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The thesis enhances the strategy of non-destructive fluorescence read-out in rylene bisimide-diarylethene containing photochromic systems. The fluorescence of the emitter unit is quenched by a photoinduced electron transfer only to one of the isomeric forms of the photochrome. The driving force of the fuorescence-quenching electron transfer was calculated by the help of the Rehm-Weller equation. The novel photochromic systems satisfy the necessary requirements for non-destructive read-out in write/read/erase fluorescent memory devices.
In this thesis the syntheses and detailed investigations on two foldable PBI systems were presented. The reversible, solvent-dependet folding/unfolding-behavior was used to study the ground and excited states properties of folda-dimer and folda-trimer by means of different spectroscopic methods as well as theoretical studies. The switching between charge transfer or excimer formation pathways of photoexcited molecules influenced by the spatial arrangement of chromophores within defined dye systems illustrates the impact of conformational preferences on functional properties.
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.
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 Å lead to an intramolecular folding, whereas linker moieties with a length between 7 to 11 Å 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 Å 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 Å) 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 Å 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.
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.
In this work the influence of “active” bridge units on the electron transfer (ET) mechanism within organic donor-bridge-electrode arrays in self-assembled monolayers (SAMs) was studied by spectroscopic and electrochemical methods. In the first part of this work ferrocenealkanethiols 1 – 3 and the ferrocenearylthiols 4, 5 were investigated to get experience in the monolayer preparation for measuring ET rates. Cyclic voltammetry of the monolayers indicates that homogeneously mixed monolayers containing redox active molecules and dummy molecules were formed. For the known ferrocenealkanethiols 1 – 3 the ET rates could be confirmed compared to the ones measured by Creager et al. [206]. As expected the ET rate decreases by increasing chain length of the alkane spacer from 2 to 3. Changing the bonding between the redox centre and the alkane spacer with the same bridge lenght, e. g. by using a carboxy-group in case of 1, does not influence the ET behaviour very strong. The aromatic ferrocenethiols 4 and 5 show very high ET rates due to the strong conjugated system although the distance between the redox centre and the electrode is comparable to the C8-alkyl compound 2. The electronic coupling factors all indicate a nonadiabatic ET between the redox centre and the electrode. As expected the electronic coupling factors increase with decreasing spacer length or with an enlarged conjugated system. To sum up, experience in monolayer preparation could be obtained, the measured ET rates for well known ferrocenealkane-compounds 1 - 3 could be verified and the information could be transferred to the conjugated systems 4 and 5. In the second part the triarylamine- 29, 32 and the phenothiazinealkanethiol 35 have been examined relative to their ET behaviour in mixed monolayers. The cyclic voltammograms of the diluted monolayers indicate that homogeneously formed monolayers are present. The ET rates of triarylamine- 29, 32 and phenothiazinealkanethiols 35 are 10 to 100 times higher than compared to ferrocenealkanethiols with equal chain length[183, 206], whereas in a [Ru(bpy)2(pp)]+-containing monolayer the same value was observed [177]. Almost two parameters influence the ET rate constant: the electronic coupling matrix element and the reorganisation energy  [209]. The ET rate in donor substituted alkanethiols is mainly influenced by the reorganisation energy  [177] and even small changes have a dramatic effect on the observed processes, therefore an increasing ET rate from the ferrocene (high reorganisation energy) over the phenothiazine 35 and the [Ru(bpy)2(pp)]+ to the triarylamine chromophores 29 and 32 (low reorganisation energy) is observed. Furthermore the bonding between the redox centres and the alkane spacer plays an important role on the ET rate in case of the triarylamines 29 and 32 opposite to the assumption made by Creager et al. that the connection does not play any role. For the electron rich ether connected compound 29 the ET is not only dominated by the reorganisation energy but also by mesomeric effects where the positive charge of the electron rich derivative 29 is more located at the ether function so that the chain is formally shortend by one atom resulting in higher ET rates than compared to 32. In the third part