@phdthesis{Schaefer2018, author = {Sch{\"a}fer, Julian}, title = {Synthesis and Photophysical Investigation of Donor-Acceptor-Substituted meta- and para-Benzene Derivatives}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-155007}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2018}, abstract = {Im ersten Teil dieser Arbeit wurde die erfolgreiche Synthese einer Serie von bisTriarylamin (bisTAA) Verbindungen vorgestellt. Zum einen wurde das Substitutionmuster an der Benzol Br{\"u}ckeneinheit in Form einer meta- bzw. para-St{\"a}ndigkeit der Redoxzentren (pX bzw. mX), und zum anderen die energetische Lage der Br{\"u}ckeneinheit durch zwei elektronen-schiebende oder ziehende Substituenten X (mit X = OMe, Me, Cl, CN, NO2) in 2,5-Position variiert. Im Falle der meta-Serie wurden auch einige in 4,6-Position substituierte Verbinungen hergestellt (mX46). Die neutral Verbindungen wurden bez{\"u}glich ihrer elektrochemischen und photophysikalischen Eigenschaften untersucht. Durch Oxidation konnten die gemischt valenten (MV), kationischen bisTAA-Verbindungen erzeugt werden. Der thermisch induzierte Lochtransfer (HT) wurde durch temperatur-abh{\"a}ngige ESR-Spektroskopie untersucht. W{\"a}hrend die HT-Rate k und HT-Barriere ΔG in mX unbeeinflusst von den Substituenten X sind, steigen gleichzeitig k und ΔG in der pX-Serie mit zunehmenden Elektonenschub von X an. Diese zun{\"a}chst widerspr{\"u}chliche Beobachtung konnte durch einen ansteigenden Einfluss von L{\"o}sungsmitteleffekten und dadurch resultierend, einer zus{\"a}tzlichen effektiven Barriere erkl{\"a}rt werden. Der optisch induzierte Lochtransfer wurde mittels UV/Vis/NIR-Spektroskopie untersucht. Die pX-Serie zeigte eine Zuhname der elektronischen Kopplung V und dementsprechende eine Abnahme von ΔG, mit Anstieg des elektonenschiebenden Charakters von X. F{\"u}r mX war eine spektroskopische Bestimmung dieser Parameter nicht m{\"o}glich. Die mX46-Serie zeigte ein intermedi{\"a}res Verhalten, wobei MV-Verbindungen mit stark elektronenschiebenden X eine {\"a}hnliche hohe Kopplungen wie pX aufwiesen, was mit Hilfe von DFT-Rechnungen bez{\"u}glich der Molek{\"u}lorbitale erkl{\"a}rt werden konnte. Im zweiten Teil dieser Arbeit wurde die Synthese einer Serie von Verbindungen mit Triarylamin (TAA) als Donor und Naphthalindiimid (NDI) als Akzeptor vorgestellt. Auch hier wurde zum einen das Substitutionmuster an der Benzol-Br{\"u}ckeneinheit in Form einer meta- bzw. para-St{\"a}ndigkeit der Redoxzentren (pXNDI bzw. mXNDI) variieiet und die energetische Lage der durch X (mit X = OMe, Me, Cl, CN, NO2) in 2,5-Position variiert. Außerdem wurde die in 4,6-Position substituierte Verbinungen mOMe46NDI hergestellt. Alle Verbindungen wurden bez{\"u}glich ihrer elektochemischen und photophysikalischen Eigenschaften untersucht. Die Elektronentransferprozesse der Ladungsseparierung (CS) und Ladungsrekombination (CR) dieser Verbindungen sollten mittels transienter Absorptionsspektroskopie (TA) in Toluol untersucht werden. F{\"u}r die Nitroverbindungen p-/mNO2NDI war dies nicht m{\"o}glich, da sich diese unter Bestrahung zersetzten. Die CR von pXNDI waren nicht im ns-Bereich detektierbar, weshalb sich auf die mXNDI-Serie (mit X = OMe-CN) konzentriert wurde. Die CS wurde mittels fs-TA untersucht. Nach optischer Anregung konnte die Bildung eines CS-Zustandes detektiert werden, dessen Bildungsgeschwindigkeit hin zu elektronen-ziehenden Substituenten X steigt. Die CR wurde mit ns-TA untersucht. Sie findet in der Marcus invertierten Region statt und zeichnet sich wird durch ein biexponentialles Abklingverhaten, was durch ein Singulet-Triplett Gleichgewicht im CS-Zustand zustande kommt, aus. Durch Anlegen eines externen Magnetfeldes ließ sich das Abklingverhalten entscheidend ver{\"a}ndern und es konnte eine Singulett-Triplett Aufspaltung nachgewiesen werden. Dieser Befund konnte weiterhin durch Simulation der Abklingkurven best{\"a}tigt werden. In beiden Teilen dieser Arbeit konnte ein entscheidender Einfluss der Benzolbr{\"u}cke auf die auftretenden Ladungstransferprozesse gezeigt werden. F{\"u}r den HT in Grundzustand der MV bisTAA Verbindungen, sowie der ET im angeregten Zustand der Donor-Akzeptor-Verbindungen, wurden die h{\"o}chsten ET-Raten f{\"u}r die para-Serien pX und pXNDI gefunden, w{\"a}hrend die meta-Serien mX und mXNDI deutlch kleine Transferraten aufwiesen. In beiden Studien zeigten die meta46-Verbindungen mX46 und mOMeNDI46 ein intermedi{\"a}res Verhalten, zwischen denen der para- und meta-Verbindungen.}, subject = {Synthese}, language = {en} } @phdthesis{Auerhammer2018, author = {Auerhammer, Nina A.}, title = {Energy Transfer and Excitonic Interactions in Conjugated Chromophore Arrangements of Bodipys and Pyrenes and Squaraines}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-166721}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2018}, abstract = {In this work the energy transfer and excitonic coupling in different chromophore arrangements were investigated. A difference in the coupling strength was introduced by varring the connecting unit and the spacial orientation relative to each other. The synthesis of the 2,7-substituted pyrene compounds could be optimised and good yields of HAB 1 and HAB 2 and small amounts of HAB 2 could be achieved by cobalt-catalysed trimerisation or Diels Alder reaction in the end. Absorption and fluorescence spectra reveal strong intramolecular interactions between the pyrene molecules in the HAB 1. Excitation spectra recorded at the high and low energy fluorescence suggest the contribution of two components to the spectra. One being similar to the ground state aggregate and a second species similar to undisturbed pyrene. All these feature can be accounted to two different fluorescent states which are due to electronical decoupling in the excited state. Due to the strong intramolecular coupling already in the ground state of the molecule, no energy transfer could be studied, as the six pyrene units cannot be seen as separate spectroscopic entities between which energy could be transferred. In the second part of this thesis dye conjugates of different size and alignment were synthesised to study the interaction of the transition-dipole moments. Therefore a systematic investigation of Sonogashira conditions was performed in order to obtain good yields of the desired compounds and keep dehalogenation at a minimum level. Nevertheless only the symmetrical triads could be purified as the asymmeric triads and pentades proved to decompose during purification. The pyrene containing triads Py2B and Py2SQB show small interactions already in the ground state represented by red shifts of the spectra and a broadening of the bands. Nevertheless, these interactions are in the weak coupling regime and energy transfer between the constituents is possible. On the contrary in the TA spectra it is obvious that always the whole triad, at least to some extend is excited. To question if the excitation of the high energy state is deactivated by energy transfer or rather IC in a superchromophore could not be distinguished in the course of this work. At present additional time-dependent calculations of the dynamics are in progress to get a deeper understanding of the photophysical processes taking place in the triads. The dye conjugates B2SQB-3 and (SQB)2B-4 can be assigned to the strong interaction range and hence are describable by exciton theory. The transition-dipole moments proved to be more than additive and increase for both compounds from absorption to fluorescence. This can be explained by an enhancement of the coupling in the relaxed excited state compared to the absorption into the Franck-Condon state due to a more steep potential energy surface in the excited state and hence smaller fluctuations. In the last part of this thesis the influence of disrupting electronical communication by implementing a rigid non-conjugated bridge in a bichromophoric trans-squaraine system was tested. While the flexible linked squaraines show complex spectra due to different conformers the SQA2Anth compound is rigified and no rotation is possible. This change in flexibility is represented in the steady-state spectra where just one main absorption and fluorescence band is present due to a single allowed excitonic state. The system proves to own an excited state that is completely delocalised over the whole molecule.}, subject = {Chromophor}, language = {en} } @phdthesis{Eckstein2019, author = {Eckstein, Klaus}, title = {Linear and Nonlinear Spectroscopy of Doped Carbon Nanotubes}, doi = {10.25972/OPUS-18897}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-188975}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2019}, abstract = {Doping plays a decisive role for the functionality of semiconductor-based (opto-)electronic devices. Hence, the technological utilization of semiconductors necessitates control and a fundamental understanding of the doping process. However, for low-dimensional systems like carbon nanotubes, neither concentration nor distribution of charge carriers is currently well known. The research presented in this thesis investigated the doping of semiconducting carbon nanotubes by spectroscopic methods. Samples of highly purified, intrinsic (6,5) single-wall carbon nanotubes were fabricated using polymer stabilization. Chapter 4 showed that both electro- and redox chemical \$p\$-doping lead to identical bleaching, blueshift, broadening and asymmetry of the S\$_1\$ exciton absorption band. The similar spectral changes induced by both doping schemes suggest that optical spectra can not be used to infer what process was used for doping. Perhaps more importantly, it also indicates that the distribution of charges and the character of the charge transfer states does not depend on the method by which doping was achieved. The detailed analysis of the doping-induced spectral changes in chapter 5 suggests that surplus charges are distributed inhomogeneously. The hypothesis of carrier localization is consistent with the high sensitivity of the S\$_1\$ exciton photoluminescence to additional charge carriers and with the stretched-exponential decay of the exciton population following ultrafast excitation. Both aspects are in good agreement with diffusion-limited contact quenching of excitons at localized charges. Moreover, localized charges act - similar to structural defects - as perturbations to the bandstructure as evidenced by a doping-induced increase of the D-band antiresonance in the mid-infrared spectrum. Quantum mechanical model calculations also suggest that counterions play a crucial role in carrier localization. Counterion adsorption at the nanotube surface is thus believed to induce charge traps of more than 100 meV depth with a carrier localization length on the order of 3 - 4 nm. The doping-induced bleach of interband absorption is accompanied by an absorption increase in the IR region below 600 meV. The observed shift of the IR peak position indicates a continuous transition from localized to rather delocalized charge carriers. This transition is caused by the increase of the overlap of charge carrier wavefunctions at higher charge densities and was modeled by classical Monte-Carlo simulations of intraband absorption. Chapter 6 discussed the spectroscopy of heavily (degenerately) doped nanotubes, which are characterized by a Drude-response of free-carrier intraband absorption in the optical conductivity spectrum. In the NIR spectral region, the S\$_1\$ exciton and X\$+^_1\$ trion absorption is replaced by a nearly 1 eV broad and constant absorption signal, the so-called H-band. The linear and transient absorption spectra of heavily doped nanotubes suggest that the H-band can be attributed to free-carrier interband transitions. Chapter 7 dealt with the quantification of charge carrier densities by linear absorption spectroscopy. A particularly good measure of the carrier density is the S\$_1\$ exciton bleach. For a bleach below about 50 \%, the carrier density is proportional to the bleach. At higher doping levels, deviations from the linear behavior were observed. For doping levels exceeding a fully bleached S\$_1\$ band, the determination of the normalized oscillator strength f\$\text{1st}\$ over the whole first subband region (trion, exciton, free e-h pairs) is recommended for quantification of carrier densities. Based on the nanotube density of states, the carrier density \$n\$ can be estimated using \$n = 0.74\,\text{nm}^{-1} \cdot (1 - f_\text{1st})\$. In the last part of this thesis (chapter 8), the time-resolved spectroelectrochemistry was extended to systems beyond photostable carbon nanotube films. The integration of a flowelectrolysis cell into the transient absorption spectrometer allows the investigation of in-situ electrochemically generated but photounstable molecules due to a continuous exchange of sample volume. First time-resolved experiments were successfully performed using the dye methylene blue and its electrochemically reduced form leucomethylene blue.