Oxidation of GaN{0001}-11 surfaces at room temperature

The interaction of unexcited oxygen molecules with clean GaN{0001}-11 surfaces was investigated using X-ray photoemission spectroscopy (XPS), Auger electron spectroscopy (AES), and low-energy electron diffraction (LEED). Clean surfaces were prepared by a HF dip followed either by desorption of Ga films deposited at room temperature or by nitrogen-ion bombardment and annealing. During exposures in the range from 0.3 up to 10¹⁵ L-O₂ any excitations of the oxygen were avoided. Oxygen coverages determined from the XPS and the AES data differ by a factor of two. The larger XPS-derived coverages are considered to be more reliable since the AES signals decayed during data recording. The oxygen uptake takes place in two consecutive stages. The first one is identified as dissociative chemisorption and the second one is tentatively attributed to field-assisted diffusion by the Mott-Cabrera mechanism. The dissociative chemisorption is characterized by an initial sticking coefficient of and a saturation coverage of monolayers that is reached after exposures of 10³ L-O₂. The second mechanism sets in at exposures to 10⁸ L-O₂ but reaches no saturation even with the largest doses applied. Received 4 September 1998 and Received in final form 6 November 1998     

TDS and EELS observations for CO,O2, and CH3OH bound to Ru(0001)/Cu

The electronic properties of monolayers of copper atoms adsorbed onto a Ru(0001) single crystal surface have been studied with thermal desorption spectroscopy (TDS) and high resolution electron energy loss spectroscopy (EELS) utilizing carbon monoxide (CO), dioxygen (O₂), methanol (CH₃OH), and to some extent water (H₂O) as chemical probes. Whereas a three-monolayer-thick film exhibits most properties of a Cu(111) crystal distinct deviations are found at lower Cu coverages. TDS as well as EELS show a weakened RuCO bond and a strengthened CuCO bond as a result of metal-metal interaction. The stronger CuCO bond is accompanied by a higher probability for O₂ dissociation. The mobilities of copper and oxygen atoms are such that annealing to 650 K produces an overlayer structure which is independent of adsorption sequence: Cu/O₂ or O₂/Cu, but where RuO as well as CuO vibrations can be identified. Methanol adsorbs reversibly on a monolayer of copper atoms. Metal bound methoxy species are formed in the presence of oxygen atoms. The decomposition paths of such methoxy intermediates alter towards more formaldehyde (CH₂O) relative to CO with increasing copper and methoxy coverages.     

The interaction of an O2 molecular beam with an Fe(110) surface

The initial interaction between an O₂ molecular beam and a cleaned Fe(110) surface has been studied by a combination of Auger electron spectrometric (AES) and mass spectrometric techniques. The incident molecular beam intensity was calibrated using a stagnation detector, and the initial sticking coefficient for chemisorption was determined by mass spectrometric measurement of the transient in molecular scattering behavior observed when the cleaned surface was exposed to the molecular beam. This permitted an absolute calibration of the AES system for oxygen, and allowed comparison of the kinetic measurements of the oxygen adsorption process by the two techniques. Results indicate that the initial sticking coefficient is 0.2 ± 0.01. Oxygen is initially chemisorbed up to a coverage of 1.6 ± 0.16 × 10¹⁵ cm^?2, by a process following Langmuir kinetics. Beyond this point AES studies indicate a slower rate of oxygen uptake which is independent of gas-phase oxygen pressure. The mass spectrometric studies further indicate that for a cleaned, annealed surface those oxygen molecules which are not chemisorbed are scattered in a non-diffuse manner.     

