26 research outputs found

    Low-Temperature Dissociation of CO<sub>2</sub> on a Ni/CeO<sub>2</sub>(111)/Ru(0001) Model Catalyst

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    The adsorption of CO<sub>2</sub> on CeO<sub>2‑<i>x</i></sub>(111) and Ni/CeO<sub>2‑<i>x</i></sub>(111)/Ru­(0001) surfaces has been studied with reflection absorption infrared spectroscopy (RAIRS) and X-ray photoelectron spectroscopy (XPS). On the maximal-oxidized CeO<sub>2</sub>(111) surface physisorbed linear CO<sub>2</sub> and a CO<sub>2</sub><sup>–</sup> species are identified at 97 K. The reduced CeO<sub>2‑<i>x</i></sub>(111) surface exhibits higher reactivity toward adsorbed CO<sub>2</sub>, which leads to higher coverages of CO<sub>2</sub><sup>–</sup> and promotes CO<sub>2</sub> dissociating into CO and an active oxygen species at higher temperature, reoxidizing the reduced CeO<sub>2‑<i>x</i></sub>(111) films. Deposition of Ni on the maximal-oxidized CeO<sub>2</sub> thin films leads to slight reduction of ceria films. Adsorption of CO<sub>2</sub> on Ni/CeO<sub>2‑<i>x</i></sub>(111) films causes dissociation at 97 K and leads to Ni-CO adsorbates plus partial oxidation of Ni nanoparticles. This process is inhibited when Ni nanoparticles on CeO<sub>2</sub> are fully oxidized. In contrast to the results reported for CO<sub>2</sub> adsorption on Ni single-crystals, where the dissociation temperature was found to be higher than 240 K, the much lower dissociation temperature (∼97 K) for CO<sub>2</sub> on Ni nanoparticles supported on CeO<sub>2</sub>(111) suggests that the Ni/CeO<sub>2</sub> catalyst exhibits high activity toward CO<sub>2</sub> activation

    Structural and Optical Interplay of Palladium-Modified TiO<sub>2</sub> Nanoheterostructure

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    The electronic structure and optical properties of Pd-modified TiO<sub>2</sub> nanotubes (NTs) with a vertically aligned nanotubular structure grown by a two-step electrochemical anodization method have been studied using X-ray spectroscopy. X-ray absorption near-edge structure (XANES) at the Ti L<sub>3,2</sub>- and O K-edges was used to investigate the TiO<sub>2</sub> NTs before and after Pd modification. It was found that Pd nanoparticles (NPs) are uniformly coated on the NT surface. The Pd L<sub>3</sub>-edge of the deposited Pd NPs shows a more intense whiteline and a blue shift for the Pd L<sub>3</sub>-edge absorption threshold relative to Pd metal, indicating charge depletion from the Pd 4d orbital as a result NP formation. The lattice of Pd is slightly contracted upon NP formation, although it remains fcc as revealed by extended X-ray absorption fine structure (EXAFS) analysis at the Pd K-edge. X-ray-excited optical luminescence (XEOL) together with XANES with element and site specificity was used to study the optical luminescence from TiO<sub>2</sub> NTs. It was found that the defect-originated XEOL intensity dropped noticeably in the Pd NP-coated NTs, suggesting a Pd NP–TiO<sub>2</sub>-interaction-mediated reduction in the radiative recombination of electrons and holes. Further evidence is provided by Ti 2p resonant inelastic X-ray scattering (RIXS), in which no low-energy loss features (d–d transitions) were observed. The implications of these results are discussed

    Traces of Potassium Induce Restructuring of the Anatase TiO<sub>2</sub>(001)-(1×4) Surface from a Reactive to an Inert Structure

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    Reconstruction of solid surfaces is generally accompanied by changes in surface activities. Here, via a combined experimental and theoretical study, we successfully identified that a trace amount of potassium dopant restructures the mineral anatase TiO2(001) single-crystal surface from an added molecule (ADM) termination to an added oxygen (AOM) one without changing the (1×4) periodicity. The anatase TiO2(001)-(1×4)-ADM surface terminated with 4-fold coordinated Ti4c and 2-fold coordinated O2c sites is (photo)catalytically active, whereas the anatase TiO2(001)-(1×4)-AOM surface terminated with O2c and inaccessible 5-fold coordinated Ti5c sites is inert. These results unveiled a mechanism of dopant-induced transformation from a reactive to an inert TiO2(001)-(1×4) surface, which unifies the existing arguments about the surface structures and (photo)catalytic activity of anatase TiO2(001)-(1×4)

    Tracking the Local Effect of Fluorine Self-Doping in Anodic TiO<sub>2</sub> Nanotubes