}, subject = {Dotierung}, language = {en} } @phdthesis{Schreck2018, author = {Schreck, Maximilian}, title = {Synthesis and Photophysics of Linear and Star-Shaped Oligomers of Squaraine Dyes}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-174272}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2018}, abstract = {In this thesis, the synthesis and photophysics of a great variety of squaraine dyes are presented. This variety is based on four parent squaraines containing either indolenine or quinoline heterocycles. By a suitable choice of the donor and acceptor unit, the optical properties can already be adapted to the properties desired on the stage of the monomer. To promote a further derivatisation of these dyes, diverse functional groups are attached to the monomers using transition metal-catalysed C-C coupling reactions. However, this has to be preceded by the synthesis of bromine-functionalised derivatives as a direct halogenation of squaraine dyes is not feasible. Therefore, the halogen function is already introduced in precursor molecules giving rise to a molecular building block system containing bromine-, boronic ester-, and alkyne-functionalised monomer units, which pave the way to a plethora of squaraine oligomers and polymers. The indolenine homopolymer pSQB-1 as well as the corresponding small molecular weight oligomers dSQB-1 and tSQB were synthesized applying Ni-mediated Yamamoto and Pd-catalysed Suzuki coupling methodologies, respectively. The motivation for this project relied on the fundamental investigations by V{\"o}lker et al. on pSQB-V. A progressive red-shift of the lowest energy absorption maximum from the dimer to the polymer was observed in CHCl3 compared to the monomer. With increasing number of monomer units, the exciton coupling decreases from the dimer to the polymer. In addition, the shape of the absorption band manifold shows a strong dependence on the solvent, which was also observed by V{\"o}lker et al. J-type aggregate behavior is found in chlorinated solvents such as CHCl3 and DCM, whereas H-type aggregates are formed in acetone. Temperature-dependent absorption studies in PhCN reveals a reversible equilibrium of diverse polymer conformers, which manifests itself in a gradual change from H-aggregate behavior to a mixture with a more pronounced J-aggregate behavior upon raising the temperature. It isassumed that both characteristic aggregate bands correlate in borderline cases with two polymer structures which can be assigned to a zig-zag and a helical structure. As no experimental evidence for these structures could hitherto be provided by NMR, TD-DFT computations on oligomers (22-mers) can reproduce very closely the characteristic features of the spectra for the two conformational isomers. The subsequent chapters are motivated by the goal to influence the optical properties through a control of the superstructure and thus of the intramolecular aggregate formation. On the one hand, bulky groups are implemented in the 3-position of the indolenine scaffold to provoke steric repulsion and thus favoring J-aggregate behavior at the expense of helical arrangements. The resulting homopolymer pDiPhSQB bearing two phenyl groups per indolenine exhibits J-type aggregate behavior with red-shifted absorption maxima in all considered solvents which is explained to be caused by the formation of elongated zig-zag structures. Furthermore, single-crystal X-ray analysis of monomer DiPhSQB-2-Br2 reveals a torsion of the indolenine moieties as a consequence of steric congestion. The twist of the molecular geometry and the resulting loss of planarity leads to a serious deterioration of the fluorescence properties, however a significant bathochromic shift of ca. 1 200 cm-1 of the lowest absorption band was observed compared to parent SQB, which is even larger than the shift for dSQB-1 (ca. 1 000 cm-1). On the other hand, a partial stiffening of the polymer backbone is attempted to create a bias for elongated polymer chains. In this respect, the synthetic approach is to replace every second biarylaxis with the rigid transoid benzodipyrrolenine unit. Despite a rather low average degree of polymerization < 10, exclusively red-shifted absorption maxima are observed in all solvents used. In order to complete the picture of intramolecular aggregates through the selective design of H-aggregates, a squaraine-squaraine copolymer was synthesised containing the classic cisoid indolenine as well as the cisoid quinoline building block. Taking advantage of the highly structure directing self-assembly character of the quinoline moiety, the copolymer pSQBC indeed showes a broad, blue-shifted main absorption band in comparison with the monomer unit dSQBC. The shape of the absorption band manifold solely exhibited a minor solvent and temperature dependence indicating a persistent H-aggregate behaviour. Hence, as a proof of concept, it is shown that the optical properties of the polymers (H- and J-aggregate) and the corresponding superstructure can be inherently controlled by an adequate design of monomer precursors. The last chapter of this work deals, in contrast to all other chapters, with intermolecular aggregates. It is shown that the two star-shaped hexasquarainyl benzenes hSQA-1 and hSQA-2 exhibit a strong propensity for self-organisation. Concentration- and temperature-dependent studies reveal a great driving force for self-assembly in acetone. While the larger hSQA-2 instantaneously forms stable aggregates, the aggregates of hSQA-1 shows a pronounced kinetic stability. Taking advantage of the kinetic persistency of these aggregates, the corresponding kinetic activation parameters for aggregation and deaggregation can be assessed. The absorption spectra of both hexasquarainyl benzenes in the aggregated state reveal some striking differences. While hSQA-1 features an intensive, very narrow and blue-shifted absorption band, two red-shifted bands are observed for hSQA-2, which are closely located at the monomer absorption. The very small bandwidth of hSQA-1 are interpreted to be caused by exchange narrowing and pointed towards highly ordered supramolecular aggregates. The concentration-dependent data of the two hexasquarainyl benzenes can be fitted to the dimer-model with excellent correlation coefficients, yielding binding constants in excess of 10^6 M-1, respectively. Such high binding constants are very surprising, considering the unfavourable bulky 3,3-dimethyl groups of the indolenine units which should rather prevent aggregation. Joint theoretical and NMR spectroscopic methods were applied to unravel the supramolecular aggregate structure of hSQA-1, which is shown to consist of two stacked hexasquarainyl benzenes resembling the picture of two stacked bowls.}, subject = {Squaraine}, language = {en} } @phdthesis{Schulze2016, author = {Schulze, Marcus}, title = {Ruthenium Complexes as Water Oxidation Catalysts and Photosensitizers}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-142454}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2016}, abstract = {In der vorliegenden Arbeit werden Aspekte der photokatalytischen Wasseroxidationsreaktion behandelt. Der erste Themenschwerpunkt der Dissertation besch{\"a}ftigt sich mit einem supramolekularen Makrozyklus, der drei Rutheniummetallzentren enth{\"a}lt. Dieser neuartige Katalysator zeigt eine sehr hohe katalytische Aktivit{\"a}t und gew{\"a}hrt neue Einblicke in den Mechanismus der Wasseroxidationsreaktion. Des Weiteren wird auf die mit Licht interagierenden Komponenten der photokatalytischen Wasseroxidation eingegangen. Hierbei haben sich azabenz-anellierte Perylenderivate als vielseitige Farbstoffklasse herausgestellt. Die Kombination dieser Farbstoffe mit Metallkomplexen liefert metallorganische Verbindungen, die als Photosensibilisatoren eingesetzt werden k{\"o}nnen.}, subject = {Farbstoff}, language = {en} } @phdthesis{Ruehl2014, author = {R{\"u}hl, Nicolas}, title = {Spektroelektrochemie an einzelnen (6,5)-Kohlenstoffnanor{\"o}hren}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-112162}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2014}, abstract = {Im Rahmen der vorliegenden Arbeit wurde durch einzelmolek{\"u}lspektroskopischer bzw. -mikroskopischer Methoden in Kombination mit einer mikrofluischen Zel- le unter Potenzialkontrolle die Elektrochemie von einzelnen einwandigen (6,5)- Kohlenstoffnanor{\"o}hren untersucht. Hierf{\"u}r wurde ein Nahinfrarot-Photolumineszenz- Mikroskop aufgebaut und eine speziell an die experimentellen Vorgaben angepasste elektrochemische Zelle entwickelt, insofern als drei Elektroden (Arbeits-, Gegen- und Referenzelektrode) in einen mikrofluidischen Chip integriert wurden. Dar{\"u}ber hinaus war f{\"u}r die Durchf{\"u}hrung der Experimente unter Wasser- und Sauerstoffaus- schluss die Konstruktion eines Handschuhkastens notwendig, sowie eine allgemeine Vorbehandlung der Elektrolytl{\"o}sungen zur Entfernung gel{\"o}ster Gase und Wasserreste. Ein weiteres Projekt umfasste den Aufbau einer chemischen Gasphasenabschei- dungsapparatur zur Synthese von Kohlenstoffnanor{\"o}hren. Die hierbei durchgef{\"u}hrten Experimente erbrachten Klarheit {\"u}ber den Einfluss der Prozessparameter Druck, Temperatur und Durchflussrate an Edukten. Aus den PL-Intensit{\"a}ts{\"a}nderungen bei Potenzialvariation konnten Reduktions- und Oxidationspotenziale (ERed = 0.15 V; EOx = 1.34 V) einzelner (6,5)-SWNTs gegen- {\"u}ber einer Platin Referenzelektrode und einem daraus resultierenden Redoxpotenzial von ∆ERedOx = 1.19 V ermittelt werden. Durch diese einzelmolek{\"u}lspektroskopische Methode konnte zum einen gew{\"a}hrleistet werden, dass nur dieser spezielle Chira- lit{\"a}tstyp untersucht wurde und zum anderen eine Verf{\"a}lschung der Resultate durch einen Potenzialabfall wie er typischerweise in CNT-Filmen auftritt aussgeschlossen werden. Eine Kombination der PL-Daten mit der Ramanintensit{\"a}tsabh{\"a}ngigkeit des (6,5)-SWNT-S2-{\"U}bergangs bei Potenzialvariation erlaubte eine genauere Analyse des L{\"o}schmechanismus der PL von Kohlenstoffnanor{\"o}hren. Mithilfe eines von Her- tel et al. entwickelten diffusionslimitierten Stoßdesaktivierungsmodells konnte eine invers-quadratische Proportionalit{\"a}t zwischen der (6,5)-SWNT-Emission und den spannungsinduzierten Ladungstr{\"a}gern ausgemacht werden. Auf Grundlage dieses Ergebnisses folgt, dass die {\"u}ber Photolumineszenz{\"a}nderungen ermittelten Reduktions-und Oxidationswerte nicht mit den Bandkanten der CNTs {\"u}bereinstimmen m{\"u}ssen, und dass f{\"u}r deren Bestimmung vielmehr auf Raman- bzw. Absorptionsspektroskopi- sche