Interaction of O2 with low index faces of α-CuZn

The adsorption of O₂ and initial step of oxidation have been investigated, mainly at room temperature, for three different α-CuZn (75%Cu/25%Zn) surfaces ((110), (100) and (111)) by XPS. XAES, LEED, CPD and HREELS. No superstructures were detected on the LEED patterns during O₂ admission for the three faces, and from the beginning of adsorption Zn segregated to the surface. For (110), the interaction of oxygen follows the sequence: (1) dissociative chemisorption (up to ~ 20 L), accompanied by an increase of the work function and a single site occupancy as revealed by HREELS; (2) nucleation of ZnO only, indicated by a decrease of the work function, a shift of the Zn L₃M₄₅M₄₅ Auger transition and an emergence of a vibration at 550 cm^?1. corresponding to the surface phonon of ZnO. The (111) face follows the same scheme, except that the sticking coefficient for oxygen is very low. For (100), it is clear that two states of oxygen exist simultaneously, even at the beginning, as revealed by HREELS and CPD measurements. No copper oxides are ever detected, even after heat treatment. In addition, different bonding properties of OH groups on the three surfaces are reported.     

A LEED-AES study of the initial stages of oxidation of Fe (001)

LEED and AES have been used to study the structural changes and kinetics of the initial interaction between Fe(001) and oxygen at room temperature. The AES oxygen signal was quantified by using a two-dimensional oxide layer as a calibration point. This reproducible oxide layer was prepared by the high temperature reaction of H₂O at 10^?6 torr with Fe(001). The initial oxygen sticking coefficient was observed to be close to unity, which suggests that the chemisorption is non-activated and involves a mobile adsorption step. The rate of chemisorption decreased as (1-Θ) and exhibited a minimum at Θ = 0.5. LEED data indicate that the minimum value of the sticking coefficient corresponded to the completion of a c (2 × 2) surface structure. Upon additional exposure to oxygen, an increase in the sticking coefficient was observed in conjunction with the disappearance of the c (2 × 2) and a gradual fade out of all diffraction features. After mild heating, epitaxial FeO (001) and FeO (111) structures were observed. The simultaneous appearance of a shifted M_2,3M_4,5M_4,5 iron Auger transition with the increase in the sticking coefficient and the disappearance of the c (2 × 2) indicated that oxide nucleated on the surface after the complete formation of the c (2 × 2) structure. The relatively high sticking coefficient during the initial oxidation indicates that formation of a mobile adsorbed oxygen state precedes the formation of oxide.     

Study of chemisorption on copper low-index and stepped surfaces

Adsorption of CHCl₃, O₂, and hydrocarbons has been studied on Cu(111) and stepped surfaces using LEED, AES, and UPS at room temperature. We find that ordered Cl overlayers form upon Cu(111), Cu[3(111) × (100)], and Cu[5(111) × (100)] surfaces upon exposure to CHCl₃. Exposure to O₂ results in rearrangement of the Cu[5(111) × (100)] surface to hill-and-valley regions with large (111) areas, whereas Cu[2(111) × (100)] is stable for the same exposure. The photoemission spectra show new energy levels due to C1 above and below the Cu d band region and a small splitting of the halogen p orbitals. Effects consistent with interaction with the Cu d band are observed. Similar effects are observed with oxygen adsorption. The initial rate of Cl or O₂ chemisorption as measured by photoemission is proportional to the density of steps on these surfaces. Apparently, structural effects play an important role in chemisorption on metals (such as copper) with low density of states at the Fermi energy.     

Magnetism and superconductivity in R1.5Ce0.5MSr2Cu2O10‐δ (M=Ru and Fe) compounds

It is shown here, that the superconducting (SC) R_1.5Ce_0.5RuSr₂Cu₂O_10-δ (RCeRuSCO, R= Eu and Gd) materials (T_c ～ 32 and 42 K) are also antiferromagnetically (AFM) ordered at T _N(Ru) ～ 122 and 180 K, respectively, thus, T_N ? T_c, a trend which is contrary to that obtained in “magnetic‐SC” intermetallic systems. Mössbauer spectroscopy (MS) on 0.5% ⁵⁷Fe doped samples shows that all Fe ions reside in the Ru site which is magnetically ordered, whereas SC is confined to the CuO₂ planes. On the other hand, for Y_1.5Ce_0.5FeSr₂Cu₂O₉ (YCeFSCO) no SC is found and the Cu–O planes order AFM at T _N(Cu)=31 K. MS studies reveal two in equivalent Fe sites, and that Fe resides predominantly (60%) in the Cu(1) site. In both sites, the Fe does not order magnetically, and the low T _N(Cu) obtained is due to frustration of the Cu moments by the presence of Fe. T _N is sensitive to oxygen concentration and shifts toward 260 K when oxygen is depleted.     

