Ar and Kr adsorption on Ag(111)

Precise structural and thermodynamic studies of Kr and of Ar adsorbed on Ag(111) are made using low energy electron diffraction. The phase diagram, lattice constants of the unconstrained monolayer and of the monolayer in equilibrium with the bilayer, latent heats of adsorption and isosteric heats are measured. The results are similar to those of an earlier study of Xe adsorbed on Ag(111). The results are compared to model calculations using effective lateral interactions which are similar to those for Xe/Ag(111). Comparison of the results for Xe, Kr, and Ar on Ag(111) is made using corresponding states scalings. A comparison is also made with properties of the non-registry phases of Xe, Kr, and Ar on basal plane graphite.     

Electronic transitions of Ar,Xe, N2, CO physisorbed on Ag(111) and Al(111)

High Resolution Electron Energy Loss Spectroscopy has been extended to study also the excitonic (low lying electronic) transitions of physisorbed rare gas atoms (Ar, Xe) and diatomic molecules (N₂, CO) on Ag(111) and Al(111) surfaces at ～20K. Electron Loss Spectra were performed using a pair of hemispherical analyzers mounted at a fixed scattering angle (90°). This spectrometer allowed high transmission in the range of 0–15eV loss energies and incident beam energies up to 2OeV. AES, LEED and UV Photoemission (HeI) were also used in situ to characterize these surfaces and to identify the adsorbed gases and delineate their absolute coverage regimes.In contrast to optical absorption experiments, we observe both, optical (dipole) forbidden and allowed electronic transitions which show vibrational line structure for condensed multilayers. By comparison to gas phase data we find only weak perturbations in the condensed state. The observed electronic excitations show changes in intensity and FWHM depending on the coverage of the adsorbed gases.The FWHM of the electronic excitations of CO and N₂ adsorbed in the monolayer regime is larger than in multilayers. Nitrogen, on both surfaces exhibits an increase from 60meV to 120meV (FWHM) whereas for CO the vibronic features are broadened out leaving peaks with FWHM of ～1eV.The intensities of the electronic losses for all gases are smaller in the first monolayer than in the second or in multilayers. At submonolayer coverage the loss intensifies due to electronic excitations are strongly reduced and no longer observable although vibrational bands and photoelectron spectra show the presence of physisorbed adsorbates.Our results will be compared to optical absorption experiments (ref.1) on similar systems and to atom-on-jellium calculations (ref.2).     

铝和银在铱（111）宽范围吸附的稳定性、原子构型及电子特性研究

利用第一性原理密度泛函理论研究了铝和银在铱的111面的宽范围吸附特性。基于密度泛函理论计算了覆盖度在0.11ML到2.00ML的结构稳定性、原子构型及平均结合能。对于铝原子在铱111面的吸附,最稳定的结构是铝原子覆盖度为0.5ML位于密堆六方空位（hcp-hollow）,相应的结合能为-4.68eV;对于亚层铝原子的吸附,最稳定结构是铝原子覆盖度为1.00ML时位于octahedral位置,相应的结合能为-5.28eV。对于覆盖度为2.00ML的满覆盖度混合结构的表层及亚层吸附,最稳定结构是Al位于六方密堆及八方密堆位置,相应的结合能为-4.70eV。这意味着当铝原子以满覆盖度吸附在铱的111面上时,趋向于在铱的111面的亚层形成化学键,而非吸附于表层。相比于铝吸附在铱111面,银的吸附特性呈现出很大的不同,面心位置更为稳定,在覆盖度为0.25ML时其结合能为3.89eV,略微高出密堆六方位置处3.88eV的结合能。     

