Ce travail a pour objectif l’élaboration de surfaces permettant le contrôle de l’adsorption protéique et de l’adhésion cellulaire. Deux axes d’études permettent de répondre à cette problématique : d’une part l’optimisation des conditions de greffage par réaction thiol-ène de chaînes éthylène glycol (OEG ou PEG) comportant une fonction thiol sur une monocouche auto-assemblée de trichlorosilane d’undécényle, d’autre part la caractérisation chimique de surface (mesures d’angle de contact, ellipsométrie, microscopie de fluorescence, infrarouge en réflexion totale atténuée IR-ATR, spectroscopie de photoélectrons induits par rayons X XPS, spectrométrie de masse d’ions secondaires à temps de vol ToF-SIMS) à l’issue de chaque étape de traitement. L’étude méthodologique des conditions de greffage thiol-ène montre la mise au point d’un système bicouche structuré après 1 minute de réaction pour le greffage OEG, 1 heure pour le greffage PEG. Par l’emploi de divers substrats (oxyde de silicium, titane, verre), différentes molécules OEG-thiol ou PEG-thiol (longues de 7 à 220 unités éthyléniques, terminées –méthyle, -carboxyle ou –amine), nous mettons en avant les déclinaisons possibles de cette stratégie. Ces terminaisons chimiques conduisent, au choix, à l’inhibition de l’adsorption protéique ou à l’adsorption de biomolécules, albumine de sérum bovin (BSA) ou fibronectine (Fn), permettant de faire de l’adhésion spécifique. Le contrôle, dans le plan de l’échantillon, des zones exposées à la lumière par photochimie lors du greffage thiol-ène autorise le photopatterning des surfaces permettant la maîtrise de l’adsorption protéique et également de l’adhésion cellulaire à la surface. / The aim of this work is to design surfaces allowing controlling cellular adhesion by the study of protein adsorption and cell adhesion. Two main parts were investigated in order to answer this challenge: on one side the optimization of grafting conditions using the thiol-ene reaction of thiol-terminated ethylene glycol chains (OEG or PEG) on a undecenyltrichlorosilane self-assembled monolayer, on the other side the surface chemical characterization (angle contact measurement, ellipsometry, fluorescence microscopy, attenuated total reflection infrared IR-ATR, X-ray Photoelectron Spectroscopy XPS, Time-of-Flight Secondary Ion Mass Spectrometry ToF-SIMS) after each reaction step. The methodological investigation of thiol-ene grafting conditions exhibits the development of a bilayer structured system after a 1 minute reaction time concerning OEG grafting, 1 hour in case of PEG grafting. By using different substrates (silicon oxide, titanium, glass), different molecules OEG-thiol or PEG-thiol (from 7 to 220 ethylene unit long, methyl-, carboxyl- or amine-terminated), we highlight the range of available versions of this strategy. These chemical extremities lead on demand either to protein adsorption inhibition or to biomolecule adsorption, bovine serum albumin (BSA) or fibronectin (Fn) giving access to specific adhesion.By controlling the light-exposed areas in the sample plan, the photochemistry occurring during the thiol-ene grafting allows to design surface patterning for addressing both protein adsorption and cell adhesion on the sample surface.

No description available.