Coadsorption of oxygen and cesium on Ru(001)

The coadsorption of oxygen and Cs on Ru(001) has been studied by means of thermal desorption, Auger and electron loss spectroscopy and work function measurements. The initial sticking coefficients for oxygen adsorption and oxygen saturation coverages increase with increasing Cs coverage, θ_Cs. Irrespective of the initial θ_Cs, the Cs desorption energy always increases under the influence of the coadsorbed oxygen, the effect becoming stronger with increasing oxygen coverage. At θ_O>0.5and θ_Cs>0.14 the work function, electron loss changes and thermal desorption data give evidence of strong CsO interactions and the formation of a CsO “surface compound”.     

Coadsorption of electropositive and electronegative elements: II. Cs and O2 on W (100)

The coadsorption of Cs and O₂ on W (100) surface has been studied systematically. The results were analogous to those of the CsH₂ system. Independent of the sequence of deposition, the adsorbates formed a double layer with the oxygen underneath the Cs layer. The presence of Cs caused a transformation of a(4 × 1) structure of O₂ to a c (2 × 2) structure. Cesium also caused submerged oxygen atoms in the crystal to diffuse to the surface. The initially adsorbed O₂ enabled an increase in saturation coverage of Cs. This effect was more drastic in the O₂ case than that found with preadsorbed hydrogen. The presence of oxygen caused an increase in the work function at the saturation coverage of the subsequently adsorbed Cs, and a shift of the Cs coverage at the work function minimum to lower values. But both of these changes were small compared to those found for the Cs + H₂ system. The sticking coefficient of O₂ on Cs covered W (100) was higher than that for O₂ on clean W. This was attributed to an active chemisorption of O₂ on the Cs film and a place exchange mechanism.     

A photoelectron and energy-loss spectroscopy study of Ti and its interaction with H2, O2, N2 and NH3

A unified electron spectroscopic study of polycrystalline Ti and its interaction with H₂, O₂, N₂, and NH₃ are described. Auger electron spectroscopy (AES), electron energy-loss spectroscopy (ELS), ultraviolet and X-ray photoelectron spectroscopy (UPS and XPS) are combined to provide detailed information about the electronic structure of the titanium surface and its interaction with these adsorbates. X-ray and ultraviolet photoelectron spectra and electron energy-loss spectra are presented for the clean titanium surface, and following exposure to H₂, O₂, N₂ and NH₃. Spectral assignments are provided in each case. The electron spectra of oxygen exposed Ti and nitrogen sputtered Ti are quite similar, and are interpreted with reference to band structure calculations for TiO and TiN. Electron spectroscopy indicates essentially complete dissociative adsorption of NH₃ on the clean titanium surface.     

Electron beam induced effects on gas adsorption utilizing auger electron spectroscopy: Co and O2 on Si: I. Adsorption studies

The effect of electron beam monitored gas adsorption on the clean Si surface is studied using Auger electron spectroscopy. It is shown that the beam affects the AES adsorption signal of CO and O₂ on Si by dissociating the adsorbed molecules on the surface and subsequently promoting diffusion of atomic oxygen into the bulk. A qualitative explanation of the adsorption data is presented and the initial sticking probability of O₂ on Si (111) surface is estimated to be S0 = 0.21.     

Initial stages of the autocatalytic oxidation of the InAs(0 0 1)-(4 × 2)/c(8 × 2) surface by molecular oxygen

