Chemical bath deposition (CBD) is the analog in liquid phase of the well-known chemical vapor deposition technique in the vapor phase. In CBD, deposition of thin films takes place from aqueous solutions at low temperatures by a chemical reaction between dissolved precursors, with the help of a complexing agent. Among all techniques used to grow Group II-VI semiconductors, CBD has the advantage of being a simple, low temperature, and inexpensive large-area deposition technique. So far, its contribution in thin film solar cells industry has been mainly limited to growing n-type CdS and/or ZnS window layers for CdTe-based and CIGS-based solar cells. In this work we first optimize the CBD process of CdS using nitrilotriacetic acid and hydrazine as complexing agents as an alternative to ammonia. We then study the effect of the cadmium precursor on the optical/electrical properties, as well as crystal structure, morphology, and composition of CBD-CdS films. A better understanding of the CBD process of CdS as a whole has been achieved and high quality CBD-CdS films have been obtained. Next, we investigate in-situ doping of CBD-CdS with group III elements, such as B, Al, In, and Ga. The objective is to show that CBD is capable of not only growing CdS but also of doping it to reduce its resistivity and, as a result, facilitate its use in solar cells as well as other optoelectronic device fabrication. A four orders of magnitude drop of film resistivity has been achieved without a significant change in film bandgap, structure, or morphology. Finally, we test the possibility of using CBD to grow transparent conducting oxide (TCO) films, such as Al-doped ZnO films and cadmium stannate films. First, we study CBD of ZnO and later in-situ doping of ZnO using Al. High quality ZnO thin films have been grown using CBD with the help of four different complexing agents. Post heat treatment in argon ambient helped reduce resistivity of CBD-ZnO undoped films to ~ 10-1 Ω-cm. In-situ doping of such films using Al shows promising results. Such films could be an alternative to indium tin oxide (ITO) layers that are commonly used as TCO layers for solar cells. Another approach is to use CBD to grow CdO and SnO2 thin films, with the goal of obtaining Cd2SnO4 by later annealing of these two layers. Cadmium stannate is another TCO candidate that could replace ITO in the near future. We have succeeded in growing CBD-CdO thin films using three different complexing agents. Undoped CBD-CdO films with a resistivity as low as 1.01 x10-2 Ω-cm and a carrier density as high as 2.59 x 1020 cm-3 have been obtained. SnO2 films have been successfully grown using CBD. Fabrication of Cadmium stannate thin films using CBD is investigated. In summary, our objective to expand the use of CBD beyond just growing CdS and ZnS, and to test the possibility of using it for in-situ doping of group II-VI semiconductors as well as TCO layers fabrication proved to be successful. We believe that this may have a significant impact on solar cells as well as other optoelectronic devices fabrication industry, due to the simplicity and the cost-effectiveness of CBD.