Philosophiae Doctor - PhD / In this study, the OMCVD method is demonstrated as a powerful, fast, economic and environmental friendly method to produce a set of PGMelectrocatalysts with different supports, metal content and metal alloys in one step and without the multiple processing stages of impregnation, washing, drying, calcinationsand activation. / South Africa

Transparent conductive oxides (TCOs) are key functional materials in existing and future electro-optical devices in the fields of energy efficiency, energy generation and information technology. The main application of TCOs is as thin films transparent electrodes where a combination of maximum electrical conductivity and transmittance in the visible to nearinfrared spectral range is required. However, due to the interdependence of the optical properties and the free electron density and mobility, respectively, these requirements cannot be achieved simultaneously in degenerately doped wide band-gap oxide semiconductors. Therefore, a detailed understanding of the mechanisms governing the generation of free charge carriers by extrinsic doping and the charge transport in these materials is essential for further development of high performance TCOs and corresponding deposition methods. The present work is aimed at a comprehensive investigation of the electrical, optical and structural properties as well as the elemental composition of (Al,Ga) doped ZnO and Nb doped TiO2 thin films prepared by pulsed DC reactive magnetron sputtering. The evolution of the film properties is studied in dependence of various deposition parameters through a combination of characterization techniques including Hall-effect, spectroscopic ellipsometry, spectral photometry, X-ray diffraction, X-ray near edge absorption, Rutherford backscattering spectrometry and particle induced X-ray emission. This approach resulted in the development of an alternative process control method based on the material specific current-voltage pressure characteristics of the reactive magnetron discharge which allows to precisely control the oxygen deficiency of the sputter deposited films. Based on the experimental data, models have been established that describe the room temperature charge transport properties and the dielectric function of the obtained ZnO and TiO2 based transparent conductors. On the one hand, these findings allow the prediction of material specific electron mobility limits by identifying the dominating charge carrier scattering mechanisms. On the other hand, new insight is gained into the origin of the observed transition from highly conductive to electrically insulating ZnO layers upon the incorporation of increasing concentrations of Al at elevated growth temperatures. Moreover, the Al and Ga dopant activation in ZnO have been quantified systematically for a wide range of Al concentrations and deposition conditions. A direct comparison of the Ga and Al doping efficiency demonstrates that Ga is a more efficient electron donor in ZnO. Further, it has been shown that high free electron mobilities in polycrystalline and epitaxial Nb:TiO2 layers can be achieved by reactive magnetron sputtering of TiNb alloy targets. The suppression of rutile phase formation and the control of the Nb dopant activation by fine tuning the oxygen deficiency have been identified as crucial for the growth of high quality TiO2 based TCO layers.

Arsenic (As) contamination is a worldwide problem, and millions of people are suffering from it. There are two major inorganic forms of As in waters: arsenate(V) and arsenite(III), and adsorption to a sorbent material may be an efficient method to handle them. In this study, we focused on As(III), the more toxic form, which predominates under reducing conditions. The As(III) removal properties of four sorbent materials: hydrotalcite, Mg−Al layered double hydroxide, amorphous aluminium hydroxide and amorphous titanium oxide, are examined from the following viewpoints: As(III) adsorption, the effects of pH, the effects of adsorbent concentration, adsorption as a function of dissolved As(III), and the effect of co-existing anions (HCO3− and PO43−). The maximum adsorption of As(III) to HT (0.1 mmol As(III)/g adsorbent), Mg-Al LDH (0.1 mmol As(III)/g adsorbent), am-Al(OH)3 (0.22 mmol As(III)/g adsorbent), and am-TiO2 (0.21 mmol As(III)/g adsorbent) occurred at pH 7.5, 7, 7, 8, respectively. At this pH, approximately 20%, 62%, 35%, and 98.3%, respectively, of the added As(III) was adsorbed. When the As(III) to sorbent ratio was increased, the adsorption was instead around 7% to am-Al(OH)3 (2.2 mmol As(III)/g adsorbent), and 46.3% to am-TiO2 (2.1 mmol As(III)/g adsorbent). These figures show that am-TiO2is the most efficient sorbent for As(III) adsorption of the four materials tested, Mg-Al LDH is second best, while HT and am-Al(OH)3 are not suitable for As(III) removal. The adsorption of As(III) to Mg-Al LDH as a function of dissolved As(III) could be adequately described by a linear equation, suggesting that As(III) adsorption to Mg-Al LDH was governed by anion exchange. As a