Made available in DSpace on 2014-06-11T19:35:08Z (GMT). No. of bitstreams: 0 Previous issue date: 2008-06-30Bitstream added on 2014-06-13T19:45:03Z : No. of bitstreams: 1 goncalves_as_dr_araiq.pdf: 8384691 bytes, checksum: 99f915f60f4aa419101cf4839adc9f92 (MD5) / Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES) / Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP) / Com o objetivo de melhorar o transporte eletrônico no eletrodo nanoestruturado de ZnO, íons Ga3+ foram utilizados neste trabalho como dopantes e/ou modificadores da superfície. Nanopartículas de ZnO e ZnO:Ga 1, 3 e 5% cristalinas foram preparadas pelo método da precipitação a baixa temperatura. Nenhuma evidência da formação de ZnGa2O4, mesmo na amostra ZnO:Ga 5%, foi detectada por DRX. Dados de XPS revelaram que Ga está presente na matriz de ZnO como Ga3+. O tamanho de partícula diminuiu com o aumento na quantidade de gálio, como observado por FE-SEM, provavelmente devido a uma velocidade de hidrólise mais rápida. O menor tamanho de partícula proporcionou filmes com maior porosidade e área superficial, possibilitando uma maior quantidade de corante adsorvida. Quando estes filmes foram aplicados em células solares, o dispositivo baseado em ZnO:Ga 5% apresentou eficiência global na conversão de energia de 6% (a 10 mW cm-2), um valor três vezes maior que o observado para as células solares de ZnO neste trabalho. Este é um dos maiores valores já relatados para células solares de ZnO. Estudos por TAS da dinâmica fotoinduzida em filmes de ZnO:Ga sensibilizados revelaram um maior rendimento do cátion do corante com o aumento na quantidade de gálio, além de uma aceleração no processo de recombinação de carga. Este estudo indica que a dopagem de ZnO com íons Ga3+ possibilita um aumento na fotocorrente e eficiência global do dispositivo. O coeficiente de difusão (D) e o tempo de vida do elétron (τ) foram estudados em células solares seladas por SLIM-PCV. Em comparação às células solares de ZnO, menores valores de D e maiores valores de τ foram observados nas células solares de ZnO:Ga. O mesmo comportamento foi também observado por EIS. Em condições de densidade eletrônica equivalente, os menores valores de Voc em células solares de ZnO:Ga comparados... / In order to enhance the electron transport properties in the ZnO nanostructured electrode, Ga3+ was used in this work as the impurity ions as either surface modifiers and/or dopants. Highly crystalline ZnO and Ga-modified zinc oxide (ZnO:Ga) nanoparticles containing 1, 3, and 5 at.% of Ga3+ were prepared by the precipitation method at low temperature. No evidence of ZnGa2O4, even in the samples containing 5 at.% of Ga3+, was detected by XRD. XPS data revealed that Ga is present into the ZnO matrix as Ga3+. The particle size decreased as the gallium concentration was raised as observed by SEM, which might be related to a faster hydrolysis reaction rate. The smaller particle size provided films with higher porosity and surface area, enabling a higher dye loading. When these films were applied to DSSCs as photoelectrodes, the device based on ZnO:Ga 5 at.% presented an overall conversion efficiency of 6% (at 10 mW cm-2), a three-fold increase compared to the ZnObased DSSCs under the same condition. This is one of the highest efficiencies reported so far for ZnO-based DSSCs. The transient absorption (TAS) study of the photoinduced dynamics of dye-sensitized ZnO:Ga films showed the higher the gallium content, the higher the amount of dye cation formed, while a faster recombination dynamics was observed. The study indicates that Ga-modification of nanocrystalline ZnO leads to an improvement of photocurrent and overall efficiency in the corresponding device. The diffusion coefficient (D) and electron lifetime (τ) were studied in sealed DSSCs by SLIM-PCV. In comparison to the DSSCs based on ZnO electrodes, the ZnO:Ga-based cells provided lower D values and higher values of τ. The result was interpreted with transport limited recombination. The same behavior was also observed by EIS. At matched electron densities, a lower open-circuit voltage (Voc) of DSSCs based on ZnO:Ga was observed... (Complete abstract click electronic access below)

Submitted by Maria Medeiros (maria.dilva1@ufcg.edu.br) on 2018-10-19T13:45:26Z No. of bitstreams: 1 JACYELLI CARDOSO MARINHO DOS SANTOS - DISSERTAÇÃO (PPGEQ) 2017.pdf: 1181213 bytes, checksum: 831251b803f8b040ed40be41dac19267 (MD5) / Made available in DSpace on 2018-10-19T13:45:26Z (GMT). No. of bitstreams: 1 JACYELLI CARDOSO MARINHO DOS SANTOS - DISSERTAÇÃO (PPGEQ) 2017.pdf: 1181213 bytes, checksum: 831251b803f8b040ed40be41dac19267 (MD5) Previous issue date: 2017-03-17 / Atualmente existem três gerações de células solares, sendo a mais recente a Dye-Sensitized Solar Cells-DSSC, também denominadas como células de Grätzel. Uma das partes essenciais desse tipo de célula solar são os eletrodos transparentes formados a partir de óxido metálicos, sendo o mais comum o de estanho (SnO2). Esse óxido vem sendo largamente utilizado como película condutora em vidro, uma vez que combina características como condutividade elétrica com transparência na região do visível do espectro eletromagnético, podendo assim ser aplicado a- uma grande quantidade de dispositivos eletrônicos. Porém, devido o dióxido de estanho se tratar de um material de alto valor agregado, alternativas para sua obtenção estão sendo estudadas, um desses estudos é a utilização de cloreto de estanho para formação do filme condutor em vidro. Dessa forma, esse trabalho tem como objetivo obtenção de uma solução promotor de estanho a partir de liga de solda comercial. Duas técnicas foram avaliadas, o tratamento ácido e o hidrometalúrgico. Amostras de liga de solda (Sn/Pb) foram submetidas a um tratamento ácido e térmico, com a realização da separação chumbo do estanho e formação da solução de cloreto de estanho. Foram realizados ensaios de dopagem com a utilização da solução de cloreto de estanho juntamente com fluoreto de amônia, utilizadas na formação dos filmes em superfícies