This thesis describes the development of a fast rate method for the deposition of high quality CdS and CdTe thin films. The technique uses Pulsed DC Magnetron Sputtering (PDCMS). Surprisingly, the technique produces highly stable process conditions. CREST is the first laboratory worldwide to show that pulsed DC power may be used to deposit CdS and CdTe thin films. This is a very promising process technology with potential for eventual industrial deployment. The major advantage is that the process produces high deposition rates suitable for use in solar module manufacturing. These rates are over an order of magnitude faster than those obtained by RF sputtering. In common with other applications it has also been found that the energetics of the pulsed DC process produce excellent thin film properties and the power supply configuration avoids the need for complex matching circuits. Conventional deposition methodologies for CdS, Chemical Bath Deposition (CBD) and CdTe thin films, Electrodeposition (ED), have been chosen as baselines to compare film properties with Pulsed DC Magnetron Sputtering (PDCMS). One of the issues encountered with the deposition of CdS thin films (window layers) was the presence of pinholes. A Plasma cleaning process of FTO-coated glass prior to the deposition of the CdS/CdTe solar cell has been developed. It strongly modifies and activates the TCO surface, and improves the density and compactness of the deposited CdS thin film. This, in turn, improves the optical and morphological properties of the deposited CdS thin films, resulting in a higher refractive index. The pinhole removal and the increased density allows the use of a much thinner CdS layer, and this reduces absorption of blue spectrum photons and thereby increases the photocurrent and the efficiency of the thin film CdTe cell. Replacing the conventional magnetic stirrer with an ultrasonic probe in the chemical bath (sonoCBD) was found to result in CdS films with higher optical density, higher refractive index, pinhole and void-free, more compact and uniform along the surface and through the thickness of the deposited material. PDCMS at 150 kHz, 500 W, 2.5 μs, 2 s, results in a highly stable process with no plasma arcing. It allows close control of film thickness using time only. The CdS films exhibited a high level of texture in the <001> direction. The grain size was typically ~50 nm. Pinholes and voids could be avoided by reducing the working gas pressure using gas flows ii below 20 sccm. The deposition rate was measured to be 1.33 nm/s on a rotating substrate holder. The equivalent deposition rate for a static substrate is 8.66 nm/s, which is high and much faster than can be achieved using a chemical bath deposition or RF magnetron sputtering. The transmission of CdS can be improved by engineering the band gap of the CdS layer. It has been shown that by adding oxygen to the working gas pressure in an RF sputtering deposition process it is possible to deposit an oxygenated CdS (CdS:O) layer with an improved band gap. In this thesis, oxygenated CdS films for CdTe TF-PV applications have been successfully deposited by using pulsed DC magnetron sputtering. The process is highly stable using a pulse frequency of 150 kHz and a 2.5 μs pulse reverse time. No plasma arcing was detected. A range of CdS:O films were deposited by using O2 flows from 1 sccm to 10 sccm during the deposition process. The deposition rates achieved using pulsed DC magnetron sputtering with only 500 W of power to the magnetron target were in the range ~1.49 nm/s ~2.44 nm/s, depending on the oxygen flow rate used. The properties of CdS thin films deposited by pulsed DC magnetron sputtering and chemical bath deposition have been studied and compared. The pulsed DC magnetron sputtering process produced CdS thin films with the preferred hexagonal <001> oriented crystalline structure with a columnar grain growth, while sonoCBD deposited films were polycrystalline with a cubic structure and small grainy crystallites throughout the thickness of the films. Examination of the PDCMS deposited CdS films confirmed the increased grain size, increased density, and higher crystallinity compared to the sonoCBD CdS films. The deposition rate for CdS obtained using pulsed DC magnetron sputtering was 2.86 nm/s using only 500 W power on a six inch circular target compared to the much slower (0.027 nm/s) for the sonoChemical bath deposited layers. CdTe thin films were grown on CdS films prepared by sonoCBD and Pulsed DC magnetron sputtering. The results showed that the deposition technique used for the CdS layer affected the growth and properties of the CdTe film and also determined the deposition rate of CdTe, being 3 times faster on the sputtered CdS. PDCMS CdTe layers were deposited at ambient temperature, 500 W, 2.9 μs, 10 s, 150 kHz, with a thickness of approximately 2 μm on CdS/TEC10 coated glass. The layers appear iii uniform and smooth with a grain size less than 100 nm, highly compact with the morphology dominated by columnar grain growth. Stress analysis was performed on the CdTe layers deposited at room temperature using different gas flows. Magnetron sputtered thin films deposited under low gas pressure are often subject to compressive stress due to the high mobility of the atoms during the deposition process. A possible way to reduce the stress in the film is the post-deposition annealing treatment. As the lattice parameter increased; the stress in the film is relieved. Also, a changing the deposition substrate temperature had an effect on the microstructure of CdTe thin films. Increasing the deposition temperature increased the grain size, up to ~600 nm. CdTe thin films with low stress have been deposited on CdS/TEC10 coated glass by setting the deposition substrate temperature at ~200°C and using high argon flows ~ 70 sccm Ar. Finally, broadband multilayer ARCs using alternate high and low refractive index dielectric thin films have been developed to improve the light transmission into solar cell devices by reducing the reflection of the glass in the extended wavelength range utilised by thin-film CdTe devices. A four-layer multilayer stack has been designed and tested, which operates across the wavelength range used by thin-film CdTe PV devices (400 850 nm). Optical modelling predicts that the MAR coating reduces the WAR (400-850 nm) from the glass surface from 4.22% down to 1.22%. The application of the MAR coating on a thin-film CdTe solar cell increased the efficiency from 10.55% to 10.93% or by 0.38% in absolute terms. This is a useful 3.6% relative increase in efficiency. The increased light transmission leads to improvement of the short-circuit current density produced by the cell by 0.65 mA/cm2. The MAR sputtering process developed in this work is capable of scaling to an industrial level.

