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The self-assembly of molecules based on π-π-interactions and hydrogen bonding is of significant importance in nature. These processes enable the formation of complex supramolecular structures with diverse functions. For the transfer of the concepts from nature to artificial supramolecular structures, a basic understanding of those processes is needed. For this purpose, π-conjugated aromatic molecules with an easy synthetic access are suitable as their functionalities can be changed effortless. Perylene bisimide (PBIs) dyes are attractive candidates since they fulfill these requirements owing to their tendency to self-assemble in solution due to their large aromatic π-surfaces. Furthermore, the changes of the optical properties (for instance absorption, emission or circular dichroism) of PBI dyes, caused by their self-assembly, are easy to study experimentally. Structural variations of PBI dyes including additional non-covalent interactions, such as hydro-gen bonding, enable to direct their self-assembly process. Thus, the formation of interesting su-pramolecular structures of PBI dyes could be realized, although, often of undefined size. The aim of this thesis was to develop strategies to restrict the aggregate size of PBI dyes. Therefore, de-fined structural features of PBI molecules were combined and a variation of external influences such as solvent and concentration included. Furthermore, DNA was utilized as a template for the limitation of the aggregate size of PBI dyes.
Chapters 1 and 2 provide general information and describe examples from literature which are necessary to understand the following experimental work. The first chapter is based on the inter-actions of various molecules with DNA. Therefore, DNA is considered as a supramolecular biom-acromolecule containing specific structural and functional features to interact with small mole-cules. Afterwards, the main interaction modes of small molecules with DNA such as electrostatic interaction, intercalation and groove binding with corresponding examples are discussed. Among all techniques applied to study the interaction of ligands with DNA, UV/Vis absorption, fluores-cence and circular dichroism spectroscopy were described in detail. At the end of this chapter, examples of already pre-associated systems showing interactions with DNA are presented.
The second chapter is focused on the determination and mathematic evaluation of the self-assembly processes. The simplest models such as monomer-dimer and isodesmic model are de-scribed and supplemented by examples. Furthermore, the simplest modification of the isodesmic model, the K2-K model, is presented. Additionally, experimental problems, which may arise dur-ing the investigations of the self-assembly processes, are addressed. For the description of the entire self-assembly process, a sufficiently large concentration range and an appropriate measure-ment method that is sensitive in this concentration range is necessary. Furthermore, the full transi-tion from the monomeric to the aggregated species has to be spectroscopically ascertainable. This enables an accurate mathematic evaluation of the self-assembly process and provides meaningful binding constants. The self-assembly pathway can be controlled by the variation of solvent, con-centration or temperature. However, this pathway can also be directed by a rational design of the molecular structure of the considered system. For example, a specific interplay of π-π-interactions and hydrogen bonding may promote isodesmic as well as cooperative growth into large struc-tures.
The main focus of this thesis is to develop strategies to control the aggregate size of PBI dyes (Chapter 3). For this purpose, a PBI scaffold was designed which contains hydrogen bonding amide functions at the imide positions derived from the amino acid L-alanine and solubilizing side groups in the periphery (Figure 81). The variations of the residues R/R’ range from didodecylox-yphenyl, didodecylphenyl, dioligo(ethylene glycol)phenyl to branched and linear alkyl chains.
The most extensive study of the aggregation behavior was performed for the PBI dye 5. Concen-tration-dependent 1H NMR and UV/Vis absorption measurements clearly revealed the formation of dimers in chloroform. Further investigations by means of 2D NMR, VPO and ITC confirmed the exclusive presence of dimer aggregates of PBI 5 in the investigated concentration range. Mo-lecular modelling studies, supported by NMR and FT-IR experiments, provided structural reasons for the absence of further growth into larger aggregates. The specific combination of π-π interac-tions and hydrogen bonds between the NH groups of the amide groups and the carbonyl oxygen atoms of the PBI core are decisive for the formation of the discrete dimer stack (see Figure 82). The investigations of the aggregation behavior of PBIs 6-9 were less extensive but consistent with the results obtained for PBI 5. However, the determined binding constants vary over a considera-ble range of 1.1 x 102 M-1 (PBI 8) to 1.4 x 104 M-1 (PBI 5). These differences could be attributed to structural variations of the dyes. The electron-rich phenyl substituent promoted the aggregation tendency of PBIs 5-7 compared with 8 and 9 that carry only alkyl side chains. Thus, the π-π in-teractions of bay-unsubstituted PBI cores in combination with hydrogen bonding of the amide functions control the formation of discrete dimers of these PBI dyes.