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    We report herein a study in which we reveal the role of F<sup>–</sup> incorporated in the very anodic TiO<sub>2</sub> nanotubes prepared electrochemically from a Ti foil using a fluoride based electrolyte. X-ray absorption near edge structure (XANES), resonant X-ray emission spectroscopy (RXES), and X-ray photoelectron spectroscopy (XPS) have been used to examine the as-prepared and the annealed TiO<sub>2</sub> nanotubes. It is found that the additional electron resulting from the substitution of O<sup>2–</sup> by self-doped F<sup>–</sup> in the TiO<sub>2</sub> lattice is localized in the t<sub>2g</sub> state. Consequently, a localized Ti<sup>3+</sup> state can be tracked by a d–d energy loss peak with a constant energy of 1.6 eV in the RXES, in contrast to TiO<sub>2</sub> nanostructures where this peak is hardly noticeable when F<sup>–</sup> is driven out of the lattice upon annealing

    Traces of Potassium Induce Restructuring of the Anatase TiO<sub>2</sub>(001)-(1×4) Surface from a Reactive to an Inert Structure

    No full text
    Reconstruction of solid surfaces is generally accompanied by changes in surface activities. Here, via a combined experimental and theoretical study, we successfully identified that a trace amount of potassium dopant restructures the mineral anatase TiO2(001) single-crystal surface from an added molecule (ADM) termination to an added oxygen (AOM) one without changing the (1×4) periodicity. The anatase TiO2(001)-(1×4)-ADM surface terminated with 4-fold coordinated Ti4c and 2-fold coordinated O2c sites is (photo)catalytically active, whereas the anatase TiO2(001)-(1×4)-AOM surface terminated with O2c and inaccessible 5-fold coordinated Ti5c sites is inert. These results unveiled a mechanism of dopant-induced transformation from a reactive to an inert TiO2(001)-(1×4) surface, which unifies the existing arguments about the surface structures and (photo)catalytic activity of anatase TiO2(001)-(1×4)

    Confined Synthesis of Organometallic Chains and Macrocycles by Cu–O Surface Templating

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    The bottom-up construction of low-dimensional macromolecular nanostructures directly on a surface is a promising approach for future application in molecular electronics and integrated circuit production. However, challenges still remain in controlling the formation of these nanostructures with predetermined patterns (such as linear or cyclic) or dimensions (such as the length of one-dimensional (1D) chains). Here, we demonstrate that a high degree of structural control can be achieved by employing a Cu(110)-(2×1)O nanotemplate for the confined synthesis of organometallic chains and macrocycles. This template contains ordered arrays of alternating stripes of Cu–O chains and bare Cu, the widths of which are controllable. Using scanning tunneling microscopy and low-energy electron diffraction, we show that well-defined, ordered 1D zigzag organometallic oligomeric chains with uniform lengths can be fabricated on the Cu stripes (width >5.6 nm) of the Cu(110)-(2×1)O surface. In addition, the lengths of the <i>meta</i>-terphenyl (MTP)-based chains can be adjusted by controlling the widths of the Cu stripes within a certain range. When reducing the widths of Cu stripes to a range of 2.6 to 5.6 nm, organometallic macrocycles including tetramer (MTP-Cu)<sub>4</sub>, hexamer (MTP-Cu)<sub>6</sub>, and octamer (MTP-Cu)<sub>8</sub> species are formed due to the spatial confinement effect and attraction to the Cu–O chains. An overview of all formed organometallic macrocycles on the Cu stripes with different widths reveals that the origin of the formation of these macrocycles is the <i>cis</i>-configured organometallic dimer (MTP)<sub>2</sub>Cu<sub>3</sub>, which was observed on the extremely narrow Cu stripe with a width of 1.5 nm

    Interaction of Au with Thin ZrO<sub>2</sub> Films: Influence of ZrO<sub>2</sub> Morphology on the Adsorption and Thermal Stability of Au Nanoparticles