de placas de vidro. O parâmetro de verificação da formação do filme condutor foi a resistência elétrica, obtida a partir da condutividade elétrica. A solução de cloreto de estanho gerada pelo processo hidrometalúrgico da liga de solda possibilitou a deposição de uma camada condutora em vidro, sendo resistência obtida com filme condutor com essa metodologia foi de 0,4 a 3 KΩ.Apesar da resistência estar acima da dos valores comerciais, a obtenção da solução de cloreto de estanho da partir da solda comercial, ou de lixo eletrônico, minimiza significativamente o custo de produção dos filmes finos condutores, tornando ainda o processo reciclável, se aproveitada a liga de solda de lixos eletrônicos. / There are currently three generations of solar cells, the most recent being the Dye-Sensitized Solar Cells-DSSC, also referred to as Grätzel cells. One of the essential parts of this type of solar cell is transparent electrodes formed from metal oxide, the most common being tin(SnO2). T-his oxide has been widely used as a conductive glass film, since it combines characteristics such as electrical conductivity with transparency in the visible region of the electromagnetic spectrum, and can be applied to a large number of electronic devices. However, because tin dioxide is a high value-added material, alternatives for its production are being studied, one of these studies is the use of tin chloride to form the conductive glass film. Thus, this work has as objective to obtain a solution promoter of tin from commercial welding alloy. Two techniques were evaluated: acid and hydrometallurgical treatment. Samples of solder alloy (Sn/Pb) were subjected to an acid and thermal treatment, with the lead separation of the tin and formation of the tin chloride solution. Doping tests were carried out using the tin chloride solution together with ammonium fluoride used in the formation of films on glass plate surfaces. The verification parameter of the conductive film formation was the electrical resistance, obtained from the electrical conductivity. The solution of tin chloride generated by the hydrometallurgical process of the weld alloy allowed the deposition of a conductive layer in glass, and resistance obtained with conductive film with this methodology was of 0.4 to 3 KΩ. Although the resistance is above commercial values, obtaining the tin chloride solution from the commercial solder or electronic waste minimizes significantly the cost of production of the conductive thin films, making the process even more recyclable, if the alloy is used Soldering of electronic waste.

Orientador: Marian Rosaly Davolos / Coorientador: Ana Flávia Nogueira / Banca: Luiz Antonio Andrade de Oliveira / Banca: Fernando Aparecido Sigoli / Banca: Ivo Alexandre Hummelgen / Banca: Koiti Araki / Resumo: Com o objetivo de melhorar o transporte eletrônico no eletrodo nanoestruturado de ZnO, íons Ga3+ foram utilizados neste trabalho como dopantes e/ou modificadores da superfície. Nanopartículas de ZnO e ZnO:Ga 1, 3 e 5% cristalinas foram preparadas pelo método da precipitação a baixa temperatura. Nenhuma evidência da formação de ZnGa2O4, mesmo na amostra ZnO:Ga 5%, foi detectada por DRX. Dados de XPS revelaram que Ga está presente na matriz de ZnO como Ga3+. O tamanho de partícula diminuiu com o aumento na quantidade de gálio, como observado por FE-SEM, provavelmente devido a uma velocidade de hidrólise mais rápida. O menor tamanho de partícula proporcionou filmes com maior porosidade e área superficial, possibilitando uma maior quantidade de corante adsorvida. Quando estes filmes foram aplicados em células solares, o dispositivo baseado em ZnO:Ga 5% apresentou eficiência global na conversão de energia de 6% (a 10 mW cm-2), um valor três vezes maior que o observado para as células solares de ZnO neste trabalho. Este é um dos maiores valores já relatados para células solares de ZnO. Estudos por TAS da dinâmica fotoinduzida em filmes de ZnO:Ga sensibilizados revelaram um maior rendimento do cátion do corante com o aumento na quantidade de gálio, além de uma aceleração no processo de recombinação de carga. Este estudo indica que a dopagem de ZnO com íons Ga3+ possibilita um aumento na fotocorrente e eficiência global do dispositivo. O coeficiente de difusão (D) e o tempo de vida do elétron (τ) foram estudados em células solares seladas por SLIM-PCV. Em comparação às células solares de ZnO, menores valores de D e maiores valores de τ foram observados nas células solares de ZnO:Ga. O mesmo comportamento foi também observado por EIS. Em condições de densidade eletrônica equivalente, os menores valores de Voc em células solares de ZnO:Ga comparados... (Resumo completo, clicar acesso eletrônico abaixo) / Abstract: In order to enhance the electron transport properties in the ZnO nanostructured electrode, Ga3+ was used in this work as the impurity ions as either surface modifiers and/or dopants. Highly crystalline ZnO and Ga-modified zinc oxide (ZnO:Ga) nanoparticles containing 1, 3, and 5 at.% of Ga3+ were prepared by the precipitation method at low temperature. No evidence of ZnGa2O4, even in the samples containing 5 at.% of Ga3+, was detected by XRD. XPS data revealed that Ga is present into the ZnO matrix as Ga3+. The particle size decreased as the gallium concentration was raised as observed by SEM, which might be related to a faster hydrolysis reaction rate. The smaller particle size provided films with higher porosity and surface area, enabling a higher dye loading. When these films were applied to DSSCs as photoelectrodes, the device based on ZnO:Ga 5 at.% presented an overall conversion efficiency of 6% (at 10 mW cm-2), a three-fold increase compared to the ZnObased DSSCs under the same condition. This is one of the highest efficiencies reported so far for ZnO-based DSSCs. The transient absorption (TAS) study of the photoinduced dynamics of dye-sensitized ZnO:Ga films showed the higher the gallium content, the higher the amount of dye cation formed, while a faster recombination dynamics was observed. The study indicates that Ga-modification of nanocrystalline ZnO leads to an improvement of photocurrent and overall efficiency in the corresponding device. The diffusion coefficient (D) and electron lifetime (τ) were studied in sealed DSSCs by SLIM-PCV. In comparison to the DSSCs based on ZnO electrodes, the ZnO:Ga-based cells provided lower D values and higher values of τ. The result was interpreted with transport limited recombination. The same behavior was also observed by EIS. At matched electron densities, a lower open-circuit voltage (Voc) of DSSCs based on ZnO:Ga was observed... (Complete abstract click electronic access below) / Doutor