result, the co-existing anions (HCO3- and PO43-) showed a significant influence on As(III) adsorption to Mg-Al LDH. Considering the interfering effects of co-existing anions on am-TiO2, HCO3− did not influence As(III) adsorption, while PO43- caused a slight but clear competition effect. Overall, am-TiO2 would be the best choice of these four materials in contact with As-contaminated groundwater due to its superior As(III) removal properties and the limited competition from co-existing anions on As(III) adsorption. / Alltför höga halter av arsenik (As) i vatten är ett världsomspännande problem som orsakar hälsoproblem för miljontals människor. Det finns två huvudsakliga oorganiska former av As i vatten: arsenat(V) och arsenit(III), och adsorption till ett material (s.k. ”sorbent”) kan vara eneffektiv metod för att avlägsna dem från vatten. I denna studie fokuserade vi på arsenit(III), den mer giftiga formen, vilken dominerar under reducerande förhållanden. Vi undersökte adsorptionsegenskaperna för arsenit(III) för fyra sorbentmaterial som kan vara tänkbara när det gäller arsenikrening av förorenade vatten: hydrotalkit, s.k. Mg-Al LDH (Mg-Al-skiktad dubbelhydroxid), am-Al(OH)3 (amorf aluminiumhydroxid), och am-TiO2 (amorf titandioxid). Dessa material undersöktes när det gäller följande: adsorption av arsenit(III) som funktion av pH,betydelsen av sorbentkoncentration, adsorption som funktion av löst arsenit(III) (”isoterm”), och konkurrens från samexisterande anjoner (HCO3− och PO43−). Den maximala adsorptionen av As (III) till HT (0,1 mmol As(III)/g sorbent), Mg-Al LDH (0,1 mmol As(III)/g sorbent), am-Al(OH)3 (0,22 mmol As(III)/g sorbent) och am-TiO2(0,21 mmol As(III)/g sorbent) inträffade vid pH 7,5, 7, 7, respektive 8. Vid dessa pH-värden adsorberades ungefär 20%, 62%, 35% respektive 98,3% tillsatt As(III). När kvoten mellan As(III) till sorbent ökades blev adsorptionen istället cirka 7% till am-Al(OH)3 (2,2 mmol As(III)/g sorbent) och 46,3% till am-Ti02(2,1mmol As(III)/g sorbent). Dock var adsorptionsmängden per viktsenhetsorbenthögre över hela pH-området. Dessa siffror visar att am-TiO2 är det mest effektiva av de fyra testade materialen för As(III)-adsorption, Mg-Al LDH det näst bästa, medan HT och am-Al(OH)3 är olämpliga för detta ändamål. Adsorptionen av As(III) till Mg-Al LDH som funktion av löst As(III) kunde beskrivas väl med en linjär ekvation, vilket antyder att adsorptionen av As(III) till Mg-Al LDH styrdes av anjonbyte. I konsekvens med detta hade de samexisterande anjonerna (HCO3- och PO43-) ett betydande inflytande på As(III)-adsorptionen till Mg-Al LDH. För am-TiO2 påverkade HCO3− inte As(III)-adsorptionen, medan PO43- orsakade en liten men tydlig konkurrenseffekt. Sammantaget är am-TiO2 det bästa valet av dessa fyra material i kontakt med As- kontaminerat grundvatten på grund av dess betydligt bättre förmåga att avskilja arsenit(III) och den förhållandevis blygsamma konkurrensen från andra anjoner.

A bench-scale tubular reactor with recirculation was built in order to study the efficiency of the photocatalytic oxidation of phenol on fluidized titanium oxide-coated silica gel beads. A UV-C lamp placed along the central vertical axes of the reactor was used as source of photons. A bed of silica gel beads was fluidized by means of fluid recirculation and forced to follow upward helical flow around the lamp. Anatase was successfully synthetized on silica gel particles of average diameters 224, 357 and 461 µm, as confirmed by scanning electron micrographs, through a sol-gel technique using a titanium (iv)isopropoxide / hydrochloric acid / ethanol precursor. Data was obtained from multiple 8-hours photocatalytic experiments using a determined mass of beads fluidized in an aqueous solution of known initial phenol concentration. Contaminant degradation with irradiation time was measured as COD. Beads that had been subjected to three consecutive coating procedures produced an 8-h removal efficiency 10% higher than beads with a single coat. 20 g L-1 of silica beads was found to be the optimum load for the experimental reactor configuration regardless of beads size, although efficiency increased with decreasing size of the latter. Experimental results confirmed that the efficiency of phenol photocatalytic degradation decreases with increasing pollutant concentration. Also, the highest removal was achieved with initial pH 3, and it decreased with increasing pH. When NaCl was added to the solution, COD removal increased with increasing salinity. Additionally, it was found that dissolved oxygen is indispensable for photocatalysis to proceed, and that saturation of the treated mixture with oxygen was effectively achieved by keeping the liquid surface in contact with pure oxygen at 1 atm. Finally, statistical analysis of the data showed that photocatalytic mineralization of phenol-derived COD under the experimental conditions follows exponential decay. Based on this finding, a correlation model was proposed for the accurate prediction (minimum R2 = 0.9840) of the COD removal efficiency of the reactor for any given initial COD.

