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Um den jahrtausendealten Weg der Menschheit vom Papyrus über Buchdruck und siliziumbasierte Halbleiter in Richtung noch leistungsfähigerer Technologien zu gehen und weiterhin Heureka-Momente zu schaffen, bieten Kohlenstoffnanoröhren ein weites Forschungsfeld. Besonders die halbleitenden Charakteristika von SWNTs sowie die Manipulation dieser durch Dotierung bergen viele Möglichkeiten für zukünftige Anwendungen in moderner Elektrotechnologie. Der Weg zu einer industriellen Implementierung von SWNTs in neuartigen optoelektronischen Bauteilen ließe sich durch eine Ausweitung des Wissens bezüglich SWNTs und der dotierungsbasierten Anpassung ihrer Eigenschaften ebnen.
Mit dieser Erkenntniserweiterung als Zielsetzung wurden im Rahmen dieser Dissertation halbleitende, einwandige (6,5)-Kohlenstoffnanoröhren als chiralitätsreine, polymerstabilisierte Proben untersucht. Die ultrakurzzeitaufgelöste Spektroskopie der SWNTs erfolgte an organischen Suspensionen wie auch Dünnschichtfilmen, die je mittels eines gewissen Quantums an Gold(III)-chlorid dotiert worden waren. So konnten die ablaufenden Dynamiken auf einer ps-Zeitskala untersucht werden.
In Kapitel 4 konnte mittels transienter Absorptionsexperimente an redoxchemisch p-dotierter SWNT-Suspensionen zunächst gezeigt werden, dass sich die bei optischer Anregung gebildeten Trionen nicht analog zu Exzitonen diffusiv entlang der Nanoröhre bewegen, sondern lokalisiert vorliegen. Die längere trionischen Zerfallsdauer nach X$_1$- verglichen mit X$_1^+$-resonanter Anregung zeugt außerdem davon, dass das Trion aus dem Exziton gespeist wird. Der Einfluss der Dotierung auf die Zerfallsdynamiken von X$_1$ und X$_1^+$ wurde an SWNT-Dünnschichtfilmen untersucht. Das Photobleichsignal des Exzitons verschiebt hypsochrom und zerfällt schneller mit zunehmender Ladungsträgerdichte durch höherer Gold(III)-chloridkonzentrationen. Dies resultiert aus dem verringerten Abstand zwischen den Ladungsträgern, welche als nichtstrahlende Löschstellen fungieren. Für das X$_1^+$-PB ist ein ähnliches Verhalten zu beobachten. Dabei wird dieses Signal mit weiter steigender Dotierung von einer der H-Bande zuzuordnenden Photoabsorption überlagert. Diese lässt sich in einer starken Sättigung der Dotierung wie auch einer hohen Bandkantenverschiebung begründen.
In Kapitel 5 wurde die Größe der Exzitonen und Trionen in dotierten SWNT-Dünnschichtfilmen mittels des Phasenraumfüllmodells bestimmt. Dabei lag besonderes Augenmerk auf der Kompensation des PB/PA-Überlapps, dem schnellen Zerfall, einem Ausgleich von Differenzen zwischen Anrege- und Absorptionsspektrum sowie dem Anteil intrinsischer/dotierter Nanorohrsegmente, um korrigierte Größen $\xi_\mathrm{k}$ zu erhalten. Für die Trionengröße wurde zusätzlich der Überlapp der Absorptionsbanden einbezogen, um korrigierte Werte $\xi_{\mathrm{T,k}}$ zu bestimmen. $\xi_\mathrm{k}$ beträgt in der intrinsischen Form 6$\pm$2\,nm und bleibt bis zu einer Ladungsträgerdichte $n_{\mathrm{LT}}<0.10$\,nm$^{-1}$ etwa gleich, anschließend ist ein Absinken bis auf etwa 4\,nm bei $n_{\mathrm{LT}}\approx0.20$\,nm$^{-1}$ zu beobachten. Für diesen Trend ist die Überlagerung von Exziton- und H-Bande verantwortlich, da so der Faktor zur Bestimmung des Anteils intrinsischer Nanorohrsegmente an der SWNT verfälscht wird. Die Abweichung der intrinsischen Größe von den in der Literatur berichteten 13$\pm$3\,nm ist möglicherweise auf Unterschiede in der Probenpräparation zurückzuführen. Für die Trionengröße ergibt sich bei steigender Dotierung ein ähnliches Verhalten: Sie beträgt für $n_{\mathrm{LT}}<0.20$\,nm$^{-1}$ 1.83$\pm$0.47\,nm, was in der Größenordnung in guter Übereinstimmung mit der Literatur ist. Für höhere Dotierungen sinkt $\xi_{\mathrm{T,k}}$ bis auf 0.92$\pm$0.26nm ab. Dies erklärt sich dadurch, dass bei höherer $n_{\mathrm{LT}}$ die H-Bande das Spektrum dominiert, sodass der Einfluss der Absorptionsbandenüberlagerung nicht mehr vollständig durch den entsprechenden Korrekturfaktor kompensiert werden kann.
