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Abstract

Thin film series consisting of Ti, V, TiO2 and V2O5 layer with different layer geometries, sequences and thicknesses have been prepared by the sputtering technique. The hydrogen depth profile of selected films upon hydrogen charging at 1 bar and/or hydrogenation at pressure up to 102 bar was determined by using secondary ion mass spectrometry and nuclear reaction analysis using a N-15 beam. The highest hydrogen storage with a concentration up to 50 at.% was found in the pure Ti and Ti-contained layer, while it amounts to around 30% in the metallic Ti-V-Ni layer. Hydrogen can diffuse through the TiO2 layer without accumulation, but can be stored in the VO2 layer in some cases. Hydrogen can remove the preferential Ti orientation in the films and induce a complete transition of V2O5 into VO2 in the films.

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... RBS and XRR experiments have been performed on films before and after each hydrogenation to underline the changes of the film composition and structure upon hydrogenation. Details of XRR and RBS data analysis, especially the estimate of composition and layer-thickness, have been reported in [15,19]. ...
... The hydrogen quantity in the thin film systems is very small to be qualified by desorption. Thus we used a secondary ion mass spectroscopy (SIMS) and Nuclear Reaction Analysis using the 15 N beam ( 15 N-NRA method with 1 H( 15 N, a,g) 12 C reaction) for determination of hydrogen concentration in the films [18,19]. Besides, unlike the bulk samples, for the thin film systems as in our case with very thin layers, it is convenient to use the atomic percent for the very small amount of hydrogen. ...
... For both films, the stoichiometric TiO 2 and/or V 2 O 5 layer was well preserved on the film surface: the layer thickness is almost unchanged upon hydrogen charging [19]. Thus the swelling effect seems to be related the mixed TiO 2 eVO 2 eSiO 2 layer (i.e. ...
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Series of thin films of single-, bi- and tri-layered structure consisting of Ti, V, TiO2 and V2O5 layer and/or mixed Ti-V-Ni layer with different layer sequences and thicknesses were prepared by the sputtering technique on Si and SiO2 substrates. The layer chemical composition and thickness were determined by a combined analysis of X-ray diffraction, X-ray reflectometry, Rutherford backscattering and optical reflectivity spectra. The films were hydrogenated at 1 bar at 300oC and/or at high pressures up to 100 bar at room temperature. The hydrogen concentration and hydrogen profile was determined by means of a secondary ion mass spectroscopy and N-15 Nuclear Reaction Analysis. The highest hydrogen storage with a concentration up to 50 at.% was found in the pure Ti layers, while it amounts to about 30 at.% in the metallic Ti-V-Ni layers. A large hydrogen storage (up to 20 at. %) was also found in the V2O5 layers, while no hydrogen accumulation was found in the TiO2 layers. Hydrogen could remove the preferential orientation of the Ti films and induce a complete transition of V2O5 to VO2.
... The model used to calculate and fit the XRR pattern is V 2 O 5 /SiO 2 /Si, which gives a good fit and reveals that the film density is ∼3.15 g cm −3 which is reasonably close to the reported bulk value of 3.36 g cm −3 . 48,49 The data fitting revealed a film thickness of ∼33 nm, which is slightly thicker than our ellipsometry-measured values, and the film surface roughness of ∼1.7 nm was calculated. A similar fitting approach for VO 2 film is performed using VO 2 /SiO 2 /Si model and the XRR pattern is displayed in Fig. 7(b). ...
... The density found is smaller than the reported bulk density value of 4.57 g/cm 3 . 49 However, the higher roughness is attributed to the discontinuity of VO 2 film triggered by the postdeposition annealing, which can be overcome by growing thicker films as will be demonstrated with the HCP-ALD grown and postdeposition annealed samples. Figure 8 shows the elemental content and atomic concentrations of the ICP-ALD grown V 2 O 5 film for air-exposed as-received samples without any Ar sputtering, extracted via XPS measurements from the surface of the samples. ...