O presente trabalho tem como objetivo contribuir para o conhecimento, entendimento e desenvolvimento das células solares sensibilizadas por corantes. Assim foram abordadas rotas sintéticas com o fim de obter novas espécies supramoleculares constituídos por fragmentos que apresentam separadamente ótimas propriedades eletrônicas e eletroquímicas. A abordagem sintética feita é muito importante dado que dá as bases para sistemas supramoleculares como o apresentado nas perspectivas, nos quais estase visando diminuir os processos de recombinação e melhor aproveitamento do espectro solar através da estabilização do corante foto-oxidado e da transferência vetorial de elétron/energia. Na série de complexos apresentada e aplicada no presente trabalho realizou-se um estudo comparativo buscando determinar qual é o melhor sistema de injeção de elétrons na banda de condução do TiO2, obtendo uma diferença considerável entre os sistemas estudados, sendo assim o sistema com o ligante acido 2,2 -bipiridine-4,4 -dicarboxilico o complexo que melhor injeta elétrons na BC. / The present work aims to contribute to the knowledge, understanding and development of solar cells sensitized by dyes. Thus, synthetic routes were approached in order to obtain new supramolecular species constituted by fragments that separately present excellent electronic and electrochemical properties. The synthetic approach is very important since it provides the basis for supramolecular systems such as that presented in the perspectives, in which stasis is aimed at decreasing the processes of recombination and better utilization of the solar spectrum through the stabilization of the photo-oxidized dye and the vectorial transfer of electron /energy. In the series of complexes presented and applied in the present work, a comparative study was carried out to determine which is the best electron injection system in the conduction band of TiO2, obtaining a considerable difference between the studied systems, being thus the complex with the ligand 2,2 -Bipyridine-4,4 -dicarboxylic acid the best system that injects electrons into BC.

The polymer electrolyte membrane fuel cell (PEMFC) converts the chemical energy of hydrogen and oxygen (air) into usable electrical energy. At the cathode (the positive electrode), a considerable amount of platinum is generally required to catalyse the sluggish oxygen reduction reaction (ORR). This has implications regarding the cost in high-power applications, and for making a broad commercialisation of the PEMFC technology possible, it would be desirable to lower the amount of Pt used to catalyse the ORR. In this thesis a number of techniques are described that have been developed in order to investigate catalytic activity at the cathode of the PEMFC. These methodologies resemble traditional three-electrode research in liquid electrolytes, including cyclic voltammetry in inert gas, but with the advantage of performing the experiments in the true PEMFC environment. From the porous electrode studies it was seen that it is possible to reach mass activities close to 0.2 gPt/kW at potentials above 0.65 V at 60 ◦C, but that the mass activities may become considerably lower when raising the temperature to 80 ◦C and changing the measurement methodology regarding potential cycling limits and electrode manufacturing. The model electrode studies rendered some interesting results regarding the ORR at the Pt/Nafion interface. Using a novel measurement setup for measuring on catalysed planar glassy carbon disks, it was seen that humidity has a considerable effect on the ORR kinetics of Pt. The Tafel slopes become steeper and the activity decreases when the humidity level of the inlet gases decreases. Since no change in the the electrochemical area of the Pt/Nafion interface could be seen, these kinetic phenomena were ascribed to a lowered Pt oxide coverage at the lower humidity level, in