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Inserido no contexto de fontes de energia renováveis, este trabalho consiste na síntese e caracterização de filmes de bastões de ZnO modificados com quantum dots de CdTe a fim de serem aplicados em células fotoeletroquímicas. Bastões de ZnO são materiais interessantes, porque este tipo de estrutura facilita o transporte de portadores de carga, minimizando a perda destes nos contornos de grão, sua recombinação e aniquilação. A modificação do filme de ZnO com nanocristais de CdTe deve aumentar a eficiência da fotoconversão, facilitando a separação de carga e transferência de elétrons, e isso aumenta a estabilidade dos nanocristais, impedindo a corrosão anódica e a decomposição destes. O filme de ZnO foi eletrodepositado potenciostaticamente sobre a superfície de ITO. As análises de MEV e EDX indicaram que filme de ZnO obtido é homogêneo e consiste de bastões com razão atômica de Zn e O de acordo com a estequiometria 1:1. O resultado de DRX apresentou três planos característicos do ZnO na forma cristalina wurtzita. O plano (002) foi o predominante, indicando a orientação dos bastões no eixo c vertical ao substrato. O filme de ZnO tem espessura de 550 nm, bandgap 3,27 eV, potencial de banda plana de 0,4 V e densidade de portadores de carga de 8,9 x 1019 cm-3. O procedimento sintético dos pontos quânticos de CdTe ocorreu a partir da dissolução de óxido de cádmio em ácido tetradecilfosfônico e octadeceno (ODE) a 300 °C. Subsequentemente, a solução precursora de cádmio foi resfriada a 260 °C e então a solução precursora de telúrio, preparada pela dissolução de telúrio e tributilfosfina em ODE, foi injetada. Os nanocristais obtidos foram dispersos em hexano, precitados com etanol e finalmente os quantum dots foram armazenados em tolueno. A partir das análises de UV-Vis e TEM foi possível estimar o tamanho dos pontos quânticos de CdTe com aproximadamente 4 nm. O DRX dos nanocristais de CdTe apresentou os planos característicos principais da estrutura da blenda de zinco. O eletrodo de ZnO modificado com os quantum dots de CdTe (ZnO/CdTe) foi obtido após 24 h de imersão em uma solução de acetonitrila contendo ácido mercaptopropiônico e ácido propiônico. Subsequentemente, o filme de ZnO modificado com o ligante foi imerso por 48 h na dispersão de pontos quânticos de CdTe. O espectro de FTIR revelou a ausência do estiramento simétrico de C=O em 1700 cm-1. Por outro lado o espectro revelou a presença dos modos assimétrico e simétrico vas(CO2-) e vs(CO2-) que foram observados em 1631 e 1417 cm-1, respectivamente. A transformação de Kulbeka-Munk do espectro de reflectância do eletrodo ZnO/CdTe apresentou a banda relativa ao CdTe no mesmo comprimento de onda observado quando este encontrava-se na dispersão. O eletrodo ZnO/CdTe mostrou um valor de fotocorrente de 138 µA, um valor 10 vezes maior que o obtido para o ZnO. Nos experimentos de IPCE (eficiência de conversão do fóton incidente à corrente) um aumento de aproximadamente cinco vezes também foi observado para o eletrodo de ZnO/CdTe. A dinâmica dos portadores de carga foi investigada por TAS (Espectroscopia de Absorção Transiente) nas escalas de tempo fs e µs para os eletrodos de ZnO e de ZnO/CdTe. A análise TAS indicou um tempo de vida menor para o filme ZnO/CdTe em comparação com filme ZnO. A medidas com o eletrodo de Clark demonstraram uma