Dye-sensitized solar cells (DSSCs) or Grätzel cells are electrochemical devices in where physicochemical properties of different materials are combined to obtain electric energy. These photoconversion devices have evolved from a pioneering concept of molecular photovoltaics to industrial development with confirmed record efficiencies of 14.3%. Their efficiency combined with low-cost production methods and a high aesthetic interest enables the production of DSSC products for consumer electronics market. The strengths of this technology and the fact that its drawbacks are not limiting for this application makes consumer electronics and DSSC a perfect match for the development of self-powered devices. Some companies have already spot a potential market and are currently launching different consumer electronics and other devices with embedded DSSC. This thesis provides an overview of the operation principles of DSSC and the possible routes to improve the efficiency of these devices to emerge and thrive. Additionally, improvements in efficiency, stability and manufacturing needed to be addressed in the near future for this technology are discussed and its suitability to represent a breakthrough in the market of consumer electronics. An overview of the main companies developing DSSC and current prototypes and products is included.

In the latter half of the 20th century the first active environmentalist movements such as Greenpeace and the International Energy Agency were born and initiated a gradual rethinking of environmental awareness. Against all expectations the sole agency under international law for climate protection policy, called the United Nations Framework Convention on Climate Change, was formed 20 years later. Today the awareness of sustained, regenerative and environmental policies permeates throughout all areas of life, science and industry. But energy provision is the most decisive topic, especially since the discussions concerning the phase out of nuclear power where the voices calling for alternative energy sources have become much more vociferous. In addition the depletion of fossil fuels is expected to occur in the not too distant future. All new energy generation methods are required to meet the present and future energy demands, need to be ecological and need to exhibit the same or significantly lower cost expenditure than current energy sources. Unfortunately mankind is confronted with the problem that current commercial alternative energies are more expensive and not yet remotely as efficient as the present energy sources. Although energy provision based on water, wind, sun and geothermal sources have a huge potential because of their continuous presence, unfortunately, they are plagued by inefficient energy conversion caused by the state of technology i.e. the conversion of sun light into electricity loses energy through heat emission, reflection of the sun light, the inability of the material to absorb the entire sun spectrum and the ohmic losses in the transmission of electric current. The sun power is the most exhaustless resource and moreover through photovoltaic action, one of the most direct and cleanest source for use in energy conversion. Presently incoming sun light is not transformed in its entirely, as much degradation occurs during photon absorption and electron transfer processes. A number of other innovative possibilities have also been researched. With respect to cost and efficiency one of the most promising devices is injection solar cells (ISC). By dint of the dye sensitised solar cell (DSSC) Grätzels findings provided the foundations for much research into this type of solar cell where the light absorbing molecule employed in is a dye.[1] The current is obtained through charge separation in the dye, which is initiated through the connection between the dye and a metal oxide on the one hand and a matched redox couple on the other. In a variant of the DSSC the charge separation processes can also occur between a nanoporous metal oxide and nanoparticles giving rise to a quantum dot sensitised solar cell (QDSSC).[2] The use of nanoparticle (NP) properties can be utilized for the harvesting of solar energy, as demonstrated by Kamat and coworkers[3] who were able to exploit these findings subsequently and prepare a number of nanoparticle based solar cells. Nanoparticle research has comprised a wide field of science and nanotechnology for a number of years. As the size of a material approaches dimensions on the nm scale the surface properties contribute proportionally more to the sum of the properties than the volume due to the increase in the surface to volume ratio. These dimensions also constitute a threshold in which quantum physical effects need to be taken into account. Hence the properties of devices or materials in this size regime are inevitably size dependent. The basic principles can be described by two different theories, one of which is based on molecular orbital theory in which the particle is treated as a molecule. For this reason n atomic orbitals with the same symmetry and energy can build up n molecular orbitals through their linear combination based on the LCAO method (Linear Combination of Atomic Orbitals).