combination with a lower proton activity. Using bi-layered nm-thick model electrodes deposited directly on Nafion membranes, the behaviour of TiO2 and other metal oxides in combination with Pt in the PEMFC environment was investigated. Kinetically, no intrinsic effect could be seen for the model electrodes when adding a metal oxide, but compared to porous electrodes, the surface (specific) activity of a 3 nm film of Pt deposited on Nafion seems to be higher than for a porous electrode using ∼4 nm Pt grains deposited on a carbon support. Comparing the cyclic voltammograms in N2, this higher activity could be ascribed to less Pt oxide formation, possibly due to a particle size effect. For these bi-layered films it was also seen that TiO2 may operate as a proton-conducting electrolyte in the PEMFC. / I polymerelektrolytbränslecellen (PEMFC) omvandlas den kemiska energin hos vätgas och syrgas (luft) direkt till användbar elektrisk energi. På katoden (den positiva elektroden) krävs betydande mängder platina för att katalysera den tröga syrereduktionsreaktionen (ORR). Detta inverkar på kostnaden för högeffektsapplikationer, och för att göra en bred kommersialisering av PEMFC-teknologin möjlig skulle det vara önskvärt att minska den Pt-mängd som används för att katalysera ORR. I denna avhandling beskrivs ett antal tekniker som utvecklats för att undersöka katalytisk aktivitet på katoden i PEMFC. Metodiken liknar traditionella treelektrodexperiment i vätskeformig elektrolyt, med cyklisk voltammetri i inert gas, men med fördelen att försöken utförs i den riktiga PEMFC-miljön. I försök med porösa elektroder visades att det är möjligt att nå massaktiviteter nära 0.2 gPt/kW för potentialer över 0.65 V vid 60 ◦C, men massaktiviteterna kan bli betydligt lägre om temperaturen höjs till 80 ◦C, och om potentialsvepgränser och elektrodentillverkningsmetod ändras. Försök med modellelektroder resulterade i intressanta resultat rörande ORR i gränsskiktet Pt/Nafion. Genom att använda en ny metodik för att mäta på katalyserade plana elektroder av vitröst kol (glassy carbon), var det möjligt att se att gasernas fuktighet har en betydande inverkan på ORR-kinetiken hos Pt. Tafellutningarna blir brantare och aktiviteten minskar när inloppsgasernas fuktighetsgrad minskar. Eftersom den elektrokemiska arean hos Pt/Nafion-gränsskiktet inte ändrades, ansågs dessa kinetiska effekter bero på en lägre täckningsgrad av Ptoxider vid lägre fuktigheter, i kombination med lägre protonaktivitet. Genom att använda Nafionmembran belagda med nm-tjocka tvåskiktsmodellelektroder undersöktes hur Pt i kombination med TiO2 och andra metalloxider verkar i PEMFC-miljön. Kinetiskt sett hade tillsatsen av metalloxider ingen inre påverkan på aktiviteten, men vid jämförelse med porösa elektroder tycks den specifika ytaktiviteten vara högre hos en 3 nm film av Pt på Nafion än för en porös elektrod baserad på ∼4 nm Pt-korn belagda på ett kolbärarmaterial. Jämför man de cykliska voltammogrammen i N2, kan den högre aktiviteten tillskrivas en lägre grad av Pt-oxidbildning, vilket i sin tur kan bero på en storlekseffekt hos Pt-partiklarna. Försöken med dessa tvåskiktselektroder visade också att TiO2 kan verka som protonledande elektrolyt i PEMFC. / QC 20100706

La tesi s’engloba en un context energètic en el que les tendències actuals del subministrament i el consum d’energia són clarament insostenibles. No és exagerat dir que el futur de la prosperitat de la humanitat depèn de la manera en què responguem als dos principals reptes que se’ns plantegen en l’actualitat en matèria d’energia: assegurar un subministrament d’energia fiable i assequible, i passar ràpidament a un nou sistema de subministrament de l’energia amb baixes emissions de carbó, eficient i respectuós amb el medi ambient. De entre totes les tecnologies disponibles, la generació d’hidrogen solar mitjançant el trencament fotoelectroquímic de l’aigua