Techniken zur{\"u}ckgegriffen werden muss. Die einzelmolek{\"u}lspektroskopische Herangehensweise erm{\"o}glichte ferner eine statis- tische Analyse der Verteilung der Reduktions- und Oxidationspotenziale im Vergleich zu den jeweiligen Erwartungswerten. Hierdurch konnte eine Einteilung der Modifika- tionseinfl{\"u}sse auf das SWNT-Redoxverhalten in zwei Grenzf{\"a}lle erfolgen. Es wurde angenommen, dass diese als "Dispergiermitteleffekte" und "CNT-Strukturdefekte" be- zeichneten Auswirkungen entweder das Resultat einer heterodispersen Verteilung an DOC auf der CNT-Oberfl{\"a}che oder eine Folge von Defekten in der CNT-Gitterstruktur waren. In diesem Zusammenhang ergab sich aus der interpartikul{\"a}ren Analyse der Reduktions- und Oxidationswerte eine Korrelation, die einem dominierenden Einfluss der "CNT-Strukturdefekte" zugeordnet werden konnte. Dieser Beobachtung entgegen- gesetzt konnten aber auch {\"u}ber Untersuchungen der Redoxpotenziale innerhalb einer (6,5)-SWNT lokale Bereiche ausgemacht werden, die eine signifikante Abh{\"a}ngigkeit von "Dispergiermitteleffekte" aufwiesen. Abgesehen von diesen Einfl{\"u}ssen auf den Emissionsverlauf wurde auch eine Be- trachtung der Breite des spannungsgesteuerten Emissionsabfall durchgef{\"u}hrt. Da- raus konnte ermittelt werden, dass diese Ausdehnung eine Konsequenz aus der PL- L{\"o}schungseffizienz der Ladungstr{\"a}ger ist und, dass bei einer Verteilung von 0.32 L{\"o}schzentren pro Nanometer eine vollst{\"a}ndige Abnahme der Photolumineszenzinten- sit{\"a}t induziert wird. Dar{\"u}ber hinaus wurde im Rahmen dieser Arbeit das redoxchemische Verhalten in- dividueller (6,5)-SWNTs in Wechselwirkung mit Ferrocenmolek{\"u}len untersucht. Die erhaltenen Ergebnisse ließen annehmen, dass die sich ausbildende Verbindung nicht-kovalenter Natur ist. Zwei verschiedene Gr{\"u}nde f{\"u}hrten zu dieser Erkennt- nis: einerseits ließen sich die Ferrocenmolek{\"u}le von der CNT-Oberfl{\"a}che durch ein Durchsp{\"u}len des mikrofluidischen Kanals mit einer reinen DMF-L{\"o}sung entfernen und andererseits war keine dauerhafte Emissionsminderung durch die Ausbildung kovalenter Bindungen zu beobachten. Aus der potenzialabh{\"a}ngigen PL wurde zudem ein Elektronentransfer der Ferrocenmolek{\"u}le in die optisch generierten L{\"o}cher des CNT-Valenzbandes festgestellt und {\"u}ber eine anregungsintensit{\"a}tsabh{\"a}ngige Messung die Zunahme dieses Ladungstransfers bei steigendem Photonenfluss nachgewiesen. Hinsichtlich der Anwendung von Kohlenstoffnanor{\"o}hren zur Elektrolyse bzw. Photo- lyse von Wasser wurde auch die Redoxchemie von (6,5)-SWNTs in diesem Solvens untersucht. Bez{\"u}glich der Emissionsintensit{\"a}t konnte gezeigt werden, dass diese im Vergleich zu organischen L{\"o}sungsmitteln reduziert vorliegt. Außerdem wurde eine irreversible Reaktion nach anodischer Polarisation {\"u}ber eine dauerhafte L{\"o}schung der PL beobachtet. Die Bestimmung der hierf{\"u}r notwendigen Reaktionsumst{\"a}nde erbrachte, dass Wasser, Exzitonen (erzeugt durch optische Anregung) und spannungs- induzierte L{\"o}cher im Valenzband zur Bildung einer [SWNT(Q)]-Spezies f{\"u}hren, welche die irreversible Minderung der CNT-Emission verursacht. Dar{\"u}ber hinaus konnte die Reaktionsgeschwindigkeit {\"u}ber eine Kinetik pseudo-nullter-Ordnung be- schrieben werden, unter der Voraussetzung, dass die soeben genannten Parameter konstant verblieben. Desweiteren zeigte sich in einer ferrocenhaltigen L{\"o}sung, dass der L{\"o}scheffekt der [SWNT(Q)]-Spezies im anodischen Potenzialbereich teilweise reduziert wird. Es wurde angenommen, dass diese Beobachtung auf eine Oxidation der L{\"o}schzentren durch die Fc+-Kationen gr{\"u}ndet. Mit Hilfe der CVD-Apparatur gelang es Kohlenstoffnanor{\"o}hren zu synthetisieren, wobei Ethanol als Kohlenstoffquelle und ein Eisen-Kobalt-Zeolith-Gemenge als Ka- talysator diente. Die Analyse der verschiedenen Prozessparameter zeigte, dass bei T = 750 °C das beste Verteilungsverh{\"a}ltnis zwischen den gew{\"u}nschten (6,5)-SWNTs und anderen CNT-Chiralit{\"a}ten bzw. dem amorphen Kohlenstoff vorliegt. Hierf{\"u}r war, dass bei T < 750 °C die Verbrennung unerw{\"u}nschter amorpher Kohlenstoffreste nur geringf{\"u}gig stattfindet, und dass bei T > 750 °C die Bildung anderer Chiralit{\"a}ten mit gr{\"o}ßerem Durchmesser als die (6,5)-SWNT bevorzugt wurde. Die Variation der Durchflussrate hingegen wirkte sich nur in einer absoluten Zunahme aller Chirali- t{\"a}ten aus. Die Steigerung des (6,5)-SWNT-Anteils f{\"u}r h{\"o}here Durchfl{\"u}sse gelang trotzdem durch die geschickte Auswahl geeigneter Druck- und Temperaturwerte. Die Experimente zur Untersuchung der Druckabh{\"a}ngigkeit wiesen auf eine Relation mit dem Gesetz von Le Chatelier hin, insofern als bei einer Druckverringerung eine Verschiebung der Ethanol-Crackreaktion auf Produktseite stattfand. In diesem Zusam- menhang wurde angenommen, dass die damit verst{\"a}rkt gebildeten Molek{\"u}le Ethan, Ethen und Methan den CNT-Anteil zwar erh{\"o}hen, jedoch auch eine Steigerung der amorphen Kohlenstoffkonzentration verursachen. Dementsprechend ergab ein Druck von p = 9 mbar das beste (6,5)-SWNT zu dem amorphen Kohlenstoffverh{\"a}ltnis. Anhand der Arbeiten in dieser Dissertation sind neue Erkenntnisse zwischen der PL-Sensitivit{\"a}t von (6,5)-SWNTs und deren Ladungszustand erhalten worden. Insbe- sondere die genaue Bestimmung der Korrelation zwischen der Photolumineszenz und den induzierten Ladungstr{\"a}gern erm{\"o}glicht einen gezielteren Einsatz von Kohlenstoff- nanor{\"o}hren - so zum Beispiel im Bereich der Sensorik. In diesem Zusammenhang zeigen auch die interpartikul{\"a}ren Analysen der Redoxpotenzialverteilung die genau- en Auswirkungen vom L{\"o}sungsmittel und der Defektdichte auf die elektronische Struktur der CNTs auf. Dar{\"u}ber hinaus kann aus der Ursachenbestimmung f{\"u}r die Varianz der literaturbekannten Reduktions- bzw. Oxidationspotenziale fortan die ge- eignete spektroskopische Methode zur Evaluierung der Position von Leitungs- und Valenzband in Kohlenstoffnanor{\"o}hren besser eingegrenzt werden. Die spektroelektro- chemischen Analysen von (6,5)-SWNTs im L{\"o}sungsmittel Wasser und speziell die Bestimmung der Kinetik f{\"u}r die auftretende Reaktion liefern einen tieferen Einblick in die Wechselwirkung (6,5)-SWNT-H2O. Diese Ergebnisse sind insbesondere bei der Verwendung von Kohlenstoffnanor{\"o}hren als Elektrodenmaterial f{\"u}r die photolytische bzw. elektrolytische Spaltung von Wasser in Wasserstoff und Sauerstoff von Bedeu- tung. Neben der Untersuchung der SWNT-Wasser Interaktion unter andoischer und optischer Anregung, die zu einer kovalenten Bindung f{\"u}hrte, wurde mit Hilfe der (6,5)- SWNT-Ferrocen Wechselwirkung ein Beispiel f{\"u}r eine nichtkovalente Redoxreaktion dargestellt, womit ein Vergleich dieser beiden Spezies und ihrer unterschiedlichen Auswirkungen auf die elektronische Struktur aufgezeigt werden konnte.}, subject = {Spektroelektrochemie}, language = {de} } @phdthesis{Steeger2015, author = {Steeger, Markus}, title = {Energy and Charge Transfer in Donor-Acceptor Substituted Hexaarylbenzenes}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-112520}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2015}, abstract = {The focus of this work was the investigation of energy transfer between charge transfer states. For this purpose the multidimensional chromophores HAB-S, HAB-A, B1 and B2 were synthesised, each consisting of three electron donor and three electron acceptor redox centres linked symmetrically or asymmetrically by the hexaarylbenzene framework. Triarylamines represent in all these compounds the electron donors, whereas the electron poor centres were triarylboranes in B1 and B2 and PCTM centres in HAB-S and HAB-A, respectively. The hexaarylbenzenes were obtained by cobalt catalysed cyclotrimerisation of the respective tolan precursors. In addition, Star was synthesised, which consists of a central PCTM linked to three triarylamin centres by tolan bridging units in a star-like configuration. The hexaarylbenzene S1a/b substituted with six squaraine chromophores could not be realised. It is assumed that the cyclotrimerisation catalyst Co2(CO)8 does not tolerate the essential hydroxyl groups in the tolan precursor S2a. The alternative reaction pathway to execute the cyclotrimerisation reaction first and introduce the hydroxyl groups thereafter failed as well, because the required hexaarylbenzene substituted by six semisquaric acid moieties could not be synthesised. However, energy transfer interactions could be investigated in the tolan precursor S2a with two squaraine units to obtain information about the electronic coupling provided by the tolan bridge. For all multidimensional compounds model molecules were synthesised with only a single donor-acceptor pair (B3, Star-Model and HAB-Model). This allows a separate consideration of energy and charge transfer processes. It has to be stressed that in all before mentioned multidimensional compounds the "through bond" energy transfer interaction between neighbouring IV-CT states is identical to a transfer of a single electron between two redox centres of the same kind (e.g. TAA -> TAA+). The latter can be analysed by electron transfer theory. This situation is observed when the two IV-CT states transferring energy share one redox centre. All compounds containing PCTM centres were characterised by paramagnetic resonance spectroscopy. Thereby, a weak interaction between the three PCTM units in HAB-S and HAB-A was observed. In addition, when oxidising Star-Model, a strongly interacting singlet or triplet state was obtained. In contrast, signals corresponding to a weakly interacting biradical were obtained for HAB-Model+. This indicates a strong electronic coupling between the redox centres provided by the tolan bridge and a weak coupling when linked by the hexaarylbenzene. This trend is supported by UV/Vis/NIR absorption measurements. The analysis of the observed IV-CT absorption bands by electron transfer theory reveals a weak electronic coupling of V = 340 cm-1 in HAB-Model and a distinctly stronger coupling of V = 1190-2900 cm-1 in Star-Model. In the oxidised HAB-S+, Star+ and Star-Model+ a charge transfer reversed from that of the neutral species, that is, from the PCTM radical to the electron poorer cationic TAA centre, was observed by spectroelectrochemistry. The temporal evolution of the excited states was monitored by ultrafast transient absorption measurements. Within the first picosecond stabilisation of the charge transfer state was observed, induced by solvent rotation. Anisotropic transient absorption measurements revealed that within the lifetime of the excited state (tau = 1-4 ps) energy transfer does not occur in the HABs whereas in the star-like system ultrafast and possibly coherent energy redistribution is observed. Taken this information together the identity between energy transfer and electron transfer in the specific systems were made apparent. It has to be remarked that neither energy transfer nor charge transfer theory can account for the very fast energy transfer in Star. The electrochemical and photophysical properties of B1 and B2 were investigated by cyclic voltammetry, absorption and fluorescence measurements and were compared to B3 with only one neighbouring donor-acceptor pair. For the asymmetric B2 CV measurements show three oxidations as well as three reduction peaks whose peak separation is greatly influenced by the conducting salt due to ion-pairing and shielding effects. Consequently, peak separations cannot be interpreted in terms of electronic couplings in the generated mixed valence species. Transient absorption, fluorescence solvatochromism and absorption spectra show that charge transfer states from the amine to the boron