[4] In the case of solids the orbitals build up energy bands, where the unoccupied states form the quasi continous conduction band (CB) and the occuppied states form the quasi continous valence band (VB). The energy \"forbidden\" area in between these two bands is called the band gap. The band gap is a fixed material property for bulk solids but depends on size in the case of the nanoparticles. In contrast to the LCAO method, simplified solid state theory will be used throughout the present work, the theoretical background of which is provided by the effective mass approximation.[5] When an absorption of a photon occurs, an exciton (electron-hole pair) can be generated. By promoting an electron (e-) from the valence band into the conduction band a hole (h+) may be said to remain in the valence band. By comparison to bulk solids, in a small particle the free charges can sense the potential barrier i.e. the edges of the nanoparticle. Analogous to the particle in a box model this potential barrier interaction results in an increase in the band gap as the particle size decreases. In a solar cell NPs with a particle size which possess a band gap energy in the near infrared (NIR) may be utilised and therefore the NPs will be able to absorb in this spectral region. However NPs also have the ability to absorb higher energy photons due to the continuum present in their band structure, so that almost the entire sun spectral range from the NIR up to UV wavelengths may be absorbed just by using the appropriate NP material and size. Suitable NPs are metal chalcogenides e.g. MX (where M = cadmium, zinc or lead and X = sulfur, selenium or tellurium) because of their bandgap size[6–10] and their relative band positions compared to those of the semiconductor oxide states. Both the TiO2/CdSe[11–14] and TiO2/CdTe[15–18] systems have already been successfully fabricated and many of the anomalies reported.[3] Much interest in the lead chalcogenides has been generated by reports that they may feature the possibility to exhibit multiple exciton generation (MEG) where the absorption of one high energy photon can result in more than one electron-hole pairs.[19–25] Currently electrochemical impedance spectroscopy (EIS) is being used more and more to clarify processes at polarisable surfaces and materials such as nanoparticles. Likewise this method has been rediscovered in photovoltaic research and its use in the characterisation of DSSCs has been discussed in the literature.[26–31] In a number of publications the evaluation of nanoporous and porous structures has been quite extensively explored.[28,29,32–34] Since the mid-20th century Jaffé’s[35] theoretical work concerning the steady- state ac response of solid and liquid systems lead to the formation of the basics of EIS. Further developments in the measurement technology have lead to a broader range of analysis becoming possible. Nevertheless the most challenging part still remains the interpretation of the results and especially to merge the measured data with the theoretical model. EIS quantifies the changes in a small ac current response at electrode electrolyte interfaces i.e. the rate at which the polarized domain will respond, when an ac potential is applied. In this way dielectric properties of materials or composites, such as charge transfers, polarization effects, charge recombination and limitations can be measured as a function of frequency and mechanistic information may be unveiled. Hence EIS allows one to draw a conclusion concerning chemical reactions, surface properties as well as interactions between the electrodes and the electrolyte. Other very useful tools that may be employed for quantifying electron transfer processes and their time domains are intensity modulated photocurrent spectroscopy (IMPS) and intensity modulated photovoltage spectroscopy (IMVS). IMPS permits the generation of time-resolved plots of particular photo-processes in the system, each of which may be specifically addressed through varying the excitation wavelength. For the IMPS technique a sinusoidal wave with a small amplitude is applied, analogous to that of electrochemical impedance spectroscopy, but in this case the modulation is applied to a light source and not to the electrochemical cell as in EIS.[35] The current response is associated with the photogenerated charge carriers which flow through the system and finally discharge into the circuit. The amount of generated and discharged charge carriers is often different due to the presence of recombination and capture processes in surface or trap states. Ultimately the phase shift and magnitude of these currents reveal the kinetics of such processes. The only processes that will be addressed will be those that occur in the same frequency domain or on the same time scale as that of the modulated frequency of the illuminated light. In the literature some explanation of the kinetics of simple systems can be found and basic theories and introductive disquisitions may be found elsewhere.[36–38] Furthermore in solar cell research a multiplicity of studies are available which give an account of IMPS measurements on TiO2 nanoporous structures. Such studies permitted proof for the electron trapping and detrapping mechanism in TiO2 surface states.[39,40] An analysis of TiO2 electrodes combined with a dye sensitization step was established in the work of Peter and Ponomarev.[41–43] Hickey et.al.[44,45] have previously published kinetic studies on CdS nanoparticle (NP) modified electrodes. A theory was presented which allows for the IMPS data to be the interpreted in the case of CdS NP based electrodes. The back transfer, recombination and surface states have been demonstrated to be important as was determined from their inclusion in the theory. Similar attempts to explain the kinetics of CdS quantum dots are described by Bakkers et.al.