of the thesis a series of “molecular wires” consisting of methoxy- or chloro-substituted triarylamines and phenothiazines with different bridge units and bridge length between the redox centre and the anchor thiol function have been prepared in order to investigate their ET-behaviour. Cyclic voltammetry and UV/vis-spectroscopy show that the oxidation potential and the energetic states could be controlled very well by introducing different redox centres and bridge units resulting in a decreasing oxidation potential of the redox centres and a bathochromic shift of the absorption bands in the UV/vis-spectra. Also the densitiy of the chromophores in mixed monolayers could be controlled very well for only three compounds (49, 52 and 87) with nitrile-substituted bridges reliable ET rates could be obtained. In these chromophores the ET rate decreases by increasing the density of the redox active molecules in the mixed monolayers indicating that the adsorption geometry changes with coverage with the chromophores tilting to a more upright orientation as the surface becomes more crowded. For all other compounds the measurements were limited by the fast ET rates. Conformational, as well as a very weak distance dependence of the ET resulting in very high ET rates [172] or unfavourable HOMO-LUMO energies of the donor, bridge and the electrode are reasons for this behaviour. The fact that compound 49 shows almost the same rate constant independent of the length (n = 2 or n = 3) may indicate that a hopping process is operating for which a much weaker length dependence is expected than in the case of a superexchange.
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.
In the first part of this thesis, the synthesis of a series of bistriarylamine (bisTAA) compounds was presented. On the one hand, the substitution pattern of the TAA at the benzene bridging unit was varied from meta- to para-position (pX and mX), on the other hand, the energetic position of the bridging unit was tuned by use of two electron-donating or electron-accepting substituents X (with X = OMe, Me, Cl, CN, NO2) in 2,5-position. In case of the meta-series, compounds with X in 4,6-position were synthesized (mX46). The photophysical and electrochemical properties of the neutral compounds were investigated.
The cationic mixed valence (MV) bisTAA compounds could be generated by oxidation. Thermally induced hole transfer (HT) in the groud state was investigated by temperature depending ESR spectroscopy. While the HT rate k and HT barrier ΔG in mX are unaffected by the substituents X, k and ΔG in the pX series increase simultaneously with increasing electron-donating strength of X. This, at first contradictory observation can be explained by an increasingly important solvent dynamic effect and an additional, effective barrier. The optically induced HT was examined by UV/Vis/NIR spectroscopy. The pX-series revealed an increase of the electronic coupling V, and correspondingly a decrease of ΔG, with an increase of the electron donating character of X. For mX, a spectroscopic determination of these parameters was not possible. mX46 showed an intermediate behavior, MV compounds with strong electron-donating X, obtained coupling of similar magnitude as pX, which could be explained by means of DFT calculations, with regard to the molecular orbitals.
In the second part of this work, the synthesis of a series of dyads with triarylamine (TAA) as a donor and naphthalene diimide (NDI) as an acceptor was presented. Again, the substitution pattern of the redox centers at the benzene bridging unit was varied in the form of a meta- or para-position (pXNDI or mXNDI) and the energetic position of the bridging unit was varied by X (with X = OMe, Me, Cl, CN, NO2) attached in the 2,5-position. Additionally, compound mOMe46NDI with methoxy substitution in 4,6-position was synthesized. The photophysical and electrochemical properties of these compounds were investigated. The electron transfer (ET) processes of charge separation (CS) and charge recombination (CR) of these were investigated by means of transient absorption (TA) spectroscopy in toluene. This was not possible for the nitro-compounds p-/mNO2NDI, since they decomposed under irradiation. In addition to that, the CR of pXNDI was not detectable by ns-setup, which is why the focus was given to the mXNDI series (with X = OMe–CN).The CS was examined by fs-TA spectroscopy, where the formation of a CS state could be detected. The rise time of the CS states decreases with increasing electron-withdrawing substituents X. CR was examined with ns-TA spectroscopy and shows a biexponential decay behavior, which is caused by singlet-triplet equilibrium in the CS state. By applying an external magnetic field, the decay behavior was decisively changed and the singlet-triplet splitting could be determined. This finding could also be confirmed by simulating the decay curves.
