A theoretical study of CO adsorption on FeCo(100) and the effect of alloying

FeCo catalysts are modeled for optimizing the Fischer–Tropsch synthesis process since they can be tuned to enhance CO activity and resist poisoning. The electronic properties associated with CO adsorption are studied using plane-wave density functional theory (DFT). The range of computed adsorption energies from this work falls between the CO adsorption energies on pure Fe and Co surfaces. It was found that CO prefers to adsorb on the top site of the Co surface of FeCo alloys, whereas CO has stronger adsorption on pure Fe rather than pure Co surface. The trend in adsorption energy is top-Co > hollow-Fe > top-Fe > hollow-Co > bridge-Co > bridge-Fe. This change in preferable metal for adsorption (i.e., from Fe in a pure system to Co in the FeCo alloy surface in the current investigation) is due to the shift in the d-band center of the alloyed material. It implies that alloying Fe with Co changes the properties of the pure metal and ultimately affects the CO adsorption energy; however, the mechanism of adsorption remains similar and can be explained using the Nilsson–Pettersson model. Additional CO configurations consisting of hollow-site adsorption with a tilted geometry, was also investigated. The corresponding adsorption energy was found to be slightly higher than the adsorption energy when CO is adsorbed on the top-Co site.     

覆盖度对S原子在Ir(001)表面吸附性质的影响

采用第一性原理方法模拟了覆盖度对S原子在Ir(001)表面吸附能和电子结构的影响。结果表明：在覆盖度0.50 ML以下,S原子吸附在Hollow空位最稳定,且吸附能几乎不随覆盖度变化;在覆盖度0.66 ML以上吸附能随覆盖度增加而减小。吸附体系金属表面d带电子结构随覆盖度变化与O/Pt(111)吸附体系相似。这些结果与Hammer-Nørskov模型吻合。     

Synchrotron radiation study of chemisorptive bonding of CO on transition metals — Polarization effect on Ir(100)

Photoemission spectra in the photon energy range 15 eV to 30 eV on clean Ir(100) show considerable dependence of spectral structure on photon energy. In addition, phtoionization cross-sections for the 4σ, 1π and 5σ levels of chemisorbed CO are strongly dependent on the polarization of the incident radiation. Finally, analysis of a broad body of published data on CO chemisorption for many metals in addition to that of this study leads to the conclusion that the separation in energy between the 4σ and 1π peaks of chemisorbed CO varies systematically with the position of the adsorbent in the Periodic Table. This is ascribed to a systematic geometrical stretching of the bonds in the adsorbate. The susceptibility of the CO molecule to discociation upon chemisorption is also found to vary systematically depending on the position of the adsorbent in the Periodic Table.     

CO在Pu(100)表面吸附的研究

采用密度泛函理论(DFT)研究了CO分子在Pu (100)面上的吸附. 计算结果表明：CO在Pu (100)表面的C端吸附比O端吸附更为有利,属于强化学吸附. CO吸附态的稳定性为穴位倾斜>穴位垂直>桥位>顶位. CO分子与表面Pu原子的相互作用主要源于CO分子的杂化轨道和Pu原子的杂化轨道的贡献. 穴位倾斜吸附的CO分子的离解能垒较小(0.280eV),表明在较低温度下,CO分子在Pu (100)表面会发生离解吸附,离解的C,O原子将占据能量最低的穴位. 关键词： 密度泛函理论 Pu (100) CO 分子和离解吸附     

CO在Pu(100)表面吸附的研究

采用密度泛函理论(DFT)研究了CO分子在Pu (100)面上的吸附. 计算结果表明：CO在Pu (100)表面的C端吸附比O端吸附更为有利，属于强化学吸附. CO吸附态的稳定性为穴位倾斜>穴位垂直>桥位>顶位. CO分子与表面Pu原子的相互作用主要源于CO分子的杂化轨道和Pu原子的杂化轨道的贡献. 穴位倾斜吸附的CO分子的离解能垒较小(0.280eV)，表明在较低温度下，CO分子在Pu (100)表面会发生离解吸附，离解的C，O原子将占据能量最低的穴位.     

Chemisorption of CO on Ir(100) studied by photoemission

Chemisorption of cabon monoxide on a reconstructed Ir(100) surface has been studied by means of LEED and photoemission. In the photoemission spectrum, apart from a low lying peak due to the 4σ-orbital of CO, there is also a broad bump divided by a clear dip. The upper part of this double peak is assigned to the 5σ orbital and the lower part to the 1 π orbital of CO.     