Kapitel 6 beschäftigte sich anstelle redoxchemischer Dotierung der nanoskaligen Halbleiter mit der (spektro-)elektrochemischen Untersuchung von Vorläufern molekularer Radikale. SWV-Messungen weisen dabei darauf hin, dass die Pyrene Pyr1-Pyr3 entsprechend der Anzahl ihrer Substituenten bei Reduktion Mono-, Bi- beziehungsweise Tetraradikale bilden. Die strukturelle Ähnlichkeit der Moleküle äußert sich in gleichen Reduktionspotentialen wie auch ähnlichen potentialabhängigen Absorptionsspektren. Während nur marginale Unterschiede in den PL-Spektren der neutralen und reduzierten Spezies festgestellt werden konnte, lieferte das zeitkorrelierte Einzelphotonenzählen aufschlussreichere Ergebnisse: So wird die Fluoreszenzlebensdauer stark von der Polarität der Umgegbung beeinflusst - bereits die Zugabe des Leitsalzes führt hier zu Änderungen. Die durchschnittliche Fluoreszenzlebensdauer $\tau_{\mathrm{av}}$ sinkt außerdem mit Reduktion und Radikalbildung; für höhere Emissionswellenlängen ist $\tau_{\mathrm{av}}$ außerdem höher. Insgesamt verdeutlichten die Experimente die gute Abschirmung zwischen Pyrenkern und Naphthalimidsubstituenten der Moleküle sowie die Sensibilität gegenüber dem Medium durch TICT, das Vorhandensein von Bi- und Tetraradikalen kann allerdings nicht vollständig belegt werden, wofür EPR-Messugen notwendig wären.
This work is concerned with the syntheses and photophysical properties of para-xylylene bridged macrocycles nPBI with ring sizes from two to nine PBI units, as well as the complexation of polycyclic aromatic guest compounds.
With a reduced but substantial fluorescence quantum yield of 21% (in CHCl3) the free host 2PBI(4-tBu)4 can be used as a dual fluorescence probe. Upon encapsulation of rather electron-poor guests the fluorescence quenching interactions between the chromophores are prevented, leading to a significant fluorescence enhancement to > 90% (“turn-on”). On the other hand, the addition of electron-rich guest molecules induces an electron transfer from the guest to the electron-poor PBI chromophores and thus quenches the fluorescence entirely (“turn-off”). The photophysical properties of the host-guest complexes were studied by transient absorption spectroscopy. These measurements revealed that the charge transfer between guest and 2PBI(4-tBu)4 occurs in the “normal region” of the Marcus-parabola with the fastest charge separation rate for perylene. In contrast, the charge recombination back to the PBI ground state lies far in the “inverted region” of the Marcus-parabola.
Beside complexation of planar aromatic hydrocarbons into the cavity of the cyclophanes an encapsulation of fullerene into the cyclic trimer 3PBI(4-tBu)4 was observed. 3PBI(4-tBu)4 provides a tube-like structure in which the PBI subunits represent the walls of those tubes. The cavity has the optimal size for hosting fullerenes, with C70 fitting better than C60 and a binding constant that is higher by a factor of 10. TA spectroscopy in toluene that was performed on the C60@3PBI(4-tBu)4 complex revealed two energy transfer processes. The first one comes from the excited PBI to the fullerene, which subsequently populates the triplet state. From the fullerene triplet state a second energy transfer occurs back to the PBI to generate the PBI triplet state.
