Microcalorimetric measurements of the heat of adsorption of Pb on well-defined oxides: MgO(100) and p(2×1)-oxide on Mo(100)

Effect of surface vacancies on the adsorption of Pd and Pb on MgO(100)

Abstract

Theoretical quantum mechanical calculations have been carried out to establish the effect of surface vacancies on the adsorption of Pd and Pb atoms on the defective MgO(100) surface. The investigated defects included neutral, singly and doubly charged O and Mg vacancies on the (100) surface of MgO. These vacancies played the role of F_sⁿ⁺ and V_sⁿ⁻ (n = 0, 1, 2) adsorption centers for a single Pd or Pb atom. From the results of calculations, it is clear that the Pd- and Pb-atom adsorption at the F_sⁿ⁺ and V_sⁿ⁻ centers shows different characteristics than at the regular O²⁻ and Mg²⁺ centers. Drastic changes in geometric, energetic, and electronic parameters are evident in Pd/V_sⁿ⁻ and Pb/V_sⁿ⁻. The effect of F_s⁰ and F_s⁺, which in practice are the most important vacancies, is smaller, yet the adsorption of Pd and Pb at these centers is more energetically favorable than at the regular O²⁻ center. Of the two metals studied, the atom of Pd is bound by the F_s⁰ and F_s⁺ centers with higher adsorption energies.

Graphical abstract

Electronic supplementary material

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Trends in Adhesion Energies of Metal Nanoparticles on Oxide Surfaces: Understanding Support Effects in Catalysis and Nanotechnology

Nanoparticles on surfaces are ubiquitous in nanotechnologies, especially in catalysis, where metal nanoparticles anchored to oxide supports are widely used to produce and use fuels and chemicals, and in pollution abatement. We show that for hemispherical metal particles of the same diameter, D, the chemical potentials of the metal atoms in the particles (μ_M) differ between two supports by approximately -2(E_adh,A - E_adh,B)V_m/D, where E_ad,i is the adhesion energy between the metal and support i, and V_m is the molar volume of the bulk metal. This is consistent with calorimetric measurements of metal vapor adsorption energies onto clean oxide surfaces where the metal grows as 3D particles, which proved that μ_M increases with decreasing particle size below 6 nm and, for a given size, decreases with E_adh. Since catalytic activity and sintering rates correlate with metal chemical potential, it is thus crucial to understand what properties of catalyst materials control metal/oxide adhesion energies. Trends in how E_adh varies with the metal and the support oxide are presented. For a given oxide, E_adh increases linearly from metal to metal with increasing heat of formation of the most stable oxide of the metal (per mole metal), or metal oxophilicity, suggesting that metal-oxygen bonds dominate interfacial bonding. For the two different stoichiometric oxide surfaces that have been studied on multiple metals (MgO(100) and CeO₂(111), the slopes of these lines are the same, but their offset is large (∼2 J/m²). Adhesion energies increase as MgO(100) ≈ TiO₂(110) < α-Al₂O₃(0001) < CeO₂(111) ≈ Fe₃O₄(111).

Adsorption calorimetry during metal vapor deposition on single crystal surfaces: increased flux, reduced optical radiation, and real-time flux and reflectivity measurements

Thin films of metals and other materials are often grown by physical vapor deposition. To understand such processes, it is desirable to measure the adsorption energy of the deposited species as the film grows, especially when grown on single crystal substrates where the structure of the adsorbed species, evolving interface, and thin film are more homogeneous and well-defined in structure. Our group previously described in this journal an adsorption calorimeter capable of such measurements on single-crystal surfaces under the clean conditions of ultrahigh vacuum [J. T. Stuckless, N. A. Frei, and C. T. Campbell, Rev. Sci. Instrum. 69, 2427 (1998)]. Here we describe several improvements to that original design that allow for heat measurements with ~18-fold smaller standard deviation, greater absolute accuracy in energy calibration, and, most importantly, measurements of the adsorption of lower vapor-pressure materials which would have previously been impossible. These improvements are accomplished by: (1) using an electron beam evaporator instead of a Knudsen cell to generate the metal vapor at the source of the pulsed atomic beam, (2) changing the atomic beam design to decrease the relative amount of optical radiation that accompanies evaporation, (3) adding an off-axis quartz crystal microbalance for real-time measurement of the flux of the atomic beam during calorimetry experiments, and (4) adding capabilities for in situ relative diffuse optical reflectivity determinations (necessary for heat signal calibration). These improvements are not limited to adsorption calorimetry during metal deposition, but also could be applied to better study film growth of other elements and even molecular adsorbates.

The energetics of supported metal nanoparticles: relationships to sintering rates and catalytic activity