In both parts of this work, the decisive influence of the benzene bridging unit on the appearing ET processes became obvious. For the HT in the ground state of the MV compound, as well as for the ET in the exited states of the DA compounds, the highest transfer rates were found for the para-series pX and pXNDI, and much smaller rates for the meta-series mX and mXNDI. The meta46-compounds mX46 and mOMeNDI46 showed an intermediate behavior in both parts of this work.
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 this work the synthesis of dendritic macromolecules and small redox cascades was reported and studies of their energy and electron transfer properties discussed.
The chromophores in the dendrimers and the redox cascades are linked via triazoles, which were built up by CuAAC. Thereby, a synthetic concept based on building blocks was implemented, which allowed the exchange of all basic components. Resulting structures include dendrimers composed exclusively of TAAs (G1–G3), dendrimers with an incorporated spirobifluorene core (spiro-G1 and spiro-G2) and the donor-acceptor dendrimer D-A-G1, in which the terminal groups are exchanged by NDIs.
Furthermore, a series of model compounds was synthesised in order to achieve a better understanding of the photophysical processes in the dendrimers.
A modification of the synthetic concept for dendrimers enabled the synthesis of a series of donor-acceptor triads (T-Me, T-Cl and T-CN) consisting of two TAA donors and one NDI acceptor unit. The intermediate TAA chromophore ensured a downhill redox gradient from the NDI to the terminal TAA, which was proved by cyclic voltammetry measurements. The redox potential of the intermediate TAA was adjusted by different redox determining substituents in the “free” p-position of the TAA. Additionally, two dyads (Da and Db) were synthesised which differ in the junction of the triazole to the TAA or the NDI, respectively. In these cascades a nodal-plane along the N-N-axes in the NDI and a large twist angle between the NDI and the N-aryl substituent guaranteed a small electronic coupling.
The photophysical investigations of the dendrimers focused on the homo-energy transfer properties in the TAA dendrimers G1–G3. Steady-state emission spectroscopy revealed that the emission takes place from a charge transfer state. The polar excited state resulted in a strong Stokes shift of the emission, which in turn led to a small spectral overlap integral between the absorption of the acceptor and the emission of the donor in the solvent relaxed state. According to the Förster theory, the overlap integral strongly determines the energy transfer rate. Fluorescence up-conversion measurements showed a strong and rapid initial fluorescence anisotropy decay and a much slower decrease on the longer time scale. The experiment revealed a fast energy transfer in the first 2 ps followed by a much slower energy hopping. Time resolved emission spectra (TRES) of the model compound M indicated a solvent relaxation on the same time scale as the fast energy transfer.
The Förster estimation of energy transfer rates in G1 explains fast energy transfer in the vibrotionally relaxed state before solvent relaxation starts. Thereby, the emission spectrum of G1 in cyclohexane served as the time zero spectrum. Thus, solvent relaxation and fast energy transfer compete in the first two ps after excitation and it is crucial to discriminate between energy transfer in the Franck-Condon and in the solvent relaxed state. Furthermore, this finding demonstrates that fast energy transfer occurs even in charge transfer systems where a large Stokes shift prevents an effective spectral overlap integral if there is a sufficient overlap integral in before solvent relaxation.
Energy transfer upon excitation was also observed in the spiro dendrimers spiro-G1 and spiro-G2 and identified by steady-state emission anisotropy measurements. It was assumed that the energy in spiro-G1 is completely distributed over the entire molecule while the energy in spiro-G2 is probably distributed over only one individual branch. This finding was based on a more polarised emission of spiro-G2 compared to spiro-G1. This issue has to be ascertained by e.g. time resolved emission anisotropy measurements in further energy transfer studies.