In all cycles that were studied by TA spectroscopy, symmetry-breaking charge separation (SB-CS) was observed in dichloromethane. This process is fastest within the PBI cyclophane 2PBI(4-tBu)4 and slows down for larger cycles, suggesting that the charge separation takes place through space and not through bonds. The charges then recombine to the PBI triplet state via a radical pair intersystem crossing (RP-ISC) mechanism, which could be used to generate singlet oxygen in yields of ~20%.
By changing the solvent to toluene an intramolecular folding of the even-numbered larger cycles was observed that quenches the fluorescence and increases the 0-1 transition band in the absorption spectra. Force field calculations of 4PBI(4-tBu)4 suggested a folding into pairs of dimers, which explains the remarkable odd-even effect with respect to the number of connected PBI chromophores and the resulting alternation in the absorption and fluorescence properties. Thus, the even-numbered macrocycles can fold in a way that all chromophores are in a paired arrangement, while the odd-numbered cycles have open conformations (3PBI(4-tBu)4, 5PBI(4-tBu)4, 7PBI(4-tBu)4) or at least additional unpaired PBI unit (9PBI(4-tBu)4).
With these experiments we could for the first time give insights in the interactions between cyclic PBI hosts and aromatic guest molecules. Associated with the encapsulation of guest molecules a variety of possible applications can be envisioned, like fluorescence sensing, chiral recognition and photodynamic therapy by singlet oxygen generation. Particularly, these macrocycles provide photophysical relaxation pathways of PBIs, like charge separation and recombination and triplet state formation that are hardly feasible in monomeric PBI dyes. Furthermore, diverse compound specific features were found, like the odd-even effect in the folding process or the transition of superficial nanostructures of the tetrameric cycle influenced by the AFM tip. The comprehensive properties of these macrocycles provide the basis for further oncoming studies and can serve as an inspiration for the synthesis of new macrocyclic compounds.
In terms of the need of environmentally benign renewable and storable energy sources, splitting of water into hydrogen and oxygen by using sunlight is a promising approach. Hereby, water oxidation catalysts (WOCs) are required to perform the water oxidation comprising the transfer of four electrons to provide the reducing equivalents for producing hydrogen. The class of Ru(bda) (bda = 2,2'-bipyridine-6,6'-dicarboxylate) catalysts has proven to be efficient for this reaction.
In this thesis, ligand exchange processes in Ru(bda) complexes have been analyzed and the formation of multinuclear macrocyclic WOCs was studied. Based on the knowledge acquired by these studies, new multinuclear cyclic Ru(bda) complexes have been synthesized and their catalytic efficiencies in homogeneous water oxidation have been investigated. Going one step further for setting up functional devices, molecular WOCs have been immobilized on conducting or semiconducting supporting materials. Direct anchoring on carbon nanotubes generated a promising materials for further applications.
The chirality of the interlocked bay-arylated perylene motif is investigated upon its material prospect and the enhancement of its chiroptical response to the NIR spectral region. A considerable molecular library of inherently chiral perylene bisimides (PBIs) was utilized as acceptors in organic solar cells to provide decent device performances and insights into the structure-property relationship of PBI materials within a polymer blend. For the first time in the family of core-twisted PBIs, the effects of enantiopurity on the device performance was thoroughly investigated. The extraordinary structural sensitivity of CD spectroscopy served as crucial analytical tool to bridge the highly challenging gap between molecular properties and device analytics by proving the excitonic chirality of a helical PBI dimer. The chirality of this perylene motif could be further enhanced on a molecular level by both the expansion and the enhanced twisting of the π-scaffold to achieve a desirable strong chiroptical NIR response introducing a new family of twisted QBI-based nanoribbons. These achievements could be substantially further developed by expanding this molecular concept to a supramolecular level. The geometrically demanding supramolecular arrangement necessary for the efficient excitonic coupling was carefully encoded into the molecular design. Accordingly, the QBIs could form the first J-type aggregate constituting a fourfold-stranded superhelix of a rylene bisimide with strong excitonic chirality. Therefore, this thesis has highlighted the mutual corroboration of experimental and theoretical data from the molecular to the supramolecular level. It has demonstrated that for rylene bisimide dyes, the excitonic contribution to the overall chiroptical response can be designed and rationalized. This can help to pave the way for new organic functional materials to be used for
chiral sensing or chiral organic light-emitting devices.
