13 research outputs found

    Structureā€“Property Relationships in the Y<sub>2</sub>O<sub>3</sub>ā€“ZrO<sub>2</sub> Phase Diagram: Influence of the Yā€‘Content on Reactivity in C1 Gases, Surface Conduction, and Surface Chemistry

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    The C1 chemistry of Y-doped ZrO<sub>2</sub> samples (3, 8, 20, and 40 mol % Y<sub>2</sub>O<sub>3</sub>; 3-YSZ, 8-YSZ, 20-YSZ, and 40-YSZ) was comparatively studied with respect to the correlation of electrochemical properties and surface chemistry in CH<sub>4</sub>, CO, and CO<sub>2</sub> atmospheres by electrochemical impedance (EIS) and spectroscopic (FT-IR) methods up to 1273 K to unravel the influence of the Y-doping level. A consistent picture with respect to qualitative and quantitative surface modifications as a function of temperature and gas-phase composition evolves by performing highly correlated <i>operando/in situ</i> measurements. A detailed study of carbon deposition in CH<sub>4</sub> and CO and adsorption of CO and CO<sub>2</sub>, but also proof of the strong influence of the surface chemistry, is included. Carbon deposition during treatment in CH<sub>4</sub> and CO at temperatures <i>T</i> ā‰„ 1023 K is a common feature on all materials, irrespective of the Y content. On the 40-YSZ sample, the thinnest, but at the same time fully percolated, carbon layer was generated, and hence, ā€œmetallicā€ conductivity was apparent. This goes along with the fact that 40-YSZ is most unreactive toward adsorption, suggesting a direct link between homogeneous deposition and suppressed reactivity. For all Y-doped samples, temperature regions with different charge carrier activation energies could be identified, perfectly corresponding to significant changes in surface chemistry. Due to the different degree of hydroxylation and the different ability to chemisorb CO and CO<sub>2</sub>, the influence of the surface chemistry on the electrochemical properties is varying strongly as a function of Y-content

    The Nanoscale Kirkendall Effect in Pd-Based Intermetallic Phases

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    Hollow particles of Pdā€“X intermetallic phases (X = Ga, Ge, Sn) are prepared by reduction of the respective oxide-supported Pd/XO<sub>2</sub> and Pd/X<sub>2</sub>O<sub>3</sub> thin films via the nanoscale Kirkendall effect. Void formation and stability was investigated by (scanning) high-resolution transmission electron microscopy and spectroscopy. Analysis of the selected area electron diffraction patterns after different reductive steps revealed a direct correlation of void size and stability with the composition of the respective intermetallic compounds. Voids only appear for Pd-rich Pd<sub>2</sub>X phases, whereas for intermetallic compounds of lower Pd content, PdX, the particles are solid again. Energy-filtered electron microscopic images show that the voids are indeed empty and formed by faster Pd outward diffusion compared to X inward diffusion

    Alloying and Structure of Ultrathin Gallium Films on the (111) and (110) Surfaces of Palladium

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    Growth, thermal stability, and structure of ultrathin gallium films on Pd(111) and Pd(110) are investigated by low-energy ion scattering and low-energy electron diffraction. Common to both surface orientations are growth of disordered Ga films at coverages of a few monolayers (<i>T</i> = 150 K), onset of alloy formation at low temperatures (<i>T</i> ā‰ˆ 200 K), and formation of a metastable, mostly disordered 1:1 surface alloy at temperatures around 400ā€“500 K. At higher temperatures a Ga surface fraction of āˆ¼0.3 is slightly stabilized on Pd(111), which we suggest to be related to the formation of Pd<sub>2</sub>Ga bulk-like films. While on Pd(110) only a Pd-up/Ga-down buckled surface was observed, an inversion of buckling was observed on Pd(111) upon heating. Similarities and differences to the related Zn/Pd system are discussed