centres are generated after optical excitation. The electronic donor-acceptor interaction is weak though as the charge transfer has to occur predominantly through space. The electronic coupling could not be quantified as the CT absorption band is superimposed by pi-pi* transitions localised at the amine and borane centres. However, this trend is in good agreement to the weak coupling measured for HAB-Model. Both transient absorption and fluorescence upconversion measurements indicate an ultrafast stabilisation of the charge transfer state in B1- B3 similar to the corresponding observations in HAB-S and Star. Moreover, the excitation energy of the localised excited charge transfer states can be redistributed between the aryl substituents of these multidimensional chromophores within fluorescence lifetime (ca. 60 ns). This was proved by steady state fluorescence anisotropy measurements, which further indicate a symmetry breaking in the superficially symmetric HAB. Anisotropic fluorescence upconversion measurements confirm this finding and reveal a time constant of tau = 2-3 ps for the energy transfer in B1 and B2. It has to be stressed that, although the geometric structures of B1 and HAB-S are both based on the same framework and furthermore the neighbouring CT states show in both cases similar Coulomb couplings and negligible "through bond" couplings, very fast energy transfer is observed in B1 whereas in HAB-S the energy is not redistributed within the excited state lifetime. To explain this, it has to be kept in mind that the energy transfer and the relaxation of the CT state are competing processes. The latter is influenced moreover by the solvent viscosity. Hence, it is assumed that this discrepancy in energy transfer behaviour is caused by monitoring the excited state in solvents of varying viscosity. Adding fluoride ions causes the boron centres to lose their acceptor ability due to complexation. Consequently, the charge transfer character in the donor-acceptor chromophores vanishes which could be observed in both the absorption and fluorescence spectra. However, the fluoride sensor ability of the boron centre is influenced strongly by the moisture content of the solvent possibly due to hydrogen bonding of water to the fluoride anions. UV/Vis/NIR absorption measurements of S2a show a red-shift by 1800 cm-1 of the characteristic squarain band compared to the model compound S20. From exciton theory a Coulomb coupling of V = 410 cm-1 is calculated which cannot account for this strong spectral shift. Consequently, "through-bond" interactions have to contribute to the strong communication between the two squaraine chromophores in S2a. This is in accordance with the strong charge transfer coupling calculated for the tolan spacer in Star-Model.}, subject = {Energietransfer }, language = {en} } @phdthesis{Ceymann2016, author = {Ceymann, Harald}, title = {Synthesis and Optical Spectroscopic Properties of Squaraine Superchromophores}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-136850}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2016}, abstract = {In this work the successful synthesis, the linear and nonlinear spectroscopic properties as well as the electrochemical behaviour of some linear and star-shaped squaraine superchromophores that are based on indolenine derivatives were presented. The attempt to synthesise similar chromophores which contained only benzothiazole squaraines failed unfortunately. However, one trimer that contained mixed benzothiazole indolenine squaraines could be synthesised and investigated as well. The linear spectroscopic properties, like red-shift and broadening of the absorption, of all superchromophores could be explained by exciton coupling theory. The heterochromophores (SQA)2(SQB)-N, (SQA)(SQB)2-N and (SQA)(SQB)-NH displayed additional to the typical squaraine fluorescence from the lowest excited state some properties that could be assigned to localised states. While the chromophores with N-core showed very small emission quantum yields, the chromophores with the other cores and the linear oligomers display an enhancement compared to the monomers. Transient absorption spectroscopy experiments of the star-shaped superchromophores showed, that their formally degenerated S1 states are split due to a deviation of the ideal C3 symmetry. This is also the reason for the observation of an absorption band for the highest exciton state, which is derived from the S1-state of the monomers, as its transition-dipole moment would be zero in the symmetrical case. The linear oligomers and the star-shaped superchromophores with a benzene or triarylamine core showed at least additive, sometimes even weak cooperative, behaviour in the two-photon absorption experiments. Additional to higher two-photon absorption cross sections the chromophores showed a pronounced broadening of the nonlinear absorption, due to symmetry breaking and a higher density of states. Unfortunately it was not possible to solve the problem of the equilibrium of the cisoid and the transoid structure of donor substituted azulene squaraines, due to either instability of the squaraines or steric hindrance.}, subject = {Squaraine}, language = {en} } @phdthesis{Steinbacher2015, author = {Steinbacher, Andreas Edgar}, title = {Circular dichroism and accumulative polarimetry of chiral femtochemistry}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-116500}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2015}, abstract = {This work brings forward successful implementations of ultrafast chirality-sensitive spectroscopic techniques by probing circular dichroism (CD) or optical rotation dispersion (ORD). Furthermore, also first steps towards chiral quantum control, i.e., the selective variation of the chiral properties of molecules with the help of coherent light, are presented. In the case of CD probing, a setup capable of mirroring an arbitrary polarization state of an ultrashort laser pulse was developed. Hence, by passing a left-circularly polarized laser pulse through this setup a right-circularly polarized laser pulse is generated. These two pulse enantiomers can be utilized as probe pulses in a pump--probe CD experiment. Besides CD spectroscopy, it can be utilized for anisotropy or ellipsometry spectroscopy also. Within this thesis, the approach is used to elucidate the photochemistry of hemoglobin, the oxygen transporting protein in mammalian blood. The oxygen loss can be triggered with laser pulses as well, and the results of the time-resolved CD experiment suggest a cascade-like relaxation, probably through different spin states, of the metallo-porphyrins in hemoglobin. The ORD probing was realized via the combination of common-path optical heterodyne interferometric polarimetry and accumulative femtosecond spectroscopy. Within this setup, on the one hand the applicability of this approach for ultrafast studies was demonstrated explicitly. On the other hand, the discrimination between an achiral and a racemic solution without prior spatial separation was realized. This was achieved by inducing an enantiomeric excess via polarized femtosecond laser pulses and following its evolution with the developed polarimeter. Hence, chiral selectivity was already achieved with this method which can be turned into chiral control if the polarized laser pulses are optimized to steer an enhancement of the enantiomeric excess. Furthermore, within this thesis, theoretical prerequisites for anisotropy-free pump--probe experiments with arbitrary polarized laser pulses were derived. Due to the small magnitude of optical chirality-sensitve signals, these results are important for any pump--probe chiral spectroscopy, like the CD probing presented in this thesis. Moreover, since for chiral quantum control the variation of the molecular structure is necessary, the knowledge about rearrangement reactions triggered by photons is necessary. Hence, within this thesis the ultrafast Wolff rearrangement of an α-diazocarbonyl was investigated via ultrafast photofragment ion spectroscopy in the gas phase. Though the compound is not chiral, the knowledge about the exact reaction mechanism is beneficial for future studies of chiral compounds.}, subject = {Ultrakurzzeitspektroskopie}, language = {en} } @phdthesis{Hartleb2015, author = {Hartleb, Holger Edgar Heinz Erich}, title = {Spektroelektrochemische Untersuchung von halbleitenden Kohlenstoffnanor{\"o}hren}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-116628}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2015}, abstract = {Der Schwerpunkt dieser Arbeit lag auf der spektroelektrochemischen Untersuchung von halbleitenden SWNTs. Hierbei wurden erstmalig Absorptions- und Photolumineszenzspektren ein und derselben SWNT-Probe simultan unter elektrochemischer Potentialkontrolle aufgenommen. Hierbei konnte gezeigt werden, dass die Messmethode einen entscheidenden Einfluss auf die erhaltene Bandl{\"u}cke besitzt und der in der Literatur gepr{\"a}gte Begriff der Elektrochemischen Bandl{\"u}cke aufgrund einer fehlenden allgemeing{\"u}ltigen Definition problembehaftet ist. So ergeben Photolumineszenzmessungen im Vergleich zu Raman- oder Absorptionsmessungen die kleinste Bandl{\"u}cke. Dies wurde auf die diffusionskontrollierte L{\"o}schung der Exzitonen an Ladungszentren zur{\"u}ckgef{\"u}hrt. Weiterhin wurden die optischen Spektren von SWNTs unter Ladungseinfluss analysiert und die zugrundeliegenden {\"A}nderungen der elektronischen Eigenschaften diskutiert. Neben SWNTs wurden die {\"U}bergangsmetalldichalkogenide MoS2 und WS2 spektroelektrochemisch untersucht. Auffallend im Vergleich zu den Messungen an SWNTs war der breite Potentialbereich, {\"u}ber den die Abnahme der exzitonischen Signale zu beobachten war. Dies kann auf die unterschiedliche elektronische Struktur von TMDs und SWNTs und den geringen Anteil von Einzellagen in den TMD-Proben zur{\"u}ckgef{\"u}hrt werden. Weiterhin konnte in den Absorptionsspektren unter Ladungseinfluss ein Signal beobachtet werden, welches auf die Entstehung von Trionen hindeutet. In einem weiteren Teilprojekt wurde eine elektrochemische Zelle zur Untersuchung von metallischen SWNT-Filmen als Elektrode f{\"u}r die Wasserstoffproduktion entwickelt und getestet. Hierbei gelang es die von Das et al. publizierte Aktivierung von SWNTs mit Schwefels{\"a}ure erfolgreich nachzuvollziehen und einen katalytischen Effekt der SWNTs auf die Wasserstoffentwicklung zu beobachten.}, subject = {Kohlenstoff-Nanor{\"o}hre}, language = {de} } @phdthesis{Klein2015, author = {Klein, Johannes Hubert}, title = {Electron Transfer and Spin Chemistry in Iridium-Dipyrrin Dyads and Triads}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-118726}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2015}, abstract = {The successful synthesis of a family of donor-iridium complex-acceptor triads (T1-T6, pMV1 and mMV1) and their electrochemical and photophysical properties were presented in this work. Triarylamines (TAA) were used as donors and naphthalene diimide (NDI) as acceptor. A bis-cyclometalated phenylpyrazole iridium dipyrrin complex acts as a photosensitiser. In addition, a molecular structure of T1 was obtained by single crystal X-ray diffraction. Transient absorption spectroscopy experiments of these triads resembled that upon excitation a photoinduced electron transfer efficiently generates long-lived, charge-separated (CS) states. Thereby, the electron-transfer mechanism depends on the excitation energy. The presence of singlet and triplet CS states was clarified by magnetic-field dependent transient-absorption spectroscopy in the nanosecond time regime. It was demonstrated that the magnetic field effect of charge-recombination kinetics showed for the first time a transition from the coherent to the incoherent spin-flip regime. The lifetime of the CS states could be drastically prolonged by varying the spacer between the iridium complex and the NDI unit by using a biphenyl instead of a phenylene unit in T4. A mixed-valence (MV) state of two TAA donors linked to an iridium metal centre were generated upon photoexcitation of triad pMV1 and mMV1. The mixed-valence character in these triads was proven by the analysis of an intervalence charge-transfer (IV-CT) band in the (near-infrared) NIR spectral region by femtosecond pump-probe experiments. These findings were supported by TD-DFT calculations. The synthesis of dyads (D1-D4) was performed. Thereby the dipyrrin ligand was substituted with electron withdrawing groups. The electrochemical and photophysical characterisation revealed that in one case (D4) it was possible to generate a CS state upon photoexcitation.