Dipolar merocyanines are very attractive supramolecular building blocks, as they combine interesting functional properties with strong, directional intermolecular interactions. The pyridine dioxocyano-pyridine (PYOP) chromophore (Chapter 2.2), used in this thesis, stands out because of its exceptionally high ground state dipole moment (g ~ 17 D), in combination with the option to retain good solubility also in unpolar solvents, by decoration with solubilizing groups.
The reliable binding motif of anti-parallel -stacking due to dipole-dipole interactions has allowed the design of molecular building blocks that form assemblies of predictable geometry. The intense unstructured charge transfer UV/Vis absorption band (eg ~ 10.7 D) is a result of the dominant contribution of the zwitterionic resonance structure which brings the PYOP chromophore just beyond the cyanine limit in solvents of low polarity (c2 = 0.60, 1,4 dioxane). The high sensitivity of the S0 – S1 UV/Vis absorption band to the environment manifests itself in a pronounced negative solvatochromism and strong H-type exciton coupling within -stacked PYOP assemblies. In accordance with the classical molecular exciton theory, an increasing hypsochromic shift of the dominant absorption band of these H aggregates can be observed as the stack size increases up to about six chromophores, where it levels out at about max ~ 440 nm (CHCl3). This allows a uniquely simple estimation of the number of interacting chromophores within the self-assembled structure from a single UV/Vis absorption spectrum of an aggregate.
The defined and well investigated PYOP dimer formation was employed in this thesis to probe the applicability and limitations of concentration-, temperature-, and solvent-dependent self-assembly studies (Chapter 3). Straightforward theoretical models to evaluate datasets of concentration-, temperature-, and solvent-dependent UV/Vis absorption by nonlinear regression analysis were derived for the case of dimer formation (Chapter 2.1). Although the dimer model is well known and widely applied in literature, this detailed derivation is helpful to understand assumptions and potential problems of the different approaches for the determination of thermodynamic parameters. This helps to decide on the most appropriate method to analyse a system of interest. In this regard it should be noted that covering a large portion of the self-assembly process with the experimental data is a prerequisite for the accuracy of the analysis. Additionally, many of the insights can also be transferred to other self-assembly systems like supramolecular polymerization or host-guest interactions.
The concentration-dependent analysis is the most straightforward method to investigate self-assembly equilibria. No additional assumptions, besides mass balance and mass action law, are required. Since it includes the least number of parameters (only K, if M/D are known), it is the most, or even only, reliable method, to elucidate the self-assembly mechanism of an unknown system by model comparison. To cover a large concentration range, however, the compound must be soluble enough and generally sample amounts at least in the low mg scale must be available.
The temperature-dependent analysis has the advantage that all thermodynamic parameters G0, H0 and S0 can be obtained from a single sample in one automated measurement. However, the accessible temperature-range is experimentally often quite limited and dependent on the solvent. For systems which do not show the transition from monomer to aggregate in a narrow temperature range, as given for, e.g., cooperative aggregation or processes with a high entropy contribution, often not the entire self-assembly process can be monitored. Furthermore, the assumptions of temperature-independent extinction coefficients of the individual species as well as temperature-independent H0 and S0 must be met. Monte Carlo simulations of data sets demonstrated that even minor changes in experimental data can significantly impact the optimized values for H0 and S0. This is due to the redundancy of these two parameters within the model framework and even small thermochromic effects can significantly influence the results. The G0 value, calculated from H0 and S0, is, however, still rather reliable.
Solvent-dependent studies can often cover the entire self-assembly process from monomeric (agg = 0) to the fully aggregated state (agg = 1). However, for dyes with strong solvatochromic effects, such as the dipolar merocyanines investigated in this thesis, the results are affected. Also, the assumption of a linear relation of the binding energy G0 and the fraction of denaturating solvent f, which is based on linear free energy relationships between G0 and the solvent polarity, can lead to errors. Especially when specific solvent effects are involved.
For the evaluation of experimental data by nonlinear regression, general data analysis software can be used, where user-defined fit models and known parameters can be implemented as desired. Alternatively, multiple specialized programs for analysing self-assembly data are available online. While the latter programs are usually more user-friendly, they have the disadvantage of being a “black box” where only pre-implemented models can be used without the option for the user to adapt models or parameters for a specific system.
