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1.
The reaction mechanism for the styrene selective oxidation on the oxygen preadsorbed Cu(111) surface has been studied by the density functional theory calculation with the periodic slab model. The calculated result indicated that the process includes two steps: forming the oxametallacycle intermediate (OMMS) and then producing the products. In addition, it was found that the second step, from OMMS to the product, is the rate‐controlling step, which is similar to the previous work of ethylene selective oxidation. The present result indicated that the selectivity towards the formation of styrene epoxide on Cu(111) is much higher than that on Au(111). More importantly, we found that the mechanism via the OMMS (2) (i.e., the preadsorbed atomic oxygen bound to the CH2 group involved in C6H5? CH?CH2) to produce styrene epoxide is kinetically favored than that of OMMS (1). We also found that the selectivity toward the styrene epoxide formation on Cu2O is similar to that of Cu(111). © 2009 Wiley Periodicals, Inc. J Comput Chem, 2010  相似文献   

2.
采用密度泛函理论研究了吸附有O原子的Au(111)表面上乙醇选择性氧化的反应机理.反应结果表明,除O原子和中间产物二齿醋酸根(CH3CHOO)外,其他中间产物在Au(111)表面扩散能垒均较低,不会对反应速控步骤的确定造成影响.乙醇羟基氧化脱氢为反应的第一步骤,当氧化剂为吸附态的O原子或者为OH基时,反应活化能分别为0.20和0.17eV.氧化产物乙氧基(CH3CH2O)进一步氧化脱氢生成乙醛则需要表面吸附的O原子或另一表面吸附的OH基的参与,所需活化能为0.29或0.27eV.同时,乙醛易与表面吸附的乙氧基反应生成乙氧基半缩醛(CH3CHOOC2H5),其可进一步与O原子作用,脱氢形成乙酸乙酯.此外,在乙醛深度氧化成酸的过程中需要克服较高的反应能垒,因而在表面反应温度较低时无法进行,这与实验结果相符.  相似文献   

3.
The mechanisms of methanol (CH3OH) oxidation on the PtPd(111) alloy surface were systematically investigated by using density functional theory calculations. The energies of all the involved species were analyzed. The results indicated that with the removal of H atoms from adsorbates on PtPd(111) surface, the adsorption energies of (i) CH3OH, CH2OH, CHOH, and COH increased linearly, while those of (ii) CH3OH, CH3O, CH2O, CHO, and CO exhibited odd‐even oscillation. On PtPd(111) surface, CH3OH underwent the preferred initial C H bond scission followed by successive dehydrogenation and then CHO oxidation, that is, CH3OH → CH2OH → CHOH → CHO → CHOOH → COOH → CO2. Importantly, the rate‐determining step of CH3OH oxidation was found to switch from CO → CO2 on Pt(111) to COOH → CO2 + H on PtPd(111) with a lower energy barrier of 0.96 eV. Moreover, water also decomposed into OH more easily on PtPd(111) than on Pt(111). The calculated results indicate that alloying Pt with Pd could efficiently improve its catalytic performance for CH3OH oxidation through altering the primary pathways from the CO path on pure Pt to the non‐CO path on PtPd(111).  相似文献   

4.
The adsorption of multivalent thiols on gold (111) surface was investigated using density functional theory applying the Perdew–Burke–Ernzerhof functional. Through the comparison of differences in energetics, structure and charge density distribution of a set of monodentate and polydentate thiols, we have described in detail the factors affecting the adsorption energy and the role played by the multivalence, which causes a decreasing of adsorption energy because of both electronic and steric hindrance effects. Finally, the comparison between the adsorption of 1,2‐ and 1,3‐disulfides revealed how the chain length may affect the cleavage of the S? S bond when they adsorb on Au(111) surface. © 2013 Wiley Periodicals, Inc.  相似文献   