    Reduction of Different GeO<sub>2</sub> Polymorphs

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    A combination of volumetric adsorption, thermal desorption and structure-determining methods was used to study and compare the hydrogen reduction behavior of three different GeO<sub>2</sub> polymorphs: tetragonal, water-free hexagonal, and water-containing (hydroxylated) commercial hexagonal GeO<sub>2</sub>. Marked differences in the onset and extent of reduction between the two water-free polymorphs have been observed. Tetragonal GeO<sub>2</sub> adsorbs more hydrogen at temperatures <i>T</i> ā‰¤ 673 K and tends to be more easily reducible at low temperatures, but extended Ge metal formation at elevated temperatures is rather suppressed compared to both hexagonal GeO<sub>2</sub> phases. Temperature-programmed hydrogen desorption spectra indicate the reduction-induced formation of weakly bonded hydrogen adsorption sites both on hydroxylated and pure hexagonal GeO<sub>2</sub>. The existence of the most weakly bonded hydrogen is linked to the transformation of initially present hydroxylated species into a tetragonal structure fraction upon annealing at āˆ¼500 K. Thus, analogous forms of hydrogen were not observed on any of the pure (dehydroxylated) structures

    Surface Reactivity of YSZ, Y<sub>2</sub>O<sub>3</sub>, and ZrO<sub>2</sub> toward CO, CO<sub>2</sub>, and CH<sub>4</sub>: A Comparative Discussion

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    The C1-surface chemistry of catalytically and technologically relevant oxides (YSZ, ZrO<sub>2</sub>, and Y<sub>2</sub>O<sub>3</sub>) toward CH<sub>4</sub>, CO, and CO<sub>2</sub> was comparatively studied by electrochemical impedance (EIS) and spectroscopic (FT-IR) methods. Highly correlated <i>in situ</i> measurements yield a consistent picture with respect to qualitative and quantitative surface modifications as a function of temperature and gas phase composition. This includes not only a detailed study of carbon deposition in methane and adsorption of CO and CO<sub>2</sub> but also proof of the strong influence of surface chemistry. On all studied oxides, carbon deposited during methane treatment grows dynamically forming interconnected islands and eventually a continuous conducting carbon layer at <i>T</i> ā‰„ 1073 K. Before methane dissociation via gas phase radical reactions/H-abstraction and carbon growth, a complex redox interplay of total oxidation as well as formate and carbonate formation leads to associated surface and grain conductivity changes. For CO adsorption, these measurements yield data on the time and temperature dependence of the adsorbate- and carburization-induced conductivity processes. In that respect, an equivalent circuit model in dry CO allows to disentangle the different contributions of grain interiors, grain boundaries, and electrode contributions. For YSZ, temperature regions with different charge carrier activation energies could be identified, perfectly corresponding to significant changes in surface chemistry. Hydroxyl groups, carbonates, or formates strongly influence the impedance properties, suggesting that the conductivity properties of YSZ, e.g., in a realistic reforming gas mixture, cannot be reduced to exclusive bulk ion conduction. Because of the different degree of hydroxylation and the different ability to chemisorb CO and CO<sub>2</sub>, the influence of the surface chemistry on the electrochemical properties is varying strongly: in contrast to ZrO<sub>2</sub>, the impact of the studied C1-gases on YSZ and Y<sub>2</sub>O<sub>3</sub> is substantial. This also includes the reoxidation/reactivation behavior of the surfaces

    In Situ FT-IR Spectroscopic Study of CO<sub>2</sub> and CO Adsorption on Y<sub>2</sub>O<sub>3</sub>, ZrO<sub>2</sub>, and Yttria-Stabilized ZrO<sub>2</sub>

