AVS2012 Session SS-TuM: Surface Reactivity of Oxides
Time Period TuM Sessions | Abstract Timeline | Topic SS Sessions | Time Periods | Topics | AVS2012 Schedule
Start | Invited? | Item |
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8:00 AM | Invited |
SS-TuM-1 Preparation, Characterization and Catalytic Activity of Model WO3 Catalysts
Zdenek Dohnalek (Pacific Northwest National Laboratory) Supported early transition metal oxides have important applications in numerous catalytic reactions. In our studies, conversion of small aliphatic alcohols to alkenes, aldehydes/ketons, and ethers is employed to probe the structure-activity relationships on model WO3 catalysts. To understand how the structure and binding of WO3 species affect catalytic properties we prepared a number of well-characterized systems. Direct sublimation of WO3 solid was used to generate cyclic gas-phase ( WO3)3 clusters. As shown in our matrix isolation experiments, sublimation leads to pure (WO3)3 clusters. The ( WO3)3 clusters were embedded in alcohol matrices and their support-free chemistry was explored in subsequent temperature programmed reaction experiments. Model supported catalysts were created by depositing (WO3)3 clusters on TiO2(110) and FeO(111) and subsequently characterized using scanning tunneling microscopy and surface sensitive spectroscopies. In other studies, epitaxial and nanoporous thin WO3 films were prepared on Pt(111). The catalytic chemistry of all the systems is compared and contrasted with that observed on unsupported (WO3)3 clusters. Calculations employing Density Functional Theory provide molecular-level mechanistic insight into the role structure and binding of (WO3)3 clusters to the support plays in determining their catalytic properties. This work was supported by the US Department of Energy, Office of Basic Energy Sciences, Division of Chemical Sciences, Geosciences & Biosciences and performed in Environmental Molecular Sciences Laboratory (EMSL), a national scientific user facility sponsored by the Department of Energy's Office of Biological and Environmental Research and located at Pacific Northwest National Laboratory (PNNL). PNNL is a multiprogram national laboratory operated for DOE by Battelle. |
8:40 AM |
SS-TuM-3 EUV Photon Enhanced Oxidation of Carbonaceous Layer at a TiO2 Film Surface
Nadir Faradzhev, John T. Yates, Jr. (University of Virginia); Shannon Hill, Thomas Lucatorto (National Institute of Standards and Technology) We report the photo oxidation of a carbonaceous layer originally grown by 92 eV radiation-induced chemistry. The C film is supported on a surface of a nm thick amorphous TiO2 film. Photo oxidation is achieved using various oxygen-containing molecules. The TiO2 film mimics one of the possible protective layers of EUV Lithography optics, and the C film mimics optics contamination produced by 92 eV photons in a EUVL stepper apparatus. The C layer (~4 nm) is deposited by photodecomposition of the linear hydrocarbon molecule, n-tetradecane, using the NIST synchrotron ultraviolet facility (SURF III) in an UHV cell. The kinetics of C growth and C removal are monitored in real time using in situ single wavelength ellipsometric measurements. After each set of experiments, ex-situ XPS is used to detect the residual thickness of the carbonaceous film and the changes in its chemical state. We found that exposure to a vapor beam of several O-containing molecules has little or no effect on the C film in the dark. In the presence of EUV photons, the ability of these molecules to volatilize carbon as either CO or CO2 increases significantly. The carbon removal rate increases with the partial pressure of the oxidizer. The substrate temperature has little effect on the carbon removal rate and this is in contrast to the rate of radiation-induced C growth that exhibits a very strong temperature dependence. The rate of removal of C depends upon the EUV irradiation and does not occur appreciably in the dark. Although the studies are not finished yet, our results indicate that processes of C growth and C removal may proceed via different routes. In an earlier study, we found that during C growth, the hydrocarbon molecule arrives at the surface in its ground state and forms a weak bond to the bare or C- covered TiO2 surface. The molecule is not trapped permanently and will thermally desorb within a characteristic time. It can also be either photo-desorbed or photo-decomposed to produce the carbonaceous film via direct (photo excitation) or indirect (secondary electron excitation, e.g. DEA) processes. For photo oxidation, the first step requires the formation of a strong bond of the oxidizer molecule to the surface. An oxidizer molecule will either arrive at the surface in an electronically excited molecular state or arrive in its ground state and find an EUV-activated long-lived electronically excited state at the surface. In both cases, the oxidizer molecule will stay on the surface for a sufficiently long time to decompose and react to produce a volatile product (e.g. CO). This study is being performed as a part of EUVL Contamination cooperative research at NIST and UVA. |
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9:00 AM |
SS-TuM-4 Reactions of Water with Vacuum Fracture Surfaces of Sodium-Aluminosilicate Glass: Effects of Composition on Reactivity