铝和银在铱（111）宽范围吸附的稳定性、原子构型及电子特性研究

利用第一性原理密度泛函理论研究了铝和银在铱的111面的宽范围吸附特性。基于密度泛函理论计算了覆盖度在0.11ML到2.00ML的结构稳定性、原子构型及平均结合能。对于铝原子在铱111面的吸附,最稳定的结构是铝原子覆盖度为0.5ML位于密堆六方空位（hcp-hollow）,相应的结合能为-4.68eV;对于亚层铝原子的吸附,最稳定结构是铝原子覆盖度为1.00ML时位于octahedral位置,相应的结合能为-5.28eV。对于覆盖度为2.00ML的满覆盖度混合结构的表层及亚层吸附,最稳定结构是Al位于六方密堆及八方密堆位置,相应的结合能为-4.70eV。这意味着当铝原子以满覆盖度吸附在铱的111面上时,趋向于在铱的111面的亚层形成化学键,而非吸附于表层。相比于铝吸附在铱111面,银的吸附特性呈现出很大的不同,面心位置更为稳定,在覆盖度为0.25ML时其结合能为3.89eV,略微高出密堆六方位置处3.88eV的结合能。     

An EELS and TPD study of the adsorption and decomposition of acetic acid on the Al(111) surface

The adsorption and decomposition of acetic acid on Al(111) have been studied using electron energy loss spectroscopy (EELS), temperature programmed desorption (TPD), and Auger electron spectroscopy (AES). Acetic acid reacts with clean Al(111) at 120 K to form a surface acetate species. The adsorbed acetate bonds to the surface in a symmetric configuration with C_s symmetry at 120 K. The adsorption of molecular acetic acid occurs at this temperature only after saturation of the surface acetate layer; this physisorbed multilayer desorbs molecularly at 167 K. Thermal decomposition of the adsorbed acetate leads to a carbon- and oxygen-covered surface; the only detectable thermal decomposition product is H₂. Electron irradiation induces a similar decomposition process of the surface acetate.     

H原子在Al(111)和Ag(111)面上的吸附

本文用电荷自洽的EHT方法,研究了H原子在Al(111)和Ag(111)面上的吸附,结果指出:在Al(111)面上,H以原子状态吸附在某些对称位置上,它也能渗透到表面层中去,成为填隙原子;H₂分子在表面处发生解离吸附。在Ag(111)表面上,H原子有可能以分子状态吸附,H—H键平行于表面,这与高分辨率电子能量损失谱所得到的实验结果一致;但H₂分子在Ag(111)表面也可能发生解离吸附。 关键词：     

Adsorption of Xe atoms on metal surfaces: new insights from first-principles calculations

The adsorption of rare gases on metal surfaces serves as the paradigm of weak adsorption where it is typically assumed that the adsorbate occupies maximally coordinated hollow sites. Density-functional theory calculations using the full-potential linearized augmented plane wave method for Xe adatoms on Mg(0001), Al(111), Ti(0001), Cu(111), Pd(111), and Pt(111), show, however, that Xe prefers low coordination on-top sites in all cases. We identify the importance of polarization and a site-dependent Pauli repulsion in actuating the site preference and the principle nature of the rare-gas atom-metal surface interaction.     

Photoemission from physisorbed Co on clean and Xe-covered Al(111)

Molecular-orbital energy shifts are observed in photoemission from weakly physisorbed CO on clean and Xe-covered Al(111) surfaces. These shifts in ionization potentials are mainly due to final-state relaxation effects, which can be described approximately by a point-charge image-potential model. Differential distance- and orbital-dependent energy shifts suggest that CO molecules lie flat on the substrates. CO is adsorbed on Al(111) with a heat of formation of 0.21 eV/molecule.     

A scanning tunneling microscopy study of the adsorption of Xe on Pt(111) up to one monolayer

The adsorption of Xe on Pt(111) has been investigated from the arrival of the very first atoms up to completion of the monolayer using a variable-temperature Scanning Tunneling Microscope (STM). Surprisingly, in the initial stages of the adsorption Xe preferentially binds to a low coordination site, theupper edge of the platinum steps. The strong binding to these sites leads to a local repulsive interaction with further Xe atoms. Therefore, the Xe atoms located at the upper edge of the steps do not serve as nuclei for 2D Xe islands, which, instead, form on the terraces and at thelower edges of the platinum steps. Only during completion of the monolayer do these islands make contact with the atoms adsorbed at the beginning in the upper-edge positions. The full monolayer exhibits the Hexagonal Incommensurate Rotated (HIR) phase already known from earlier helium-diffraction experiments.     