Transition metal nanoparticles on the surfaces of oxide and carbon support materials form the basis for most solid catalysts and electrocatalysts, and have important industrial applications such as fuel production, fuels, and pollution prevention. In this Account, I review my laboratory group's research toward the basic understanding of the effects of particle size and support material on catalytic properties. I focus on studies of well-defined model metal nanoparticle catalysts supported on single-crystalline oxide surfaces. My group structurally characterized such catalysts using a variety of ultrahigh vacuum surface science techniques. We then measured the energies of metal atoms in these supported nanoparticles, using adsorption calorimetry tools that we developed. These metal adsorption energies increase with increasing size of the nanoparticles, until their diameter exceeds about 6 nm. Below 6 nm, the nature of the oxide support surface reaches also greatly affects the metal adsorption energies. Using both adsorption calorimetry and temperature programmed desorption (TPD), we measured the energy of adsorbed catalytic intermediates on metal nanoparticles supported on single crystal oxide surfaces, as a function of particle size. The studies reveal correlations between a number of characteristics. These include the size- and support-dependent energies of metal surface atoms in supported metal nanoparticles, their rates of sintering, how strongly they bind small adsorbates, and their catalytic activity. The data are consistent with the following model: the more weakly the surface metal atom is attached to the nanomaterial, the more strongly it binds small adsorbates. Its strength of attachment to the nanomaterial is dominated by the number of metal-metal bonds which bind it there, but also by the strength of metal/oxide interfacial bonding. This same combination of bond strengths controls sintering rates as well: the less stable a surface metal atom is in the nanomaterial, the greater is the thermodynamic driving force for it to sinter, and the faster is its sintering rate. These correlations provide key insights into how and why specific structural properties of catalyst nanomaterials dictate their catalytic properties. For example, they explain why supported Au catalysts must contain Au nanoparticles smaller than about 6 nm to have high activity for combustion and selective oxidation reactions. Only below about 6 nm are the Au atoms so weakly attached to the catalyst that they bind oxygen sufficiently strongly to enable the activation of O₂. By characterizing this interplay between industrially important rates (of net catalytic reactions, of elementary steps in the catalytic mechanism, and of sintering) and their thermodynamic driving forces, we can achieve a deeper fundamental understanding of supported metal nanoparticle catalysts. This understanding may facilitate development of better catalytic nanomaterials for clean, sustainable energy technologies.

Adsorption Energy, Growth Mode, and Sticking Probability of Ca on Poly(methyl methacrylate) Surfaces with and without Electron Damage

The adsorption of Ca atoms on pristine and electron-irradiated poly(methyl methacrylate) (PMMA) surfaces at 300 K has been studied by adsorption microcalorimetry, atomic beam/surface scattering, and low-energy He+ ion scattering spectroscopy (ISS). On pristine PMMA, the initial sticking probability of Ca is 0.5, increasing quickly with Ca coverage. Below 0.5 ML, the heat of adsorption is 730-780 kJ/mol, much higher than Ca's sublimation energy (178 kJ/mol). The Ca here is invisible to ISS, which is attributed to Ca binding to ester groups below the CH3/CH2-terminated PMMA surface. The adsorption energy increases with coverage, suggesting attractions between neighboring Ca-ester complexes. Above 0.5 ML, Ca starts to grow as three-dimensional (3D) Ca clusters on top of the surface, which dominate growth after 2 ML. It is proposed that each Ca reacts with two esters to form the Ca carboxylate of PMMA, because this reaction's heat would be close to that observed. The total amount of Ca that binds to subsurface sites is estimated from the integral heat of adsorption to involve 4-6 layers of ester groups. Exposing the PMMA surface to electrons increases Ca's initial sticking probability but lowers its adsorption energy. This is attributed to electron-induced defects acting as nucleation sites for 3D Ca islands, whose growth now competes kinetically with Ca diffusing to subsurface esters. Consequently, only two layers of subsurface esters get populated at saturation. The heat eventually reaches Ca's bulk heat of sublimation on all PMMA surfaces, where pure, bulk-like Ca thin films form.

The effect of size-dependent nanoparticle energetics on catalyst sintering

Calorimetric measurements of metal adsorption energies directly provide the energies of metal atoms in supported metal nanoparticles. As the metal coverage increases, the particles grow, revealing the dependence of this energy on particle size, which is found to be much stronger than predicted with the usual Gibbs-Thompson relation. It is shown that this knowledge is crucial to accurately model long-term sintering rates of metal nanoparticles in catalysts.

Metal adsorption and adhesion energies on MgO(100)

The calormetically measured heats of adsorption of Cu, Ag, and Pb on MgO(100), previously measured in our group, are correlated with bulk properties of the metals and their sticking probabilities and film morphologies. The low-coverage heats of adsorption (when the metals are mainly in two-dimensional (2D) islands) are used to estimate metal-MgO(100) bond energies within a pairwise bond additivity model. These values correlate well with the observed initial sticking probabilities and saturation island densities of the metals. This supports a transient mobile precursor model for adsorption. The values also correlate with their bulk sublimation energies, which suggests that covalent metal-Mg bonding dominates the interaction at low coverage, probably due to very strong bonding at defects. The heats of adsorption integrated up to multilayer coverages provide the metal-MgO(100) adhesion energies and metal-MgO(100) bond energies for metals in 3D films. These values correlate with the sum of magnitudes of the metal's bulk sublimation energy plus the heat of formation of the bulk oxide of the metal per mole of metal atoms. This suggests that local chemical bonds, both metal-oxygen and covalent metal-Mg, dominate the interfacial bonding for 3D films.

Measurement of the energetics of metal film growth on a semiconductor: Ag/Si(100)-(2 x 1)

The first direct calorimetric measurements of the energetics of metal film growth on a semiconductor surface are presented. The heat of adsorption of Ag on Si(100)-(2 x 1) at 300 K decreases from approximately 347 to 246 kJ/mol with coverage in the first monolayer (ML) due to overlap of substrate strain from nearby Ag islands. It then rises quickly toward the bulk sublimation enthalpy (285 kJ/mol) as 3D particles grow. A wetting layer grows to 1.0 ML, but is metastable above approximately 0.55 ML and dewets when kinetics permit. This may be common when adsorbate islands induce a large strain in the substrate surface nearby.