Le développement d’architectures nanostructurées originales composées de matériaux abondants et non-toxiques fait l’objet d’un fort intérêt de la communauté scientifique pour la fabrication de dispositifs fonctionnels efficaces et à bas coût suivant des méthodes d’élaborations faciles à mettre en œuvre. Les réseaux de nanofils de ZnO élaborés par dépôt en bain chimique sont, à ce titre, extrêmement prometteurs. L’étude des propriétés de ces réseaux de nanofils et leur intégration efficace au sein de dispositifs nécessitent toutefois un contrôle avancé de leurs propriétés structurales et physiques, notamment en terme de polarité, à l’aide de techniques de lithographies avancées.Le dépôt en bain chimique des nanofils de ZnO est d’abord effectué sur des monocristaux de ZnO de polarité O et Zn préparés par lithographie assistée par faisceau d’électrons. Par cette approche de croissance localisée, un effet significatif de la polarité des nanofils de ZnO est mis en évidence sur le mécanisme de croissance des nanofils, ainsi que sur leurs propriétés électriques et optiques. La possibilité de former des nanofils de ZnO sur des monocristaux de ZnO semipolaires nous a de plus permis d’affiner la compréhension de leurs mécanismes de croissance sur les couches d’amorces polycristallines de ZnO. Par la suite, le dépôt des nanofils de ZnO en bain chimique est développé sur des couches d’amorces polycristallines de ZnO préparés à l’aide de la lithographie assistée par nano-impression. Suivant cette approche, des réseaux de nanofils de ZnO localisés sont formées sur de grandes surfaces, ce qui permet d’envisager leur intégration future au sein de dispositifs fonctionnels.Les nanofils de ZnO sont ensuite combinés avec des coquilles semiconductrices de type p par des méthodes de dépôt chimique en phase liquide ou en phase vapeur afin de fabriquer des hétérostructures cœurs-coquilles originales. Le dépôt de couches successives par adsorption et réaction (SILAR) d’une coquille absorbante de SnS de phase cubique est optimisé sur des nanofils de ZnO recouverts d’une fine couche protectrice de TiO2, ouvrant la voie à la fabrication de cellules solaires à absorbeur extrêmement mince. Enfin, un photo-détecteur UV autoalimenté prometteur, présentant d’excellentes performances en termes de réponse spectrale et de temps de réponse, est réalisé par le dépôt chimique en phase vapeur d’une coquille de CuCrO2 sur les nanofils de ZnO. / Over the past decade, the development of novel nanostructured architectures has raised increasing interest within the scientific community in order to meet the demand for low-cost and efficient functional devices composed of abundant and non-toxic materials. A promising path is to use ZnO nanowires grown by chemical bath deposition as building blocks for these next generation functional devices. However, the precise control of the ZnO nanowires structural uniformity and the investigation of their physical properties, particularly in terms of polarity, remain key technological challenges for their efficient integration into functional devices.During this PhD, the chemical bath deposition of ZnO nanowires is combined with electron beam lithography prepared ZnO single crystal substrates of O- and Zn-polarity following the selective area growth approach. The significant effects of polarity on the growth mechanism of ZnO nanowires, as well as on their electrical and optical properties, are highlighted by precisely investigating the resulting well-ordered O- and Zn-polar ZnO nanowire arrays. An alternative nano-imprint lithography technique is subsequently used to grow well-ordered ZnO nanowire arrays over large areas on various polycrystalline ZnO seed layers, thus paving the way for their future integration into devices. We also demonstrate the possibility to form ZnO nanowires by chemical bath deposition on original semipolar ZnO single crystal substrates. These findings allowed a comprehensive understanding of the nucleation and growth mechanisms of ZnO nanowires on polycrystalline ZnO seed layers.In a device perspective, the ZnO nanowires are subsequently combined with p type semiconducting shells by liquid and vapor chemical deposition techniques to form original core-shell heterostructures. The formation of a cubic phase SnS absorbing shell is optimized by the successive ionic layer adsorption and reaction (SILAR) process on ZnO nanowire arrays coated with a thin protective TiO2 shell, which pave the way for their integration into extremely thin absorber solar cells. A self-powered UV photo-detector with fast response and state of the art performances is also achieved by the chemical vapor deposition of a CuCrO2 shell on ZnO nanowire arrays.

Le présent travail porte sur l'élaboration de couches minces du matériau binaire SnS avec des propriétés physico-chimiques répondant le mieux possible aux exigences d'une bonne alternative au composé ternaire CuInS2, dans les cellules solaires. Nous avons utilisé la technique de dépôt chimique en solution (ou Chemical Bath Deposition CBD) qui est une technique peu coûteuse, non toxique et facile à manipuler. Les couches fabriquées sont testées sur le plan cristallographique, chimique, morphologique et optique à différentes échelles, en utilisant les techniques de diffraction des rayons X, de profilométrie, de microscopie électronique à balayage associée à la dispersion en énergie des photons X, de microscopie à force atomique ou électrostatique, et de mesures par spectrophotométrie. Des recuits à différentes températures et des dopages à différentes concentrations sont effectués. Un calcul de l'épaisseur des films minces de SnS, basé sur la méthode des enveloppes des franges d'interférences dans les spectres de transmission optique calculés et expérimentaux, a été effectué à l'aide d'une modélisation utilisant les théories de Manifacier et de Heavens. / The present work deals with the fabrication of SnS thin films as a potential substitute to CuInS2 absorber material in thin film solar cells. The Chemical Bath Deposition method (CBD) is applied to this binary material, as it is non toxic and relatively inexpensive. Structural, chemical, morphological and optical properties of the fabricated layers are investigated by X-Ray diffraction, profilometry, scanning electron microscopy associated with energy dispersive spectrometry, atomic force microscopy, and visible to infrared spectrophotometry. Annealing and doping of the SnS thin layer is also investigated. Theoretical modelling of the thin film thickness is obtained from optical transmission and reflexion spectra based on the envelope of interference fringes.