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Vanadium oxide (VO x ) compounds feature various polymorphs, including V 2 O 5 and VO 2 , with attractive temperature-tunable optical and electrical properties. However, to achieve the desired material property, high-temperature post-deposition annealing of as-grown VO x films is mostly needed, limiting its use for low-temperature compatible substrates and processes. Herein, we report on the low-temperature hollow-cathode plasma-enhanced atomic layer deposition (ALD) of crystalline vanadium oxide thin films using tetrakis(ethylmethylamido)vanadium and oxygen plasma as a precursor and coreactant, respectively. To extract the impact of the type of plasma source, VO x samples were also synthesized in an inductively coupled plasma-enhanced ALD reactor. Moreover, we have incorporated in situ Ar-plasma and ex situ thermal annealing to investigate the tunability of VO x structural properties. Our findings confirm that both plasma-ALD techniques were able to synthesize as-grown polycrystalline V 2 O 5 films at 150 °C. Postdeposition thermal annealing converted the as-grown V 2 O 5 films into different crystalline VO x states: V 2 O 3 , V 4 O 9 , and VO 2 . The last one, VO 2 is particularly interesting as a phase-change material, and the metal-insulator transition around 70 °C has been confirmed using temperature-dependent x-ray diffraction and resistivity measurements.
... g/cm 3 . 60 The lower film density can be explained by the void structures in the film morphology confirmed via HR-SEM images [ Fig. 15(b)], which were formed during the post-deposition annealing process. Likely, the roughness increased from 1.70 to 2.87 nm due to the impact of post-deposition annealing. ...
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... Furthermore, we also note that when the pulse frequencies lower than 200 KHz, the deposition rate of the VOx films deposited in the reactive atmosphere was higher than the V films deposited in the pure argon atmosphere. This is because the densities of metal V (6.0 g/cm 3 ) was higher than its oxide (V 2 O 3 , 4.87/cm 3 ) (VO 2 , 4.57/cm 3 ) (V 2 O 5 , 3.36 g/cm 3 ), which leads to the oxide films possess a larger mole volume compare with the metal films [40]. And besides that, the oxygen will also incorporate into the growing film during the reactive sputtering, which further reduced the density of the film, and in fact, similar phenomena has also been observed in many reactive sputtering process, i.e. with the increase of the reactive gas flow, the deposition rate of the coatings first increase slightly when the reactive gas flow was low, and then it dropped significantly when the reactive gas flow exceed the critical level [39]. ...
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Scientific studies on photocatalysis started about two and a half decades ago. Titanium dioxide (TiO2), which is one of the most basic materials in our daily life, has emerged as an excellent photocatalyst material for environmental purification. In this review, current progress in the area of TiO2 photocatalysis, mainly photocatalytic air purification, sterilization and cancer therapy are discussed together with some fundamental aspects. A novel photoinduced superhydrophilic phenomenon involving TiO2 and its applications are presented.
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Vertically oriented nanotubular TiO2 arrays were formed by a simple anodization process. Hydrogen storage studies were carried out on the TiO2 nanotubular arrays having different diameters by charging and discharging hydrogen with potentiostatic/galvanostatic control. The hydrogen storage capacities of the nanotubes were only marginally affected by the tube diameter. Concentration of oxygen vacancies as defects influenced the hydrogen storage of the nanotubes. Annealing of the TiO2 nanotubes in argon atmosphere increased the defect density and decreased the hydrogen discharge during initial charge–discharge cycles. Hydrogen storage studies through electrochemical route did not show significant storage capacity of TiO2 nanotubes. Diffusion of hydrogen as protons and interference of the double layer capacitance of nanotubes could be attributed to the lower hydrogen storage capacity.