[46]. In the present work the most important questions concern the behaviour of the photovoltaic assembly. Such assemblies can be equated with an electrode in contact with an electrolyte. Preliminary remarks about such electrodes as components of an electrochemical cell will be introduced in the first part of chapter 2. Thereafter the properties of electrodes in contact with the electrolyte and under illuminated conditions are illustrated. This is followed by a description of the important electrochemical and opto-electrochemical methods which have been employed in these studies. In particular, two separate subsections are dedicated to the methods of EIS and IMPS and the experimental section which are then linked to the theoretical section. The synthesis of all substances used and the preparation of the solar cell substrates are also dealt with in this section as will the equipment used and the instrument settings employed. The optical response of the working photoactive electrode is not only dependent on the substances used but also on their arrangement and linkage. The substrate which was employed in chapter 3 consists of a nanoporous ZnO gel layer upon which an organic linker has been placed in order to connect the oxide layer with the light absorbing component, the PbS NPs. Chapter 3 deals with the linker dependence on the ZnO layer and reports the typical optical characteristics and assembly arrangements of six different linkers on the ZnO layer which is an important intermediate stage in the fabrication of an ISC. The questions concerning how the type of linking affects the photo response and other electrochemical interactions of the complete solar cell substrate will be outlined in chapter 4. Further an examination of the electrochemical and opto-electrochemical behaviours of the samples will be presented similar to that presented in chapter 3. The most interesting substrate resulting from the investigations as described in chapter 3 and 4 will be used for a more in-depth characterisation by EIS in chapter 5. A suitable model and the results of the calculation of the ISC and the intermediate stages will be presented. The potential dependence, the dependence on the illuminated wavelength and also the size dependence of the PbS nanoparticles will be discussed. It will be revealed that ZnO is chemically unstable in contact with some of the linkers. For that reason the same linker study has been repeated with the more stable TiO2 employed as the wide band metal oxide. Comparisons between the different semiconductor metal oxides are made in chapter 6. In addition a number of open questions which previously had remained unanswered due to the instability of the ZnO can now be answered. In chapter 7 another highly porous structure different from that of the ZnO gel structure has been studied to determine its suitability as an ISC substrate. The structure arises from the electrodeposition of a ZnO reactant in the presence of eosin Y dye molecules. In the end the desorption of the dye provides a substrate with a high degree of porosity. Compared to the ZnO gel which was prepared and used for measurements in chapter 3 and 4, the electrodeposited ZnO is of a higher crystallinity and possesses a more preferential orientation. This results in a lower amount of grain boundaries which in turn results in fewer trap processes and subsequently yields a higher effective diffusion of the electron through the layer.[47,48] Optical and (opto-)electrochemical methods have been used for the basic characterisation of the untreated ZnO/Eosin Y and all other materials used in the fabrication of the ISC and a comparison with the ZnO gel used in chapter 3 and 4 will be made. Finally in chapter 8 an alternative metal oxide structure will be discussed. The background to this last chapter is to examine the influence of the ISC where the oxidic layer is present as a highly periodic arrangement, known as a photonic crystal. The TiO2 metal oxide which was also used in chapter 6 has been structured to form an inverse opal. First preparative findings and the first illustration of the (opto-)electrochemical results are presented. Consequently suggestions for improvements will be made. It is envisaged that the information gathered and presented here will help to achieve a deeper understanding of solar cells and help to improve the device efficiency and the interplay of the materials. Elementary understanding paves the way for further developments which can also contribute to providing devices for more efficient energy conversion.

Grätzel cells are liquid-electrolyte photoelectrochemical cells that contain dyesensitised titania electrodes. The sensitiser is typically an organic species that absorbs visible light and increases the spectral region in which Grätzel cells may produce electricity. A key feature in the success of Grätzel cells is the high surface area of nanostructured titania electrodes. In this study, the nanostructuring of titania has been explored by two complementary methods: templation and self-assembly. The templation of silica colloidal crystals (opals) was chosen as an inverse opal of titania would display a porous, bicontinuous structure in addition to a photonic bandgap. A diverse variety of titania inverse opals was produced, ranging from ideal ‘honeycomb’ to non-ideal ‘grape-like’ morphologies. However, the fragility of the material and difficulties in reproduction meant that the testing of such electrodes within Grätzel cells was limited. Study towards the formation of a nanoparticle superlattice of titania via chemically assisted self-assembly involved the investigation of both nanostructured titania surfaces and dye adsorption. The mode of dye binding to titania and the stability of adsorbed dyes was studied to aid work toward the design of a self-assembled titania superlattice, as well as to assist in the analysis of dye performance in Grätzel cells. Crystalline, aggregated titania and amorphous, dispersible titania was produced for dye binding studies of small organic carboxylic acid dyes. It was found that while dyes are adsorbed and intimately associated with titania, the mode of dye binding is different on a dry electrode than upon dispersed and solvated titania. The dyes appear to be bound to titania in a carboxylate form in the dry state, but in a mode that closer resembles that of the native dye upon dispersed titania.