Kaveh Adib, James Dickinson (Corning Incorporated) We have synthesized different ternary SiO2:Al2O3:Na2O glasses containing bridging oxygens and non-bridging oxygens (NBO) and fractured them in ultrahigh vacuum to produce pristine surfaces. X-ray photoelectron spectroscopy of oxygen core levels and valence band were used to determine the fraction of non-bridging oxygens (SiONa) to bridging oxygens (SiOSi and SiOAl) on the vacuum fractured surfaces. For those glasses where the NBO fractions of the total oxygen were held constant, a 0.2 eV variance was observed in the binding energies of the NBO O1s core levels consistent with substantial changes, as a function of composition, in the ionicity of the bond between the NBO and sodium. The fracture surfaces were then exposed to partial pressures of H2O at ambient temperature. It was observed that water reacts primarily with the NBO’s to produce SiOH in place of SiONa. Non-bridging oxygens from glass compositions that contained less alumina had lower electron binding energy and were more likely to react with water. Molecular dynamics simulations were used to elucidate the role of H3O+ in the reaction of water with the non-bridging oxygens. |
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9:20 AM |
SS-TuM-5 Reactivity of Highly-hydroxylated TiO2(110) Surface Prepared via Carboxylic Acid Adsorption and Photolysis
Igor Lyubinetsky, Yingge Du, Nikolay Petrik (Pacific Northwest National Laboratory); N. Aaron Deskins (Worcester Polytechnic Institute); Zhi-Tao Wang, Michael Henderson, Greg Kimmel (Pacific Northwest National Laboratory) We present a novel, photochemical approach to prepare a highly-hydroxylated TiO2(110) and discuss the reactivity of the resulting surface. TiO2(110) surfaces with an OHb coverages up to 0.5 ML have been obtained upon trimethyl acetic acid (TMAA) dissociative adsorption and subsequent photolysis at 300 K. The formation and chemistry of such surface have been examined at the atomic level by a combination of scanning tunneling microscopy, temperature-programmed desorption, photo stimulated desorption, and density functional theory methods. Deprotonation of TMAA molecules upon adsorption produces both surface bridging hydroxyls (OHb) and bidentate trimethyl acetate (TMA) species with saturation coverage of near 0.5 ML. The TMA species can be selectively removed by ultra-violet light irradiation while OHb’s survive photolysis. At high coverages, the OHb species typically occupy second-nearest neighbor sites along the bridging oxygen row locally forming linear (2´1) structures of different lengths, although the surface is less ordered on a long scale. The annealing of the highly-hydroxylated surface leads to hydroxyl recombination and H2O desorption with ~100% yield, thus ruling out the diffusion of H into the bulk. In agreement with experimental data, theoretical results show that the recombinative H2O desorption is preferred over both H bulk diffusion and H2 desorption processes. |
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9:40 AM |
SS-TuM-6 Infrared Spectroscopy of CO2 Adsorbed on TiO2(110)
Nikolay Petrik, Greg Kimmel (Pacific Northwest National Laboratory) We have studied the adsorption of CO2 on TiO2(110) using reflection-absorption infrared spectroscopy (RAIRS) and temperature programmed desorption (TPD). Infrared spectra were obtained for s- and p-polarized light with the plane of incidence parallel and perpendicular to the [001] azimuth of TiO2(110). As a result, the RAIRS provide detailed information on the adsorption geometry for the CO2 versus coverage. Initially, CO2 adsorbs in vacancies in the bridge-bonded oxygen (BBO) rows with the peak for the asymmetric stretch seen at 2346.5 cm-1 for both s- and p-polarized light. Hydroxylation or oxidation of the vacancies suppresses this feature. After filling the vacancies, CO2 adsorbs on Ti5c sites (CO2(Ti)). The asymmetric stretch for CO2(Ti) starts at ~2342 cm-1 and then red-shifts to 2332 cm-1 at 1 ML. CO2 TPD spectra show that the shift in the RAIRS spectra correlates with a decrease in the CO2 binding energy from ~47 to ~34 kJ/mol as the coverage increases from 0 to 1 ML. For CO2(Ti), the absorbances for the s-polarized spectra are similar for both azimuths indicating that the ensemble-average of the adsorbed CO2 has approximately equal components along both azimuths. The p-polarized RAIRS spectra show that CO2(Ti) also adsorbs with a component normal to the surface. Between 1 and 1.5 ML, CO2 adsorbs on BBO sites. These CO2 absorb only s-polarized light with its plane of incidence parallel to the BBO rows indicating that the molecules are oriented parallel to the surface and perpendicular to the BBO rows. The CO2 RAIRS spectra are compared with STM results and DFT theory to provide detailed insight into its molecular orientation and coverage-dependent mobility. |
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10:00 AM | BREAK - Complimentary Coffee in Exhibit Hall | |
10:40 AM |
SS-TuM-9 Low-temperature Dissociation of CO2 on Ni/CeO2/Ru(0001) Model Catalyst