Le présent travail s'articule autour de l'élaboration du matériau binaire In2S3 en couches minces en tant qu'alternative crédible au composé CdS, dans les cellules solaires à base de CuInS2. Nous avons utilisé la technique de dépôt chimique en solution (Chemical Bath Deposition ou CBD) qui est une technique non coûteuse, non toxique et facile à manipuler. Les couches fabriquées sont caractérisées de différents points de vue et à différentes échelles : caractérisations structurale par diffraction de rayons X (DRX), morphologique par Microscopie Electronique à Balayage (MEB), composition chimique par spectroscopie en dispersion d'énergie (EDS), propriétés optiques par spectrophotométrie, et électriques par la méthode du courant thermiquement stimulé (TSC) et par cartographie de courant localisé. L'objectif de ce travail est l'étude systématique des effets du dopage à l'aluminium et à l'étain, et du traitement thermique des films minces de In2S3 déposés sur verre et sur SnO2. Nous avons réalisé tout d'abord par CBD une multicouche d'In2S3 :4%Al formée par trois dépôts successifs sur des substrats verre et SnO2:F. La comparaison des caractéristiques physicochimiques est faite avec la couche non dopée en tant que caractéristiques de référence. L'étude par DRX faite pour différentes concentrations en Al, montre que ce binaire cristallise selon la structure cubique d'orientation préférentielle (400). Une meilleure cristallisation est obtenue pour une concentration en aluminium dans la solution y = [Al]/[In] = 4%. L'analyse optique montre que le gap est direct, il varie de 2,3 à 2,9 eV; la plus large bande optique est obtenue pour y = 4%. C'est une bonne valeur pour l'utilisation du composé β-In2-xAlxS3 comme fenêtre optique dans les dispositifs photovoltaïques. L'étude de l'effet du dopage à l'étain des multicouches d'In2S3, nous a permis de déduire qu'une meilleure cristallinité, une faible rugosité de la morphologie de surface et un gap optique plus proche de l'optimum théorique, sont obtenus pour des films croissants sur le substrat Pyrex avec une concentration d'étain égale à 2‰. L'analyse effectuée par MEB sur la tranche a montré que l'épaisseur moyenne des couches diminue avec l'augmentation de la concentration d'étain. La présence de l'étain, même en très petites quantités induit des changements importants dans le processus de croissance du film. L'étude TSC montre que l'augmentation de la concentration de l'étain au-delà 2 ‰ conduit à une diminution de courant thermiquement stimulé. Le recuit à différentes températures sous azote est appliqué aux couches dopées et non dopées étudiées précédemment. Le traitement thermique sous azote à 400°C provoque une augmentation nette de la taille des cristallites pour pratiquement tous les films minces dopés ou non dopés déposés sur verre ou sur SnO2. L'analyse par diffraction des rayons X a révélé une conversion de la phase cubique (400) à la phase tétragonale (109) pour l'In2S3:4%. Le changement de la forme des cristallites observé par AFM, met également en évidence l'existence d'une autre phase. Les analyses électriques par TSC montrent particulièrement le comportement électrique de type semiconducteur pour les films minces dopés à 4% Al, et recuit à 400°C, ainsi que pour les films minces dopés à l'étain après recuit