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1.
T. Pabisiak  A. Kiejna 《Surface science》2011,605(7-8):668-674
The adsorption of gold atoms and formation of nanostructures on the rutile TiO2(110) surface with different degree of oxygen reduction was studied from first principles. The Au atoms adsorb strongest at oxygen vacancy sites. Starting from a very low coverage limit the potential energy profiles or diffusion paths of the adsorbed Au monomers and dimers were calculated. Stable structures of two to nine Au atoms arranged in finite and infinite rows and in the shape of finite-size clusters were determined. All these structures are found to bind to the reduced surface stronger than 2 eV/atom. The elongated Au row-like structures bind by about 0.1 eV stronger than 3D clusters, suggesting a preference for the 1D-like Au growth mode on the missing-row reconstructed TiO2(110).  相似文献   

2.
Pt单原子在低温CO氧化反应中具有很高的催化活性. 利用扫描隧道显微术与密度泛函理论,研究了Pt单原子在还原性TiO2(110)表面的吸附行为及其与CO和O2分子的相互作用. 研究发现在80 K低温下,TiO2表面的氧空位缺陷是Pt单原子的最优吸附位. 将CO和O2分子分别通入Pt单原子吸附后的TiO2表面,研究相应的吸附构型. 实验表明在低覆盖度下,单个Pt原子会俘获一个CO分子,CO分子同时与表面次近邻的五配位Ti原子(Ti5c)成键,进而形成非对称的Pt-CO 复合物构型. 将样品从80 K升温到100 K后,TiO2表面的CO分子会迁移到Pt-CO处形成Pt-(CO)2的复合结构. 对于O2分子,单个Pt原子同样会吸附一个O2分子,O2分子也会与最近邻或次近邻的Ti5c原子成键形成两种Pt-O2构型. 这些结果在单分子尺度上揭示了CO和O2与Pt单原子的相互作用,呈现了CO与O2反应中的初始状态.  相似文献   

3.
王芒芒  宁华  陶向明  谭明秋 《物理学报》2011,60(4):47301-047301
用密度泛函理论(DFT)研究了金属Au(110)表面结构以及氧原子的吸附状态.计算得到Au(110)-(1×2)缺列再构表面原子的弛豫分别是-15.0%(Δd12/d0)和-1.1%(Δd23/d0),表面能为52.7 meV/2,功函数Φ=5.00 eV;Au(110)-(1×3)缺列再构表面的Δd1 关键词: 缺列再构Au(110)表面 STM图像 氧原子吸附  相似文献   

4.
Au/TiO2/Ru(0 0 0 1) model catalysts and their interaction with CO were investigated by scanning tunneling microscopy and different surface spectroscopies. Thin titanium oxide films were prepared by Ti deposition on Ru(0 0 0 1) in an O2 atmosphere and subsequent annealing in O2. By optimizing the conditions for deposition and post-treatment, smooth films were obtained either as fully oxidized TiO2 or as partly reduced TiOx, depending on the preparation conditions. CO adsorbed molecularly on both oxidized and reduced TiO2, with slightly stronger bonding on the reduced films. Model catalyst surfaces were prepared by depositing submonolayer quantities of Au on the films and characterized by X-ray photoelectron spectroscopy and scanning tunneling microscopy. From X-ray photoelectron spectroscopy, a weak interaction between the Au and the TiO2 substrate was found. At 100 K CO adsorption occurred on both the TiO2 film and on the Au nanoparticles. CO desorbed from the Au particles with activation energies between 53 and 65 kJ/mol, depending on the Au coverage. If the Au deposit was annealed to 770 K prior to CO exposure, the CO adsorption energy decreased significantly. STM measurements revealed that the Au particles grow upon annealing, but are not encapsulated by TiOx suboxides. The higher CO adsorption energy observed for smaller Au coverages and before annealing is attributed to a significantly stronger interaction of CO with mono- and bilayer Au islands, while for higher particles, the adsorption energy becomes more bulk-like. The implications of these effects on the known particle size effects in CO oxidation over supported Au/TiO2 catalysts are discussed.  相似文献   

