@phdthesis{Zieschang2014,
  author    = {Zieschang, Fabian},
  title     = {Energy and Electron Transfer Studies of Triarylamine-based Dendrimers and Cascades},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-101866},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2014},
  abstract  = {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 F{\"o}rster 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 F{\"o}rster 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.},
  subject      = {Sternpolymere},
  language  = {en}
}
@phdthesis{Mueller2011,
  author    = {M{\"u}ller, Christian},
  title     = {Physical Properties of Chromophore Functionalized Gold Nanoparticles},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-57657},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2011},
  abstract  = {n this work the synthesis and analysis of chromophore functionalized spherical gold nanoparticles is presented. The optical, electrochemical and spectroelectrochemical properties of these hybrid materials are furthermore studied. The work therefore is divided into two parts. The first part deals with triarylamine and PCTM-radical functionalized gold nanoparticles. The focus thereby was on the synthesis and on the investigations of chromophore-chromophore interactions and gold core-chromophore interactions. The chromopores, especially triarylamines, were attached to the gold core via different bridging units and were studied with optical and electrochemical methods. The purity and dimensions of the nanoparticles was determined by 1H-NMR spectroscopy, diffusion ordered NMR spectroscopy (DOSY), TGA, XPS and STEM. Furthermore a cyclic voltammetry technique was used to determine the composition of the particles via the Randles-Sevcik equation. An analysis of these parameters led to a model of a sea urchin-shaped nanoparticle. Optical measurements of the particles revealed an anisotropic absorption behavior of the triarylamine units due to gold core-chromophore interaction. However this behavior depends strongly on the relative orientation of the transition dipole moment of the chromophore to the gold surface and the distance of the chromophore to the surface. Hence, the anisotropic behavior was exclusively detected in the spectra of the Au-Tara1 particles. The short and rigid pi-conjugated bridging unit thereby facilitates this gold core-chromophore interaction. It was shown from electrochemical investigations that the triarylamine units can be chemically reversibly oxidized to the triarylamine monoradical cation. Furthermore, the measurements revealed a strong interligand triarylamine-triarylamine interaction which was only seen for the Au-Tara1 particles. The long pi-conjugated bridging units of the Au-Tara2 and Au-Tara3 particles as well as the aliphatic bridging unit of Au-Tara4 prevent any detectable interligand interactions. One may conclude that both the gold core-chromophore and the interligand triarylamine-triarylamine interaction depend on the length and the rigidity of the bridging unit. The electron transfer behavior of the triarylamine units adsorbed onto the gold core was additionally studied via spectroelectrochemical (SEC) measurements which are able to reveal weaker interactions. The investigations of Au-Tara1 and Au-Tara2 revealed a significant strong coupling between neighboring triarylamine units which is due to through-space intervalence interactions. This behavior was not detected for Au-Tara3 or for Au-Tara4. The SEC analysis also revealed that these observed interligand interactions depend on the length and the rigidity of the bridging unit. Thus, the systematic variation of the bridging unit gave a basic insight in the optical and electrochemical properties of triarylamines, located in the vicinity of a gold nanoparticle. The second part of this work aimed at the synthesis of new molecules, denoted as SERS-markers, for