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    The model catalysts of ZrO<sub>2</sub>-supported Au nanoparticles have been prepared by deposition of Au atoms onto the surfaces of thin ZrO<sub>2</sub> films with different morphologies. The adsorption and thermal stability of Au nanoparticles on thin ZrO<sub>2</sub> films have been investigated using synchrotron radiation photoemission spectroscopy (SRPES) and X-ray photoelectron spectroscopy (XPS). The thin ZrO<sub>2</sub> films were prepared by two different methods, giving rise to different morphologies. The first method utilized wet chemical impregnation to synthesize the thin ZrO<sub>2</sub> film through the procedure of first spin-coating a zirconium ethoxide (Zr­(OC<sub>2</sub>H<sub>5</sub>)<sub>4</sub>) precursor onto a SiO<sub>2</sub>/Si­(100) substrate at room temperature followed by calcination at 773 K for 12 h. Scanning electron microscopy (SEM) investigations indicate that highly porous “sponge-like nanostructures” were obtained in this case. The second method was epitaxial growth of a ZrO<sub>2</sub>(111) film through vacuum evaporation of Zr metal onto Pt(111) in 1 × 10<sup>–6</sup> Torr of oxygen at 550 K followed by annealing at 1000 K. The structural analysis with low energy electron diffraction (LEED) of this film exhibits good long-range ordering. It has been found that Au forms smaller particles on the porous ZrO<sub>2</sub> film as compared to those on the ordered ZrO<sub>2</sub>(111) film at a given coverage. Thermal annealing experiments demonstrate that Au particles are more thermally stable on the porous ZrO<sub>2</sub> surface than on the ZrO<sub>2</sub>(111) surface, although on both surfaces, Au particles experience significant sintering at elevated temperatures. In addition, by annealing the surfaces to 1100 K, Au particles desorb completely from ZrO<sub>2</sub>(111) but not from porous ZrO<sub>2</sub>. The enhanced thermal stability for Au on porous ZrO<sub>2</sub> can be attributed to the stronger interaction of the adsorbed Au with the defects and the hindered migration or coalescence resulting from the porous structures

    Surface-Assisted Formation, Assembly, and Dynamics of Planar Organometallic Macrocycles and Zigzag Shaped Polymer Chains with C–Cu–C Bonds

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    The formation, structure, and dynamics of planar organometallic macrocycles (<i>meta</i>-terphenyl-Cu)<sub><i>n</i></sub> and zigzag-shaped one-dimensional organometallic polymers on a Cu(111) surface were studied with scanning tunneling microscopy (STM) and X-ray photoelectron spectroscopy (XPS). Vapor deposition of 4,4″-dibromo-<i>meta</i>-terphenyl (DMTP) onto Cu(111) at 300 K leads to C–Br bond scission and formation of C–Cu–C bonds, which connect neighboring <i>meta</i>-terphenyl fragments such that room-temperature stable macrocycles and zigzag chains are formed. The chains self-assemble to form islands, which are elongated in the direction of the chains. If DMTP is deposited onto Cu(111) held at 440 K, the island size is drastically increased (>200 × 200 nm<sup>2</sup>). STM sequences show the formation of ordered structures through reversible scission and reformation of the C–Cu–C bonds. The cyclic organometallic species such as the hexamer (<i>meta</i>-terphenyl-Cu)<sub>6</sub> may represent intermediates in the surface-confined Ullmann synthesis of hydrocarbon macrocycles such as the recently discovered hyperbenzene

    Unravelling the Mechanism of Glaser Coupling Reaction on Ag(111) and Cu(111) Surfaces: a Case for Halogen Substituted Terminal Alkyne

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    The mechanisms of Glaser coupling reaction on metal surfaces have been poorly understood. Herein, we propose a reaction pathway toward surface-confined Glaser coupling which is initiated by single-molecule dehydrogenation of terminal alkyne. This is inspired by our experimental observations of alkynyl–Ag–alkynyl and alkynyl–Cu–alkynyl type organometallic intermediates in the coupling reaction of 1,1′-biphenyl,4-bromo-4′-ethynyl (BPBE) on Ag(111) and Cu(111), respectively. Theoretical calculations reveal that the dehydrogenation process of terminal ethynyl of BPBE is most likely catalyzed by a stray H adatom on Ag(111) but by a Cu adatom on Cu(111), followed by the formation of the organometallic intermediates. After the release of interstitial metal adatoms, the final C–C coupling occurs easily on Ag(111) but shows extremely low efficiency on Cu(111), due to the too strong interaction between ethynylene and the Cu(111) substrate

    Interplay between Interfacial Structures and Device Performance in Organic Solar Cells: A Case Study with the Low Work Function Metal, Calcium

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    A better understanding of how interfacial structure affects charge carrier recombination would benefit the development of highly efficient organic photovoltaic (OPV) devices. In this paper, transient photovoltage (TPV) and charge extraction (CE) measurements are used in combination with synchrotron radiation photoemission spectroscopy (SRPES) to gain insight into the correlation between interfacial properties and device performance. OPV devices based on PCDTBT/PC<sub>71</sub>BM with a Ca interlayer were studied as a reference system to investigate the interfacial effects on device performance. Devices with a Ca interlayer exhibit a lower recombination than devices with only an Al cathode at a given charge carrier density (<i>n</i>). In addition, the interfacial band structures indicate that the strong dipole moment produced by the Ca interlayer can facilitate the extraction of electrons and drive holes away from the cathode/polymer interface, resulting in beneficial reduction in interfacial recombination losses. These results help explain the higher efficiencies of devices made with Ca interlayers compared to that without the Ca interlayer
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