5.
《Surface Science Reports》2014,69(4):366-388
Both density functional theory calculations and numerous experimental studies demonstrate a variety of unique features in metal supported oxide films and transition metal doped simple oxides, which are markedly different from their unmodified counterparts. This review highlights, from the computational perspective, recent literature on the properties of the above mentioned surfaces and how they adsorb and activate different species, support metal aggregates, and even catalyse reactions. The adsorption of Au atoms and clusters on metal-supported MgO films are reviewed together with the cluster׳s theoretically predicted ability to activate and dissociate O2 at the Au–MgO(100)/Ag(100) interface, as well as the impact of an interface vacancy to the binding of an Au atom. In contrast to a bulk MgO surface, an Au atom binds strongly on a metal-supported ultra-thin MgO film and becomes negatively charged. Similarly, Au clusters bind strongly on a supported MgO(100) film and are negatively charged favouring 2D planar structures. The adsorption of other metal atoms is briefly considered and compared to that of Au. Existing computational literature of adsorption and reactivity of simple molecules including O2, CO, NO2, and H2O on mainly metal-supported MgO(100) films is discussed. Chemical reactions such as CO oxidation and O2 dissociation are discussed on the bare thin MgO film and on selected Au clusters supported on MgO(100)/metal surfaces. The Au atoms at the perimeter of the cluster are responsible for catalytic activity and calculations predict that they facilitate dissociative adsorption of oxygen even at ambient conditions. The interaction of H2O with a flat and stepped Ag-supported MgO film is summarized and compared to bulk MgO. The computational results highlight spontaneous dissociation on MgO steps. Furthermore, the impact of water coverage on adsorption and dissociation is addressed. The modifications, such as oxygen vacancies and dopants, at the oxide–metal interface and their effect on the adsorption characteristics of water and Au are summarized. Finally, more limited computational literature on transition metal (TM) doped CaO(100) and MgO(100) surfaces is presented. Again, Au is used as a probe species. Similar to metal-supported MgO films, Au binds more strongly than on undoped CaO(100) and becomes negatively charged. The discussion focuses on rationalization of Au adsorption with the help of Born–Haber cycle, which reveals that the so-called redox energy including the electron transfer from the dopant to the Au atom together with the simultaneous structural relaxation of lattice atoms is responsible for enhanced binding. In addition, adsorption energy dependence on the position and type of the dopant is summarized.  相似文献   

6.
魏彦薇  杨宗献 《物理学报》2008,57(11):7139-7144
采用基于广义梯度近似的投影缀加平面波(projector augmented wave)雁势和具有三维周期性边界条件的超晶胞模型,用第一性原理方法,计算并分析了Au在CeO2(110)和Zr掺杂的CeO2(110) 面的吸附能,吸附结构和电子结构等特征.从而得出Zr掺杂对Au/CeO2(110)吸附体系的影响.结果表明:Zr的掺杂增大了Au在CeO2(110) 面的吸附能,并改变了最强吸附位置,且导致了吸附体系中衬底结 关键词: Au Zr掺杂 2')" href="#">CeO2 吸附  相似文献   

7.
利用同步辐射高分辨光电子能谱研究了金团簇在部分还原TiO2-(1×1)表面的生长和稳定性.价带谱实验结果观察到非常少量金团簇的沉积导致了Ti3+的3d峰完全消失,表明金团簇成核在TiO2-(1×1)表面的氧缺陷位.Au4f芯电子光电子能谱实验结果证明了TiO2-(1×1)表面氧缺陷位向金团簇转移电荷.还对比研究了化学剂量比和部分还原的TiO2-(1×1)表面上金团簇的热稳定性.当金团簇尺寸相近时部分还原的TiO2-(1×1)表面上金团簇要比化学剂量比的TiO2-(1×1)面上金团簇稳定;在相同的表面上尺寸大的金团簇要比尺寸小的金团簇稳定.  相似文献   

