29 research outputs found

    Origin of Coverage Dependence in Photoreactivity of Carboxylate on TiO<sub>2</sub>(110): Hindering by Charged Coadsorbed Hydroxyls

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    The influence of reactant coverage on photochemical activity was explored using scanning tunneling microscopy (STM) and ultraviolet photoelectron spectroscopy (UPS). We observed diminished reactivity of carboxylate species (trimethyl acetate, TMA) on TiO<sub>2</sub>(110) as a function of increasing coverage. This effect was not linked to intermolecular interactions of TMA but to the accumulation of the coadsorbed bridging hydroxyls (HO<sub>b</sub>) deposited during (thermal) dissociative adsorption of the parent, trimethylacetic acid (TMAA). Confirmation of the hindering influence of HO<sub>b</sub> groups was obtained by the observation that HO<sub>b</sub> species originated from H<sub>2</sub>O dissociation at O-vacancy sites have a similar hindering effect on TMA photochemistry. Though HO<sub>b</sub>’s are photoinactive on TiO<sub>2</sub>(110) under ultrahigh vacuum conditions, UPS results show that these sites trap photoexcited electrons, which in turn likely (electrostatically) attract and neutralize photoexcited holes, thus suppressing the hole-mediated photoreactivity of TMA. This negative influence of surface hydroxyls on hole-mediated photochemistry is likely a major factor in other anaerobic photochemical processes on reducible oxide surfaces

    Direct Observation of Site-Specific Molecular Chemisorption of O<sub>2</sub> on TiO<sub>2</sub>(110)

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    Molecularly chemisorbed O<sub>2</sub> species were directly imaged on reduced TiO<sub>2</sub>(110) at 50 K with high-resolution scanning tunneling microscopy (STM). Two different O<sub>2</sub> adsorption channels, one at bridging oxygen vacancies (V<sub>O</sub>) and another at 5-fold coordinated terminal titanium atoms (Ti<sub>5c</sub>), have been identified. While O<sub>2</sub> species at the Ti<sub>5c</sub> site appears as a single protrusion centered on the Ti<sub>5c</sub> row, the O<sub>2</sub> at V<sub>O</sub> manifests itself by a disappearance of the V<sub>O</sub> feature. It is found that the STM tip can easily dissociate O<sub>2</sub> species, unless extremely low magnitude of the tunneling parameters are used. The O<sub>2</sub> molecules chemisorbed at low temperatures at these two distinct sites are the most likely precursors for the two O<sub>2</sub> dissociation channels, observed at temperatures above 150 and 230 K at the V<sub>O</sub> and Ti<sub>5c</sub> sites, respectively

    Characterization of the Active Surface Species Responsible for UV-Induced Desorption of O<sub>2</sub> from the Rutile TiO<sub>2</sub>(110) Surface

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    We have examined the chemical and photochemical properties of molecular oxygen on the (110) surface of rutile TiO<sub>2</sub> at 100 K using electron energy loss spectroscopy (EELS), photon stimulated desorption (PSD), and scanning tunneling microscopy (STM). Oxygen chemisorbs on the TiO<sub>2</sub>(110) surface at 100 K through charge transfer from surface Ti<sup>3+</sup> sites. The charge-transfer process is evident in EELS by a decrease in the intensity of the Ti<sup>3+</sup> d-to-d transition at ∼0.9 eV and formation of a new loss at ∼2.8 eV. On the basis of comparisons with the available homogeneous and heterogeneous literature for complexed/adsorbed O<sub>2</sub>, the species responsible for the 2.8 eV peak can be assigned to a surface peroxo (O<sub>2</sub><sup>2–</sup>) state of O<sub>2</sub>. This species was identified as the active form of adsorbed O<sub>2</sub> on TiO<sub>2</sub>(110) for PSD. The adsorption site of this peroxo species was assigned to that of a regular five-coordinated Ti<sup>4+</sup> (Ti<sub>5c</sub>) site based on comparisons between the UV exposure-dependent behavior of O<sub>2</sub> in STM, PSD, and EELS data. Assignment of the active form of adsorbed O<sub>2</sub> to a peroxo species at normal Ti<sub>5c</sub> sites necessitates reevaluation of the simple mechanism in which a single valence band hole neutralizes a singly charged O<sub>2</sub> species (superoxo or O<sub>2</sub><sup>–</sup>), leading to desorption of O<sub>2</sub> from a physisorbed potential energy surface