In the latter half of the 20th century the first active environmentalist movements such as Greenpeace and the International Energy Agency were born and initiated a gradual rethinking of environmental awareness. Against all expectations the sole agency under international law for climate protection policy, called the United Nations Framework Convention on Climate Change, was formed 20 years later. Today the awareness of sustained, regenerative and environmental policies permeates throughout all areas of life, science and industry. But energy provision is the most decisive topic, especially since the discussions concerning the phase out of nuclear power where the voices calling for alternative energy sources have become much more vociferous. In addition the depletion of fossil fuels is expected to occur in the not too distant future. All new energy generation methods are required to meet the present and future energy demands, need to be ecological and need to exhibit the same or significantly lower cost expenditure than current energy sources. Unfortunately mankind is confronted with the problem that current commercial alternative energies are more expensive and not yet remotely as efficient as the present energy sources. Although energy provision based on water, wind, sun and geothermal sources have a huge potential because of their continuous presence, unfortunately, they are plagued by inefficient energy conversion caused by the state of technology i.e. the conversion of sun light into electricity loses energy through heat emission, reflection of the sun light, the inability of the material to absorb the entire sun spectrum and the ohmic losses in the transmission of electric current. The sun power is the most exhaustless resource and moreover through photovoltaic action, one of the most direct and cleanest source for use in energy conversion. Presently incoming sun light is not transformed in its entirely, as much degradation occurs during photon absorption and electron transfer processes. A number of other innovative possibilities have also been researched. With respect to cost and efficiency one of the most promising devices is injection solar cells (ISC). By dint of the dye sensitised solar cell (DSSC) Grätzels findings provided the foundations for much research into this type of solar cell where the light absorbing molecule employed in is a dye.[1] The current is obtained through charge separation in the dye, which is initiated through the connection between the dye and a metal oxide on the one hand and a matched redox couple on the other. In a variant of the DSSC the charge separation processes can also occur between a nanoporous metal oxide and nanoparticles giving rise to a quantum dot sensitised solar cell (QDSSC).[2] The use of nanoparticle (NP) properties can be utilized for the harvesting of solar energy, as demonstrated by Kamat and coworkers[3] who were able to exploit these findings subsequently and prepare a number of nanoparticle based solar cells. Nanoparticle research has comprised a wide field of science and nanotechnology for a number of years. As the size of a material approaches dimensions on the nm scale the surface properties contribute proportionally more to the sum of the properties than the volume due to the increase in the surface to volume ratio. These dimensions also constitute a threshold in which quantum physical effects need to be taken into account. Hence the properties of devices or materials in this size regime are inevitably size dependent. The basic principles can be described by two different theories, one of which is based on molecular orbital theory in which the particle is treated as a molecule. For this reason n atomic orbitals with the same symmetry and energy can build up n molecular orbitals through their linear combination based on the LCAO method (Linear Combination of Atomic Orbitals).[4] In the case of solids the orbitals build up energy bands, where the unoccupied states form the quasi continous conduction band (CB) and the occuppied states form the quasi continous valence band (VB). The energy \"forbidden\" area in between these two bands is called the band gap. The band gap is a fixed material property for bulk solids but depends on size in the case of the nanoparticles. In contrast to the LCAO method, simplified solid state theory will be used throughout the present work, the theoretical background of which is provided by the effective mass approximation.[5] When an absorption of a photon occurs, an exciton (electron-hole pair) can be generated. By promoting an electron (e-) from the valence band into the conduction band a hole (h+) may be said to remain in the valence band. By comparison to bulk solids, in a small particle the free charges can sense the potential barrier i.e. the edges of the nanoparticle. Analogous to the particle in a box model this potential barrier interaction results in an increase in the band gap as the particle size decreases. In a solar cell NPs with a particle size which possess a band gap energy in the near infrared (NIR) may be utilised and therefore the NPs will be able to absorb in this spectral region. However NPs also have the ability to absorb higher energy photons due to the continuum present in their band structure, so that almost the entire sun spectral range from the NIR up to UV wavelengths may be absorbed just by using the appropriate NP material and size. Suitable NPs are metal chalcogenides e.g. MX (where M = cadmium, zinc or lead and X = sulfur, selenium or tellurium) because of their bandgap size[6–10] and their relative band positions compared to those of the semiconductor oxide states. Both the TiO2/CdSe[11–14] and TiO2/CdTe[15–18] systems have already been successfully fabricated and many of the anomalies reported.[3] Much interest in the lead chalcogenides has been generated by reports that they may feature the possibility to exhibit multiple exciton generation (MEG) where the absorption of one high energy photon can result in more than one electron-hole pairs.[19–25] Currently electrochemical impedance spectroscopy (EIS) is being used more and more to clarify processes at polarisable surfaces and materials such as nanoparticles. Likewise this method has been rediscovered in photovoltaic research and its use in the characterisation of DSSCs has been discussed in the literature.[26–31] In a number of publications the evaluation of nanoporous and porous structures has been quite extensively explored.