immuno SERS applications. For this purpose, the SERS-markers were designed to have a Raman-active unit and a thiol group for chemisorptions to Au/Ag nanoshells. In cooperation with the group of Schl{\"u}cker (University of Osnabr{\"u}ck) the SERS-markers were absorbed onto Au/Ag nanoshells, denoted as SERS-labels, and characterized. The SERS spectra of the SERS-labels exhibited intense and characteristic SERS-signals for each marker. For immuno SERS investigations SEMA3 was functionalized with a hydrophilic end unit. This marker was adsorbed onto an Au/Ag nanoshell and encapsulated with silica. An anti-p63 antibody was bound to the silica surface in order to generate a SERS-labeled antibody for the detection of the tumor suppressor p63 in benign prostate. Immuno-SERS imaging of prostate tissue incubated with SERS-labeled anti-p63 antibodies demonstrated the selective detection of p63 in the basal epithelium. The results show the potential of the method for the detection of several biomolecules in a multiplexing SERS experiment.},
  subject      = {Gold},
  language  = {en}
}
@phdthesis{Amthor2005,
  author    = {Amthor, Stephan},
  title     = {Redox properties of Bis-Triarylamines and ligand properties of Thianthrenophane},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-15916},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2005},
  abstract  = {The one electron oxidation potential of ten TAAs with all permutations of Cl , OMe- and Me-substituents in the three p-positions were determined by CV. The half wave potential of the first oxidation wave correlates linearly with the number of Cl- and OMe-substituents. AM1-CISD derived values of the absorption energies are in good agreement with the experiments but differ strongly for the oscillator strengths as well as for neutral compounds and their corresponding mono radical cations. The small solvent dependence of the experimental UV/Vis spectra in CH2Cl2 and MeCN reflects a minor charge transfer character of the electronic transitions. The UV/Vis/NIR spectra of the series of TAAs and their corresponding radical cations and the AM1 computations reveal that even small substituents may lead to strong symmetry breaking and to a modified electronic structure. The spectroscopic properties of a series of four bis-TAA donor-bridge-donor X-B-X dimers, composed of two asymmetric TAA chromophores (monomers) were investigated. UV/vis-, fluorescence and transient absorption spectra were recorded and compared with those of the corresponding X-B monomers. The excited states of the dimers are described as MV states which show, depending on the chemical nature of the bridge, a varying amount of interactions. It was found that superradiant emission only proceeds in the case of weak and medium coupling. Whether the first excited state potential energy surface of the dimers is a single minimum or a double minimum potential depends on the solvent polarity and the electronic coupling. In the latter case, the dimer relaxes in a symmetry broken CT state. The [2.2]paracyclophane bridged dimer is an example for a weakly coupled system, because the spectroscopic behavior is very similar to the corresponding p xylene monomer. In contrast, anthracene as well as p-xylene bridges mediate a stronger coupling and reveal a significant cooperative influence on the optical properties. A series of [2.2]paracylophane bridged bis-TAA MV radical cations X-B-X+ were analyzed by a GMH three-level model which takes two transitions into account: the IV-CT band and the bridge band. From the GMH analysis, one can conclude that the [2.2]paracyclophane moiety is not the limiting factor which governs the intramolecular charge transfer. The electronic interactions are of course smaller than direct conjugation but from the order of magnitude of the couplings of the [2.2]paracyclophane MV species it can be assumed that this bridge is