Unique geometric and electronic structure of CO adsorbed on Ge(100): A DFT study

CO adsorption on the Ge(100) surface has been investigated using a slab model with density functional theory implemented in SIESTA. CO was found to be exclusively adsorbed on the asymmetric dimer with C attaching on the lower Ge dimer atom. The adsorption process is barrierless. The calculated adsorption energy and vibration frequencies are comparable to previous experimental results. The crystal orbital Hamilton analysis showed that the bonding between Ge and CO is mainly attributable to the Ge 4p_z orbital overlapping with C 2 s, or with CO molecular orbitals 3σ and 4σ. The repulsive energy between adsorbed CO molecules is less than 1 kcal/mol. The diffusion barrier of CO on the Ge(100) surface is about 14 kcal/mol.     

The adsorption of CO on Ir(111) investigated with FT-IRAS

The adsorption of CO on Ir(111) has been investigated with Fourier transform infrared reflection-absorption spectroscopy, temperature programmed desorption, and low-energy electron diffraction. At sample temperatures between 90 and 350 K, only a single absorption band, above 2000 cm⁻¹, has been observed at all CO coverages. For fractional coverages above approximately 0.2, the bandwidth becomes as narrow as 5.5 cm⁻¹. The linewidth is attributed mainly to inhomogeneous broadening at low CO coverages and to the creation of electron-hole pairs at higher CO coverages. The coverage-dependent frequency shift of the IR band can be described quantitatively using an improved dipolar coupling model. The contribution of the dipole shift and the chemical shift to the total frequency shift were separated using isotopic mixtures of CO. The chemical shift is positive with a constant value of approximately 12 cm⁻¹ for all coverages, whereas the dipole shift increases with coverage up to a value of 36 cm⁻¹ at a coverage of 0.5 ML.     

CO adsorption on alkali-metal covered Ni(100)

The effect of preadsorbed alkali metal atoms Na, K and Cs on CO adsorption on Ni(100) has been studied using Auger spectroscopy and thermal desorption. It was found that the presence of alkali metals causes an appearance of several more tightly bound states in the CO thermal desorption spectra. The observed difference in carbon and oxygen Auger peak line shape on a bare and alkali modified Ni(100) is indicative that the presence of alkali adatoms induces CO decomposition on the Ni(100) surface. The fraction of dissociated CO increases with the amount of alkali adatoms present. At the same overlayer coverage the dissociation probability increases in the sequence Na, K, Cs. A comparison of the strength of the promoting effect on CO dissociation with the changes in the surface electron density in the presence of alkali adatoms has shown that at low overlayer coverages the electronic factor plays a major role in explaining the action of the surface modificators.     

Adsorption of O and CO on Ir(100) from first principles

The adsorption of O and CO on Iridium (100) surface with different coverages (Θ = 1.0, 0.5, 0.25 monolayer (ML)) is studied using density functional theory (DFT). The most energetically preferred site of adsorption for O is found to be the bridge site. However, the top site is the preferred one for CO at coverages of 0.25 ML and 0.5 ML. Oxygen adsorbed on the bridge site at 0.25 ML and 0.5 ML coverages causes a row pairing. A missing row reconstruction appears in the case of 0.25 ML coverage. We find that the adsorption of O (CO) on Ir(100) surface causes disruptions of Ir–Ir bonds in the metal, which reduces (increases) the Ir–Ir bond length.     

The adsorption of Xe and CO on Au(100)

The adsorption of Xe and CO on Au(100) has been studied by LEED, Auger electron spectroscopy, electron energy loss spectroscopy (EELS) and surface potential measurements. The physical adsorption of xenon showed successive stages preceding the completion of a monolayer. The heat of adsorption was 22 (±2) kJ mol^?1 and the maximum surface potential was 0.45 V. Carbon monoxide gave a surface potential of 0.85 V at the highest coverage reached. The heat of adsorption showed a continuous fall from an initial value of 58 (±3) kJ mol^?1 as the coverage increased. Ordered adsorption structures were not observed in LEED for either Xe or CO. The EEL spectrum of clean Au(100) agreed well with spectra of polycrystalline gold. New loss features observed with adsorbed Xe and CO are discussed.     

Sulfur adsorption on Fe(1 1 0): a DFT study

The adsorption of atomic S on the Fe(1 1 0) surface is examined using density functional theory (DFT). Three different adsorption sites are considered, including the atop, hollow and bridge sites and the S is adsorbed at a quarter monolayer coverage in a p(2 × 2) arrangement. The hollow site is found to be the most stable, followed by the bridge and atop sites. At all three sites, S adsorption results in relatively minor surface reconstruction, with the most significant being that for the hollow site, with lateral displacements of 0.09 Å. Comparisons between S-adsorbed and pure Fe surfaces revealed reductions in the magnetic moments of surface-layer Fe atoms in the vicinity of the S. At the hollow site, the presence of S causes an increase in the surface Fe d-orbital density of states between 4 and 5 eV. However, S adsorption has no significant effect on the structure and magnetic properties of the lower substrate layers.     