}, subject = {Elektronentransfer}, language = {en} } @phdthesis{Turkin2022, author = {Turkin, Arthur}, title = {Vom Monomer zum Polymer: Iterative Synthese und optische Spektroskopie von Squarain-Oligomeren}, doi = {10.25972/OPUS-25795}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-257950}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2022}, abstract = {Mittels einer Schutzgruppenstrategie wurden Squarain-basierte monodisperse Oligomere synthetisiert. Die l{\"o}sungsmittelabh{\"a}ngigen Konformationen (Random Coil vs. Helix) wie auch der Faltungsprozess der Homooligomere wurden mittels optischer Spektroskopie, verschiedener NMR-Experimenten, Kleinwinkelneutronenstreuungsexperimenten sowie quantenchemischen Berechnungen n{\"a}her beleuchtet. Die optisch-spektroskopischen Beobachtungen wurden mithilfe der Exzitonenkopplungstheorie und einer Orientierungs- und Winkelabh{\"a}ngigkeit der {\"U}bergangsdipolmomente der Oligomere erkl{\"a}rt. Der hohe Windungsabstand der helikalen Konformation f{\"u}hrt zu einer Interkalation von L{\"o}sungsmittel, wodurch eine Art Klathrat gebildet wird. Zus{\"a}tzlich wurden mittels eines Frenkel-Exzitonenmodells die Absorptions- und Fluoreszenzspektren modelliert. Es konnten die Exzitonendelokalisationsl{\"a}ngen abgesch{\"a}tzt und die Auswirkung der energetischen und strukturellen Unordnungen auf die Absorptions- und Fluoreszenzspektren bestimmt werden. Die Absorptionsspektren werden vorwiegend durch strukturelle Unordnungen verbreitert, die Fluoreszenzspektren dagegen von energetischen {\"U}bergangsenergieabweichungen. Weiterhin wurden auch alternierende Squarain-Cooligomere synthetisiert und mittels optischer Spektroskopie untersucht. Es wurde, abh{\"a}ngig von dem gew{\"a}hlten L{\"o}sungsmittel, eine Verschiebung der Hauptbande beobachtet, was durch einen Random Coil vs. helikale-/schlaufenartige Konformation erkl{\"a}rt wird. Gest{\"u}tzt wurde dies mittels quantenchemischen Berechnungen der jeweiligen Konformationen. Abschließend wurden alternierende Squarain-Copolymere synthetisiert, in verschiedenen Gr{\"o}ßen aufgetrennt und mittels optischer Spektroskopie untersucht. Mittels EEI2D-Experimenten wurde die Exzitonendynamik in Abh{\"a}ngigkeit von der Kettenl{\"a}nge eingehender untersucht. Hierbei wird eine steigende, aber relativ abnehmende Koh{\"a}renzl{\"a}nge bestimmt, die Auswirkungen auf die Exzitonendynamik hat. Der Exzitonentransport weist erst wellenf{\"o}rmiges und dann subdiffuses Verhalten auf.}, subject = {Squarain}, language = {de} } @phdthesis{Voelker2014, author = {V{\"o}lker, Sebastian}, title = {Synthesis, Spectroscopic and Electrochemical Properties of Squaraine Polymers}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-101638}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2014}, abstract = {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.}, subject = {Squaraine}, language = {en} } @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{Kaiser2014, author = {Kaiser, Conrad}, title = {Donor-Bridge-Acceptor Systems with Varying Bridge Units for the Investigation of Intramolecular and Intermolecular Electron Transfer Processes}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-97614}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2014}, abstract = {Within this study, the influence of the energetics of the bridge unit on electron transfer (ET) in an electrode-bridge-donor system was investigated in a monolayer environment. This was realized by specifically designing molecules containing ferrocene carboxylic ester donors and hydroquinone derivatives as bridge units and by using a gold electrode as acceptor. The energetics of the hydroquinone derivatives was adjusted by synthetically varying its substituents with the intention of changing the ET speed and mechanisms. Thereby the choice of the substituents was based on the literature known half-wave potentials of similar solvated hydroquinone derivatives and successively confirming them by conducting cyclic voltammetry on the actual bridge units synthesized. Then, a synthetic pathway, which accommodated the limited stability of the integrated terminal ferrocene carbon acid ester, was developed and successfully employed. This was followed by developing a procedure for preparing very dense and highly ordered monolayers from the target molecules on self-made gold microelectrodes. For the electrochemical investigations, several electrolyte solutions were tested until one, which ensured low susceptibility of the characterization setup towards slight changes of the electrode arrangement and measurement parameters while ensuring sufficient stability of the monolayers, was found. Furthermore, a new, commercially available potentiostat was established for the impedance measurements, which reduced the stress on the monolayers during the electrochemical characterizations in comparison to the equipment used in many former studies. Regarding the determination of the ET rates, the data analysis protocol for the impedance measurements developed by Creager et al. was slightly adapted to allow analysis of the investigated monolayers despite their non-ideal behavior. In addition, the influence of changes to the electrical parameters of the impedance scans was investigated to minimize the error in the acquired data. The electrochemical analysis of the monolayers by conducting cyclic voltammetry on MA, MB and MC prepared from A, B and C confirmed the accomplishment of near ideal surface coverage and exceptionally high order. The surface coverages of MB and MC were, probably due to the space filled by the substituents on their bridge units, slightly lower than those of MA. Furthermore, the shape of the redox waves of the ferrocene carboxylic acid redox center in the voltammogram of MA showed a broadening and a shift towards higher potentials, which was assigned to electrostatic interference of oxidized terminal redox centers due to the especially dense packing. However, in the voltammogram of MB, no sharp redox waves of the bridge units, as predicted by the analysis of preliminary monolayers of the same type with low surface coverage, were present. This was attributed to the different and varying microenvironment of the bridge units deeply embedded within high-density monolayers. In detail, the different degree of shielding of each individual bridge unit from counter ions and solvent molecules probably resulted in the half wave potential being shifted to varying higher potentials, thus preventing the formation of sharp redox waves. In addition, electrostatic effects of oxidized bridge units could have enhanced this effect. This leads to the conclusion that the half-wave potentials of fully solvated bridge units determined by the cyclic voltammetry are not suited to predict the energetics of the oxidized bridge states embedded within the prepared high density monolayers. Finally, the monolayers were successfully analyzed by impedance spectroscopy, which showed that the ET rate of MA is slightly higher than that of MB, and both are higher than that of MC. All of the values were, according to literature, in the expected region considering the length and degree of conjugation of the backbone. However, this picture is relativized when considering the targeted energetic alignment of the bridge units. According to the predicted very small energy gap between the oxidized states of the donor and the bridge unit in MB, a domination of the hopping mechanism should have led to a several orders of magnitude higher ET rate than in MA and MC. That this was not the case was attributed to the underestimation of the energy of the oxidized bridge states by utilizing cyclic voltammetry of the fully solvated bridge units (see above). According to the small differences of the ET rates the superexchange process was assumed to be the dominating mechanism not only in MA and MC but also in MB. However, even when shifted, the predicted energetic order of the oxidized bridge states should have led to a moderately decreasing ET rate from MB over MA to MC. The reason for the actual ET rate in MA being slightly higher than in MB might be found in the electrostatic interference of the terminal redox centers in MA (see above). In conclusion, the targeted model systems were prepared and the ET rates were successfully determined. However, the problems concerning the relative energetic positioning of the involved states within the dense monolayers prevented the specific alteration of the speed and mechanism of the ET. The reason for this can be probably found in the high density and order of the monolayers prepared within this work, which hamper the intrusion of the components of the electrolyte solutions. This various degree of stabilization for the individual bridge units by counter ions and solvent molecules leads to the energy of the oxidized bridge states being splitted and shifted towards higher potentials with respect to fully solvated bridge units. This effect might be further enhanced by electrostatics of neighboring already oxidized bridge states. All this makes the predetermination of the energetics of the embedded bridge units extremely difficult. On one hand, this behavior can be considered an obstacle and could probably be circumvented by designing molecules with bulky anchor groups and rigid molecular backbones, which would ensure perpendicular arrangement to the surface and full exposure of the bridge and terminal redox centers to the solvent molecules and counter ions. On the other hand, monolayers which completely embed integral redox centers might open up the opportunity to study the effects of microenvironments similar to those in solid state materials. Regarding mixed valence compounds, the present study focuses on bistriarylamine radical cation F∙+, which contains the [3.3]paracyclophane bridge unit. The results were compared to the, except for the bridge units, identical literature known compounds G∙+ and N∙+ with [2.2]paracyclophane and p-xylene bridges respectively. This led to the conclusion that slightly different bridge units can induce substantial changes to the internal reorganization energy. This is especially noteworthy since it is usually believed that structural adaption limited to the redox centers taking part in the charge transfer dominates the internal reorganization energy. Furthermore, the application of the two-state Mulliken-Hush approach shows that compounds F∙+ and G∙+ have near identical couplings and similar thermal barriers. Confirmation of the latter finding as well as near identical thermal electron transfer rates for both compounds were provided via a cooperation project by Grampp et al. in which these values were directly extracted from temperature dependent electron paramagnetic resonance measurements. These results are quite unexpected since the "through-space" distances of the stacked pi-systems in the paracyclophane bridges differ significantly. They are well within the sum of the van