On the mechanism of the interaction between oxygen and close-packed single-crystal aluminum surfaces

Using periodic first principles simulations we investigate the interaction of oxygen molecules with both regular Al(111) and Al(001) surfaces as well as a stepped Al(111) substrate. The limitation of this approach is the use of thin metallic slabs with a limited range for their coverage by adsorbed oxygen. The advantage is the detailed modeling that is possible at an atomic level. On the regular Al(111) surface, we have been able to follow the oxidation process from the approach of O₂ molecules to the surface, through the chemisorption and absorption of O atoms, up to the formation of first Al₂O₃ formula units. An energetically feasible mechanism for the formation of these Al₂O₃ ‘molecules’ is proposed but their aggregation to Al₂O₃ growth nuclei can only be surmised. On the Al(001) surface, absorption of oxygen atoms occurs more readily without any restrictions on the density of their surface overlayer, in agreement with the failure to observe a distinct chemisorption stage for O on Al(001) experimentally. The stepped Al(111) surface contains both {111} and {001} microfacets: the latter are obviously preferred for penetration of the oxygen adatoms into the subsurface space of the substrate. Before considering the O/Al interfaces the computational method is tested thoroughly by simulations on bulk Al and close-packed aluminum surfaces.     

铝团簇Al13的结构、电子性质和氧原子吸附的第一原理计算

利用密度泛函理论对Al13团簇的几种典型异构体进行了计算.对几种不同对称性(Ih,D5h,D3h,Oh)的中性和带电团簇Al13、Al13-、Al13 进行了结构优化和总能计算,得到了各种带电状态下的最低能量结构,并计算了Al13团簇的电离势、电子亲和能和结合能.理论结果与实验值比较,比以前的理论计算符合的更好.从中性和负电状态下的正二十面体的最低能量结构出发,研究了氧原子在Al13和Al13-上的吸附行为,并与单个氧原子在铝fcc表面的吸附行为做了比较.计算发现,高稳定性的幻数团簇如Al13-,较中性团簇和铝表面,更不易于氧化.     

X-ray photoelectron spectroscopic study of the physical adsorption of xenon and the chemisorption of oxygen on tungsten (111)

X-ray photoelectron spectroscopy (ESCA) has been used to study the physical adsorption of Xe and the chemisorption of oxygen by W (111). An ultrahigh vacuum ESCA spectrometer has been modified such that thermal desorption behavior from the W (111) crystal can be directly compared with ESCA spectra of the adsorbed species. In addition, since the work function of a W (111) crystal covered with one monolayer of Xe is accurately known from previous work, the binding energy of the $\text{Xe}\text{(3}\text{d}{}_{\mathrm{<mtext>5</mtext><mtext>2</mtext>}}\text{)}$ adsorbate level can be accurately compared to the gaseous $\text{Xe}\text{(3}\text{d}{}_{\mathrm{<mtext>5</mtext><mtext>2</mtext>}}\text{)}$ level.When Xe is physisorbed to 1 monolayer the $\text{Xe}\text{(3}\text{d}{}_{\mathrm{<mtext>5</mtext><mtext>2</mtext>}}\text{)}$ level exhibits a binding energy (relative to the vacuum level) which is 2.1 eV below that found for Xe (g). At lower Xe coverages the shift becomes monotonically greater, approaching 2.6 eV at a Xe coverage of 0.05. This 0.5 eV shift downward is accompanied by an increase of only 0.05 eV in adsorption energy as coverage decreases, and may be partially caused by the presence of ~ 10–20 % of extraneous adsorption sites other than W (111) which adsorb Xe with higher adsorption energy. The adsorption energy of Xe may also be increased by coadsorption of oxygen and the $\text{Xe}\text{(3}\text{d}{}_{\mathrm{<mtext>5</mtext><mtext>2</mtext>}}\text{)}$ binding energy exhibits a corresponding shift downward as adsorbed oxygen coverage is increased to θ_o = 0.5. Electronic relaxation processes affecting the final state are dominant factors in determining the magnitude of the chemical shift upon adsorption, in agreement with the predictions of Shirley. The magnitude of the relaxation effect seems to be very sensitive to small changes in Xe adsorption energy. Similar effects have been seen for chemisorption of CO.The adsorption of O₂ at 120 K by W (111) yields a single broad O(1s) peak whose line-width decreases with increasing coverage. The final spectra at θ_o = 1 monolayer are very similar to those obtained at temperatures of 300 K or above on polycrystalline tungsten.     