8.
王云江  王崇愚  王山鹰 《中国物理 B》2011,20(3):36801-036801
CO adsorption on small Au n(n = 1-7) clusters which are supported by a partially reduced rutile TiO 2(110) surface has been investigated by the first-principles method.The low coordinated sites of Au clusters are favorable for CO adsorption.CO-Au n-TiO 2 system displays surface magnetism.There is a strong interaction between the adsorbed CO molecule and the supported Au clusters.  相似文献   

9.
黄平  杨春 《物理学报》2011,60(10):106801-106801
采用基于密度泛函理论的平面波超软赝势法,计算了TiO2分子在GaN(0001)表面的吸附成键过程、吸附能量和吸附位置. 计算结果表明不同初始位置的TiO2分子吸附后,Ti在fcc或hcp位置,两个O原子分别与表面两个Ga原子成键,Ga-O化学键表现出共价键特征,化学结合能达到7.932-7.943eV,O-O连线与GaN[1120]方向平行,与实验观测(100)[001] TiO2//(0001)[1120]GaN一致. 通过动力学过程计算分析,TiO2分子吸附过程经历了物理吸附、化学吸附与稳定态形成的过程,稳定吸附结构和优化结果一致. 关键词: GaN(0001)表面 2分子')" href="#">TiO2分子 密度泛函理论 吸附  相似文献   

10.
赵巍  汪家道  刘峰斌  陈大融 《物理学报》2009,58(5):3352-3358
采用第一性原理研究了H2O分子在Fe(100),Fe(110),Fe(111)三个高对称晶面上的表面吸附.结果表明,H2O分子在三个晶面上的最稳定结构皆为平行于基底表面的顶位吸附结构.H2O分子与三个晶面相互作用的吸附能及几何结构计算结果表明H2O分子与三个晶面的相互作用程度不同,H2O分子与Fe(111)晶面的相互作用最强,其次是Fe(100),相互作用最弱的是Fe(110)表面,而这与晶面原子 关键词: 第一性原理 Fe单晶表面 2O分子')" href="#">H2O分子 分子吸附  相似文献   

11.
The interaction of CO with Au atoms adsorbed on terrace and low-coordinates sites (edge and corner) of the MgO(1 0 0) surface was studied using the density functional theory (DFT) in combination with embedded cluster models. Surface anionic (O2−) and neutral oxygen vacancy (Fs) sites were considered. In all the cases, the CO stretching frequencies are shifted with respect to free CO with values between −232 and −358 cm−1. In particular, the values for Au on Fs at edge and corner are shifted to higher stretching frequencies by 100 and 59 cm−1, respectively, with respect to the value on a perfect MgO(1 0 0) surface. This result is in agreement with recent scanning tunneling microscopy and infrared spectroscopy experiments where a corresponding shift of 70 cm−1 was observed by comparing the measurements on perfect and O-deficient MgO(1 0 0) surfaces. However, these results are different than expected because Au atoms on Fs centers are negatively charged and, therefore, according to the generally accepted scheme the CO frequency should be red-shifted with respect to the adsorption on anionic five-coordinated site where the Au atom is essentially neutral. The following picture emerges from the present results: the single occupied HOMO(α) of Au atom on Fs at low-coordinated sites consists in two lobes extended sideward the Au atom. For symmetry reasons, this MO overlaps efficiently with the 2π MO of CO. This bonding contribution to the Au-CO link is counteracted by a Pauli repulsion between the 5σ MO of CO and more internal orbitals (the HOMO-1(α) and the HOMO(β)) centered on Au. In consequence, CO is forced to vibrate against a region with a high electron density. This is the so-called “wall effect” which by itself contributes to higher CO frequency values.  相似文献   