der Waals radii in G∙+ and barely within them in compound F∙+. In addition, these findings weaken the common assumption of the ethylene bridges in G∙+ substantially adding to the electronic coupling, since then, in F∙+, due to its propylene linkers, the coupling should be substantially reduced. Finally, relying on the fact that the electronic couplings are only three times higher and the thermal electron transfer rates are only one order of magnitude higher for N∙+ than for compounds F∙+ and G∙+ shows that intermolecular electron transfer in solid state materials can remain efficient, if the interacting pi-systems stay within the sum of van der Waals radii of their carbons. Concerning the donor-acceptor dyads, the current investigation centers on triarylamine-cyclophane-naphtalene diimide (TAA-CP-NDI) compounds which display almost complete photoinduced charge separation. Furthermore, their singlet charge separated states show lifetimes of hundreds of nanoseconds, which is rarely found in such simple dyads. In the present case they can be attributed to the particular amount of electronic coupling V (on the order of 100 cm^-1), which is brought about by incorporation of the smallest model systems for pi-stacks, the CPs, together with the nodes on the NDI lowest unoccupied molecular orbital, which electronically decouples the central NDI from its nitrogen substituents. In agreement with studies of [2.2]- and [3.3]paracyclophane bridged mixed valence compounds (see above), the cycolphane bridged dyads show very similar electronic coupling when dealing with ground state processes like charge recombination. However, when investigating excited state processes, like charge separation in the TAA-CP-NDI dyads, one has to bear in mind that the CP orbitals are involved in the formation of intermediate states that likely possess charge transfer character. In this case, the [2.2]paracyclophane bridge obviously induces a stronger coupling than the [3.3]paracyclophane. Another interesting property of the dyads studied here is the substantial population of the triplet charge separated (CS) state of ca. one third regarding both CS states, which is brought about by singlet-triplet interconversion from the singlet CS state. Thus, the triplet CS state with a lifetime of several microseconds acts as a kind of buffer for the CS state before recombining to the ground state and, thus, leads to distinctly prolonged overall lifetimes of the charge separated states. Thus it can be concluded that the intersystem crossing and charge recombination (CR) processes of the CS states are governed by a delicate balance of a large electronic coupling V and a large exchange interaction 2J (both with regard to systems containing a through-space pathway). The latter appears to be induced by second order interaction with a local triplet state lying close in energy to the CS state. This balance results in slow CR- and singlet-triplet- interconversion rates, which differ only by one order of magnitude. Compared to the many NDI containing dyads studied so far, these features of the dyads studied here are, to the best of our knowledge, unique. Especially the combination of high quantum yield of charge separation, long lifetimes and high energy of the charge separated state make the investigated systems interesting for practical applications. Furthermore, the presented unraveling of the underlying mechanisms is of substantial value for the future design of dyads for practical applications regarding the implementation and adjustment of these favorable properties.}, subject = {Elektronentransfer}, language = {en} } @phdthesis{Duerrbeck2013, author = {D{\"u}rrbeck, Nina}, title = {Photoinduced Charge-Transfer Processes in Redox Cascades based on Triarylamine Donors and the Perchlorinated Triphenylmethyl Radical Acceptor}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-90078}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2013}, abstract = {In this work, a series of redox cascades was synthesised and investigated in view of their photophysical and electrochemical properties. The cascades are based on a perchlorinated triphenylmethyl radical acceptor and two triarylamine donors. Absorption spectra showed the presence of charge-transfer bands in the NIR range of the spectra, which pointed to the population of a charge-transfer state between a triarylamine donor and the radical acceptor. A weak to moderate emission in the NIR range of the spectra was observed for all compounds in cyclohexane. Spectroelectrochemical measurements were used to investigate the characteristic spectral features of the oxidised and reduced species of all compounds. Transient absorption spectra in the ns- and fs-time regime revealed an additional hole transfer in the cascades between the triarylamine donors, resulting in a charge-separated state. Charge-separation and -recombination processes were found to be located in the ps-time regime.}, subject = {Ladungstransfer}, language = {en} } @phdthesis{Riese2019, author = {Riese, Stefan}, title = {Photophysics and Spin Chemistry of Donor-Acceptor substituted Dipyrrinato-Metal-Complexes}, doi = {10.25972/OPUS-18022}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-180228}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2019}, abstract = {In this thesis, the photophysics and spin chemistry of donor-photosensitizer-acceptor triads were investigated. While all investigated triads comprised a TAA as an electron donor and a NDI as an electron acceptor, the central photosensitizers (PS) were different chromophores based on the dipyrrin-motif. The purity and identity of all target compounds could be confirmed by NMR spectroscopy, mass spectrometry and elemental analysis. The first part of the work dealt with dipyrrinato-complexes of cyclometalated heavy transition metals. The successful synthesis of novel triads based on Ir(III), Pt(II) and Pd(II) was presented. The optical and electrochemical properties indicated charge separation (CS), which was confirmed by transient absorption (TA) spectroscopy. TA-spectroscopy also revealed that the process of CS is significantly slower and less efficient for the triads based on Pt(II) and Pd(II) than for the analogous Ir(III) triads. This is mostly due to a much more convoluted reaction pathway, comprising several intermediate states before the formation of the final charge separated state (CSS2). On the other hand, CSS2 exhibits long lifetimes which are dependent on the central metal ion. While the Ir(III) triads show lifetimes of about 0.5 µs in MeCN, the Pt(II) and Pd(II) analogues show lifetimes of 1.5 µs. The magnetic field effect on the charge recombination (CR) kinetics of CSS2 was investigated by magnetic field dependent ns-TA spectroscopy and could be rationalized based on a classical kinetic scheme comprising only one magnetic field dependent rate constant k±. The behavior of k± shows a clear separation of the coherent and incoherent spin interconversion mechanisms. While the coherent spin evolution is due to the isotropic hyperfine coupling with the magnetic nuclei of the radical centers, the incoherent spin relaxation is due to a rotational modulation of the anisotropic hyperfine coupling tensor and is strongly dependent on the viscosity of the solvent. This dependence could be used to measure the nanoviscosity of the oligomeric solvent pTHF, which was found to be distinctly different from its macroviscosity. The second part of the work dealt with bisdipyrrinato complexes and their bridged porphodimethenato (PDM) analogues. Initially, the suitability of the different chromophores for the use as PS in donor-acceptor substituted triads was tested by a systematic investigation of their steady state and transient properties. While the PDM-complex of Zn(II) and Pd(II) exhibited promising characteristics such as a high exited state lifetime and relatively intense emission, the purely organic parent PDM and the non-bridged bisdipyrrinato-Pd(II) complex were less suitable. The difference between the two Pd(II) complexes could be explained by a structural rearrangement of the non-bridged complex which results in a non-emissive metal centered triplet state with disphenoidal geometry. This rearrangement is prevented by the dimethylmethylene-bridges in the bridged analogue resulting in higher phosphorescence quantum yields and excited state lifetimes. With the exception of the Zn(II)PDM-complex, the synthesis of novel donor acceptor substituted triads could be realized for all desired central chromophores. They were investigated equivalently to the cyclometalated triads described in the first part. The steady state properties indicate a stronger electronic coupling between the subunits due to the lack of unsaturated bridges between the donor and the central chromophore. Photoinduced CS occurs in all investigated triads. Due to the low exited state lifetimes of the central chromophores, CSS is formed less efficiently for the triads based on the unbridged Pd(II)-complex as well as the purely organic PDM. In the triad based on the bridged Pd(II) complex, the CR of CSS2 is faster than its formation resulting in low intermediate concentrations. For its elongated analogue, this is not the case and CSS2 can be observed clearly. Although the spin-chemistry of the triads based on bisdipyrrinato-Pd(II) and porphodimethenato-Pd(II) is less well understood, first interpretations of the magnetic field dependent decay kinetics gave results approximately equivalent to those obtained for the cyclometalated triads. Furthermore, the MFE was shown to be useful for the investigation of the quantum yield of CS and the identity of the observed CSSs. In both parts of this work, the influence of the central photosensitizer on the photophysics and the spin chemistry of the triads could be shown. While the process of CS is directly dependent on the PS, the PS usually is not directly involved in the final CSSs. None the less, it can still indirectly affect the CR and spin chemistry of the CSS since it influences the electronic coupling between donor and acceptor, as well as the geometry of the triads.