Two-dimensional gas phases of Ar,Kr, AND Xe on Ag(111)

Observations and calculations are reported for the 2D gas phase of Ar, Kr, and Xe adsorbed on the (111) face of Ag. The measurement of the coverage of 2D gas is sensitive to the gas adsorbed on the coherently diffracting regions of the Ag; appreciable contributions to the measured coverage from gas adsorbed at extrinsic sites can be excluded. The gas density at the condensation of the solid monolayer is remarkably high, of the order of 15% of the 2D solid density. Statistical mechanical calculations, using Monte Carlo simulations, show that the unusually dense 2D gas is stabilized against condensation because substrate-mediated interactions raise the energy of the 2D solid relative to the value which would be calculated using the bare 3D pair potentials. The simulations show that the gas is very nonideal, with large specific heat and large density fluctuations. The only comparable states of a 3D gas occur near the gas-liquid critical point.     

Femtosecond electron dynamics at adsorbate–metal interfaces and the dielectric continuum model

2 overlayers adsorbed on Cu(111). With increasing number of adsorbate layers the binding energies of the image potential states are found to decrease while their lifetimes increase (except for the second image potential state on 2 to 3 ML Xe/Cu(111)). These trends are most pronounced for nitrogen, where the binding energy of the first image potential state decreases by a factor of 3.5 from 0 to 2 ML N₂/Cu(111); at the same time the lifetime increases from 22 to 700 fs. The results are discussed in the framework of the dielectric continuum model, which approximates the adsorbate layers by a dielectric slab in front of the metal surface. For Xe, the agreement between measured and calculated lifetimes improves significantly if the full dispersion curve of the Xe 6s conduction band is taken into account. Received: 2 November 1998     

Optical excitation spectra of rare-gas atoms physisorbed on metal surfaces

Numerical computations are presented for the optical excitation spectra of neutral rare-gas atoms physisorbed on various metal surfaces. At low coverage and when the damping of the surface plasmons is much greater than the effective radiative damping, the occasional disappearance of the spectral lines of the optical absorption is due to a cancellation process, which occurs between the frequency profiles arising from two nearby excited states of the adsorbed atom. The red (blue) shifted peak of the symmetric mode of the higher (lower) excited state and the blue (red) shifted peak of the antisymmetric mode of the lower (higher) excited state of the atom cancel each other out provided that the frequency profiles of their lineshapes nearly coincide. Results of numerical calculations indicate that at low coverage the peaks of excited Xe on Ti and Au and excited Kr on Mg, in addition to those of Xe on Al and Kr on Au, vanish; this is compatible with the experimental observations. Predictions have been made for the adsorption spectra as a function of the distance from the atom to the surface of excited Xe and Kr, which are physisorbed on the surfaces of W, Ni, and Rh, respectively.Issued as NRCC No. 29204     