[28,29,32–34] Since the mid-20th century Jaffé’s[35] theoretical work concerning the steady- state ac response of solid and liquid systems lead to the formation of the basics of EIS. Further developments in the measurement technology have lead to a broader range of analysis becoming possible. Nevertheless the most challenging part still remains the interpretation of the results and especially to merge the measured data with the theoretical model. EIS quantifies the changes in a small ac current response at electrode electrolyte interfaces i.e. the rate at which the polarized domain will respond, when an ac potential is applied. In this way dielectric properties of materials or composites, such as charge transfers, polarization effects, charge recombination and limitations can be measured as a function of frequency and mechanistic information may be unveiled. Hence EIS allows one to draw a conclusion concerning chemical reactions, surface properties as well as interactions between the electrodes and the electrolyte. Other very useful tools that may be employed for quantifying electron transfer processes and their time domains are intensity modulated photocurrent spectroscopy (IMPS) and intensity modulated photovoltage spectroscopy (IMVS). IMPS permits the generation of time-resolved plots of particular photo-processes in the system, each of which may be specifically addressed through varying the excitation wavelength. For the IMPS technique a sinusoidal wave with a small amplitude is applied, analogous to that of electrochemical impedance spectroscopy, but in this case the modulation is applied to a light source and not to the electrochemical cell as in EIS.[35] The current response is associated with the photogenerated charge carriers which flow through the system and finally discharge into the circuit. The amount of generated and discharged charge carriers is often different due to the presence of recombination and capture processes in surface or trap states. Ultimately the phase shift and magnitude of these currents reveal the kinetics of such processes. The only processes that will be addressed will be those that occur in the same frequency domain or on the same time scale as that of the modulated frequency of the illuminated light. In the literature some explanation of the kinetics of simple systems can be found and basic theories and introductive disquisitions may be found elsewhere.[36–38] Furthermore in solar cell research a multiplicity of studies are available which give an account of IMPS measurements on TiO2 nanoporous structures. Such studies permitted proof for the electron trapping and detrapping mechanism in TiO2 surface states.[39,40] An analysis of TiO2 electrodes combined with a dye sensitization step was established in the work of Peter and Ponomarev.[41–43] Hickey et.al.[44,45] have previously published kinetic studies on CdS nanoparticle (NP) modified electrodes. A theory was presented which allows for the IMPS data to be the interpreted in the case of CdS NP based electrodes. The back transfer, recombination and surface states have been demonstrated to be important as was determined from their inclusion in the theory. Similar attempts to explain the kinetics of CdS quantum dots are described by Bakkers et.al.[46]. In the present work the most important questions concern the behaviour of the photovoltaic assembly. Such assemblies can be equated with an electrode in contact with an electrolyte. Preliminary remarks about such electrodes as components of an electrochemical cell will be introduced in the first part of chapter 2. Thereafter the properties of electrodes in contact with the electrolyte and under illuminated conditions are illustrated. This is followed by a description of the important electrochemical and opto-electrochemical methods which have been employed in these studies. In particular, two separate subsections are dedicated to the methods of EIS and IMPS and the experimental section which are then linked to the theoretical section. The synthesis of all substances used and the preparation of the solar cell substrates are also dealt with in this section as will the equipment used and the instrument settings employed. The optical response of the working photoactive electrode is not only dependent on the substances used but also on their arrangement and linkage. The substrate which was employed in chapter 3 consists of a nanoporous ZnO gel layer upon which an organic linker has been placed in order to connect the oxide layer with the light absorbing component, the PbS NPs. Chapter 3 deals with the linker dependence on the ZnO layer and reports the typical optical characteristics and assembly arrangements of six different linkers on the ZnO layer which is an important intermediate stage in the fabrication of an ISC. The questions concerning how the type of linking affects the photo response and other electrochemical interactions of the complete solar cell substrate will be outlined in chapter 4. Further an examination of the electrochemical and opto-electrochemical behaviours of the samples will be presented similar to that presented in chapter 3. The most interesting substrate resulting from the investigations as described in chapter 3 and 4 will be used for a more in-depth characterisation by EIS in chapter 5. A suitable model and the results of the calculation of the ISC and the intermediate stages will be presented. The potential dependence, the dependence on the illuminated wavelength and also the size dependence of the PbS nanoparticles will be discussed. It will be revealed that ZnO is chemically unstable in contact with some of the linkers. For that reason the same linker study has been repeated with the more stable TiO2 employed as the wide band metal oxide. Comparisons between the different semiconductor metal oxides are made in chapter 6. In addition a number of open questions which previously had remained unanswered due to the instability of the ZnO can now be answered. In chapter 7 another highly porous structure different from that of the ZnO gel structure has been studied to determine its suitability as an ISC substrate. The structure arises from the electrodeposition of a ZnO reactant in the presence of eosin Y dye molecules. In the end the desorption of the dye provides a substrate with a high degree of porosity. Compared to the ZnO gel which was prepared and used for measurements in chapter 3 and 4, the electrodeposited ZnO is of a higher crystallinity and possesses a more preferential orientation. This results in a lower amount of grain boundaries which in turn results in fewer trap processes and subsequently yields a higher effective diffusion of the electron through the layer.