}, subject = {Charge-transfer-Komplexe}, language = {en} } @phdthesis{Steinmetzger2020, author = {Steinmetzger, Christian}, title = {Fluorogenic Aptamers and Fluorescent Nucleoside Analogs as Probes for RNA Structure and Function}, doi = {10.25972/OPUS-20760}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-207604}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2020}, abstract = {RNA plays a key role in numerous cellular processes beyond the central dogma of molecular biology. Observing and understanding this wealth of functions, discovering new ones and engineering them into purpose-built tools requires a sensitive means of observation. Over the past decade, fluorogenic aptamers have emerged to fill this niche. These short oligonucleotides are generated by in vitro selection to specifically interact with small organic fluorophores and can be utilized as genetically encoded tags for RNAs of interest. The most versatile class of fluorogenic aptamers is based on derivatives of hydroxybenzylidene imidazolone (HBI), a conditional fluorophore mimicking the chromophore structure found in green and red fluorescent proteins. The respective aptamers are well-known by the "vegetable" nomenclature, including Spinach, Broccoli and Corn, and have found numerous applications for studying RNA function in vitro and in cells. Their success, however, is somewhat overshadowed by individual shortcomings such as a propensity for misfolding, dependence on unphysiologically high concentrations of magnesium ions or, in the case of Corn, dimerization that might affect the function of the tagged RNA. Moreover, most fluorogenic aptamers exhibit limited ligand promiscuity by design, thereby restricting their potential for spectral tuning to a narrow window of wavelengths. This thesis details the characterization of a new fluorogenic aptamer system nicknamed Chili. Chili is derived from an aptamer that was originally selected to bind 4-hydroxy-3,5-dimethoxy¬hydroxy-benzylidene imidazolone (DMHBI), resulting in a green fluorescent complex. Unlike other aptamers of its kind, Chili engages in a proton transfer cycle with the bound ligand, resulting in a remarkably large Stokes shift of more than 130 nm. By means of an empirical ligand optimization approach, several new DMHBI derivatives were found that bind to Chili with high affinity, furnishing complexes up to 7.5 times brighter compared to the parent ligand. In addition, Chili binds to π-extended DMHBI derivatives that confer fluorescence in the yellow-red region of the visible spectrum. The highest affinity and degree of fluorescence turn-on for both green and red fluorogenic ligands were achieved by the incorporation of a unique, positively charged substituent into the HBI scaffold. Supplemented by NMR spectroscopy, kinetic and thermodynamic studies showed that the binding site of Chili is loosely preorganized in the absence of ligand and likely forms a G-quadruplex upon ligand binding. To showcase future applications, Chili was incorporated into a FRET sensor for monitoring the cleavage of an RNA substrate by a 10-23 DNAzyme. Besides aptamers as macromolecular fluorescent complexes, fluorescent nucleobase analogs are powerful small isomorphic components of RNA suitable for studying structure and folding. Here, the highly emissive nucleobase analog 4-cyanoindole (4CI) was developed into a ribonucleoside (r4CI) for this purpose. A new phosphoramidite building block was synthesized to enable site-specific incorporation of 4CI into RNA. Thermal denaturation experiments confirmed that 4CI behaves as a universal nucleobase, i.e. without bias towards any particular hybridization partner. Photophysical characterization established r4CI as a generally useful fluorescent ribonucleoside analog. In this work, it was employed to gain further insight into the structure of the Chili aptamer. Using several 4CI-modified Chili-HBI complexes, a novel base-ligand FRET assay was established to obtain a set of combined distance and orientation restraints for the tertiary structure of the aptamer. In addition to their utility for interrogating structure and binding, supramolecular FRET pairs comprising a fluorescent nucleobase analog donor and an innately fluorogenic acceptor hold great promise for the construction of color-switchable RNA aptamer sensor devices.}, subject = {Aptamer}, language = {en} } @phdthesis{Kaufmann2019, author = {Kaufmann, Christina}, title = {Discrete Supramolecular Architectures of Bay-linked Perylene Bisimide Dimers by Self-Assembly and Folding}, doi = {10.25972/OPUS-17300}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-173005}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2019}, abstract = {Supramolecular self-assembly of perylene bisimide (PBI) dyes via non-covalent forces gives rise to a high number of different PBI architectures with unique optical and functional properties. As these properties can be drastically influenced by only slightly structural changes of the formed supramolecular ensembles (Chapter 2.1) the controlled self-assembly of PBI dyes became a central point of current research to design innovative materials with a high potential for different applications as for example in the fields of organic electronics or photovoltaics. As PBI dyes show a strong tendency to form infinite aggregated structures (Chapter 2.2) the aim of this thesis was to precisely control their self-assembly to create small, structurally well-defined PBI assemblies in solution. Chapter 2.3 provides an overview on literature known strategies that were established to realize this aim. It could be demonstrated that especially backbone-directed intra- and intermolecular self-assembly of covalently linked Bis-PBI dyes evolved as one of the most used strategies to define the number of stacked PBI chromophores by using careful designed spacer units with regard to their length and flexibility. By using conventional spectroscopic methods like UV/Vis and fluorescence experiments in combination with NMR measurements an in-depth comparison of the molecular and optical properties in solution both in the non-stacked and aggregated state of the target compounds could be elucidated to reveal structure-property relationships of different PBI architectures. Thus, it could be demonstrated, that spacer units that pre-organize two PBI chromophores with an inter-planar distance of r < 7 {\AA} lead to an intramolecular folding, whereas linker moieties with a length between 7 to 11 {\AA} result in an intermolecular self-assembly of the respective Bis-PBIs dyes via dimerization to form well-defined quadruple PBI pi-stacks. Hence, if the used spacer units ensure an inter-planar distance r > 14 {\AA} larger oligomeric PBI pi-stacks are generated. In Chapter 4 a detailed analysis of the exciton coupling in a highly defined H-aggregate quadruple PBI pi-stack is presented. Therefore, bay-tethered PBI dye Bis-PBI 1 was investigated by concentration-dependent UV/Vis spectroscopy in THF and toluene as well as by 2D-DOSY-NMR spectroscopy, ESI mass spectrometry and AFM measurements confirming that Bis-PBI 1 self-assembles exclusively into dimers with four closely pi-stacked PBI chromophores. Furthermore, with the aid of broadband fluorescence upconversion spectroscopy (FLUPS) ensuring broadband detection range and ultrafast time resolution at once, ultrafast Frenkel exciton relaxation and excimer formation dynamics in the PBI quadruple pi-stack within 1 ps was successfully investigated in cooperation with the group of Dongho Kim. Thus, it was possible to gain for the first time insights into the exciton dynamics within a highly defined synthetic dye aggregate beyond dimers. By analysing the vibronic line shape in the early-time transient fluorescence spectra in detail, it could be demonstrated that the Frenkel exciton is entirely delocalized along the quadruple stack after photoexcitation and immediately loses its coherence followed by the formation of the excimer state. In Chapter 5 four well-defined Bis-PBI folda-dimers Bis-PBIs 2-4 were introduced, where linker units of different length (r < 7 {\AA}) and steric demand were used to gain distinct PBI dye assemblies in the folded state. Structural elucidation based on in-depth UV/Vis, CD and fluorescence experiments in combination with 1D and 2D NMR studies reveals a stacking of the two PBI chromophores upon folding, where geometry-optimized structures obtained from DFT calculations suggest only slightly different arrangements of the PBI units enforced by the distinct spacer moieties. With the resulting optical signatures of Bis-PBIs 2-4 ranging from conventional Hj-type to monomer like absorption features, the first experimental proof of a PBI-based "null-aggregate" could be presented, in which long- and short-range exciton coupling fully compensate each other. Hence, the insights of this chapter pinpoint the importance of charge-transfer mediated short-range exciton coupling that can significantly influence the properties of pi-stacked PBI chromophores In the last part of this thesis (Chapter 6), spacer-controlled self-assembly of four bay-linked Bis-PBI dyes Bis-PBIs 5-8 into well-defined supramolecular architectures was investigated, where the final aggregate structures are substantially defined by the nature of the used spacer units. By systematically extending the backbone length from 7 to 15 {\AA} defining the inter-planar distance between the tethered chromophores, different assemblies from defined quadruple PBI pi-stacks to larger oligomeric pi-stacks could be gained upon aggregation. In conclusion, the synthesis of nine covalently linked PBI dyes in combination with a detailed investigation of their spacer-mediated self-assembly behaviour in solution concerning structure-properties-relationships was presented within this thesis. The results confirm a strong exciton coupling in different types of Bis-PBI architectures e.g. folda-dimers or highly defined quadruple pi-stacks, which significantly influences their optical properties upon self-assembly.}, subject = {Supramolekulare Chemie}, language = {en} } @phdthesis{Michail2021, author = {Michail, Evripidis}, title = {Design and Development of a Two-Photon Absorption Induced Fluorescence Spectrometer and the Investigation of Nonlinear Optical Properties of Organic Chromophores}, doi = {10.25972/OPUS-24218}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-242185}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2021}, abstract = {Main objectives of the present dissertation can be divided in two parts. The first part deals with setting up a spectroscopic technique for reliable and accurate measurements of the two-photon absorption (2PA) cross section spectra. In the second part, this firmly established experimental technique together with conventional spectroscopic characterization, quantum-chemical computations and theoretical modelling calculations was combined and therefore used as a tool to gain information for the so-called structure-property relationship through several molecular compounds.}, subject = {Nonlinear Optical Properties of Organic Materials}, language = {en} } @phdthesis{Selby2022, author = {Selby, Joshua}, title = {Design and Chiroptical Properties of Chirally Substituted Indolenine Squaraine Mono-, Oligo-, and Polymers}, doi = {10.25972/OPUS-28206}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-282067}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2022}, abstract = {A series of monomeric chirally substituted indolenine squaraine monomers were successfully synthesized and utilized for the construction of various oligo- and polymers, in order to study their chiroptical properties in terms of exciton chirality. The quaternary carbon atom at the 3-position of the indolenine subunit, as well as the alkyl side chain attached to the indolenine nitrogen were selected as the most suitable site for chiral functionalization. For the C(3)-chiral derivatives, two synthetic routes depending on the desired substitution at the stereogenic center were established. The chiral side chains were prepared via Evans asymmetric alkylation where the resulting branching point at the 2 position constituted the chiral center. While the chiral substitution only had minor effects on the linear optical properties and geometric structure of the chromophore, all compounds exhibited a distinct and measurable CD signal that correlated with the distance of the chiral center to the central chromophore. Polymers bearing chiral side chains exhibited a solvent- and temperature-dependent helix-coil equilibrium, which was influenced by the type of side chain used. CD spectroscopy revealed the helical conformation to possess a preferred twist sense, and temperature-dependent measurements showed the degree of homohelicity to be nearly complete in certain cases. Furthermore, a CPL signal was able to be obtained for the helical conformer of one polymer. Various (co)oligo- and polymers comprising the C(3)-chiral monomers only displayed a solvent-independent J-type absorption behavior and thus did not form helical conformations in solution. CD spectroscopy revealed a solvent-dependent adoption of quasi-enantiomeric conformers, which was elucidated by quantum chemical TDDFT calculations.