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  • 1
    Online Resource
    Online Resource
    San Diego :Elsevier Science & Technology,
    Keywords: Grenzfl'achenchemie. ; Electronic books.
    Type of Medium: Online Resource
    Pages: 1 online resource (533 pages)
    Edition: 1st ed.
    ISBN: 9780080551913
    DDC: 541.2242
    Language: English
    Note: Front Cover -- Chemical Bonding at Surfaces and Interfaces -- Copyright Page -- Table of Contents -- Preface -- Chapter 1 Surface Structure -- 1. Why surface structure? -- 2. Methods of surface adsorbate structure determination -- 2.1. General comments -- 2.2. Electron scattering -- 2.3. X-ray scattering -- 2.4. Ion scattering -- 2.5. Spectroscopic methods and scanning probe microscopy -- 3. Adsorbate-induced surface reconstruction -- 4. Molecular adsorbates - local sites, orientations and intramolecular bondlengths -- 4.1. General issues and the case of CO on metals -- 4.2. Simple hydrocarbons on metals -- 4.3. Carboxylates on metals -- 4.4. Other substrates: molecules on Si -- 5. Chemisorption bondlengths -- 5.1. Metal surfaces -- 5.2. Oxide surfaces -- 6. Conclusions -- Chapter 2 Adsorbate Electronic Structure and Bonding on Metal Surfaces -- 1. Introduction -- 2. Probing the electronic structure -- 3. Adsorbate electronic structure and chemical bonding -- 4. Adsorbate systems -- 5. Radical atomic adsorption -- 5.1. The electronic structure of N on Cu(100) -- 5.2. Chemical bonding of atomic adsorbates -- 6. Diatomic molecules -- 6.1. N2 adsorbed on Ni(100) -- 6.2. CO adsorbed on Ni(100) -- 6.3. CO adsorbed on Cu(100) and other metals -- 6.4. CO adsorbed in different sites -- 6.5. Coadsorption of CO and K on Ni(100) -- 7. Unsaturated hydrocarbons -- 7.1. Ethylene (C2H4) adsorbed on Ni(110) and Cu(110) -- 7.2. Benzene on Ni and Cu surfaces -- 7.3. Bond energetics and rehybridization from spin-uncoupling -- 8. Saturated hydrocarbons -- 8.1. n-Octane adsorbed on Cu(110) -- 8.2. Difference between octane on Ni and Cu surfaces -- 9. Lone pair interactions -- 9.1. Water adsorption on Pt and Cu surfaces -- 9.2. Adsorption of ammonia and the amino group in glycine on Cu(110) -- 10. Summary. , Chapter 3 The Dynamics of Making and Breaking Bonds at Surfaces -- 1. Introduction -- 2. Theoretical background -- 2.1. Adiabatic dynamics (Born-Oppenheimer approximation) -- 2.2. Generic PES topologies -- 2.3. Dynamics vs. kinetics -- 2.3.1. Direct dissociation -- 2.3.2. Precursor-mediated dissociation -- 2.4. Detailed balance -- 2.5. Lattice coupling -- 2.5.1. Energy transfer in adsorption/scattering -- 2.5.2. Lattice coupling in direct molecular dissociation -- 2.6. Non-adiabatic dynamics -- 2.6.1. Hot electrons from chemistry -- 2.6.2. Chemistry from hot electrons -- 3. Experimental background -- 3.1. Experimental techniques -- 3.2. Typical measurements -- 3.2.1. Rate measurements -- 3.2.2. Adsorption-trapping and sticking -- 3.2.3. Desorption -- 3.2.4. Scattering -- 3.2.5. Initial state preparation -- 3.2.6. Photochemistry/femtochemistry -- 3.2.7. Single molecule chemistry (STM) -- 4. Processes -- 4.1. Atomic adsorption/desorption/scattering -- 4.1.1. Ar/Pt(111) -- 4.1.2. H/Cu(111) -- 4.2. Molecular adsorption/desorption/scattering -- 4.2.1. NO/Ag(111) -- 4.2.2. NO/Pt(111) -- 4.3. Direct dissociation/associative desorption -- 4.3.1. Activated dissociation -- 4.3.2. Weakly activated dissociation -- 4.3.3. Non-activated dissociation -- 4.4. Precursor-mediated dissociation/associative desorption -- 4.4.1. O2/Pt(111) -- 4.5. Direct and precursor-mediated dissociation -- 4.5.1. N2/W(100) -- 4.5.2. NH3/Ru(0001) -- 4.6. Langmuir-Hinschelwood chemistry -- 4.6.1. (O+CO)/Pt(111) -- 4.7. Eley-Rideal/Hot atom chemistry -- 4.7.1. H+H/Cu(111) -- 4.8. Hot electron chemistry -- 4.8.1. Photochemistry/femtochemistry -- 4.8.2. Single molecule chemistry -- 5. Summary and outlook -- Chapter 4 Heterogeneous Catalysis -- 1. Introduction -- 2. Factors determining the reactivity of a transition metal surface. , 3. Trends in adsorption energies on transition metal surfaces -- 4. The d-band model -- 4.1. One-electron energies and bond energy trends -- 4.2. The Newns-Anderson model -- 5. Trends in chemisorption energies -- 5.1. Variations in adsorption energies from one metal to the next -- 5.2. Ligand effects in adsorption - changing the d band center -- 5.2.1. Variations due to changes in surface structure -- 5.2.2. Variations due to alloying -- 5.3. Ensemble effects in adsorption - the interpolation principle -- 6. Trends in activation energies for surface reactions -- 6.1. Electronic