    Diffusion and Photon-Stimulated Desorption of CO on TiO<sub>2</sub>(110)

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    Thermal diffusion of CO adsorbed on rutile TiO<sub>2</sub>(110) was studied in the 20–110 K range using photon-stimulated desorption (PSD), temperature-programmed desorption (TPD), and scanning tunneling microscopy. During UV irradiation, CO desorbs from certain photoactive sites (e.g., oxygen vacancies). This phenomenon was exploited to study CO thermal diffusion in three steps: first, empty these sites during a first irradiation cycle, then replenish them with CO during annealing, and finally probe the active site occupancy in the second PSD cycle. The PSD and TPD experiments show that the CO diffusion rate correlates with the CO adsorption energystronger binding corresponds to slower diffusion. Increasing the CO coverage from 0.06 to 0.44 monolayer (ML) or hydroxylation of the surface decreases the CO binding and increases the CO diffusion rate. Relative to the reduced surface, the CO adsorption energy increases and the diffusion decreases on the oxidized surface. The CO diffusion kinetics can be modeled satisfactorily as an Arrhenius process with a “normal” prefactor (i.e., ν = 10<sup>12</sup> s<sup>–1</sup>) and a Gaussian distribution of activation energies where the peak of the distribution is ∼0.26 eV and the full width at half-maximum (fwhm) is ∼0.1 eV at the lowest coverage. The observations are consistent with a significant electrostatic component of the CO binding energy on the TiO<sub>2</sub>(110) surface which is affected by changes in the surface dipole and dipole–dipole interactions

    Deprotonated Water Dimers: The Building Blocks of Segmented Water Chains on Rutile RuO<sub>2</sub>(110)

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    Despite the importance of RuO<sub>2</sub> in photocatalytic water splitting and catalysis in general, the interactions of water with even its most stable (110) surface are not well understood. In this study we employ a combination of high-resolution scanning tunneling microscopy imaging with density functional theory based <i>ab initio</i> molecular dynamics, and we follow the formation and binding of linear water clusters on coordinatively unsaturated ruthenium rows. We find that clusters of all sizes (dimers, trimers, tetramers, extended chains) are stabilized by donating one proton per every two water molecules to the surface bridge bonded oxygen sites, in contrast with water monomers that do not show a significant propensity for dissociation. The clusters with odd number of water molecules are less stable than the clusters with even number and are generally not observed under thermal equilibrium. For all clusters with even numbers, the dissociated dimers represent the fundamental building blocks with strong intradimer hydrogen bonds and only very weak interdimer interactions resulting in segmented water chains

    Light Makes a Surface Banana-Bond Split: Photodesorption of Molecular Hydrogen from RuO<sub>2</sub>(110)

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    The coordination of H<sub>2</sub> to a metal center via polarization of its σ bond electron density, known as a Kubas complex, is the means by which H<sub>2</sub> chemisorbs at Ru<sup>4+</sup> sites on the rutile RuO<sub>2</sub>(110) surface. This distortion of electron density off an interatomic axis is often described as a ‘banana-bond.’ We show that the Ru–H<sub>2</sub> banana-bond can be destabilized and split using visible light. Photodesorption of H<sub>2</sub> (or D<sub>2</sub>) is evident by mass spectrometry and scanning tunneling microscopy. From time-dependent density functional theory, the key optical excitation splitting the Ru–H<sub>2</sub> complex involves an interband transition in RuO<sub>2</sub> which effectively diminishes its Lewis acidity, thereby weakening the Kubas complex. Such excitations are not expected to affect adsorbates on RuO<sub>2</sub> given its metallic properties. Therefore, this common thermal cocatalyst employed in photocatalysis is, itself, photoactive
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