In Chapter 3 comprehensive UV/Vis absorption datasets are presented for the dimerization of merocyanine derivative 1 in 1,4-dioxane, which allowed for the first time a direct comparison of the results derived from concentration-, temperature-, and solvent-dependent self-assembly studies.
The results for the binding constant K and corresponding G0 from the concentration- and temperature-dependent analysis were in very good agreement, also in comparison to the results from ITC. For the temperature-dependent analysis, though, multiple datasets of samples with different concentration had to be evaluated simultaneously to cover a meaningful part of the self-assembly process. Furthermore, a significant dependence of the optimized parameters H0 and S0 on the wavelength chosen for the analysis was observed. This can be rationalized by the small thermochromic shifts of both the monomer and the dimer UV/Vis absorption band. The results from the solvent-dependent evaluation showed the largest deviation, as expected for the highly solvatochromic merocyanine dye.
However, even here by evaluation at 491 and 549 nm the deviation for G0 was only 2.5 kJ mol1 (9%) with respect to the results from the concentration-dependent analysis (G0 = 29.1 kJ mol1). Thus, despite the strong solvatochromism of the dipolar chromophore, it can still be considered a reliable method for estimating the binding strength. Furthermore, multiple repetitions of the concentration-, temperature-, and solvent-dependent studies provided insight into the reproducibility of the results and possible sources of experimental errors. In all cases, the deviations of the results were small (G0 < 0.4 kJ mol1) and within the same range as the fit error from the nonlinear regression analysis.
The insights from these studies were an important basis for the in-depth investigation of a more complex supramolecular system in Chapter 4, as a single method is often not enough to capture the full picture of a more complicated self-assembly process. To elucidate the anti-cooperative self-assembly of the chiral merocyanine 2, a combination of multiple techniques had to be applied.
Solvent-dependent UV/Vis absorption studies in CH2Cl2/MCH mixtures showed the step-wise assembly of the merocyanine monomer (max(M) = 549 nm, CH2Cl2) to first a dimer (max(D) = 498 nm, CH2Cl2/MCH 15:85) by dipole-dipole interactions, and then a -stacked higher aggregate (max(H) = 477 nm, MCH), with pronounced H-type coupling.
The thermodynamic evaluation of this data, however, suffered from the severe solvatochromism, especially of the monomeric species (max(M, CH2Cl2) = 549 nm, max(M, MCH) = 596 nm). Therefore, concentration-dependent studies were performed at three different temperatures (298, 323, 353 K) to elucidate the self-assembly mechanism and determine reliable thermodynamic parameters. The studies at elevated temperatures were hereby necessary, to obtain experimental data over a larger agg--range. Due to the pronounced difference in the thermodynamic driving force for dimerization and higher aggregate formation (KD/K5 = 6500) a concentration range exists in MCH where almost exclusively the dimer species of 2 is present, before further self-assembly by dispersion interactions occurs. Therefore, the data could be evaluated independently for the two self-assembly steps. The self-assembly of dimers into the higher aggregate could not be described by the isodesmic model but was fitted satisfactorily to a pentamer model. This rather small size of about ten -stacked PYOP chromophores was, furthermore, consistently indicated by AFM, VPO and DOSY NMR measurements. Based on 1D and 2D NMR data as well as the strong bisignate CD signal of the higher aggregate in combination with TD-DFT calculations, a P-helical stack is proposed as its structure. The small size can be rationalized by the anti-cooperative self-assembly mechanism and the sterical demand of the solubilizing trialkoxyphenyl and the chiral tetralin substituents. Additionally, the aliphatic shell formed by the solubilizing chains around the polar chromophore stack, can account for the exceptionally high solubility of 2 in MCH (> 15 mg mL1). These combined studies of the self-assembly process enabled the identification of suitable conditions for the investigation of fluorescence properties of the individual aggregate species. Aggregation-induced emission enhancement was observed for the almost non-emissive monomer (Fl(M) = 0.23%), which can be rationalized by the increasing rigidification within the dimer (Fl(D) = 2.3%) and the higher aggregate (Fl(H) = 4.5%). The helical chirality of the PYOP decamer stack, furthermore, gave rise to a strong CPL signal with a large glum value of 0.011.