produção de oxigênio pelo eletrodo de ZnO/CdTe. Assim, o filme de ZnO/CdTe proposto apresenta-se como um material promissor para aplicações fotoeletroquímicas. / Placed in the context of renewable energy sources, this work consists of the synthesis and characterization of ZnO films modified CdTe quantum dots to be applied in photoelectrochemical cells. ZnO rods are interesting materials because this kind of structure facilitates the charge carriers transport, minimizing the loss of these at grain boundaries and their recombination and annihilation. The ZnO film modification with CdTe nanocrystals should increase the photoconversion efficiency by facilitating charge separation and electron transfer, and it increases the nanocrystals stability, preventing it from anodic corrosion and decomposition. The ZnO film was electrodeposited potenciostatically on ITO surface. SEM and EDX analysis indicated that the ZnO film obtained is homogeneous and it consists of rods with atomic ratio of Zn and O according to 1:1 stoichiometry. XRD result showed three characteristic planes of ZnO in wurtzite crystalline form. The (002) plane is the predominant, indicating the rods orientation in the c-axis vertical to the substrate. The ZnO film also has a thickness of 550 nm, bandgap of 3.27 eV, flat band potential of 0.4 V and density of charge carriers 8,9 x 1019 cm-3. The synthetic procedure of CdTe quantum dots occurred from the dissolution cadmium oxide in tetradecylphosphonic acid and octadecene (ODE) to 300 °C. Subsequently, cadmium precursor solution of was cooled to 260 °C and then the tellurium precursor solution, prepared by dissolving tellurium in tributylphosphine and in ODE was injected. The obtained nanocrystals were dispersed in hexane, precipitated with ethanol and finally the quantum dots were stored in toluene. From UV-Vis and TEM analysis was possible to estimate the quantum dots size of CdTe as 4 nm. The XRD of CdTe nanocrystals presented the main characteristic planes of zinc blend structure. ZnO electrode modified with CdTe quantum dots (ZnO/CdTe) was obtained by 24 h immersion in a solution of acetonitrile containing mecaptopropionic acid and propionic acid. Subsequently, the ZnO film modified with the linker was immersed for 48 h in CdTe quantum dots dispersion. FTIR spectrum reveals the absence of a symmetrical C=O stretching mode at approximately 1700 cm-1. Instead, the spectrum shows the presence of the asymmetric and symmetric vas(CO2-) and vs(CO2-) modes were observed at 1631 and 1417 cm-1, respectively. Kulbeka-Munk transformation of the reflectance spectrum of the ZnO/CdTe electrode presented the band related to CdTe in the same wavelength observed when this was in the dispersion. The ZnO/CdTe electrode showed a photocurrent value of 138 µA, a value 10 times greater than that obtained for ZnO. At IPCE experiments (incident photon-to-current efficiency) an increase of approximately five times was also noticed to the electrode of ZnO/CdTe. Dynamics of charge carriers was investigated by fs and µs TAS (Transient Absorption Spectroscopy) for ZnO and ZnO/CdTe electrodes. TAS analyses indicate a short life time to ZnO/CdTe electrode compared to ZnO film. Clark electrode measurements showed oxygen production by ZnO/CdTe electrode. Thus, ZnO/CdTe proposed electrode is presented as promising material for photoelectrochemical applications.