The initial stages of oxidation of the In-rich InAs(0 0 1)-(4 × 2)/c(8 × 2) surface by molecular oxygen (O₂) were studied using scanning tunneling microscopy (STM) and density functional theory (DFT). It was shown that the O₂ dissociatively chemisorbs along the rows in the [1 1 0] direction on the InAs surface either by displacing the row-edge As atoms or by inserting between In atoms on the rows. The dissociative chemisorption is consistent with being autocatalytic: there is a high tendency to form oxygen chemisorption sites which grow in length along the rows in the [1 1 0] direction at preexisting oxygen chemisorption sites. The most common site size is about 21-24 Å in length at ∼25% ML coverage, representing 2-3 unit cell lengths in the [1 1 0] direction (the length of ∼5-6 In atoms on the row). The autocatalysis was confirmed by modeling the site distribution as non-Poisson. The autocatalysis and the low sticking probability (∼10⁻⁴) of O₂ on the InAs(0 0 1)-(4 × 2)/c(8 × 2) are consistent with activated dissociative chemisorption. The results show that is it critical to protect the InAs surface from oxygen during subsequent atomic layer deposition (ALD) or molecular beam epitaxy (MBE) oxide growth since oxygen will displace As atoms.     

Basic studies of the oxygen chemistry of silver: Oxygen,dioxygen and superoxide on potassium-dosed Ag(100)

The adsorption—desorption and structural properties of oxygen phases on K-dosed Ag(100) have been investigated. At 298 K, potassium enhances the sticking probability of O₂ on Ag(100) by a factor of ?100; the initial sticking probability and saturation uptake of O₂ are proportional to the potassium coverage (θ_K) for θ_K < 0.5. For θ_K < 0.5 the desorption spectra reveal the presence of three distinct oxygen species — O(a), O₂(a) and dissolved O. The dioxygen species, O₂(a), is associated with the presence of subsurface K and its identity is confirmed by isotope-mixing experiments and CO titration. For θ_K > 1.0 LEED shows the formation of two ordered structures and two additional features appear in the O₂ desorption spectra. One of these structures is ascribed to the growth of (001) oriented potassium superoxide (KO₂). The oxygen chemistry of Na and Rb-dosed Ag surfaces is compared with the results of the present work.     

A THEORETICAL MODEL FOR H2 DISSOCIATIVE ADSORPTION ON Cu SURFACES

A theoretical model for describing H₂ dissociative chemisorption on Cu surfaces is proposed. The sticking probability S is calculated as a function of vibrational state, average kinetic energy and incident angle of hydrogen molecular beam. Within the theoretical frame of this model, the different contributions to S from H₂(v = 0) and H₂(v = 1) can be clearly distinguished. The calculated results indicate that vibrational energy significantly promotes the chemisorption of H₂ on Cu surfaces in the region of low translational energy. The equations derived can be used to analyze the experimental data for both pure and seeded molecular beams.     

Lateral interactions in the thermal desorption of H2 from clean Cu/Ni(110) alloy surfaces

The adsorption of hydrogen on a clean Cu10%/Ni90% (110) alloy single crystal was studied using flash desorption spectroscopy (FDS), Auger electron spectroscopy (AES), and work function measurements. Surface compositions were varied from 100% Ni to 35% Ni. The hydrogen chemisorption on a-surface of 100% nickel revealed strong attractive interactions between the hydrogen atoms in accordance with previous work on Ni(100). Three desorption states (β₁, β₂ and α) appeared in the desorption spectra. The highest temperature (α) state was occupied only after the initial population of the β₂-state. As the amount of copper was increased in the nickel substrate, desorption from the higher energy binding α-state was reduced, indicating a decrease in the attractive interactions among hydrogen atoms. The hydrogen coverage at saturation was not affected by the addition of copper to the nickel substrate until the copper concentration was greater than 25% at which a sharp reduction in saturation coverage occurred. This phenomenon was apparently due to the adsorption of hydrogen on Ni atoms followed by occupation of NiNi and CuNi bridged adsorption sites, while occupation of CuCu sites was restricted due to an energy barrier to migration.     