The important conclusion of this thesis is that the temperature- and solvent-dependent analyses are valid alternatives to the classical concentration-dependent analysis to determine thermodynamic parameters of self-assembly equilibria. Although, for a specific supramolecular system, one approach might be favourable over the others for a variety of reasons. The experimental limitations often demand a combination of techniques to fully elucidate a self-assembly process and to gain insights in the aggregate structure. The anti-cooperative merocyanine self-assembly, which was described here for the first time for the PYOP merocyanine 2, is no exception. Besides the interest in the merocyanine assemblies from a structural and functional point of view, the insights gained from the presented studies can also be transferred to other self-assembly systems and be a guide to find the most appropriate analysis technique.
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.
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 Völker 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 Völker 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.
Der erste Teil dieser Arbeit beschäftigte sich mit dem Ziel, amphiphile Oligoethylenglykol-funktionalisierte Perylenmonoimiddiester und Dicarbonsäure- bzw. Amino-funktionalisierte Perylenbisimide zu synthetisieren. Weiterhin wurden die optischen Eigenschaften in Lösung und das Aggregationsverhalten der Ester-, Dicarbonsäure- und der Amino-funktionalisierten Perylenfarbstoffe untersucht. (...)
Der zweite Teil dieser Arbeit widmete sich dem Ziel, die amphiphilen Oligoethylenglykol-funktionalisierten Zinkchlorine, 31-Hydroxy-Zinkchlorin (ZnChl-OH) und 31-Methoxy-Zinkchlorin (ZnChl-OCH3), herzustellen und desweiteren deren Aggregationsverhalten in wässriger Lösung vergleichend zu studieren, um den Einfluss der Lösungsmittel und des Substituenten in 31-Position auf die thermodynamischen und kinetischen Eigenschaften und auf die Aggregatstruktur zu bestimmen. (...)
The aim of the first part of this thesis was to investigate (R,R)-PBI as a model system for polymorphism at its origin by a supramolecular approach. The pathway complexity of (R,R)-PBI was fine-tuned by experimental parameters such as solvent, temperature and concentration to make several supramolecular polymorphs accessible. Mechanistic and quantum chemical studies on the kinetics and thermodynamics of the supramolecular polymerization of (R,R)-PBI were conducted to shed light on the initial stages of polymorphism. The second part of this work deals with mechanistic investigations on the supramolecular polymerization of the racemic mixture of (R,R)- and (S,S)-PBI with regard to homochiral and heterochiral aggregation leading to conglomerates and a racemic supramolecular polymer, respectively.
Supramolecular Block Copolymers by Seeded Living Supramolecular Polymerization of Perylene Bisimides
(2019)
The research on supramolecular polymerization has undergone a rapid development in the last two decades, particularly since supramolecular polymers exhibit a broad variety of functionalities and applications in organic electronics, biological science or as functional materials (Chapter 2.1). Although former studies have focused on investigation of the thermodynamics of supramolecular polymerization (Chapter 2.2), the academic interest in the recent years shifted towards gaining insight into kinetically controlled self-assembly and pathway complexity to generate novel out-of-equilibrium architectures with interesting nanostructures and features (Chapter 2.3). Along this path, the concepts of seeded and living supramolecular polymerization were recently developed to enable the formation of supramolecular polymers with controlled length and low polydispersity under precise kinetic control (Chapter 2.4). Besides that, novel strategies were developed to achieve supramolecular copolymerization resulting in complex multicomponent nanostructures with different structural motives. The classification of these supramolecular copolymers on the basis of literature examples and an overview of previously reported principles to create such supramolecular architectures are provided in Chapter 2.5.
The aim of the thesis was the non-covalent synthesis of highly desirable supramolecular block copolymers by the approach of living seeded supramolecular polymerization and to study the impact of the molecular shape of the monomeric building blocks on the supramolecular copolymerization. Based on the structure of the previously investigated PBI organogelator H-PBI a series of novel PBIs, bearing identical hydrogen-bonding amide side-groups in imide-position and various kind or number of substituents in bay-position, was synthesized and analyzed within this thesis. The new PBIs were successfully obtained in three steps starting from the respective bromo-substituted perylene-3,4:9,10-tetracarboxylic acid tetrabutylesters or from the N,N’-dicyclohexyl-1,7-dibromoperylene-3,4:9,10-tetracarboxylic acid bisimide. All target compounds were obtained in the final step by imidization reactions of the respective perylene tetracarboxylic acid bisanhydride precursors with N-(2-aminoethyl)-3,4,5-tris(dodecyloxy)-benzamide and were fully characterized by 1H and 13C NMR spectroscopy as well as high resolution mass spectrometry.