Inserido no contexto de fontes de energia renováveis, este trabalho consiste na síntese e caracterização de filmes de bastões de ZnO modificados com quantum dots de CdTe a fim de serem aplicados em células fotoeletroquímicas. Bastões de ZnO são materiais interessantes, porque este tipo de estrutura facilita o transporte de portadores de carga, minimizando a perda destes nos contornos de grão, sua recombinação e aniquilação. A modificação do filme de ZnO com nanocristais de CdTe deve aumentar a eficiência da fotoconversão, facilitando a separação de carga e transferência de elétrons, e isso aumenta a estabilidade dos nanocristais, impedindo a corrosão anódica e a decomposição destes. O filme de ZnO foi eletrodepositado potenciostaticamente sobre a superfície de ITO. As análises de MEV e EDX indicaram que filme de ZnO obtido é homogêneo e consiste de bastões com razão atômica de Zn e O de acordo com a estequiometria 1:1. O resultado de DRX apresentou três planos característicos do ZnO na forma cristalina wurtzita. O plano (002) foi o predominante, indicando a orientação dos bastões no eixo c vertical ao substrato. O filme de ZnO tem espessura de 550 nm, bandgap 3,27 eV, potencial de banda plana de 0,4 V e densidade de portadores de carga de 8,9 x 1019 cm-3. O procedimento sintético dos pontos quânticos de CdTe ocorreu a partir da dissolução de óxido de cádmio em ácido tetradecilfosfônico e octadeceno (ODE) a 300 °C. Subsequentemente, a solução precursora de cádmio foi resfriada a 260 °C e então a solução precursora de telúrio, preparada pela dissolução de telúrio e tributilfosfina em ODE, foi injetada. Os nanocristais obtidos foram dispersos em hexano, precitados com etanol e finalmente os quantum dots foram armazenados em tolueno. A partir das análises de UV-Vis e TEM foi possível estimar o tamanho dos pontos quânticos de CdTe com aproximadamente 4 nm. O DRX dos nanocristais de CdTe apresentou os planos característicos principais da estrutura da blenda de zinco. O eletrodo de ZnO modificado com os quantum dots de CdTe (ZnO/CdTe) foi obtido após 24 h de imersão em uma solução de acetonitrila contendo ácido mercaptopropiônico e ácido propiônico. Subsequentemente, o filme de ZnO modificado com o ligante foi imerso por 48 h na dispersão de pontos quânticos de CdTe. O espectro de FTIR revelou a ausência do estiramento simétrico de C=O em 1700 cm-1. Por outro lado o espectro revelou a presença dos modos assimétrico e simétrico vas(CO2-) e vs(CO2-) que foram observados em 1631 e 1417 cm-1, respectivamente. A transformação de Kulbeka-Munk do espectro de reflectância do eletrodo ZnO/CdTe apresentou a banda relativa ao CdTe no mesmo comprimento de onda observado quando este encontrava-se na dispersão. O eletrodo ZnO/CdTe mostrou um valor de fotocorrente de 138 µA, um valor 10 vezes maior que o obtido para o ZnO. Nos experimentos de IPCE (eficiência de conversão do fóton incidente à corrente) um aumento de aproximadamente cinco vezes também foi observado para o eletrodo de ZnO/CdTe. A dinâmica dos portadores de carga foi investigada por TAS (Espectroscopia de Absorção Transiente) nas escalas de tempo fs e µs para os eletrodos de ZnO e de ZnO/CdTe. A análise TAS indicou um tempo de vida menor para o filme ZnO/CdTe em comparação com filme ZnO. A medidas com o eletrodo de Clark demonstraram uma produção de oxigênio pelo eletrodo de ZnO/CdTe. Assim, o filme de ZnO/CdTe proposto apresenta-se como um material promissor para aplicações fotoeletroquímicas. / Placed in the context of renewable energy sources, this work consists of the synthesis and characterization of ZnO films modified CdTe quantum dots to be applied in photoelectrochemical cells. ZnO rods are interesting materials because this kind of structure facilitates the charge carriers transport, minimizing the loss of these at grain boundaries and their recombination and annihilation. The ZnO film modification with CdTe nanocrystals should increase the photoconversion efficiency by facilitating charge separation and electron transfer, and it increases the nanocrystals stability, preventing it from anodic corrosion and decomposition. The ZnO film was electrodeposited potenciostatically on ITO surface. SEM and EDX analysis indicated that the ZnO film obtained is homogeneous and it consists of rods with atomic ratio of Zn and O according to 1:1 stoichiometry. XRD result showed three characteristic planes of ZnO in wurtzite crystalline form. The (002) plane