ha estat considerada la més prometedora en quant a l’obtenció de sistemes estables de fotoelectrólisi. Més concretament, els òxids metàl•lics han centrat l’atenció de la comunitat científica com els materials ideals per a implementar els fotoànodes. L’òxid de titani és el material per excel•lència en fotocatàlisi. Això és degut principalment a la seva gran estabilitat en tot tipus de medis i a la gran varietat de rutes de síntesi que es poden utilitzar per a la seva obtenció (sol-gel, hidrotermal, solvotermal, oxidació directa, deposició química en fase vapor, deposició física en fase vapor, electrodeposició, mètode sonoquímic, anodització, etc). A la primera part vàrem analitzar vàries de les rutes de síntesis que permeten obtenir nanoestructures de TiO2 amb característiques ben diferents. Totes elles tenen en comú una gran superfície activa per tal que es puguin produir el màxim de reaccions a la superfície. Donades les limitacions intrínseques de l’òxid de titani degut a la seva baixa absorció a la regió visible de l’espectre solar com a conseqüència de la seva elevada banda prohibida (3.2 eV), ens centràrem en les possibles millores que se’n poden derivar de la modificació química i/o estructural mitjançant la incorporació d’elements estranys en el si de la matriu de l’òxid de titani. Vàrem diferenciar entre additius catiònics i aniònics i més concretament en la incorporació de ferro i nitrogen, respectivament. Vàrem estudiar com la presència d’aquests elements afecten les propietats òptiques i elèctriques dels nostres materials i com podíem controlar el seu impacte en aquestes propietats . Finalment, vàrem presentar com la utilització d’estructures composades de varis semiconductors permeten millorar amb escreix els rendiments obtinguts mitjançant la introducció d’additius per tal de modificar l’estructura de l’òxid de titani. En concret, estudiàrem l’heteroestructura CdS@TiO2. En aquesta mena d’estructura el CdS actua com a material absorbidor i l’òxid de titani com a material suport que proporciona la nanoestructura necessària per a dotar el dispositiu d’una bona conducció d’electrons i d’una gran superfície activa / "Synthesis of nano structured titanium dioxide for energy applications" After the pioneering work of Fujishima and Honda, who demonstrated the possibility to electrolyze water to hydrogen fuel using a solar-driven titanium dioxide photoelectrode (PE) cell, researchers looked for other semiconductor oxides or solid solutions resistant to photocorrosion. As alternatives, conventional semiconductors like Si, GaAs, InP, CuInSe and CdTe display impressive efficiencies as PEs but their low stability in water solutions and high cost hinders their use for such applications. On the other hand, TiO2 has been extensively investigated as an environmentally harmonious and clean photocatalyst. Titania’s main advantages are its reasonable optical and electronic properties, a fair photocatalytic activity, and especially its low cost, excellent chemical stability and nontoxicity. However, its practical application has been limited by its low efficiency and wide bandgap, which requires ultraviolet (UV) radiation as the excitation source. In this work, we present different routes of synthesis to obtain nanostructured titania with the aim of increase the active surface area which one of the main limiting factors. In a second part, we explored to different approaches for the improvement of the absorption range of the visible spectrum: introduction of transition metals, such as iron, and doping with non-metal such as nitrogen. Finally, we introduced a new concept that allows overcoming the intrinsic limitations of the introduction of strange elements inside de matrix of TiO2. The use of heterostructured materials, which is match two different materials, such as TiO2 and CdS, with different band gaps to take profit of a wider range of the solar spectrum.