The variation of bay-substituents strongly changes the optical properties of the monomeric PBIs which were investigated by UV/vis and fluorescence spectroscopy. The increase of the number of the methoxy-substituents provokes, for example, a red-shift of the absorption maxima concomitant with a decrease of extinction coefficients and leads to a drastic increase of the fluorescence quantum yields. Furthermore, the molecular geometry of the PBIs is also affected by variations of the bay-substituents. Thus, increasing the steric demand of the bay-substituents leads to an enlargement of the twist angles of the PBI cores as revealed by DFT calculations.
Especially the 1,7-dimethoxy bay-substituted MeO-PBI proved to be very well-suited for the studies envisioned within this thesis. The self-assembly of this PBI derivative was analyzed in detail by UV/vis, fluorescence and FT-IR spectroscopy as well as atomic force microscopy (Chapter 3). These studies revealed that MeO-PBI forms in a solvent mixture of methylcyclohexane and toluene (2:1, v/v) kinetically trapped off-pathway H-aggregated nanoparticles upon fast cooling of a monomeric solution from 90 to 20 °C. However, upon slow cooling of the monomer solution fluorescent J-type nanofibers are formed by π π interactions and intermolecular hydrogen-bonding.
The kinetically metastable off-pathway H-aggregates can be transformed into the thermodynamically more favored J-type aggregates by addition of seeds, which are produced by ultrasonication of the polymeric nanofibers. Interestingly, the living character of this seed-induced supramolecular polymerization process was proven by a newly designed multicycle polymerization experimental protocol. This living polymerization experiment clearly proves, that the polymerization can only occur at the “active” ends of the polymeric seed and that almost no recombination or chain termination processes are present. Hence, the approach of living supramolecular polymerization enables the formation of supramolecular polymers with controlled length and narrow polydispersity.
In Chapter 4 the copolymerization of MeO-PBI with the structurally similar 1,7-dichloro (Cl-PBI) and 1,7-dimethylthio (MeS-PBI) bay-substituted PBIs is studied in detail. Both PBIs form analogous to MeO-PBI kinetically trapped off-pathway aggregates, which can be converted into the thermodynamically stable supramolecular polymers by seed-induced living supramolecular polymerization under precise kinetic control. However, the stability of the kinetically trapped aggregates of Cl-PBI and MeS-PBI is distinctly reduced compared to that of MeO-PBI, because the π-π-interactions of the kinetically metastable aggregates are hampered through the increased twisting of the PBI-cores of the former PBIs. UV/vis studies revealed that the two-component seeded copolymerization of the kinetically trapped state of MeO-PBI with seeds of Cl-PBI leads to the formation of unprecedented supramolecular block copolymers with A-B-A pattern by a living supramolecular polymerization process at the termini of the seeds. Remarkably, the resulting A-B-A block pattern of the obtained copolymers was clearly confirmed by atomic force microscopy studies as the respective blocks formed by the individual monomeric units could be distinguished by the pitches of the helical nanofibers.
Moreover, detailed UV/vis and AFM studies have shown that by inverted two-component seed-induced polymerization, e.g., upon addition of seeds of MeO-PBI to the kinetically trapped aggregates of Cl-PBI, triblock supramolecular copolymers with B-A-B pattern can be generated. The switching of the block pattern could only be achieved because of the perfectly matching conditions for the copolymerization process and the tailored molecular geometry of the individual building blocks of both PBIs. These studies have demonstrated for the first time, that the block pattern of a supramolecular copolymer can be modulated by the experimental protocol through the approach of living supramolecular polymerization. Furthermore, by UV/vis analysis of the living copolymerization of MeO-PBI and MeS-PBI similar results were obtained showing also the formation of both A-B-A and B-A-B type supramolecular block copolymers. Although for these two PBIs the individual blocks could not be identified by AFM because the helical nanofibers of both PBIs exhibit identical helical pitches, these studies revealed for the first time that the approach of seeded living polymerization is not limited to a special pair of monomeric building blocks.