is the predominant, indicating the rods orientation in the c-axis vertical to the substrate. The ZnO film also has a thickness of 550 nm, bandgap of 3.27 eV, flat band potential of 0.4 V and density of charge carriers 8,9 x 1019 cm-3. The synthetic procedure of CdTe quantum dots occurred from the dissolution cadmium oxide in tetradecylphosphonic acid and octadecene (ODE) to 300 °C. Subsequently, cadmium precursor solution of was cooled to 260 °C and then the tellurium precursor solution, prepared by dissolving tellurium in tributylphosphine and in ODE was injected. The obtained nanocrystals were dispersed in hexane, precipitated with ethanol and finally the quantum dots were stored in toluene. From UV-Vis and TEM analysis was possible to estimate the quantum dots size of CdTe as 4 nm. The XRD of CdTe nanocrystals presented the main characteristic planes of zinc blend structure. ZnO electrode modified with CdTe quantum dots (ZnO/CdTe) was obtained by 24 h immersion in a solution of acetonitrile containing mecaptopropionic acid and propionic acid. Subsequently, the ZnO film modified with the linker was immersed for 48 h in CdTe quantum dots dispersion. FTIR spectrum reveals the absence of a symmetrical C=O stretching mode at approximately 1700 cm-1. Instead, the spectrum shows the presence of the asymmetric and symmetric vas(CO2-) and vs(CO2-) modes were observed at 1631 and 1417 cm-1, respectively. Kulbeka-Munk transformation of the reflectance spectrum of the ZnO/CdTe electrode presented the band related to CdTe in the same wavelength observed when this was in the dispersion. The ZnO/CdTe electrode showed a photocurrent value of 138 µA, a value 10 times greater than that obtained for ZnO. At IPCE experiments (incident photon-to-current efficiency) an increase of approximately five times was also noticed to the electrode of ZnO/CdTe. Dynamics of charge carriers was investigated by fs and µs TAS (Transient Absorption Spectroscopy) for ZnO and ZnO/CdTe electrodes. TAS analyses indicate a short life time to ZnO/CdTe electrode compared to ZnO film. Clark electrode measurements showed oxygen production by ZnO/CdTe electrode. Thus, ZnO/CdTe proposed electrode is presented as promising material for photoelectrochemical applications.

Global energy demands have escalated over the past few decades, creating a necessity for alternative energy sources. Solar technologies inspired by the primary solar energy storing process known on earth, photosynthesis, have subsequently gained popularity. The natural photosynthetic apparatus comprises a network of membrane-bound pigment-protein complexes, with the main plant light-harvesting complex (LHCII) consisting of chlorophyll (Chl) and carotenoid (Car) pigments. Electronic excitation energy transfer (ET) of the harvested energy takes place amongst these pigments on ultrafast timescales. This energy is funnelled towards a photosynthetic reaction centre where charge separation is achieved, creating a Biobattery, which powers the subsequent manufacture of energy-rich chemical compounds for photosynthetic activity. Transient absorption pump-probe spectroscopy has proven to be a useful technique for monitoring the evolution of the excited state dynamics, such as electronic transitions and excitation ET amongst Car and Chl pigments of LHCII trimers isolated from spinach leaves. This method was utilized to probe samples excited under four different conditions: at pump excitation wavelengths (𝜆𝑒𝑥) of 489 nm (preferentially exciting Cars Lutein1 and Neoxanthin) and 506 nm (targeting Cars Lutein2 and Violaxanthin), each with an intensity of either 800 nJ/pulse (relatively high) or 500 nJ/pulse (comparatively low). A global analysis was applied to each dataset using the robust, open-source Glotaran software, from which three kinetic decay lifetimes for the various processes were extracted. General spectral observations encompassed a negative pump ground state bleach (GSB) at each 𝜆𝑒𝑥; negative Chl b and Chl a GSBs, superimposed with negative stimulated emission (SE) signals; and a positive excited state absorption (ESA) band. The first lifetime of a few picoseconds corresponded mainly to Car-S2 depopulation, resulting either from energy relaxation towards Car-S1, or ET to Chls. Small, but distinct Chl b signals of less than 3 mOD were also detected on this timescale. The second lifetime, which is between 10 and 12 ps, was characteristic to the Lutein Car-S1 