[47,48] Optical and (opto-)electrochemical methods have been used for the basic characterisation of the untreated ZnO/Eosin Y and all other materials used in the fabrication of the ISC and a comparison with the ZnO gel used in chapter 3 and 4 will be made. Finally in chapter 8 an alternative metal oxide structure will be discussed. The background to this last chapter is to examine the influence of the ISC where the oxidic layer is present as a highly periodic arrangement, known as a photonic crystal. The TiO2 metal oxide which was also used in chapter 6 has been structured to form an inverse opal. First preparative findings and the first illustration of the (opto-)electrochemical results are presented. Consequently suggestions for improvements will be made. It is envisaged that the information gathered and presented here will help to achieve a deeper understanding of solar cells and help to improve the device efficiency and the interplay of the materials. Elementary understanding paves the way for further developments which can also contribute to providing devices for more efficient energy conversion.:Contents List of Abbreviations vii Legend of Symbols ix 1 Introduction and Motivation 1 2 Theoretical and Experimental Introduction 7 2.1 Basics of the (Opto-)Electrochemistry . . . . . . . . . . . . . . . . 7 2.1.1 Electrode-Electrolyte Interface Non-Illuminated . . . . . . 8 2.1.2 Electrode-Electrolyte Interface Under Illumination . . . . . 10 2.1.3 The Processes in the Injection Solar Cell (ISC) . . . . . . . 12 2.1.4 Cyclic Voltammetry (CV) . . . . . . . . . . . . . . . . . . 15 2.1.5 Chronoamperometry (CA) . . . . . . . . . . . . . . . . . . 16 2.1.6 Incident Photon to Current Conversion Efficiency (IPCE) . 16 2.1.7 Electrochemical Impedance Spectroscopy (EIS) . . . . . . 17 2.1.8 Intensity Modulated Photocurrent Spectroscopy (IMPS) . 21 2.2 Experimental . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 23 2.2.1 Synthesis of ZnO Sol-Gel . . . . . . . . . . . . . . . . . . . 23 2.2.2 Synthesis of TiO2 Sol-Gel . . . . . . . . . . . . . . . . . . 24 2.2.3 Preparation of the ZnO/Eosin Y Substrate . . . . . . . . . 24 2.2.4 Syntheses and Preparation of the Inverse Opal . . . . . . . 25 2.2.5 The Syntheses for PbS Nanoparticle . . . . . . . . . . . . . 26 2.2.6 Preparation of the PbS Coated Substrates . . . . . . . . . 30 2.2.7 Preparation of the ISC . . . . . . . . . . . . . . . . . . . . 31 2.2.8 Material Characterisations and Instrument Settings . . . . 33 3 The Linker Attachment on a ITO/ZnO Substrate 37 3.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 37 3.2 The ITO/ZnO Film . . . . . . . . . . . . . . . . . . . . . . . . . . 40 3.2.1 The ZnO Layer and the ITO/ZnO Substrate Preparation . 40 3.2.2 The ZnO Structure as a Function of the Sintering Temperature . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 43 3.3 The Linker on the ITO/ZnO Film . . . . . . . . . . . . . . . . . . 48 3.3.1 The Linker Orientation on the ZnO layer . . . . . . . . . . 48 3.3.2 The Linker Interaction with the ZnO Gel . . . . . . . . . . 52 3.4 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 57 4 The PbS Sensitized ITO/ZnO/linker Substrate 59 4.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 59 4.2 The ITO/ZnO/Linker/PbS Substrate . . . . . . . . . . . . . . . . 61 4.2.1 Spectroscopic Evidence for PbS on the ITO/ZnO/Linker Substrate . . . . . . . . . . . . . . . . . . . . . . . . . . . 61 4.2.2 The Cyclic Voltammetry Study on the Substrates . . . . . 63 4.2.3 The Opto-Electrochemistry on the Substrates . . . . . . . 70 4.3 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 73 5 The EIS Study of the ITO/ZnO/MPA/PbS Substrate 75 5.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 75 5.2 The Substrate Assembly . . . . . . . . . . . . . . . . . . . . . . . 77 5.3 The Substrate Characteristics . . . . . . . . . . . . . . . . . . . . 78 5.4 The Model for the EIS Analysis . . . . . . . . . . . . . . . . . . . 83 5.5 The Results of EIS Data Fitting . . . . . . . . . . . . . . . . . . . 86 5.5.1 The EIS Results of the FTO/ZnO Substrate . . . . . . . . 86 5.5.2 The EIS Results of the FTO/ZnO/MPA Substrate . . . . 89 5.5.3 The EIS Results of the FTO/ZnO/MPA/PbS Substrate . . 92 5.5.4 The EIS Results for Shorter Illumination Wavelength . . . 96 5.5.5 The Resistance of the Linker . . . . . . . . . . . . . . . . . 111 5.6 General Remarks on the Modelling . . . . . . . . . . . . . . . . . 112 5.7 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 115 6 TiO2 based Injection solar Cell 119 6.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 119 6.2 The ITO/TiO2 Film . . . . . . . . . . . . . . . . . . . . . . . . . 121 6.3 The Linker and PbS Attachment on the ITO/TiO2 Substrate . . . 123 6.4 The Cyclic Voltammetry Study on the Substrates . . . . . . . . . 125 6.4.1 The Linker Sensitized ITO/TiO2 Film . . . . . . . . . . . 125 6.4.2 The ITO/TiO2/Linker/PbS Substrate . . . . . . . . . . . 126 6.5 The Opto-Electrochemistry on the Substrates . . . . . . . . . . . 127 6.6 Comparison Between ZnO and TiO2 Based ISCs . . . . . . . . . . 129 6.7 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 133 7 ZnO-Eosin Y based Injection Solar Cell 135 7.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 135 7.2 The FTO/ZnO-Ey Film . . . . . . . . . . . . . . . . . . . . . . . 137 7.3 The PbS Attachment to the FTO/ZnO-Ey Film . . . . . . . . . . 137 7.4 The Cyclic Voltammetry Study on the Substrates . . . . . . . . . 140 7.5 The Opto-Electrochemistry on the Substrates . . . . . . . . . . . 142 7.5.1 The Linear Sweep Voltammetry (LSV) Study on the Substrates . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 142 7.5.2 The IPCE Measurements on the Substrates . . . . . . . . 144 7.5.3 The Photo Transient Measurements on the Substrates . . . 145 7.6 Comparison between ZnO and ZnO-Ey based ISC . . . . . . . . . 146 7.7 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 148 8 Injection Solar Cell meets Photonic Crystal 151 8.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 151 8.2 The Opal . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 153 8.3 The Inverse Opal . . . . . . . . . . . . . . . . . . . . . . . . . . . 156 8.4 The Inverse Opal based ISC . . . . . . . . . . . . . . . . . . . . . 159 8.4.1 The Substrate Characteristics . . . . . . . . . . . . . . . . 159 8.4.2 The Cyclic Voltammetry . . . . . . . . . . . . . . . . . . . 160 8.4.3 The Opto-Electrochemistry . . . . . . . . . . . . . . . . . 161 8.4.4 The EIS Measurements . . . . . . . . . . . . . . . . . . . . 163 8.5 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 165 9 Overall Conclusion 167 10 Outlook 173 Bibliography I A Acknowledgement XXV B Erklärung XXVII