à 200°C. L'analyse locale du courant de conduction dans la couche de In2S3 fait apparaître des inhomogénéités plus grandes après traitement thermique. Cependant les bons résultats macroscopiques permettent d'envisager sereinement la fabrication de cellules solaires incluant ces couches. / The present work focuses on the development of binary material In2S3 thin films as an alternative to CdS in thin film solar cells based on CuInS2. We used the technique of Chemical Bath Deposition (CBD) as it is non-expensive, non-toxic and easy to handle. Layers produced are characterized at different levels and scales: cristalline structure by X-ray diffraction (XRD), surface morphology by Scanning Electron Microscopy (SEM), chemical composition by energy dispersive spectroscopy (EDS), optical properties by spectrophotometry and electrical conduction by thermally stimulated currents (TSC) and local mapping of currents. The objective of this work is the systematic study of the effects of aluminum or tin doping, and heat treatment of In2S3 thin films deposited on glass and SnO2. We achieved first a multilayer of CBD In2S3:Al(4%) formed by three successive deposits on glass and SnO2 substrates. Comparison of physicochemical characteristics is made with the undoped layer as reference features. The XRD study done for different Al concentrations, shows that In2S3:Al crystallizes in the cubic structure with preferential orientation (400). Better crystallization is obtained for a concentration of aluminum in the solution y = [Al] / [In] = 4%. The analysis shows that the optical gap is direct, it varies from 2.3 to 2.9 eV, the largest optical band is obtained for y = 4%. It is a good value for the use of the compound β-In2-xAlxS3 as optical window in photovoltaic devices. The effect of tin doping in In2S3 multilayers induces a better crystallinity, low roughness of the surface morphology and optical gap closer to the theoretical optimum, obtained for films grown on Pyrex substrate with a tin concentration equal to 2 ‰. Analysis by SEM on the wafer cleaved-edge showed that the average thickness of the layers decreases with increasing the concentration of tin. The presence of tin, even in very small quantities induced significant changes in the growth process of the film. The TSC study shows that increasing concentration of tin beyond 2‰ leads to a reduction of thermally stimulated current.Annealing at different temperatures under nitrogen is applied to doped and undoped layers studied previously. Heat treatment under nitrogen at 400 ° C causes a net increase of crystallite size for virtually all thin films doped or undoped deposited on glass or SnO2. The analysis by XRD showed a conversion of the cubic phase (400) to the tetragonal phase (109) for In2S3:Al(4%). Change the shape of the crystallites observed by AFM, also highlights the existence of another phase. The TSC analyzes show particular electrical behavior close to semiconductor type for the thin films doped with 4% Al and annealed at 400°C, as well as thin films doped with tin after annealing at 200°C. The local analysis of the conduction current in the layer of In2S3 shows inhomogeneities larger after heat treatment. However, good macroscopic results should allow to fabricate promising solar cells incorporating these layers.