able to mediate significant through-space and through-bond interactions. From the exponential dependence of the electronic coupling V between the two TAA localized states on the distance r between the two redox centers, it was inferred that the HT proceeds via superexchange mechanism. The analysis reveals that even significantly longer conjugated bridges should still mediate significant electronic interactions, because the decay constant of a series of conjugated MV species is small. The absorption properties of a series of bis-TAA-[2.2]paracyclophane dications X+-B-X+ were presented. The localized and the CT transitions of these dications are explained and analyzed by an exciton coupling model which also considers the photophysical properties of the monomeric TAA radical cations. Together with AM1-CISD calculated transition moments, experimental transition moments and transition energies of the bis-TAA dications were used to calculate electronic couplings by a GMH approach. These couplings are a measure for interactions of the excited MV CT states. The modification of the diabatic states reveals similarities of the GMH three-level model and the exciton coupling model. Comparison of the two models shows that the transition moment between the excited mixed-valence states of the dimer equals the dipole moment difference of the ground and the excited bridge state of the corresponding monomer. Thianthrenophane (1) has a cavity which offers enough room to potentially enable endohedral coordination to small ions or molecules. For the complexation of silver(I) perchlorate, the complex stability constants of thianthrenophane logK1=5.45 and of thianthrene logK2=9.16 were determined by UV/Vis titration. Single competition transport experiments with ten metal salts demonstrate a very high selectivity of thianthrenophane as a carrier for silver(I) and a distinctly higher transport rate compared to carriers such as thianthrene and 14-ane-S4. Although the X-ray crystal structure analysis of the polymeric [Ag(1)]ClO4 shows an exohedral coordination to silver(I), the formation of an endohedral [Ag(1)]+ complex is suggested to be the explanation for the unusual carrier selectivity of silver(I) by 1 in bulk liquid membrane.},
  subject      = {Triarylamine},
  language  = {en}
}
@phdthesis{Kriegisch2005,
  author    = {Kriegisch, Volker},
  title     = {Electron transfer processes between organic redox centres and electrodes via active bridges in self-assembled monolayers},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-15892},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2005},
  abstract  = {Cyclovoltammetrische Messungen der Ferrocenalkylthiole 1 - 3 belegen, dass homogene, gemischte Monolagen aus redoxaktiven Verbindungen und redoxinaktiven Alkylthiolen gebildet werden. Die von Creager et al. bestimmten ET Raten der Ferrocenalkylthiole 1 - 3 konnten hierbei verifiziert werden. Wie erwartet erfolgt eine Abnahme der ET Geschwindigkeit bei einer Kettenverl{\"a}ngerung des Alkylspacers von 2 nach 3. Eine unterschiedliche Konnektivit{\"a}t zwischen Redoxzentrum und Alkylspacer, z. B. die Einf{\"u}hrung einer Carbonyl-Funktion im Falle von 1, unter Beibehaltung der Kettenl{\"a}nge zeigt keinen bemerkbaren Einfluß auf den ET. Trotzt vergleichbaren Abstands der aromatischen Ferrocenthiole 4 und 5 zu der C8-Alkyl-Verbindung 2 zwischen Redoxzentrum und Elektrode, weisen diese aufgrund ihrer starken Konjugation sehr hohe ET Geschwindigkeiten auf. Die elektronischen Kopplungsfaktoren selbst deuten auf einen nichtadiabtischen ET zwischen Redoxzentrum und Elektrode hin. Wie erwartet kommt es zu einem Anwachsen der Kopplungsfaktoren bei sich verk{\"u}rzender Kettenl{\"a}nge oder bei Einf{\"u}hrung konjugierter Spacersysteme. Zusammenfassend kann gesagt werden, dass Erfahrungen hinsichtlich der Pr{\"a}paration der Monolagen gesammelt, die gemessenen ET Raten