lifetime, mainly depicting Car-S1 ET to Chl a. The third lifetime, which extended from ~200 ps to the nanosecond timescale, was attributed to Chl a fluorescence. The 𝜆𝑒𝑥 of 489 nm directly excites the Chl Soret region, whilst excitation at 506 nm shows a pump intensity-dependence. Laser pulse photon density values were ~1014 photons·cm-2·pulse-1 for these datasets. Singlet-singlet annihilation calculations performed on the samples excited at 506 nm provided low annihilation probabilities of 9.0% and 11.5% for a low and high pump intensity, respectively, limiting the possibility of sample photobleaching. Optimization and redevelopment of the experimental setup significantly improved both the data quality and various recorded parameters, concluding that pump-probe spectroscopy was successful on the prepared LHCII trimers. Results acquired and calculations performed correlated with literature, where minimal changes were noticed in the timescales and ET pathways. The robustness of plant systems was confirmed through both excitation-wavelength and intensity dependence. This work paves the way for advanced studies on the role Cars play in non-photochemical quenching (NPQ), a self-protection mechanism of plants against over-illumination; and for the tailoring of artificial light-harvesting antennas based on research conducted on their natural counterparts. / Globale energievereistes het oor die afgelope paar dekades toegeneem, wat die ontwikkeling van alternatiewe energiebronne noodsaaklik maak. Sontegnologieë, geïnspireer deur die primêre sonenergiebergingsproses op aarde, fotosintese, het daarom gewild geword. Die natuurlike fotosintetiese apparaat bestaan uit 'n netwerk van membraangebonde pigment-proteïenkomplekse, met die hoof ligversamelingskompleks in plante (LHCII) wat bestaan uit chlorofil- (Chl) en karotenoïed- (Car) pigmente. Die energie wat deur die pigmente geabsorbeer word, word tussen elektroniese opgewekte toestande op verskillende pigmente op ultravinnige tydskale oorgedra. Hierdie energie word na ʼn fotosintetiese reaksiesentrum gekanaliseer, waar 'n ladingskeiding geïnduseer word en 'n Biobattery sodoende geskep word. Die energie wat in dié battery gestoor is, word gebruik om energieryke chemiese verbindings te vervaardig — wat as brandstof vir die plant dien om sy lewensfunksies te verrig. Tydopgeloste-absorpsie-pomp-tasting-spektroskopie is 'n nuttige tegniek om die dinamika tussen opgewekte toestande te volg. ‘n Voorbeeld van sulke dinamika is die elektroniese opwekking en energie-oordrag tussen die Car- en Chl-pigmente van geïsoleerde LHCII-trimere in spinasieblare. Hierdie metode is gebruik om monsters onder vier verskillende toestande te ondersoek by pompgolflengtes (𝜆𝑒𝑥) van 489 nm (waar hoofsaaklik die Cars Luteïne1 en Neoksantine opgewek word) en 506 nm (vir Cars Luteïne2 en Violaksantine), en pompenergieë van ‘n relatief hoë 800 nJ/puls, of 500 nJ/puls vir elke golflengte. / Dissertation (MSc)--University of Pretoria, 2017. / National Research Foundation (NRF) / Physics / MSc / Unrestricted

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The excited state electronic structures of several biologically important chromophores were studied by Stark spectroscopy. The extent of charge redistribution upon excitation to the lowest excited states of the oxidized and semiquinone forms of flavin adenine dinucleotide (FAD) bound to the light activated DNA repair enzyme DNA photolyase have been studied previously by this technique. This work focuses on the catalytically active form, the two-electron reduced anion. To facilitate analysis of this experiment, the Stark spectra of a simple flavin derivative that is soluble in organic solvents was measured. The results of the analysis of these data are in agreement with previously a published linear dichroism experiment that found the absorption spectrum of flavins in this redox state arises from two distinct electonic transitions in the visible/near-ultraviolet spectral range, a fact that has not been incorporated into the analysis of many ultrafast spectroscopic experiments of reduced anionic flavins/flavoproteins. The difference dipole moment of the second, more intense, transition was found to be about twice as large as that of the lowest energy transition. With the aid of ab initio calculations, the directions of these dipole moments in the molecular frame were assigned. For both transitions, it was found that negative charge