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    In situ FT-IR spectroscopy was exploited to study the adsorption of CO<sub>2</sub> and CO on commercially available yttria-stabilized ZrO<sub>2</sub> (8 mol % Y, YSZ-8), Y<sub>2</sub>O<sub>3</sub>, and ZrO<sub>2</sub>. All three oxides were pretreated at high temperatures (1173 K) in air, which leads to effective dehydroxylation of pure ZrO<sub>2</sub>. Both Y<sub>2</sub>O<sub>3</sub> and YSZ-8 show a much higher reactivity toward CO and CO<sub>2</sub> adsorption than ZrO<sub>2</sub> because of more facile rehydroxylation of Y-containing phases. Several different carbonate species have been observed following CO<sub>2</sub> adsorption on Y<sub>2</sub>O<sub>3</sub> and YSZ-8, which are much more strongly bound on the former, due to formation of higher-coordinated polydentate carbonate species upon annealing. As the crucial factor governing the formation of carbonates, the presence of reactive (basic) surface hydroxyl groups on Y-centers was identified. Therefore, chemisorption of CO<sub>2</sub> most likely includes insertion of the CO<sub>2</sub> molecule into a reactive surface hydroxyl group and the subsequent formation of a bicarbonate species. Formate formation following CO adsorption has been observed on all three oxides but is less pronounced on ZrO<sub>2</sub> due to effective dehydroxylation of the surface during high-temperature treatment. The latter generally causes suppression of the surface reactivity of ZrO<sub>2</sub> samples regarding reactions involving CO or CO<sub>2</sub> as reaction intermediates

    Structural and Electrochemical Properties of Physisorbed and Chemisorbed Water Layers on the Ceramic Oxides Y<sub>2</sub>O<sub>3</sub>, YSZ, and ZrO<sub>2</sub>

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    A combination of operando Fourier transform infrared spectroscopy, operando electrochemical-impedance spectroscopy, and moisture-sorption measurements has been exploited to study the adsorption and conduction behavior of H<sub>2</sub>O and D<sub>2</sub>O on the technologically important ceramic oxides YSZ (8 mol % Y<sub>2</sub>O<sub>3</sub>), ZrO<sub>2</sub>, and Y<sub>2</sub>O<sub>3</sub>. Because the characterization of the chemisorbed and physisorbed water layers is imperative to a full understanding of (electro-)Ā­catalytically active doped oxide surfaces and their application in technology, the presented data provide the specific reactivity of these oxides toward water over a pressure-and-temperature parameter range extending up to, e.g., solid-oxide fuel cell (SOFC)-relevant conditions. The characteristic changes of the related infrared bands could directly be linked to the associated conductivity and moisture-sorption data. For YSZ, a sequential dissociative water (ā€œice-likeā€ layer) and polymeric chained water (ā€œliquid-likeā€) water-adsorption model for isothermal and isobaric conditions over a pressure range of 10<sup>ā€“5</sup> to 24 mbar and a temperature range from room temperature up to 1173 K could be experimentally verified. On pure monoclinic ZrO<sub>2</sub>, in contrast to highly hydroxylated YSZ and Y<sub>2</sub>O<sub>3</sub>, a high surface concentration of OH groups from water chemisorption is absent at any temperature and pressure. Thus, the ice-like and following molecular water layers exhibit no measurable protonic conduction. We show that the water layers, even under these rather extreme experimental conditions, play a key role in understanding the function of these materials. Furthermore, the reported data are supposed to provide an extended basis for the further investigation of close-to-real gas adsorption or catalyzed heterogeneous reactions

    Preferentially Oriented TiO<sub>2</sub> Nanotubes as Anode Material for Li-Ion Batteries: Insight into Li-Ion Storage and Lithiation Kinetics

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    Self-organized TiO<sub>2</sub> nanotubes (NTs) with a preferential orientation along the [001] direction are anodically grown by controlling the water content in the fluoride-containing electrolyte. The intrinsic kinetic and thermodynamic properties of the Li intercalation process in the preferentially oriented (PO) TiO<sub>2</sub> NTs and in a randomly oriented (RO) TiO<sub>2</sub> NT reference are determined by combining complementary electrochemical methods, including electrochemical impedance spectroscopy (EIS), cyclic voltammetry (CV), and galvanostatic cycling. PO TiO<sub>2</sub> NTs demonstrate an enhanced performance as anode material in Li-ion batteries due to faster interfacial Li insertion/extraction kinetics. It is shown that the thermodynamic properties, which describe the ability of the host material to intercalate Li ions, have a negligible influence on the superior performance of PO NTs. This work presents a straightforward approach for gaining important insight into the influence of the crystallographic orientation on lithiation/delithiation characteristics of nanostructured TiO<sub>2</sub> based anode materials for Li-ion batteries. The introduced methodology has high potential for the evaluation of battery materials in terms of their lithiation/delithiation thermodynamics and kinetics in general