Effect of S adsorption on magnetic Co(0001) surface: a DFT study

Extended density functional theory calculations with the spin interpolation formula of Vosko, Wilk, and Nusair (VWN) are employed to study the effect of atomic S adsorption on Co(0001) surface. Besides the site preference for atom S in fcc-hollow site and adsorption geometry structures are in good agreement with experiments and previous calculations, some differences are also reported for the geometry of S in hcp-hollow site. Moreover, vibrational frequency, magnetic moments and electronic structure analysis are presented in more detail.     

Cu(100)表面c(2×2)-N原子结构与吸附行为研究

用密度泛函理论的总能计算研究了金属铜(100)面的表面原子结构以及氮原子的c(2×2)吸附状态.研究结果表明：在Cu(100) c(2×2)-N表面系统中，氮原子处于四度配位的空洞(FFH)位置，距离最表面铜原子层的垂直距离为0.20?，最短的Cu—N键长度为1.83?.结构优化的计算否定了被吸附物导致的表面再构模型，即c(2×2)元胞的两个铜原子在垂直于表面方向发生相对位移，一个铜原子运动到氮原子之上的模型.该吸附表面的功函数约为4.65eV, 氮原子的平均吸附能为4.92 eV(以孤立氮原子为能量参考点).计算结果还说明，Cu—N杂化形成的表面局域态的位置在费米面以下约1.0 eV附近出现，氮原子和第一层以及第二层铜原子均有不同程度的杂化作用.该结果为最近有关该表面的STM图像的争论提供了判据性的第一性原理计算结果. 关键词： Cu(100) c(2×2)-N 表面吸附态 密度泛函总能计算     

The growth of Fe overlayers on Ag(100)

Using LEED and Auger spectroscopy the growth of Fe overlayers on Ag(100) was observed to follow an epitaxial layer-by-layer mode for three monolayers, after which islanding occurred. The large (0.9 eV) work function change seen on deposition is not consistent with the prediction of either the uniform positive background model or the virtual level model of adsorbate-induced work function change.     

Ionic and radical adsorption on the Au(hkl) surfaces: A DFT study

Adsorption of several ionic and non-ionic species (OH^?, O, O^?, O^2?, H, H⁺ and H^?) on the low-index Miller Au(hkl) surfaces has been investigated by means of density functional theory based methods. The stability order for adsorptions on the three surfaces decreases with the increasing of the coordination number of the outermost gold atoms in each surface, i.e., Au(110) > Au(100) > Au(111), which is in agreement with the experimental evidences. The detailed COOPs analysis of the various adsorption sites for all adsorbates in the surface with the most stable adsorption(s), Au(110), evidenced that adsorption in the gold surfaces may be a function of particle size and charge and substantiates the variability in the order of preferences sites for the adsorption of the different species found in these low-index Miller Au(hkl) surfaces. This variability increases with the increasing of the stability of the adsorptions on the gold surfaces, i.e., the Au(110) presents more variability in the order of preferences sites for the adsorption of different species.     

The bonding of chalcogen overlayers on Ni (100)

We present new evidence for the character of two forms of bonding by chalcogen adsorbates on Ni(100) for two different coverages, while the adsorbate site remains the same. Comparisons with data from solid state systems, rather than molecular analogs, are used and may be appropriate sources for models in such cases of strongly chemisorbed adatoms. By comparing recent photoemission data on solid chalcogens (S, Se, Te) with that of chalcogen overlayers on Ni(100), we are able, but for different reasons, to support the previous proposal that with the chalcogen atoms adsorbed in a four-fold site that (a) for the ordered c(2×2) one half-monolayer coverage, the chalcogen adatoms on Ni(100) are bonded to two Ni atoms and that (b) for an ordered one-fourth monolayer coverage, the chalcogen is bonded to four Ni atoms. Two chalcogen adsorbate-induced levels, one largely non-bonding and the other made up of bonding electrons, should be found in the valence region when the chalcogen is two-fold coordinated, as it is in the elemental solid. Several methods for testing these proposals have been suggested. The modification of adatom bonding as a function of coverage implies important adatom-adatom interactions which may be involved in the poisoning of Ni catalysts by chalcogen compounds.     

NO在Ir(111)表面吸附与解离的第一性原理研究

本文系统研究了NO在Ir(111)表面的吸附,解离,以及可能的N_2生成机理.结果表明,顶位吸附的NO,其解离能垒较高(3.17 eV),不会发生解离,而三重Hcp和Fcc空位吸附的NO发生解离,能垒分别为1.23和1.28 eV.N_2是唯一的生成物,不会有副产物N_2O的产生.其最可能的反应路径为N和NO经过N_2O中间体而生成N_2,而不是直接N提取和N-N聚合产生N_2的机理.