Les travaux présentés dans ce manuscrit traitent des mécanismes de croissance associés au dépôt de nanofils d’oxyde de zinc (ZnO) en bain chimique. Cette technique de croissance, attractive de par sa facilité de mise en œuvre et son coût limité, consiste à immerger un substrat dans une solution de précurseurs portée à basse température (typiquement 90°) pendant quelques heures. Le dépôt préalable d’une fine couche de ZnO fortement texturée est nécessaire à l’obtention de la morphologie nanofils et il est donc nécessaire de maîtriser le processus de croissance associé. Dans un souci de cohérence, la méthode sol-gel dite de trempage consistant à immerger le substrat dans une solution de précurseurs avant de recuire la couche ainsi déposée est ici adoptée. Le ZnO, sous sa morphologie nanofils, est actuellement fortement étudié du fait de son fort potentiel applicatif. Typiquement, il peut être utilisé en tant que brique de basse dans la réalisation de cellules solaires de types Grätzel ou à absorbeur extrêmement fin. Dans ce contexte, il est nécessaire que les nanostructures élaborées présentent des propriétés physiques attractives et ces dernières doivent donc être finement caractérisées. Dans un premier temps, l’influence des paramètres expérimentaux associés au processus de trempage sur les propriétés morphologiques et structurales de films minces de ZnO déposés via ce processus est quantifiée. Il est montré à cette occasion que dans des conditions extrêmes de recuits, les couches évoluent vers une morphologie de type fil. Fort des conclusions obtenues, les mécanismes régissant la croissance de nanofils de ZnO en bain chimique, et plus particulièrement l’influence de la surface de nucléation sur ces derniers, sont étudiés. La possibilité d’obtenir des nanofils localisés et parfaitement alignés à travers la réalisation de masques est démontrée. L’ensemble des nanostructures élaborées (couches et nanofils) sont caractérisées par photoluminescence afin de pouvoir estimer leur qualité structurelle et d’étudier les défauts en présence. Pour finir, une étude plus fondamentale consistant à suivre in situ l’évolution des nanofils au cours de la croissance par rayonnement synchrotron est proposée avec une attention toute particulière aux phénomènes de polarité. / ZnO nanowires are of strong interest in the realization of solar cells based on type-II band alignment. They can be grown by chemical bath deposition, a technique in which the substrate is seeded with ZnO nanoparticles by dip-coating and then placed in a precursor solution heated at 90°C for a couple of hours. In this document, we will discuss the nucleation and growth mechanisms associated with this low cost technique. In particular, we will see how the seed layer morphology can drive the one of the nanowires. Also, advanced characterization by photoluminescence and synchrotron radiation will be performed on the grown nanostructures.