Dandan Kong (University of Science and Technology of China); Karl-Heinz Ernst (EMPA, Switzerland); Junfa Zhu (University of Science and Technology of China) Model Ni/CeO2 (111) catalysts were prepared by depositing nickel atoms onto well-ordered cerium oxide films grown on Ru(0001) and were investigated using photoelectron spectroscopy (XPS) and reflection absorption infrared spectroscopy (RAIRS). It is found that the fully oxidized CeO2 thin films are slightly reduced to CeO1.97 after 0.2 ML Ni deposition. When CO2 is exposed to the surface of clean CeO2(111) film at 97 K, the physisorbed linear molecular CO2 and carboxylate species are observed. However, on the CeO2(111) surface covered with 0.6 ML Ni, CO2 immediately dissociates upon adsorption at 97 K, leading to the formation of Ni-CO adsorbates and partial oxidation of Ni nanoparticles. This dissociation activation of CO2 is inhibited when Ni nanoparticles on CeO2 are pre-oxidzied. In contrast to the results reported for CO2 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 CO2 on Ni nanoparticles supported on CeO2(111) suggests that the Ni/CeO2 catalyst exhibits high activity toward CO2 activation. |
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11:00 AM |
SS-TuM-10 Adsorption and Diffusion of Acetone on Rutile TiO2 (110)
Bo Zhang, Yaobiao Xia (Baylor University); Jingyun Ye, Qingfeng Ge (Southern Illinois University Carbondale); Zhenrong Zhang (Baylor University) Understanding the surface reaction processes of acetone on metal oxide surfaces is important for photo-oxidation of toxic organic molecules. We have studied the adsorption and the diffusion of acetone on reduced rutile TiO2(110) surfaces using variable temperature scanning tunneling microscopy (STM). At room temperature (RT) acetone molecules prefer to adsorb on bridging-bonded oxygen vacancy sites. The sequential isothermal STM images show that acetone molecules are mobile at RT. They hop between unoccupied vacancy sites via both apparent along-row diffusion and apparent cross-row diffusion processes. Images obtained at temperatures below RT show that there are two barriers involved in these diffusion processes: (1) the diffusion barrier along the Ti row, and (2) the barrier from the vacancy site to the neighboring Ti row. The latter is the rate limiting step. DFT calculations agree with experimental results. |
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11:20 AM |
SS-TuM-11 Variations in Reactivity for Acetaldehyde and Acetic Acid with the Crystallographic Orientation of Cerium Oxide Thin Films
Peter Albrecht, David Mullins (Oak Ridge National Laboratory) Cerium oxide is a vital component in many heterogeneous catalytic processes. The various crystallographic faces of ceria present significantly different surface structures and compositions, which may result in an orientation-dependent catalytic reactivity. The structure and composition determine the availability of adsorption sites, the spacing between those adsorption sites, and the ability of surface O to participate in a reaction. |
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11:40 AM |
SS-TuM-12 The Entropies of Adsorbed Molecules
Charles Campbell, Jason Sellers (University of Washington) Adsorbed molecules are involved in many reactions on solid surface that are of great technological importance. As such, there has been tremendous effort worldwide to learn how to predict reaction rates and equilibrium constants for reactions involving adsorbed molecules. Theoretical calculation of both the rate constant and equilibrium constant for such reactions require knowing the standard entropy and enthalpy of the adsorbed molecule. While much effort has been devoted to measuring and calculating the enthalpies of well-defined adsorbates, few measurements of the entropies of adsorbates have been reported. We present here a new way to determine the standard entropies of adsorbed molecules (Sad0) on single crystal surfaces from temperature programmed desorption data, prove its accuracy by comparison to entropies directly measured using equilibrium adsorption isotherms on MgO(100), and apply it to published data to extract new entropies. Most importantly, when combined with reported entropies, we find that at high coverage they linearly track the entropy of the gas-phase molecule at the same temperature (T) as: Sad0(T) = 0.70 Sgas0(T)–3.29R, with a standard deviation of only 2R from 0 to 60R, where R is the gas constant. These entropies, which are ~2/3 of that for the gas, are huge compared to most theoretical predictions (e.g. the harmonic approximation commonly employed in combination with DFT estimates of reaction barriers). This relationship applies at temperatures where desorption rates are fast enough to perform EAI and TPD measurements (~10-3 to 100 monolayers/s). It provides an important tool to aid in estimating equilibrium constants and rate constants for reactions where these adsorbates are involved, as proven here for prefactors in the Arrhenius rate constant for desorption. The prefactor can be estimated as : ν = (kBT/h) exp{0.30 Sgas0(T)/R + 3.29 - 9.31 ln[(m/mAr)(T/298K)]}, where m/mAr is the mass of the adsorbate relative to Ar. For longer adsorbed molecules where Sgas0(T) exceeds 60 K (e.g. linear alkanes with >11 carbons), their entropies remain a constant 20.7R below gas entropies, and ~10.4R below Trouton’s Rule for liquid entropies. Work supported by NSF under CHE-1010287. |