5.
1INTRODUCTION Methoxy(CH3O)has been identified as the first intermediate in the decomposition of methanol on extensive list of clean transition metal surfaces,such as Ni(100)[1],Cu(100)[2,3],Cu(111)[4],Ag(111)[5],Au(110)[6],Pd(111)[7]and Ru(0001)[8].The electronic structure of the metal is a determining factor in OH bond scission.In fact,group IB clean surfaces have shown very low activity towards this reaction,al-though there are reports on low amounts of methoxy formed on clean Cu(…  相似文献   

6.
采用密度泛函理论并结合周期性平板模型的方法,优化了肉桂醛在Au(111)面上的吸附模型,并详细探讨了肉桂醛在Au(111)面上选择性加氢的反应机理(C=O,C=C以及1,4 共轭加成机理). 计算结果表明,肉桂醛以C=O和C=C协同吸附于Au(111)面上时,吸附构型最稳定. 此时,不同吸附模式的吸附能平均在140.0kJ·mol-1. 通过搜索不同机理下每个基元反应的过渡态,得出肉桂醛在Au(111)面上最可能的选择性加氢产物为苯丙醛,且其按照1,4 共轭加成机理间接得到苯丙醛比C=C直接加氢机理具有更低的活化能. 具体反应过程为:肉桂醛C=O的O优先加H形成烯丙基型中间体,继而该中间体中与苯环相连的C原子继续加H形成烯醇(ENOL),最终烯醇异构成苯丙醛. 其中ENOL的生成过程所需的活化能最高,是反应的控速步骤.  相似文献   

7.
采用密度泛函理论并结合周期性平板模型的方法,优化了肉桂醛在Au(111)面上的吸附模型,并详细探讨了肉桂醛在Au(111)面上选择性加氢的反应机理(C=O,C=C以及1,4共轭加成机理).计算结果表明,肉桂醛以C=O和C=C协同吸附于Au(111)面上时,吸附构型最稳定.此时,不同吸附模式的吸附能平均在140.0kJ?mol-1.通过搜索不同机理下每个基元反应的过渡态,得出肉桂醛在Au(111)面上最可能的选择性加氢产物为苯丙醛,且其按照1,4共轭加成机理间接得到苯丙醛比C=C直接加氢机理具有更低的活化能.具体反应过程为:肉桂醛C=O的O优先加H形成烯丙基型中间体,继而该中间体中与苯环相连的C原子继续加H形成烯醇(ENOL),最终烯醇异构成苯丙醛.其中ENOL的生成过程所需的活化能最高,是反应的控速步骤.  相似文献   

8.
采用密度泛函理论计算了巴豆醛4种构型的稳定性,并选取最优构型进一步研究了其Au(111)面上的吸附及选择性加氢机理.计算结果表明,具有E-(s)-trans构型的巴豆醛稳定性最高.当巴豆醛通过C O吸附于Au(111)面的顶位时,该构型吸附能最大,吸附模型最稳定;巴豆醛向Au(111)表面转移电子0.045e,且其p轨道与金属表面的d轨道发生较强相互作用,使得巴豆醛的键级减弱.此外,通过分析各基元反应的活化能、反应热以及构型变化可知,巴豆醛在Au(111)面上按照2,1-加成机理(部分加氢机理)生成巴豆醇的可能性最大,且降低温度有利于反应转化率的提高.  相似文献   

9.
甲醇在Au(111)表面吸附的密度泛函研究   总被引:2,自引:0,他引:2  
 采用基于第一性原理的密度泛函理论和周期平板模型相结合的方法,对CH3OH分子在Au(111)表面top, fcc, hcp和bridge位的吸附模型进行了构型优化、能量计算以及Mulliken布居分析,结果表明top位是较有利的吸附位. 吸附的CH3OH解离产生甲氧基CH3O和H, 对它们在Au(111)面的吸附进行的计算表明, bridge和fcc位分别是二者的最佳吸附位. 对过渡态的计算给出了CH3OH在Au表面解离吸附的可能机理: 首先发生 O-H 键的断裂,继而生成甲氧基中间体.  相似文献   