12.
负载型金纳米颗粒催化剂在许多催化反应中展现出非常好的催化活性,但是金纳米颗粒在高温等反应条件下容易烧结团聚,极大地限制了金催化剂的应用。利用原子层沉积技术在Au/TiO2催化剂表面分别精确沉积了一层超薄的二氧化钛和氧化铝包裹层,并对比研究了包裹层对金纳米颗粒的热稳定性影响。原位红外漫反射CO吸附和x-射线光电子能谱数据证实了氧化物包裹层的存在。发现亚纳米厚的氧化铝包裹层能够在600 C完全避免金纳米颗粒的团聚;相反,二氧化钛包裹层对金纳米颗粒稳定性的提高没有明显效果。通过CO氧化探针反应的活性测试,发现随着煅烧温度的升高氧化铝包裹的Au/TiO2 催化剂的活性逐渐提高,表明高温处理可以促进被包裹金原子的暴露并表现出催化活性。提供了提高金纳米颗粒稳定性的有效方法,为拓展金催化剂在条件苛刻的反应中的应用奠定了技术基础.  相似文献   

13.
The adsorption at room temperature of 1-bromo-1-fluoroethene (CH2CBrF) on TiO2 has been investigated by Fourier-transform infrared spectroscopy after a preventive assignment of the fundamentals in the gas-phase, carried out for the first time. The spectrum resulting from the adsorption has been compared with the gas-phase one and the most important differences consist in a red-shift of the CH2 stretching vibration and in the presence of two distinct absorptions for both the C=C and C–F stretching modes. Basing on the observed features it has been inferred that there is the formation of an H-bond between the CH2 group and a surface Lewis basic site and that the adsorption can occur through the double C=C bond or the F atom. Two proposed adsorbate-substrate structures have been investigated by periodic quantum-mechanical calculations at DFT/B3LYP level considering the rutile (110) surface. In the case of the adsorption by the F atom, also the formation of the H-bond has been considered. The interaction energy resulting from the adsorption through the double C = C bond is smaller than that arising from the interaction by means the F atom and the H-bond. The shifts due to the adsorption of the calculated vibrational frequencies well reproduce the experimental data.  相似文献   

14.
Xiao Han 《Molecular physics》2013,111(24):3546-3555
The trapping and detection of nitrogen oxide with tungsten trioxide has become a popular research topic in recent years. Knowledge of the complete reaction mechanism for nitrogen oxide adsorption is necessary to improve detector performance. In this work, we used density functional theory (DFT) calculations to study the adsorption characteristics and electron transfer of nitrogen dioxide on an oxygen-deficient monoclinic WO3 (0 0 1) surface. We observed different reactions of NO2 on slabs with different O- and WO-terminated WO3 (0 0 1) surfaces with oxygen vacancies. Our calculations show that the bridging oxygen atom on an oxygen defect on an O-terminated WO3 (0 0 1) surface is the active site where an NO2 molecule is oxidised into nitrate and is adsorbed onto the surface. On a WO-terminated (0 0 1) surface, one of the oxygen atoms from the NO2 molecule fills the oxygen vacancy, and the resulting NO fragment is adsorbed onto a W atom. Both of these adsorption models can cause an increase in the electrical resistance of WO3. We also calculated the adsorption energies of NO2 on slabs with different oxygen-deficient WO3 surfaces.  相似文献   

15.
We use ultra-high vacuum scanning tunneling microscopy (UHV–STM) to probe, at the atomic level, the structure of mass-selected isolated V1, V2, VO and VO2 clusters deposited on rutile TiO2(110) by ion soft landing. All four species interact differently with the TiO2 surface and the ultimate binding site and configuration strikes a balance between the gas-phase structure and the ligation of this cluster by the TiO2 surface. Our results show that vanadium atoms prefer to bind in the upper threefold hollow sites on the surface and have a slight tendency to pair along the [1–10] direction, while vanadium dimers bind to the surface oriented along the [001] direction exclusively. VO clusters bind with the vanadium atom in the upper threefold hollow site and with the oxygen atom bound to an adjacent fivefold coordinated Ti atom (5c-Ti). The VO2 cluster also binds with the vanadium atom in the upper threefold hollow site and with both oxygen atoms bound to adjacent 5c-Ti atoms or with only one oxygen bound to the surface and the other directed out of the plane of the surface.  相似文献   