Concerning the electron transfer properties of TAA-triazole systems the radical cations of G1–G2, spiro-G1 and spiro-G2 and of the model compound M were investigated by steady-state absorption spectroscopy. Experiments showed that the triazole bridge exhibits small electronic communication between the adjacent chromophores but still possesses sufficient electronic coupling to allow an effective electron transfer from one chromophore to the other.
Due to the high density of chromophores, their D-A-D structure and their superficial centrosymmetry, the presented dendrimers are prospective candidates for two-photon absorption applications.
The dyads, triads and the donor-acceptor dendrimer D-A-G1 were investigated regarding their photoinduced electron transfer properties and the effects that dominate charge separation and charge recombination in these systems.
The steady-state absorption spectra of all cascades elucidated a superposition of the absorption characteristics of the individual subunits and spectra indicated that the chromophores do not interact in the electronic ground state.
Time resolved transient absorption spectroscopy of the cascades was performed in the fs- and ns-time regime in MeCN and toluene as solvent. Measurements revealed that upon with 28200 cm-1 (355) nm and 26300 cm-1 (380 nm), respectively, an electron is transferred from the TAA towards the NDI unit yielding a CS state. In the triads at first a CS1 state is populated, in which the NDI is reduced and the intermediate TAA1 is oxidised. Subsequently, an additional electron transfer from the terminal TAA2 to TAA1 led to the fully CS2 state. Fully CS states of the dyads and triads exhibit lifetimes in the ns-time regime. In contrast for Db in MeCN, a lifetime of 43 ps was observed for the CS state together with the population of a 3NDI state. The signals of the other CS states decay biexponentially, which is a result of the presence of the 1CS and the 3CS states. While magnetic field dependent measurements of Db did not show an effect due to the large singlet-triplet splitting, T-CN exhibited a strong magnetic field dependence which is an evidence for the 1CS/3CS assignment. Further analysis of the singlet-triplet dynamics are required and are currently in progress.
Charge recombination occurred in the Marcus inverted region for compounds solved in toluene and in the Marcus normal region for MeCN as solvent. However, a significant inverted region effect was observed only for Db. Triads are probably characterised by charge recombination rates in the inverted and in the normal region near to the vertex of the Marcus parabola. Hence the inverted region effect is not pronounced and the rate charge recombination rates are all in the same magnitude. However, compared to the charge recombination rate of Db the enlarged spatial distance between the terminal TAA and the NDI in the fully CS2 states in the triads resulted in reduced charge recombination rates by ca. one order of magnitude.
More important than a small charge recombination rate is an overall lifetime of the CS states and this lifetime can significantly be enhanced by the population of the 3CS state. The reported results reveal that a larger singlet-triplet splitting in the dyads led to a CS state lifetime in the us time regime while a lifetime in the ns-time regime was observed in cases of the triads. Moreover, the singlet-triplet splitting was found to be solvent dependent in the triads, which is a promising starting point for further investigations concerning singlet-triplet splitting.
The donor-acceptor dendrimer D-A-G1 showed similar characteristics to the dyads. The generation of a CS state is assumed due to a clear NDI radical anion band in the transient absorption spectrum. Noteworthy, the typical transient absorption band of the TAA radical cation is absent for D A-G1 in toluene. Bixon-Jortner analysis yielded a similar electronic coupling in D-A-G1 compared to the dyads. However, the charge recombination rate is smaller than of Db due to a more energetic CS state, which in the inverted region slows down charge recombination. In combination a singlet-triplet splitting similar to the dyads prolongs the CS state lifetime up to 14 us in diluted solution. Both effects result in an even better performance of D-A-G1 concerning energy conversion. D A-G1 is therefore a promising key structure for further studies on light harvesting applications. In a prospective study a second generation donor-acceptor dendrimer D-A-G2 might be an attractive structure accessible by “click reaction” of 13 and 8. D-A-G2 is expected to exhibit a downhill oriented gradient of CS states as assumed from the CV studies on G1–G3.