Dynamics of confined Xe monolayers adsorbed on the Pt(997) vicinal surface

The dynamics of a confined discrete xenon monolayer adsorbed on the vicinal Pt(997) surface is analyzed within a semi-empirical potential approach. We have investigated two monolayer geometries, namely the commensurate phase and the quasi-hexagonal incommensurate phase, which seem to be stable on the (111) face of Pt, depending on the terrace size. We show that the number and the behavior of localized and side modes characteristic of the confinement are completely different in the two phases. Inelastic helium scattering experiments with a resolution better than 0.2 meV should be an efficient tool to detect the localized modes of the monolayer. This could be an additional way to elucidate the structure of Xe/Pt(997), which has not yet been well established.     

Electron energy loss spectra of the system Cu(311)/CO,Xe

The electron energy loss spectrum of a clean Cu(311) surface has been studied by reflected electrons using primary energies between 30 and 300 eV. The losses obtained are compared with literature values. Loss spectra with adsorbed CO and Xe are also reported. Some assignments of the loss mechanisms have been attempted.     

Ar adsorptions on Al (111) and Ir (111) surfaces: a first-principles study

We investigate the adsorptions of Ar on Al (111) and Ir (111) surfaces at the four high symmetry sites, i.e., top, bridge, fcc- and hcp-hollow sites at the coverage of 0.25 monolayer (ML) using the density functional theory within the generalized gradient approximation of Perdew, Burke and Ernzerhof functions. The geometric structures, the binding energies, the electronic properties of argon atoms adsorbed on Al (111) and Ir (111) surfaces, the difference in electron density between on the Al (111) surface and on the Ir (111) surface and the total density of states are calculated. Our studies indicate that the most stable adsorption site of Ar on the Al (111) surface is found to be the fcc-hollow site for the (2 × 2) structure. The corresponding binding energy of an argon atom at this site is 0.538 eV/Ar atom at a coverage of 0.25 ML. For the Ar adsorption on Ir (111) surface at the same coverage, the most favourable site is the hcp-hollow site, with a corresponding binding energy of 0.493 eV. The total density of states (TDOS) is analysed for Ar adsorption on Al (111) surface and it is concluded that the adsorption behaviour is dominated by the interaction between 3s, 3p orbits of Ar atom and the 3p orbit of the base Al metal and the formation of sp hybrid orbital. For Ar adsorption on Ir (111) surface, the conclusion is that the main interaction in the process of Ar adsorption on Ir (111) surface comes from the 3s and 3p orbits of argon atom and 5d orbit of Ir atom.     

Anomalous band broadening of adsorbed chalcogen monolayers on Al(111)

Electronic structure calculations for adsorbed chalcogen monolayers on Al(111) suggest that the anomalous broadening observed in the chalcogen p-bands is indicative of a surface rearrangement in the uppermost Al layers.     

Adsorption of H2O on Al(111)

The adsorption of H₂O on Al(111) has been studied by ESDIAD (electron stimulated desorption ion angular distributions), LEED (low energy electron diffraction), AES (Auger electron spectroscopy) and thermal desorption in the temperature range 80–700 K. At 80 K, H₂O is adsorbed predominantly in molecular form, and the ESDIAD patterns indicate that bonding occurs through the O atom, with the molecular axis tilted away from the surface normal. Some of the H₂O adsorbed at 80 K on clean Al(111) can be desorbed in molecular form, but a considerable fraction dissociates upon heating into OH_ads and hydrogen, which leaves the surface as H₂. Following adsorption of H₂O onto oxygen-precovered Al(111), additional OH_ads is formed upon heating (perhaps via a hydrogen abstraction reaction), and H₂ desorbs at temperatures considerably higher than that seen for H₂O on clean Al(111). The general behavior of H₂O adsorption on clean and oxygen-precovered Al(111) (θ_O ? monolayer) is rather similar at low temperature, but much higher reactivity for dissociative adsorption of H₂O to form OH _adsis noted on the oxygen-dosed surface around room temperature.