16.
We evaluated the adsorption of SO3 molecule on Au (1 1 1) surface using first principles calculation by a slab model with a periodic boundary condition. We find that there are six stable adsorption configurations on an Au surface, where the SO3 molecule is adsorbed above the three-fold fcc and hcp hollow sites and on the atop site. In two of these configurations, S and two O atoms are bound to the Au atoms, the next two configurations have all the three O atoms bound to the Au surface atoms, and the last two configurations have the S atom bound to an Au surface atom on the atop site and O atoms situated above the hollow sites. In these configurations, the electronic structures of SO3 on the Au surface show that molecular orbitals of SO3 and those of the Au surface are hybridized in the active metal d-band region, that the localized molecular orbitals in SO3 are stabilized, and that charge is transferred from Au to S 3p by SO3 adsorption on the Au surface though there is little other interaction of the S and O (bound to Au) component with Au. Moreover, the bond between the S and O atoms bound to Au is weakened due to SO3 adsorption on the Au surface due to the charge polarization of the O-Au bond. This interaction is likely to encourage the S-O bond to break.  相似文献   

17.
陈玉红  杜瑞  张致龙  王伟超  张材荣  康龙  罗永春 《物理学报》2011,60(8):86801-086801
采用第一性原理方法研究了H2分子在Li3N(110)晶面的表面吸附. 通过研究H2/Li3N(110)体系的吸附位置、吸附能和电子结构发现: H2分子吸附在N桥位要比吸附在其他位置稳定,此时在Li3N(110)面形成两个-NH基,其吸附能为1.909 eV,属于强化学吸附;H2与Li3N(110)面的相互作用主要是H 1s轨道与N 关键词: 第一性原理 3N(110)')" href="#">Li3N(110) 2')" href="#">H2 吸附和解离  相似文献   

18.
吴小霞  王乾恩  王福合  周云松 《物理学报》2010,59(10):7278-7284
基于密度泛函理论,在广义梯度近似下研究了Cl在γ-TiAl(111)表面的吸附.计算结果表明:γ-TiAl(111)表面的面心立方位置(fcc)和六角密排位置(hcp)为Cl吸附的稳定位置,当覆盖度Θ小于一个单层(ML)时,Cl原子倾向于吸附在γ-TiAl(111)表面近邻为多Ti的位置.电子结构分析发现,Cl原子同表面金属原子形成较强的离子键,并且成键具有一定的方向性.当Cl原子和O原子共同在γ-TiAl(111)表面吸附时,二者都趋  相似文献   

19.
采用平面波超软赝势方法计算了锐钛矿型TiO2(101)面的表面能和表面原子弛豫结构.首先对TiO2(101)面的6种不同的表面原子终止结构的体系总能量进行了计算,结果表明终止原子为两配位的O原子、次层为五配位的Ti原子的表面结构最为稳定.针对该表面研究了表面能和原子弛豫与模型中原子层数和真空厚度的关系,当原子层数为12层,真空厚度为0.4nm时,表面能收敛度小于0.01J/m2.研究发现:表面上两配位的O原子向里移动约0.0012nm,五配 关键词: 第一性原理 2')" href="#">TiO2 表面结构 弛豫  相似文献   

20.
Using all electron fully relativistic DFT calculations we have computed the EPR properties of Au atoms bound to various sites of the MgO surface. Changes in g-tensor and hyperfine coupling constants provide a way to identify the gold adsorption site and to map the surface morphology by comparison of measured and calculated EPR spectra. We found a strong reduction of the isotropic hyperfine coupling constant, aiso(Au), for adsorbed gold compared to the free atom; this reduction, which is about 45% for terrace sites, is more pronounced when Au interacts with low-coordinated sites like steps, edges and corners where it is about 60%. The reduction of aiso(Au) is accompanied by a corresponding increase of the superhyperfine interaction with the surface oxygen sites, as measured by aiso(17O). Large anisotropies in the g-tensor are computed for all sites.  相似文献   

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