In the last part of the thesis (Chapter 5) a systematic study on the two-component living copolymerization of PBIs with various sterical demanding bay-substituents is provided. Thus, a series of PBIs containing identical hydrogen-bonding amide groups in imide position but variable number (1-MeO-PBI, MeO-PBI, 1,6,7-MeO-PBI, 1,6,7,12-MeO-PBI) or size (EtO-PBI, iPrO-PBI) of alkoxy bay-substituents was investigated. The molecular geometry of the monomeric building blocks has a strong impact on the thermodynamically and even more pronounced on the kinetically controlled aggregation in solvent mixtures of MCH and Tol. While the mono- and dialkoxy-substituted PBIs form kinetically metastable species, the self-assembly of the tri- and tetramethoxy-substituted PBIs (1,6,7-MeO-PBI and 1,6,7,12-MeO-PBI) is completely thermodynamically controlled. The two 1,7-alkoxy substituted PBIs (EtO-PBI, iPrO-PBI) form very similar to MeO-PBI kinetically off-pathway H-aggregates and thermodynamically more favored J-type aggregates. However, the stability of the kinetically metastable state is drastically lower and the conversion into the thermodynamically favored state much faster than for MeO-PBI. In contrast, the monomethoxy-substituted PBI derivative (1-MeO-PBI) forms a kinetically trapped species by intramolecular hydrogen-bonding of the monomers, which can be transformed into the thermodynamically favored nanofibers by seeded polymerization.
Importantly, the two-component seeded copolymerization of the kinetically trapped MeO PBI with seeds of other PBIs of the present series was studied by UV/vis and AFM revealing that the formation of supramolecular block copolymers is only possible for appropriate combinations of PBI building blocks. Thus, the seeded polymerization of the trapped state of the moderately core-twisted MeO-PBI with the, according to DFT-calculations, structurally similar PBIs (EtO-PBI and iPrO-PBI) leads to the formation of A-B-A block copolymers, like in the seeded copolymerization of MeO-PBItrapped with seeds of Cl-PBI and MeS-PBI already described in Chapter 4. However, by addition of seeds of the almost planar PBIs (H-PBI and 1-MeO-PBI) or seeds of the strongly core-twisted PBIs (1,6,7-MeO-PBI and 1,6,7,12-MeO-PBI) to the kinetically trapped state of MeO-PBI no block copolymers can be obtained. The mismatching geometry of these molecular building blocks strongly hampers both the intermolecular hydrogen-bonding and the π-π-interactions between the two different PBIs and consequently prevents the copolymerization process.
Furthermore, the studies of the two-component seeded copolymerization of the kinetically trapped species of 1-MeO-PBI with seeds of the other PBIs also corroborated that a precise shape complementarity is crucial to generate supramolecular block copolymers. Thus, by addition of seeds of H-PBI to the kinetically trapped monomers of 1-MeO-PBI supramolecular block copolymers were generated. Both PBIs exhibit an almost planar PBI core according to DFT-calculations leading to strong non-covalent interactions between these PBIs. This perfectly matching geometry of both PBIs also enables the inverted seeded copolymerization of the kinetically trapped monomers of H-PBI with 1-MeO-PBIseed concomitant with a switching of the block pattern of the supramolecular copolymer from A-B-A to B-A-B type. In contrast, the seeding with the moderately twisted (MeO-PBI, EtO-PBI and iPrO-PBI) and the strongly twisted PBIs (1,6,7-MeO-PBI and 1,6,7,12 MeO-PBI) has no effect on the kinetically trapped state of 1-MeO-PBI, because the copolymerization of these PBIs is prevented by the mismatching geometry of the molecular building blocks.
In conclusion, the supramolecular polymerization and two-component seeded copolymerization of a series of PBI monomers was investigated within this thesis. The studies revealed that the thermodynamically and kinetically controlled self-assembly can be strongly modified by subtle changes of the monomeric building blocks. Moreover, the results have shown that living supramolecular polymerization is an exceedingly powerful method to generate unprecedented supramolecular polymeric nanostructures with controlled block pattern and length distribution. The formation of supramolecular block copolymers can only be achieved under precise kinetic control of the polymerization process and is strongly governed by the shape complementarity already imparted in the individual components. Thus, these insightful studies might enable a more rational design of monomeric building blocks for the non-covalent synthesis of highly complex supramolecular architectures with interesting properties for possible future applications, e.g., as novel functional materials.