}, subject = {Squaraine}, language = {en} } @phdthesis{Mims2023, author = {Mims, David}, title = {Einblicke in die Spinchemie durch Untersuchung des Magnetfeldeffektes in rigide gebundenen Radikalionenpaaren}, doi = {10.25972/OPUS-30354}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-303547}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2023}, abstract = {Synthese starrer Donor-Akzeptor-Verbindungen und Untersuchung des Magnetfeldeffektes auf Lebenszeit resultierender Biradikale mittels optischer Spektroskopie.}, subject = {Magnetfeldeffekt}, language = {de} } @phdthesis{Roos2021, author = {Roos, Markus}, title = {Synthesis, Photophysics and Photocatalysis of [FeFe] Complex Containing Dyads and Bimolecular Systems}, doi = {10.25972/OPUS-23453}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-234537}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2021}, abstract = {In the course of this work, a total of three photocatalytically active dyads for proton reduction could be synthesized together with the associated individual components. Two of them, D1 and D2, comprised a [Ru(bpy)3]2+ photosensitizer and D3 an [Ir(ppy)2bpy]+ photosensitizer. A Ppyr3-substituted propyldithiolate [FeFe] complex was used as catalyst in all systems. The absorption spectroscopic and electrochemical investigations showed that an inner-dyadic electronic coupling is effectively prevented in the dyads due to conjugation blockers within the bridging units used. The photocatalytic investigations exhibited that all dyad containing two-component systems (2CS) showed a significantly worse performance than the corresponding bimolecular three-component systems (3CS). Transient absorption spectroscopy showed that the 2CS behave very similarly to the associated multicomponent systems during photocatalysis. The electron that was intended for the intramolecular transfer from the photosensitizer unit to the catalyst unit within the dyads remains at the photosensitizer for a relatively long time, analogous to the 3CS and despite the covalently bound catalyst. It is therefore assumed that this intramolecular electron transfer is likely to be hindered as a result of the weak electronic coupling caused by the bridge units used. Instead, the system bypasses this through an intermolecular transfer to other dyad molecules in the immediate vicinity. In addition, with the help of emission quenching experiments and electrochemical investigations, it could be clearly concluded that all investigated systems proceed via the reductive quenching mechanism during photocatalysis.}, subject = {Fotokatalyse}, language = {en} } @phdthesis{Luettig2023, author = {L{\"u}ttig, Julian Konstantin}, title = {Coherent Higher-Order Spectroscopy: Investigating Multi-Exciton Interaction}, doi = {10.25972/OPUS-29318}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-293182}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2023}, abstract = {The goal of this thesis was the development and application of higher-order spectroscopic techniques. In contrast to ordinary pump-probe (PP) and two-dimensional (2D) spectroscopy, higher-order coherently detected spectroscopic methods measure a polarization that has an order of nonlinearity higher than three. The key idea of the techniques in this thesis is to isolate the higher-order signals from the lower-order signals either by their excitation frequency or by their excitation intensity dependence. Due to the increased number of interactions in higher-order spectroscopy, highly excited states can be probed. For excitonic systems such as aggregates and polymers, the fifth-order signal allows one to directly measure exciton-exciton annihilation (EEA). In polymers and aggregates, the exciton transport is not connected to a change of the absorption and can therefore not be investigated with conventional third-order techniques. In contrast, EEA can be used as a probe to study exciton diffusion in these isonergetic systems. As a part of this thesis, anisotropy in fifth-order 2D spectroscopy was investigated and was used to study geometric properties in polymers. In 2D spectroscopy, the multi-quantum signals are separated from each other by their spectral position along the excitation axis. This concept can be extended systematically to higher signals. Another approach to isolate multi-quantum signals in PP spectroscopy utilizes the excitation intensity. The PP signal is measured at specific excitation intensities and linear combinations of these measurements result in different signal contributions. However, these signals do not correspond to clean nonlinear signals because the higher-order signals contaminate the lower-order multi-quantum signals. In this thesis, a correction protocol was derived that uses the isolated multiquantum signals, both from 2D spectroscopy and from PP spectroscopy, to remove the contamination of higher-order signals resulting in clean nonlinear signals. Using the correction on the third-order signal allows one to obtain annihilation-free signals at high excitation intensities, i.e., with high signal-to-noise ratio. Isolation and correction in PP and 2D spectroscopy were directly compared by measuring the clean third-order signals of squaraine oligomers at high excitation intensities. Furthermore, higher-order PP spectroscopy was used to isolate up to the 13th nonlinear order of squaraine polymers. The demonstrated spectroscopic techniques represent general procedures to isolate clean signals in terms of perturbation theory. The technique of higher-order PP spectroscopy needs only small modifications of ordinary PP setups which opens the field of higher-order spectroscopy to the broad scientific community. The technique to obtain clean nonlinear signals allows one to systematically increase the number of interacting (quasi)particles in a system and to characterize their interaction energies and dynamics.}, subject = {Coherent Multidimensional Spectroscopy}, language = {en} } @phdthesis{Roger2024, author = {Roger, Chantal}, title = {Photophysics and Spin Chemistry of Triptycene Bridge Donor-Acceptor-Triads}, doi = {10.25972/OPUS-36303}, url = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-363031}, school = {Universit{\"a}t W{\"u}rzburg}, year = {2024}, abstract = {The goal of this thesis was to investigate the influence of rotational restriction between individual parts and of the varying electron density in the bridging unit of D B A systems on the exchange interaction 2J, and thus the electronic coupling between a donor state and an acceptor state. A better understanding of how to influence the underlaying spin dynamics in such donor acceptor systems can open up the door to new technologies, such as modern molecular electronics or optoelectronic devices. Therefore, three series of molecules consisting of a TAA electron donor, a TTC or ATC bridging unit and a PDI electron acceptor were studied. To investigate the influence of rotational restriction on 2J and the electronic coupling, a series of four rotationally hindered triads (chapter 6) was synthesised. The dihedral angle between the TAA and the TTC as well as between the TTC and the PDI was restricted by ortho methyl groups at the phenylene linkers of the connecting ends to the TTC bridge, producing a twist around the linking single bond which minimises the π overlap. The triads exhibit varying numbers of ortho methyl groups and therefore different degrees of rotational restriction. In order to shine light on the influence of varying electron density on 2J and the electronic coupling, a series of four substituted triptycene triads (chapter 7) was synthesised. The electron density in the TTC bridging unit was varied by electron donating and electron withdrawing groups in 12,13 position of the TTC bridging unit and thus varying its HOMO/LUMO energy. The last series of two anthracene bridge triads (chapter 8) connected both approaches by restricting the rotation with ortho methyl groups and simultaneously by varying the bridge energies. In order to obtain the electronic properties, steady state absorption and emission spectra of all triads were investigated (chapter 4). Here, all triads show spectral features associated with the separate absorption bands of TAA and the PDI moiety. The reduced QYs, compared to the unsubstituted PDI acceptor, indicate a non radiative quenching mechanism in all triads. The CV data (chapter 5) were used to calculate the energies of possible CSSs and those results were used to assign the CR dynamics into the different Marcus regions. fs TA measurements reveal that all triads form a CSS upon excitation of the PDI moiety. The lifetimes of the involved states and the rate constants were determined by global exponential fits and global target analysis. The CR dynamics upon depopulation of the CSSs were investigated using external magnetic field dependent ns TA spectroscopy. The ns TA maps show that all triads recombine via CRT pathway populating the local 3PDI state in toluene and provided the respective lifetimes. The approximate QYs of triplet formation were determined using actinometry. The magnetic field dependent ns TA data reveal the exchange interaction 2J between singlet and triplet CSS for each triad. Those magnetic field dependent ns TA data in toluene were furthermore treated using a quantum mechanical simulation (done by U.E. Steiner) to extract the rate constants kT and kS for CRT and CRS, respectively. However, the error margins of kS were rather wide. Finally, the electronic couplings between the donor and the acceptor states were obtained by combining the aforementioned experimental results of the rate constants and applying the Bixon Jortner theoretical description of diabatic ET and Andersons perturbative theory of the exchange coupling. Therefore, the experimentally determined values of 2J and the calculated values of kCS and kT were used. The rate constant kS was calculated based on the electronic coupling V1CSS 1S0. The rotationally hindered triads (chapter 6) show a strong influence of the degree of rotational restriction on the lifetimes and rate constants of the CS processes. The rate constants of CS are increasing with increasing rotational freedom. The magnetic field dependent decay data show that the exchange interactions increase with increasing rotational freedom. Based on the CR dynamics, the calculated electronic couplings of the ET processes reflect the same trend along the series. Here, only singlet couplings turned out to be strongly influenced while the triplet couplings are not. Therefore, this series shows that the ET dynamics of donor acceptor systems can strongly be influenced by restricting the rotational freedom. In the substituted triptycene triads (chapter 7), decreasing electron density in the bridging unit causes a decrease of the CS rate constants. The magnetic field dependent decay data show that with decreasing electron density in the bridge the exchange interaction decreases. The CR dynamics-based rate constants and the electronic couplings follow the same trend as the exchange interaction. This series shows that varying the HOMO/LUMO levels of the connecting bridge between donor and acceptor strongly influences the ET processes. In the anthracene bridge triads (chapter 8), the CS process is slow in both triads. The CR was fast in the anthracene triad and is slowed down in the methoxy substituted anthracene bridge triad. The increase of the exchange interaction with increasing electron density in the bridge was more pronounced than in the substituted triptycene triads. Thus, the variation of electron density in the bridge strongly influences the ET processes even though the rotation is restricted. In this thesis, it was shown that the influence of the rotational hindrance as well as the electron density in a connecting bridge have strong influence on all ET processes and the electronic coupling in donor acceptor systems. These approaches can therefore be used to modify magnetic properties of new materials.}, subject = {Rotation}, language = {en} }