f{\"u}r der literaturbekannten Verbindungen 1 - 3 best{\"a}tigt und diese Informationen auf die konjugierten Verbindungen 4 und 5 angewandt werden konnten. Im zweiten Teil wurden die Triarylamin- (29, 32) und Phenothiazinalkylthiole (35) bez{\"u}glich ihres ET Verhaltens in gemischten Monolagen untersucht. Mittels Cyclovoltammetrie konnte gezeigt werden, daß einheitlich geformte, verd{\"u}nnte Monolagen vorliegen. Die ET Raten der Triarylamin- (29, 32) und Phenithiazinalkylthiole (35) sind jedoch um den Faktor 10 bis 100 h{\"o}her als vergleichbare Ferrocenalkylthiole gleicher Kettenl{\"a}nge [1, 2], wohingegen f{\"u}r Monolagen, welche [Ru(bpy)2(pp)]+-Alkythiole enthalten, {\"a}quivalente Werte gefunden wurden [3]. Die ET Geschwindigkeit wird von zwei Parametern beeinflusst: dem elektronischen Kopplungsmatrixelement und der Regorganisationsenergie \&\#61548;\&\#61472; [4]. Die ET Geschwindigkeit in Donor-substituierten Alkylthiolen wird haupts{\"a}chlich durch \&\#61548; beeinflusst und sogar kleine {\"A}nderungen dieser zeigen eine große Auswirkung auf die zu untersuchenden Prozesse. Aus diesem Grund wird eine Zunahme der ET Geschwindigkeit von Ferrocen (hohe Reorganisationsenergie) {\"u}ber die Phenothiazinverbindung 35 und [Ru(bpy)2(pp)]+ zu den Triarylaminchromophoren 29 und 32 (niedrige Reorganisationsenergie) beobachtet. Weiterhin spielt, im Gegensatz zu Beobachtung von Creager et al. an {\"a}quivalenten Ferrocenverbingungen, die Anbindung des Redoxzentrums an den Alkylspacer eine bedeutende Rolle. Im Falle der elektronenreichen Ether-verbr{\"u}ckten Verbindung 29 wird der ET nicht alleine durch \&\#61548;, sondern ebenso durch mesomere Effekte bestimmt. Bei 29 kommt es durch Lokalisation der positiven Ladung nahe der Ether Funktion formal zu einer Kettenverk{\"u}rzung um eine „Methyleneinheit", welche schließlich in h{\"o}heren ET Geschwindigkeiten resultiert. Im dritten Teil dieser Dissertation wurde ein Serie „molekularer Dr{\"a}hte" bestehend aus Methoxy- oder Chlorid-substituierten Triarylamin- und Phenothiazinverbindungen mit unterschiedlichen Br{\"u}ckeneinheiten und Br{\"u}ckenl{\"a}ngen zwischen Redoxzentrum und Ankerfunktion dargestellt und im Hinblick auf ihr ET Verhalten untersucht. Durch cyclovoltammetrische und UV/Vis-spektroskopische Untersuchungen konnte gezeigt werden, dass sowohl die Oxidationspotentiale als auch die energetischen Zust{\"a}nde der Chromophore recht gut durch Einf{\"u}hrung unterschiedlicher Redoxzentren und Br{\"u}ckeneinheiten beeinflusst werden k{\"o}nnen. Trotz erfolgreicher Kontrolle der Dichte der Chromophoreinheiten in den gemischten Monolagen konnte nur f{\"u}r die Verbindungen 49, 52 und 87 mit Nitril-substituierten Br{\"u}ckeneinheiten verl{\"a}ssliche ET Geschwindigkeiten erhalten werden. Bei diesen Chromphoren ist ein Absinken der ET Geschwindigkeit bei zunehmender Dichte der redoxaktiven Molek{\"u}le in den gemischten Monolagen zu beobachten, welche auf eine {\"A}nderung der Adsorptionsgeometrie hindeutet. Bei zunehmender Packungsdichte der Chromophore f{\"u}hrt dies zu einer aufrechteren Stellung der redoxaktiven Spezies. F{\"u}r alle anderen Verbindungen konnten keine Werte aufgrund der zu schnellen ET Geschwindigkeiten ermittelt werden. Konformelle, wie auch die sehr geringe Abstandsabh{\"a}ngigkeit des ET, resultieren in hohen ET Geschwindigkeiten oder auch ung{\"u}nstige HOMO-LUMO Energien bez{\"u}glich des Donors, der Br{\"u}cke und der Elektrode sind Gr{\"u}nde f{\"u}r dieses Verhalten. Die Tatsache, dass Verbindung 49 und 52 beinahe die gleichen Geschwindigkeitskonstanten des ETs unabh{\"a}ngig von der Anzahl der Br{\"u}ckeneinheiten (n = 2, n = 3) besitzen, deutet darauf hin, dass ein Hopping-Prozess stattfindet, bei welchem eine geringere L{\"a}ngenabh{\"a}ngigkeit des ETs als bei eine Superexchange-Mechanismus zu erwarten ist.},
  subject      = {Monoschicht},
  language  = {en}
}