density is shifted toward the xylene ring of the flavin upon excitation. Another important consideration for the correct analysis of the photolyase spectra is the possibility of contamination by small amounts of the antenna chromophore, which also has absorption intensity in the near-ultraviolet region. We chose to study the cofactor for E. coli photolyase, 5,10-methenyltetrahydrofolate, and its photodecomposition product, 5,10-methylenetetrahydrofolate. The difference dipole moments for the lowest energy transitions of both of these chromophores were found to be quite large, ranging from 9-12 D fc and lying primarily along the transition dipole moment. Additionally, the difference polarizability of both chromophores was large, on the order of 200-300 Å3 fc2 . The Stark spectra of reduced anionic FAD in photolyase agrees well with the findings of the experiments on flavin in organic solvent; the magnitude of the difference dipole moments in both cases match within experimental error. While the direction of the difference dipole moment for the lowest transition is also the same in both cases, that of the second transition is changed in the protein matrix. The assignment of these vectors in the molecular frame shows that the two dipole moments are coincident for the cofactor bound to photolyase. This finding, where electron density is shifted toward the point of the flavin ring closes to the DNA lesion bound to the enzyme, is strong evidence that direct electron transfer takes place from the isoalloxazine ring of FAD to the DNA substrate in the catalytic cycle. The usefulness of Stark spectroscopy in investigating photoinduced charge redistribution was also shown for the donor-π-acceptor flavin dyad, azobenzylflavin (ABFL). The difference dipole moment was found to be 22 D, an approximately three-fold increase from the largest difference dipole moment found in naturally occurring flavins. This extensive charge redistribution corresponds to a large hyperpolarizability of the chromophore that suggests that ABFL may be useful in nonlinear optical applications. Transient absorption was used to supplement these experiments by monitoring the decay kinetics of ABFL after excitation. It was found that ABFL undergoes ultrafast charge recombination within 6 ps after excitation, leading to depopulation of the charge separated state before useful work can be performed for applications requiring electron transfer. These studies provide the ground work for rational design of other ABFL-like derivatives for use in a variety of applications. / Chemistry

This thesis improves our understanding of the charge-transfer dynamics in organic materials employed in dye-sensitized and nanotube-thiophene solar cells. For the purpose of this work, a femtosecond transient absorption spectroscopy setup was built. Additionally, microsecond transient absorption spectroscopy was utilised to explore dynamics on a longer time-scale. In the first study, the dependence of dye regeneration and charge collection on the pore- filling fraction (PFF) in solid-state dye-sensitized solar cells (DSSCs) is investigated. It is shown that while complete hole transfer with PFFs as low as ~30% can be achieved, improvements beyond this PFF are assigned to a stepwise increase in the charge-collection efficiency in agreement with percolation theory. It is further predicted that the chargecollection efficiency saturates at a PFF of ~82%. The study is followed by an investigation of three novel hole-transporting materials for DSSCs with slightly varying HOMO levels to systematically explore the possibility of reducing the loss-in-potential and thus improving the device efficiency. It is shown that despite one new HTM showing a 100% hole-transfer yield, all devices based on the new HTMs performed worse than those incorporating spiro-OMeTAD. Furthermore, it is demonstrated that the design of the HTM has an additional impact on the electronic density of states present at the TiO₂ electrode surface, and hence influences not only hole- but also electron-transfer from the sensitizer. Finally, a study on a polymer-single-walled carbon nanotube (SWNT) molecular junction is presented. Results from femtosecond spectroscopic techniques show that the polymer poly(3-hexylthiophene) (P3HT) is able to transfer charges to the SWNT within 430 fs. Addition of excess P3HT polymer leads to long-lived free charges making these materials a viable option for solar cells.