effects in surface reactivity -- 6.2. Geometrical effects in surface reactivity -- 7. Brønsted-Evans-Polanyi relationships in heterogeneous catalysis -- 7.1. Correlations from DFT calculations -- 7.2. Universal relationships -- 8. Activation barriers and rates -- 8.1. Transition state theory -- 8.2. Variational transition state theory and recrossings -- 8.3. Harmonic transition state theory (HTST) -- 9. Variations in catalytic rates - volcano relations -- 9.1. Dissociation rate-determined model -- 9.2. A Le Chatelier-like principle for heterogeneous catalysis -- 9.3. Including molecular precursor adsorption -- 9.4. Sabatier analysis -- 9.5. A realistic desorption model -- 9.6. Database of chemisorption energies -- 10. The optimization and design of catalyst through modeling -- 10.1. The low-temperature water gas shift (WGS) reaction -- 10.2. Methanation -- 11. Conclusions and outlook -- Chapter 5 Semiconductor Surface Chemistry -- 1. Inroduction -- 2. Structure of semiconductor surfaces -- 2.1. Silicon surface structure -- 2.2. Germanium surface structure -- 3. Surface oxidation -- 3.1. Silicon -- 3.2. Germanium -- 4. Passivation of semiconductor surfaces -- 4.1. Silicon passivation -- 4.1.1. Hydride termination of silicon -- 4.2. Germanium passivation. , 4.2.1. Sulfide passivation of germanium -- 4.2.2. Chloride passivation of germanium -- 4.2.3. Hydride termination of germanium -- 5. Reactions at passivated semiconductor surfaces -- 5.1. Organic functionalization of semiconductor surface -- 5.2. Reaction with passivated silicon (Si−H and Si−Cl) -- 5.2.1. Hydrosilylation -- 5.2.2. Grignard reactions on silicon -- 5.3. Reaction with passivated germanium (Ge−H and Ge−Cl) -- 5.3.1. Grignard reactions on germanium -- 5.3.2. Hydrogermylation -- 5.3.3. Alkanethiol reactions on germanium -- 5.4. Reaction with compound semiconductors -- 6. Adsorption of organic molecules under vacuum conditions -- 6.1. Silicon surface chemistry -- 6.1.1. Cycloaddition reaction on Si(100)-2×1 -- 6.1.2. Heterocycloadditions -- 6.1.3. Nucleophilic/electrophilic reactions -- 6.2. Germanium surface chemistry -- 6.2.1. Cycloaddition reactions on Ge(100)-2×1 -- 6.2.2. Heterocycloadditions -- 6.2.3. Nucleophilic/electrophilic reactions -- 6.2.4. Multiple-layer reactions -- 6.3. Summary of concepts in organic functionalization -- Chapter 6 Surface Electrochemistry -- 1. Introduction -- 2. Special features of electrochemical reactions -- 2.1. Electrochemical current and potential -- 2.2. Electrochemical interfaces -- 2.3. Models of electrochemical electron transfer kinetics -- 3. Electrochemistry at the molecular scale -- 3.1. Surface structure -- 3.2. Bonding of ions -- 3.3. Bonding of water -- 3.4. Experimental aspects of current/voltage properties -- 4. Electrocatalytic reaction processes -- 4.1. The electrocatalytic reduction of oxygen -- 4.1.1. Background -- 4.1.2. Mechanistic pathways -- 4.1.3. Electroreduction of oxygen on Pt and Pt alloys -- 4.1.4. Recent quantum chemical studies of the ORR mechanism -- 4.1.5. State-of-the-art ORR electrocatalyst concepts -- 4.2. The electrochemical oxidation of small organic molecules. , 4.2.1. The electrooxidation of carbon monoxide -- 4.2.2. The electrooxidation of formic acid and methanol -- 5. Summary and outlook -- Chapter 7 Geochemistry of Mineral Surfaces and Factors Affecting Their Chemical Reactivity -- 1. Introduction -- 2. Environmental interfaces -- 2.1. Common minerals in Earth's crust, soils, and atmosphere, weathering mechanisms and products, and less common minerals that contain or adsorb -- 2.2. Solubilities of Al- and Fe(III)-oxides and Al and Fe(III)-(oxy)hydroxides -- 2.3. Dissolution mechanisms at feldspar-water interfaces -- 2.4. The nature of metal oxide-aqueous solution interfaces - some basics -- 3. Factors affecting the chemical reactivity of mineral surfaces -- 3.1. The reaction of water vapor with metal oxide surfaces - surface science and theoretical studies of simplified model systems illustrating effects of -- 3.2. Grazing incidence EXAFS spectroscopic studies of Pb(II)aq adsorption on metal oxide surfaces - effect of differences in surface functional groups on -- 3.3. The structure of hydrated metal oxide surfaces from X-ray diffraction studies -- 3.4. X-ray standing wave studies of the electrical double layer at solid-aqueous solution interfaces and in situ measurements of surface reactivity -- 3.5. Effect of organic coatings and microbial biofilms on metal oxide surface reactivity - X-ray standing wave studies of metal ion partitioning between -- 4. Conclusions -- Index.