High quality ammonium oxofluorotitanate discoid crystal is successfully grown on glass with an aqueous solution of ammonium hexafluorotitanate and boric acid at the molar ratio of 0.6. The concentration of hydrofluoric acid is less on the glass substrate surface and enhances the ammonium oxofluorotitanate nucleation growth. The growth rate is much higher than that grown on dioctadecyldimethylammonium. From the examinations of X-ray diffraction and high-resolution transmission electron microscopy, the crystal shows high crystalline quality and uniformity. Each titanium oxide octahedral is linked with fluorine and nitrogen atoms. Therefore, ammonium oxofluorotitanate has high potential to be thermally decomposed into high crystalline fluorine and nitrogen co-doped titanium oxide. A simple process for the preparation of nanocrystalline anatase phase titanium oxide converted from ammonium oxofluorotitanate by thermal treatment was developed. The nanocrystalline anatase phase titanium oxide shows a large bandgap reduction due to the co-doping of high concentrations of fluorine and nitrogen. Due to the excellent nanocrystalline quality and the co-doping of higher concentrations of fluorine and nitrogen at the thermal treatment temperature of 800 OC, it is 1.3 times the photocatalytic activities of P-25 due to the visble region usage of Hg lamp light source. The 11.2 times the visible photocatalytic activities of P-25 using blue light-emitting diode as the light source is obtained from thermal treatment temperature of 600 OC. There is one to one correspondence between carrier lifetime and photocatalytic activity. As a result, a highly reactive and visible-light-driven photocatalysis is achieved. The heterostructure of zinc selenide/titanium oxide and zinc sulfide/titanium oxide were prepared by metal-organic chemical vapor deposition on the above-prepared titanium oxide. The energy bandgap of zinc sulfide is much larger than that of titanium oxide and can act as a window for titanium oxide. It would not hinder titanium oxide absorption and preserve the role of fluorine and nitrogen co-doping. The energy bandgap of zinc selenide is near the maximum intensity of solar spectrum and acts as a sensitizer of titanium oxide. The lifetime of electron and hole pairs of heterostructure are about 240 and 207 nsec, which are longer than 65 nsec of titanium oxide prepared at 800 oC thermal treatment. Their photocatalytic activities are further improved to 2.0 and 1.5 times higher than that of commercial P-25. The photocatalysis of titanium oxide is very sensitive to the surface states. Titanium oxide surface defects can act as trapping sites for photo-induced holes and facilitate the separation of photo-induced carriers. Zinc selenide and zinc sulfide can passivate the surface well. It may say that titanium oxide surface defects removal has a negative impact. The density, height, diameter, PL wavelength and intensity of zinc selenide self-assembled quantum dots grown on zinc sulfide/gallium arsenide with the zinc sulfide thickness from 15 to 160 nm are studied. For a fixed 30 sec zinc selenide self-assembled quantum dots growth, it cannot be formed with the zinc sulfide thickness below 15 nm due to the close lattice match between zinc sulfide and gallium arsenide. The zinc sulfide/gallium arsenide is fully lattice relaxed with the zinc sulfide thickness higher than 130 nm examined by X-ray diffraction. The higher quality and density of zinc selenide self-assembled quantum dots can be obtained on zinc sulfide/gallium arsenide with the zinc sulfide thickness far beyond its critical thickness. The maximum zinc selenide self-assembled quantum dots density of 4.9 x 109 cm-2 with the strongest photoluminescence intensity is obtained at the zinc sulfide/gallium arsenide thickness of 130 nm. Clusters are formed on the surface of zinc selenide/gallium arsenide. The selenium segregation is the main mechanism for the formation of clusters. The dislocations will enhance the selenium segregation. Higher zinc selenide cluster corresponds to higher density of dislocations. The non-spherical cluster is formed from the mergence of the two clusters. High quality zinc oxide rods and zinc hydroxide slices are successfully grown on gallium arsenide with the aqueous solution of zinc nitrate and hexamethylenetetramine. The growth can be controlled by the appropriate nitric acid concentration incorporation in the solution. After thermal annealing, the zinc oxide slices transformed from zinc hydroxide slices can contribute much higher photocatalytic activity to 1.2 times to P-25.