Photoelectrodes and photovoltaic devices have been prepared via multiple thin film deposition methods. Aerosol assisted chemical vapour deposition (AACVD), electrodeposition (ED), chemical bath deposition (CBD) and doctor blade technique (DB) have been used to deposit binary and ternary metal oxide films on FTO glass substrates. The prepared thin films were characterised by a combination of SEM (Scanning Electron Microscopy), powder X-ray diffraction, mechanical strength tests and photochemical measurements. Nickel oxide (NiO) thin films prepared by AACVD were determined to have good mechanical strength . with a photocurrent of 7.6 μA cm-2 at 0 V and an onset potential of about 0.10 V. This contrasted with the dark current density of 0.3 μA cm-2 at 0 V. These NiO samples have very high porosity with crystalline columns evidenced by SEM. In comparison with the AACVD methodology, NiO films prepared using a combination of ED and DB show good mechanical strength but a higher photocurrent of 24 μA cm-2 at 0 V and an onset potential of about 0.10 V with a significantly greater dark current density of 7 μA cm-2 at 0 V. The characteristic features shown in the SEM are smaller pores compared to the AACVD method. Copper (II) oxide (CuO) and copper (I) oxide (Cu2O) films were fabricated by AACVD by varying the annealing temperature between 100-325°C in air using a fixed annealing time of 30 min. It was shown by photocurrent density (J-V) measurements that CuO produced at 325 °C was most stable and provided the highest photocurrent of 173 μA cm-2 at 0 V with an onset potential of about 0.23 V. The alignment of zinc oxide (ZnO) nano-rods and nano-tubes fabricated by CBD have been shown to be strongly affected by the seed layer on the FTO substrate. SEM images showed that AACVD provided the best seed layer for aligning the growth of the nano-rods perpendicular to the surface. Nano-rods were successfully altered into nano-tubes using a potassium chloride bath etching method. NiO prepared by both AACVD and the combined ED/DB method were sensitized to absorb more of the solar spectrum using AACVD to deposit CuO over the NiO. A large increase in the photocurrent was observed for the p-type photoelectrode. These p-type photoelectrode showed a photocurrent density of approximately 100 μA cm-2 at 0 V and an onset potential of 0.3 V. This photocathode was then used as a base to produce a solid state p-type solar cell. For the construction of the solid state solar cells several n-type semiconductors were used, these were ZnO, WO3 and BiVO4. WO3 and BiVO4 were successfully produced with BiVO4 proving to be the optimum choice. This cell was then studied more in depth and optimised by controlling the thickness of each layer and annealing temperatures. The best solid state solar cell produced had a Jsc of 0.541 μA cm-2 (541 nA) and a Voc of 0.14 V, TX146 made up of NiO 20 min, CuFe2O4 50 min, CuO 10 min, BiVO4 27 min, using AACVD and then annealed for 30 min at 600°C.

Inexhaustible solar energy, which provides a clean, economic and green energy, seems to be an alternative solution, for current and future energy demands. Harvesting solar energy presents a challenge in using eco-friendly, earth abundant and inexpensive materials. Although present CdTe and Cu (In, Ga)Se2 (CIGS) technologies, provide light-to-electricity comparable to silicon technology, toxicity of Cd and scarcity of In limits the widespread utilization. Future tera-watt level module capacity would then be feasible by the low-cost technologies. The chalcogenide thin film technology would therefore provide the exceptional utilization in the large-area module monolithic integrations benefitting from the low material consumption owing to the direct band gap. The current thesis presents the results obtained from the quest of other thin film materials and their utilization to an unconventional Cd-free buffer layer. The films suitability for the future applications was assessed through photovoltaics device studies in a comparative manner. Chapter-1 deals with the motivation for the solar energy and the importance of thin film photovoltaics. Alternative materials which are abundantly available would help to reach the future tera watt level production, where the conventional silicon technology alone cannot satisfy the global energy demand. The utilization of non-conventional thin film based solar cells and their working