Article
Reliable measurement of the photoconversion efficiency for semiconductor electrodes is essential to the assessment of electrode performance. In this paper, the influence of the choice of light source on measured photoconversion efficiencies for semiconductor photoelectrodes is examined. Measurements of efficiency performed under xenon lamp and solar illumination are compared with efficiencies calculated by integrating the incident photon conversion efficiency (IPCE) over the lamp and solar spectra. It is shown that use of a xenon lamp as the light source can lead to a large overestimate of the photoconversion efficiency, relative to that obtained under standard AM1.5 solar illumination. The overestimate is greater when a water filter is fitted to the xenon lamp, and when a wide-band gap semiconductor such as TiO2 is used as the photoelectrode. Achievable photoconversion efficiencies using rutile TiO2 are calculated taking into account the losses due to imperfect absorption, reflection and charge-carrier recombination; these calculated efficiencies agree with the measurements to within experimental uncertainties. It is demonstrated that many photoconversion efficiencies presented in the literature are overestimated. It is concluded that reliable estimation of efficiency under standard conditions is best obtained by measuring the IPCE as a function of wavelength, and integrating over the AM1.5 solar spectrum, or by measuring under sunlight with a similar zenith angle to that of the AM1.5 spectrum.
Article
Water splitting and environmental cleanup are two active fields in heterogeneous photocatalysis, which are both closely related to the research in semiconductor photoelectrochemistry since the 1960s. The present review paper will attempt to describe some of the progress and resulting achievements in these two fields, and to briefly discuss the future prospects. We will cover the major developments worldwide but will highlight work carried out in Japan over the last several years. (c) 2006 International Association for Hydrogen Energy. Published by Elsevier Ltd. All rights reserved.
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The present work considers the concept of photoelectrochemical generation of hydrogen through water splitting using solar energy (solar-hydrogen). The focus is on functional material properties that are essential for the performance of photoelectrochemical cell for solar-hydrogen. The performance of the cell is discussed in terms of the energy conversion efficiency (ECE). It is argued that TiO2 and TiO2-based materials are the most promising candidates for photoelectrodes for solar-hydrogen. The modification of TiO2 in order to achieve desired performance parameters is discussed in terms of the electronic structure, concentration of charge carriers and segregation-induced surface properties, which are critical to the ECE. Challenges to the development of a bi-photoelectrode cell, equipped with both n-type and p-type TiO2, forming photoanode and photocathode, respectively, are discussed. The research strategies and pressing issues related to the optimization of key functional properties necessary for the commercialization of solar-hydrogen are outlined. It is shown that defect chemistry is the most appropriate framework for tailoring the functional properties of TiO2-based oxide systems in order to obtain high-performance photoelectrodes. The present work provides an overview of the research progress on solar-hydrogen.
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The field of surface science provides a unique approach to understanding bulk, surface and interfacial phenomena occurring during TiO2 photocatalysis. This review highlights, from a surface science perspective, recent literature that provides molecular-level insights into photon-initiated events occurring at TiO2 surfaces. Seven key scientific issues are identified in the organization of this review. These are: (1)Â photon absorption, (2)Â charge transport and trapping, (3)Â electron transfer dynamics, (4)Â the adsorbed state, (5)Â mechanisms, (6)Â poisons and promoters, and (7)Â phase and form. This review ends with a brief examination of several chemical processes (such as water splitting) in which TiO2 photocatalysis has made significant contributions in the literature.
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Vanadium oxide supported over titanium oxide is an important example of a transition-metaloxide 'monolayer' catalyst with practical relevance for various industrial applications. After a brief introduction on the concept of monolayer oxide catalysts, this review examines three main topics: (i) the nature of vanadium oxide species over the titanium oxide surface, (ii) their reactivity and structure/activity-selectivity relationships and (iii) modification of the surface properties during the catalytic reactions of o-xylene oxidation and alkylaromatic ammoxidation. An analysis of selected literature data leads to the following main conclusions: (i) the support promotes the formation of an amorphous, hydrated active layer of titanium oxide which may extend up to 3-5 layers; (ii) the reactivity of titanium oxide in this form is enhanced with respect to crystalline vanadium oxide, but the selectivity properties which are a function of the oxidation state of vanadium ion and of the modifications occurring during the catalytic reaction are not significantly different; (iii) in the presence of ammonia, the characteristics of the catalyst surface must be tuned to limit the side reaction of NH3 combustion. The optimal catalyst composition for ammoxidation reactions is thus different from that for oxidation catalysts. Simultaneous O and N insertion requires instead an intermediate catalyst composition between those optimal for oxidation and ammoxidation of alkylaromatics.