Effect of H2O chemisorption on passivation of Ge(100) surface studied by scanning tunneling microscopy

The electronic passivation of a Ge(100) surface, via the chemisorption of H₂O at room temperature (RT), and the temperature dependence of H₂O coverage were investigated using scanning tunneling microscopy (STM) and scanning tunneling spectroscopy (STS). With a saturation H₂O dose at RT, a highly-ordered structure, due to the dissociative chemisorption of H₂O, was observed on a Ge(100) surface with a coverage of 0.85 monolayers (ML). Annealing the room temperature H₂O-dosed Ge surface to 175 °C decreased the coverage of H₂O to 0.6 ML. Further annealing at 250 °C decreased the coverage of H₂O sites to 0.15 ML, and the surface reconstruction of Ge dimers was observed over much of the surface. Annealing above 300 °C induced Ge suboxide structures, similar to the oxygen-dosed Ge surface. STS measurements confirmed that the surface dangling bond states near Fermi energy are removed by the H₂O chemisorption because the dangling bonds of Ge atoms are terminated by ―OH and ―H. The H₂O pre-dose at room temperature provides a template for the ultrathin passivation of Ge(100) surface via atomic layer deposition (ALD) at RT, since near monolayer nucleation can be obtained with a 1/2 hydroxylated and 1/2 hydrogenated Ge surface.     

Coadsorption of oxygen and sodium on Ru(001)

The interaction of oxygen with sodium predosed Ru(001) is studied by means of thermal desorption, Auger and electron loss spectroscopy and work function measurements. The initial sticking coefficient of oxygen is found to increase from 0.45 for bare Ru(001) to 1 for Ru(001) with a 0.35 monolayer sodium coverage. The adsorption capacity of the sodium predosed Ru(001) surface towards oxygen is enhanced from θ_O = 0.5 for clean Ru(001) to θ_O = 1.4 for Ru(001) with a 0.7 monolayer sodium coverage. The work function, electron loss changes and thermal desorption data give evidence that as long as θ_Na is less than 0.25, the oxygen chemisorption phase is characterized mainly by oxygen-Ru bonds and by the absence of strong sodium-oxygen interactions. At high sodium coverages (θ_Na > 0.35), the experimental data indicate the formation of a Na-O compound in the second adsorption layer at high oxygen exposures. When Ru(100) is predosed with sodium (θ_Na ? 0.25), this leads to complete suppression of oxygen penetration into the bulk during heating, the latter process being observed for the oxygen-Ru(001) system.     

Partial and complete reduction of O2 by hydrogen on transition metal surfaces

The metal-catalyzed reduction of di-oxygen (O₂) by hydrogen is at the heart of direct synthesis of hydrogen peroxide (HOOH) and power generation by proton exchange membrane fuel cells. Despite its apparent simplicity, how the reaction proceeds on different metals is not yet well understood. We present a systematic study of O₂ reduction on the (111) facets of eight transition metals (Rh, Ir, Ni, Pd, Pt, Cu, Ag, and Au) based on periodic density functional theory (DFT-GGA) calculations. Analysis of ten surface elementary reaction steps suggests three selectivity regimes as a function of the binding energy of atomic oxygen (BE_O), delineated by the opposite demands to catalyze O–O bond scission and O–H bond formation: The dissociative adsorption of O₂ prevails on Ni, Rh, Ir, and Cu; the complete reduction to water via associative (peroxyl, peroxide, and aquoxyl) mechanisms prevails on Pd, Pt, and Ag; and HOOH formation prevails on Au. The reducing power of hydrogen is decreased electrochemically by increasing the electrode potential. This hinders the hydrogenation of oxygen species and shifts the optimal selectivity for water to less reactive metals. Our results point to the important role of the intrinsic reactivity of metals in the selectivity of O2 reduction, provide a unified basis for understanding the metal-catalyzed reduction of O₂ to H₂O and HOOH, and offer useful insights for identifying new catalysts for desired oxygen reduction products.     

NO在Cu(110)表面吸附的角分辨光电子能谱

本文用角分辨光电子能谱(ARUPS)(He Ⅱ),低能电子衍射(LEED)和俄歇电子能谱AES等方法研究了NO在Cu(110)表面吸附的光电子能谱。测量结果表明:在150K左右,NO在Cu(11O)表面是一个比较复杂的分解吸附过程。随着暴露量的不同,在Cu(110)表面形成的分解吸附分子是不同的。在NO5L暴露量时,主要形成O原子和N₂O分子吸附。吸附的LEED图形仍然是(1×1)。 关键词：