    Metastable Corundum-Type In<sub>2</sub>O<sub>3</sub>: Phase Stability, Reduction Properties, and Catalytic Characterization

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    The phase stability, reduction, and catalytic properties of corundum-type rhombohedral In<sub>2</sub>O<sub>3</sub> have been comparatively studied with respect to its thermodynamically more stable cubic In<sub>2</sub>O<sub>3</sub> counterpart. Phase stability and transformation were observed to be strongly dependent on the gas environment and the reduction potential of the gas phase. As such, reduction in hydrogen caused both the efficient transformation into the cubic polymorph as well as the formation of metallic In especially at high reduction temperatures between 573 and 673 K. In contrast, reduction in CO suppresses the transformation into cubic In<sub>2</sub>O<sub>3</sub> but leads to a larger quantity of In metal at comparable reduction temperatures. This difference is also directly reflected in temperature-dependent conductivity measurements. Catalytic characterization of rh-In<sub>2</sub>O<sub>3</sub> reveals activity in both routes of the waterā€“gas shift equilibrium, which gives rise to a diminished CO<sub>2</sub>-selectivity of āˆ¼60% in methanol steam reforming. This is in strong contrast to its cubic counterpart where CO<sub>2</sub> selectivities of close to 100% due to the suppressed inverse waterā€“gas shift reaction, have been obtained. Most importantly, rh-In<sub>2</sub>O<sub>3</sub> in fact is structurally stable during catalytic characterization and no unwanted phase transformations are triggered. Thus, the results directly reveal the application-relevant physicochemical properties of rh-In<sub>2</sub>O<sub>3</sub> that might encourage subsequent studies on other less-common In<sub>2</sub>O<sub>3</sub> polymorphs

    Enhanced Kinetic Stability of Pure and Yā€‘Doped Tetragonal ZrO<sub>2</sub>

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    The kinetic stability of pure and yttrium-doped tetragonal zirconia (ZrO<sub>2</sub>) polymorphs prepared via a pathway involving decomposition of pure zirconium and zirconium + yttrium isopropoxide is reported. Following this preparation routine, high surface area, pure, and structurally stable polymorphic modifications of pure and Y-doped tetragonal zirconia are obtained in a fast and reproducible way. Combined analytical high-resolution in situ transmission electron microscopy, high-temperature X-ray diffraction, and chemical and thermogravimetric analyses reveals that the thermal stability of the pure tetragonal ZrO<sub>2</sub> structure is very much dominated by kinetic effects. Tetragonal ZrO<sub>2</sub> crystallizes at 400 Ā°C from an amorphous ZrO<sub>2</sub> precursor state and persists in the further substantial transformation into the thermodynamically more stable monoclinic modification at higher temperatures at fast heating rates. Lower heating rates favor the formation of an increasing amount of monoclinic phase in the product mixture, especially in the temperature region near 600 Ā°C and during/after recooling. If the heat treatment is restricted to 400 Ā°C even under moist conditions, the tetragonal phase is permanently stable, regardless of the heating or cooling rate and, as such, can be used as pure catalyst support. In contrast, the corresponding Y-doped tetragonal ZrO<sub>2</sub> phase retains its structure independent of the heating or cooling rate or reaction environment. Pure tetragonal ZrO<sub>2</sub> can now be obtained in a structurally stable form, allowing its structural, chemical, or catalytic characterization without in-parallel triggering of unwanted phase transformations, at least if the annealing or reaction temperature is restricted to <i>T</i> ā‰¤ 400 Ā°C
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