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 88 (1984), S. 4617-4621 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 95 (1991), S. 7401-7405 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 94 (1990), S. 5471-5477 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 4954-4957 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Large-scale calculations using atomic natural orbital (ANO) basis sets have been performed on Cu5O to establish the effects of correlation of the 3d shell on oxygen chemisorption. The largest calculation performed correlated 51 electrons in a basis set containing 205 ANO's. Correlation of the 3d shell is found to increase the chemisorption energy by 13(16±2) kcal/mol and decrease the height above the surface of the oxygen by 0.23(0.38) a0 with CI superposition error corrections included. The 2E state of the bare cluster is found to be stabilized by 10(8) kcal/mol relative to the 4A2 state as a result of 3d correlation. The values in parentheses were obtained using an approximate core–valence correlation operator which thus gives results in very good agreement with the core correlated calculations.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 5377-5383 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The bonding in the X 1Σ+g state of Mg2 is investigated using near-complete valence one-particle Slater and Gaussian basis sets containing up to h functions. Full configuration interaction (FCI) calculations are used to calibrate four-electron correlation treatments. We show that the four-electron complete CI limit can be approached using a sequence of either second-order CI (SOCI) or interacting correlated fragment (ICF) calculations. At the valence level, our best estimate of the dissociation energy (De) is 464 cm−1. We show that this is a lower limit and probably within 5 cm−1 of the complete basis value. The inclusion of core–valence correlation using a model operator approach decreases De by about 35 cm−1 and increases the bond length by 0.03 a0, thereby yielding spectroscopic constants in good agreement with experiment. Attempts to compute the core–valence effect accurately by expanding the CI treatment were unsuccessful.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 4613-4616 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Two problems are addressed in the present study: the degree of copper 3d covalency involved in the chemisorption of oxygen at the fourfold hollow site of Cu(100) and the separability of the correlation energy into contributions from the 3d shells on copper and from the valence sp band. The investigation was carried out at the all-electron level using a Cu5 cluster as a model of the Cu(100) surface. The analysis shows that the 3d covalency is of practically no importance in the system considered, contributing only 1–3 kcal/mol to the total chemisorption energy of 89 kcal/mol. The correlation energy was found to be separable to within 5 kcal/mol. A configuration-interaction calculation on the Cu5O system using the one-electron effective core potential developed previously yielded a correlation energy in close agreement with the all-electron results.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 89 (1988), S. 5747-5752 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The low-lying (up to about 40 000 cm−1) doublet and quartet states of AlC have been studied at the CASSCF and MRCI levels of theory. The bonding in the X 4Σ− state is shown to involve three one-electron bonds. The first excited state, a 2Π, lies about 8700 cm−1 higher and like the X 4Σ− state is derived from ground state Al and C, but has a two-electron π bond leading to a much shorter bond length. Those states derived from Al 3s13p2 are much higher in energy, since the promotion energy is not recovered by the formation of two-electron bonds. Transition moments are presented for all the dipole-allowed transitions. The very strong B 4Σ−–X 4Σ− transition near 22 600 cm−1 is probably the best way to observe AlC in either emission or absorption.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 4024-4030 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Cluster size convergency of the chemisorption energy has been studied for the case of fluorine on Ni(100). Bond preparation of the cluster is found to be equally important for fluorine as for the previously studied hydrogen chemisorption. An estimate of the chemisorption energy for fluorine in the fourfold hollow site of Ni(100) is reached based on the average value for the bond-prepared clusters, a correction for the use of one-electron ECP's, an estimate of the basis set limit and finally adding the effect of 3d correlation. The chemisorption energy is in this way estimated to be about 120 kcal/mol. Even though the bonding between fluorine and the surface should be regarded as almost totally ionic, there is still no correspondence between the chemisorption energy for a cluster and the highest ionization energy (Fermi level) of that cluster. The critical feature of bond preparation is that it allows the fluorine lone-pair electrons pointing down towards the surface to be fitted into the electronic structure of the cluster.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 818-819 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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