessary warnings and false alarms have also been taken into account.
The results indicate that early warning direction cues have a high potential to assist drivers with an ADAS warning cluster which covers warning of collisions. In contrast, warning object cues seem to be less important for the drivers’ performance and acceptance regarding early collision warnings. According to these findings, this thesis provides recommendations which warning elements should be included into future ADAS warnings in favor of an integrated warning approach.