Article
Owing to the limited resources of fossil fuels, hydrogen is proposed as an alternative and environment-friendly energy carrier. However, its potential is limited by storage problems, especially for mobile applications. Current technologies, as compressed gas or liquefied hydrogen, comprise severe disadvantages and the storage of hydrogen in lightweight solids could be the solution to this problem. Since the optimal storage mechanism and optimal material have yet to be identified, this first handbook on the topic provides an excellent overview of the most probable candidates, highlighting both their advantages as well as drawbacks. From the contents: Physisorption. Clathrates. Metal hydrides. Complex hydrides. Amides, imides, and mixtures. Tailoring Reaction Enthalpies. Borazan. Aluminum hydride. Nanoparticles. A one-stop reference on all questions concerning hydrogen storage for physical and solid state chemists, materials scientists, chemical engineers, and physicists.
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Considerable effort has been made to design, fabricate, and manipulate nanostructured materials by innovative approaches. The precise control of nanoscale structures will pave the way not only for elucidating unique size/shape-dependent physicochemical properties but also for realizing new applications in science and technology. Nanotechnology offers unprecedented opportunities for improving our daily lives and the environment in which we live. This review mainly describes our recent progress in the design, fabrication, and modification of nanostructured semiconductor materials for environmental applications. Their potential applications in the field of energy are briefly introduced. The scope of this article covers a variety of semiconductor materials, focusing particularly on TiO(2)-based nanostructures (e.g., pure, doped, coupled, nanoporous, mesoporous, hierarchically porous, and ordered mesoporous TiO(2)). The preparation of nanoparticles, hierarchical nanoarchitectures, thin films, and single crystals by sol-gel, microemulsion, hydrothermal, sonochemical, microwave, photochemical, and nanocasting methods is discussed.
Article
ALTHOUGH the possibility of water photolysis has been investigated by many workers, a useful method has only now been developed. Because water is transparent to visible light it cannot be decomposed directly, but only by radiation with wavelengths shorter than 190 nm (ref. 1).
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TiO(2) nanotubes can reproducibly store up to approximately 2 wt % H(2) at room temperature and 6 MPa. However, only about 75% of this stored hydrogen can be released when the hydrogen pressure is lowered to ambient conditions, suggesting that both physisorption and chemisorption are responsible for the hydrogen uptake. FTIR spectroscopy, temperature-programmed desorption (TPD), and pressure-composition (P-C) isotherms suggest that 75% of the H(2) is physisorbed and can be reversibly released upon pressure reduction. Approximately 13% is weakly chemisorbed and can be released at 70 degrees C as H(2), and approximately 12% is bonded to oxide ions and released only at temperatures above 120 degrees C as H(2)O.
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The sorption of hydrogen between the layers of the multilayered wall of nanotubular TiO2 was studied in the temperature range of -195 to 200 degrees C and at pressures of 0 to 6 bar. Hydrogen can intercalate between layers in the walls of TiO2 nanotubes forming host-guest compounds TiO2 x xH2, where x < or = 1.5 and decreases at higher temperatures. The rate of hydrogen incorporation increases with temperature and the characteristic time for hydrogen sorption in TiO2 nanotubes is several hours at 100 degrees C. The rate of intercalate formation is limited by the diffusion of molecular hydrogen inside the multilayered walls of the TiO2 nanotube. 1H NMR-MAS and XRD data confirm the incorporation of hydrogen between the layers in the walls of TiO2 nanotubes. The nature and possible applications of the observed intercalates are considered.
Article
Mg nanowires with the diameters of 30-50 nm, 80-100 nm, and 150-170 nm, which were prepared via a vapor-transport method, exhibited enhanced kinetics for hydrogen absorption/desorption. The present results clearly show that thinner Mg/MgH2 nanowires have a much lower desorption energy than that of thicker nanowires or bulk Mg/MgH2, indicating that changes in kinetics and thermodynamics are expected if the diameters of the nanowires are thinner than 30 nm.
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