The variation of conditions, such as solvent, change the aggregation behavior of PBI dyes. In the solvents toluene and/or methylcyclohexane, anti-cooperative growth into larger aggregates of PBI 5 was observed (Chapter 4). The important feature of this self-assembly process is the absence of isosbestic points over the whole concentration range in the UV/Vis absorption measurements. The preference for the dimeric species of PBI 5 remained in both solvents as well as in mixtures of them, but upon increasing the concentration these dimers self-assemble into larger aggregates.
An important feature of the self-assembly process is the preferred formation of even-numbered aggregates compared to the odd-numbered ones (see Figure 83). Although, the conventional K2-K model provides plausible binding constants, it is not capable to describe the aggregation behavior adequately, since it considers a continuous size distribution. The gradual aggregation process over dimers, tetramers, hexamers, etc. was therefore analyzed with a newly developed K2-K model for anti-cooperative supramolecular polymerization. By the global analysis of the UV/Vis absorption spectra a very good agreement between the experimental and simulated spectra, which were based on the new K2-K model, was obtained. Furthermore, the calculated UV/Vis absorption spectra of a dimer and an aggregate highlighted the most important structural differences. The absorption spectrum of the dimer still has a pronounced vibronic structure which gets lost in the spectrum of the aggregate.
In another part of this work, a series of water soluble PBI dyes were described which contain similar PBI scaffolds as PBIs 5-8 (Chapter 5). These PBI dyes self-assemble into similar dimer aggregates in water due to their positively charged side chains causing electrostatic repulsion be-tween the molecules (see Figure 84). Here, however, the self-assembly behavior has not been studied thoroughly in water due to the similarities of already reported PBI dyes.
Instead, the focus here is on the characterization of the interactions of these dyes with DNA/RNA. The comprehensive studies using thermal denaturation experiments showed the high stability of these PBI/polynucleotide complexes. The spermine-functionalized PBI dyes having six positive charges showed strong interactions with DNA/RNA which was expressed in a signif-icant increase of the melting temperatures of DNA/RNA (ΔTm values between 7 and > 35 ° C). The dioxa analogues containing only two positive charges had lower enhancement of the melting temperature of DNA/RNA (ΔTm values between 3 and 30 ° C). A similar trend has been observed in the fluorimetric titrations. The spermine-functionalized PBI dyes showed high binding con-stants (log Ks = 9.2 - 9.8), independently of the used polynucleotides. In contrast, the dioxa ana-logues displayed smaller binding constants (log Ks = 6.5 - 7.9) without any correlation between binding affinity and binding strength of the PBI dyes and the applied polynucleotides. The CD-spectroscopic measurements revealed significant differences in the binding properties of the dyes with DNA/RNA. They were dependent on the steric hindrance of the amino acid residues at the imide position and their configuration on one side and the grooves properties of ds-DNA/RNA on the other side. The spectroscopic results confirmed the formation of excitonically coupled PBI dimers in the minor groove of ds-DNA and the major groove of ds-RNA. Depending on the se-quence, the grooves of the polynucleotides provide different amount of space for embedding molecules. The guanine amino groups protrude into the minor groove of the polynucleotide poly(dG-dC)2 increasing the steric hindrance, which is not the case for poly(dA-dT)2. Molecular modeling studies showed that the PBI dimers penetrate deeper into the groove of poly(dA-dT)2 due to the absence of the steric hindrance, in comparison to the groove of poly(dG-dC)2 (see Figure 85).
The presented work in the field of supramolecular chemistry describes the synthesis and detailed investigation of (bi)pyridine-based oligo(phenylene ethynylene) (OPE) amphiphiles, decorated with terminal glycol chains. The metal-ligating property of these molecules could be exploited to coordinate to Pd(II) and Pt(II) metal ions, respectively, resulting in the creation of novel metallosupramolecular π-amphiphiles of square-planar geometry.
The focus of the presented studies is on the self-assembly behaviour of the OPE ligands and their corresponding metal complexes in polar and aqueous environment. In this way, the underlying aggregation mechanism (isodesmic or cooperative) is revealed and the influence of various factors on the self-assembly process in supramolecular systems is elucidated. In this regard, the effect of the molecular design of the ligand, the coordination to a metal centre as well as the surrounding medium, the pH value and temperature is investigated.