principles were elucidated. The histories of the copper based alternative materials were introduced. Chapter-2 deals with the versatile thin film growth technique that has been designed fabricated and installed further which can handle the growth of the absorber and the top TCO layers with insitu sulphurisation. The methodology of the absorber deposition was discussed in detail. The experimental details for the co-sputtering of CuInAl alloy were presented. A novel selenization method, assisted by the combination of inert gases was developed for the annealing of CuInAl alloyed precursor films. Chapter-3 deals with the presentation of the results obtained on buffer and window layers. Chemical Bath deposition technique was employed for the growth and optimization of the conventional CdS and non-toxic buffer ZnS buffer layers. A) Cadmium sulphide thin films suitable for the utilization of high efficiency solar cells were optimized. Optimization of the buffer involved the effects of cadmium precursors, ammonia concentration and buffer capsule effect. A green route was presented so as to consume the precursors to the maximum extent possible. B) The alternative non-toxic buffer Zinc Sulphide (ZnS) thin films were successfully grown using the above optimized conditions. Moreover the window layer was also optimized for better device partner. Zinc Oxide was used as a n-type partner for the p-type CIS films. The ZnO films were grown by the RF-sputtering from the single cathode exhibited good crystallinity with Zincite structure (hexagonal ZnS, a= 3.249A0 and c= 5.205A0). All the grown films showed high resistivity. Al: ZnO thin films were optimized in two methods 1) by dc co-sputtering from the elemental cathodes, Zinc and Aluminum, 2) dc-sputtering from the single 2% Al-doped ZnO cathode. Low resistivity Al:ZnO thin films were deposited in both the cases. Effect of Aluminum doping into ZnO crystal lattice upon the optical and electrical properties were discussed. Chapter-4 deals with the synthesis of various absorber materials, characterizations and some properties. Briefly the A) Optimization of the CuIn1-xAlxSe2 phase with better adhesion and better crystallinity. Aluminum doping into the crystal lattice of CuInSe2 aided the wide band gap tuning of CIAS thin films. Morphological investigations were carried out for the different set of thin films before and after selenization. Effects of copper and Aluminum concentrations on the lattice parameter of the selenized thin films were addressed. The present chapter deals with the A) electrical properties of CIAS films and its heterojunction partners. Resistivity measurements and effects of Cu/In ratio and the effect of Al doping were described in detail. The CIAS/ZnO heterostructure, CIAS/Al:ZnO heterostructure junction properties as a function of different sun illuminations were discussed. B) The alternative earth abundant, eco-friendly, non-toxic elements Cu2ZnSnS4, absorber thin films synthesis and characterizations. Photo conductive photo measurements showed CZTS a potential candidate for near infra-red photodectection. C) Cu2CoSnS4 (CCTS) nanostructures and quantum dots were synthesized via simple chemical routes. CCTS quantum dots were tuned to exhibit the red edge effect and cold white phosphors. D) Cu3BiS3 nano rods were synthesized and characterized structurally and optically. The transport properties of Cu3BiS3 nanorods were tailored for showing the metallic to semiconducting transitions. Chapter-5 Discusses the A) Efforts made in understanding the CIAS based solar cells through interfaces such as CIAS/ZnO, Mo/CIAS, CIAS/CdS/i-ZnO/Al:ZnO and improving the open circuit voltage VOC upon a rotating substrate, involving the inline and in situ processes, for fabricating the cell/ module were discussed. The device statistics for various set of cells were analyzed. B) Solar cells of CTS absorber with the non-toxic buffer ZnS were fabricated and device properties were analyzed. C) CCTS quantum dots embedded in the polymer matrix were utilized for making the inverted hybrid solar devices in combination of ITO/AZnO bilayered contact replacing the acidic PEDOT: PSS. D) The solar cells made of CCTS hollow spheres by spin coating the absorber in the configuration SLG/Mo/CCTS/CdS/ iZno-AZnO/Ni-Al-Al showed a lower efficiency of 0.02%. Chapter-6 concludes with the summary of present investigations and the scope for future work.