Merocyanine Dyes as Organic Semiconductors for Vacuum-processed Solar Cell and Transistor Devices
(2015)
The present thesis comprises the synthesis of new functional merocyanine dyes, the study of their electro-optical properties as well as solid state packing and their application as p-type semiconductor materials in transistor and solar cell devices. The absorption properties of the obtained compounds could be modified by variation of the donor unit, the introduction of electron-withdrawing substituents in the acceptor unit or elongation of the polymethine chain. For a particular dye, the absorption band could be shifted by more than 160 nm by increasing the solvent polarity due to a conformational switch between a merocyanine-like and a cyanine-like structure. Single crystal analyses revealed that the studied dyes tend to pack either in an antiparallel fashion forming dimers with no overall dipole moment or in a staircase-like pattern where the dipole moments point to the same direction and are only balanced by another staircase oriented in the opposite direction (stair dimer). With respect to application as semiconductor materials, the latter packing arrangement resulted most favorable for charge carrier mobility. We concluded that this packing motif is preserved in the solar cell devices, where the selenium-containing dye afforded the highest performance of this series for an optimized planar-mixed heterojunction solar cell (6.2 %).
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.
Within this PhD thesis, chromophore-bridged biradicals were synthesised and their properties characterised. Therefore, it was necessary to develop novel synthetic procedures and implement several experimental characterisation methods. In summary, within this thesis the scope of pigment chromophore phenoxyl radical decoration was further explored and expanded to IIn as well as DPP colourants. HOMA analysis highlighted the importance of aromaticity in order to understand the spin crossover from heteroaromatic quinoidal to aromatic open shell DPPs. Finally, PBI, IIn and DPP biradicals were advanced towards stable materials by introduction of nitronyl nitroxide radical centres.
Analog zu den auf hochgeordneten Farbstoffarchitekturen in den biologischen Photosyntheseapparaten basierenden Energiekonversionssystemen sollte die exakte Einstellung zwischenmolekularer Wechselwirkungen auch in künstlichen Halbleitern eine entscheidende Rolle für die Weiterentwicklung organischer Elektronikmaterialien spielen. Für eine derartige, präzise Steuerung der nanoskaligen Anordnung in organischen Materialien erscheinen Merocyaninfarbstoffe wegen ihrer hochgerichteten, dipolaren Aggregation äußerst aussichtsreich. In diesem Zusammenhang war das Ziel der vorliegenden Arbeit die Ausnutzung funktionaler, stark selbstorganisierender Merocyanine, um eine gezielte Beeinflussung der Morphologie in der aktiven Schicht von BHJ-Solarzellen zu erreichen. Hierzu sollte zunächst eine umfangreiche Serie komplexer Merocyanine synthetisiert und vollständig charakterisiert werden. Im Folgenden wurde angestrebt, die optischen und elektrochemischen Eigenschaften der molekular gelösten Farbstoffe zu bestimmen und für ausgewählte, geeignete Strukturen das Selbstorganisationsverhalten im Detail zu studieren. Zuletzt sollte durch eine sorgfältige Optimierung der Prozessierungsbedingungen ein Transfer der in Lösung gefundenen, supramolekularen Strukturen in den Blend lösungsprozessierter BHJ-Solarzellen erreicht werden. Die organischen Elektronikbauteile wurden dabei im Arbeitskreis von Prof. Dr. Klaus Meerholz (Universität Köln) gefertigt und charakterisiert.
Zusammenfassend zeichnet die vorliegende Arbeit ein umfassendes Bild von der Synthese funktionaler Merocyanine, dem Studium ihrer molekularen und Selbstorganisationseigenschaften sowie ihrer Anwendung als p-Halbleitermaterialien in organischen Solarzellen. Der komplexe Molekülaufbau der dargestellten Farbstoffe führte dabei zur Ausbildung verschiedener Farbstofforganisate, deren Struktur sowohl in Lösung als auch teilweise im Festkörper aufgeklärt werden konnte. Die erfolgreiche Implementierung von H-aggregierten Spezies der Verbindung 67b in die aktive Schicht organischer BHJ-Solarzellen resultierte in der Bildung effizienter Perkolationspfade für Exzitonen und freie Ladungsträger, wodurch diese Bauteile merklich höhere Stromdichten generieren konnten und gegenüber Zellen ohne H-Spezies über 20 % gesteigerte Effizienz aufwiesen. Diese Befunde verifizieren die postulierte Hypothese, dass eine gezielte Einstellung der zwischenmolekularen Wechselwirkungen bei organischen Halbleitern zu einer Optimierung der Funktionalität organischer Elektronikmaterialien beitragen kann.
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.
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. (...)
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.