10.
赵新飞  陈浩  吴昊  王睿  崔义  傅强  杨帆  包信和 《物理化学学报》2018,34(12):1373-1380
利用NO2或O2作为氧化剂,研究了氧化锌在Au(111)和Cu(111)上的生长和结构。NO2表现了更好的氧化性能,有利于有序氧化锌纳米结构或薄膜的生长。在Au(111)和Cu(111)这两个表面上,化学计量比氧化锌都形成非极性的平面化ZnO(0001)的表面结构。在Au(111)上,NO2气氛下室温沉积锌倾向于形成双层氧化锌纳米结构;而在更高的沉积温度下,在NO2气氛中沉积锌则可同时观测到单层和双层氧化锌纳米结构。O2作为氧化剂时可导致形成亚化学计量比的ZnOx结构。由于铜和锌之间的强相互作用会促进锌的体相扩散,并且铜表面可以被氧化形成表面氧化物,整层氧化锌在Cu(111)上的生长相当困难。我们通过使用NO2作为氧化剂解决了这个问题,生长出了覆盖Cu(111)表面的满层有序氧化锌薄膜。这些有序氧化锌薄膜表面显示出莫尔条纹,表明存在一个ZnO和Cu(111)之间的莫尔超晶格。实验上观察到的超晶格结构与最近理论计算提出的Cu(111)上的氧化锌薄膜结构相符,具有最小应力。我们的研究表明,氧化锌薄膜的表界面结构可能会随氧化程度或氧化剂的不同而变化,而Cu(111)的表面氧化也可能影响氧化锌的生长。当Cu(111)表面被预氧化成铜表面氧化物时,ZnOx的生长模式会发生变化,锌原子会受到铜氧化物晶格的限域形成单位点锌。我们的研究表明了氧化锌的生长需要抑制锌向金属基底的扩散,并阻止亚化学计量比ZnOx的形成。因此,使用原子氧源有利于在Au(111)和Cu(111)表面上生长有序氧化锌薄膜。  相似文献   

11.
Chiral molecular self‐assemblies were usually achieved using short‐range intermolecular interactions, such as hydrogen‐, metal–organic, and covalent bonding. However, unavoidable surface defects, such as step edges, surface reconstructions, or site dislocations may limit the applicability of short‐range chirality recognition. Long‐range chirality recognition on surfaces would be an appealing but challenging strategy for chiral reservation across surface defects at long distances. Now, long‐range chirality recognition is presented between neighboring 3‐bromo‐naphthalen‐2‐ol (BNOL) stripes on an inert Au(111) surface across the herringbone reconstruction as investigated by STM and DFT calculations. The key to achieving such recognition is the herringbone reconstruction‐induced local dipole accumulation at the edges of the BNOL stripes. The neighboring stripes are then forced to adopt the same chirality to create the opposite edged dipoles and neutralize the neighbored dipole moments.  相似文献   

12.
三种Au(111)催化水煤气变换反应机理的比较   总被引:1,自引:0,他引:1  
采用密度泛函理论对三种水煤气变换反应(WGSR)机理(氧化还原机理、羧基机理、甲酸基的生成机理)在Au(111)面上的反应历程进行详细讨论.通过对表面吸附物种(H2O、CO、OH、O、H、CO2、COOH、HCOO)的吸附行为进行研究,得到最佳活性吸附中心.对三种机理中的14个基元反应的活化能进行分析,得出WGSR在Au(111)上按照羧基机理和氧化还原机理进行的可能性较大,按照甲酸基的生成机理进行的可能性较小.相比较羧基机理和氧化还原机理,反应更有可能按照羧基机理进行,最佳反应途径为H2O-H→OH+CO→COOH+OH→CO2.  相似文献   

13.
For the first time, we demonstrate olefin epoxidation promoted by an extended Au surface. The oxidation of styrene to styrene epoxide, benzoic acid, and benzeneacetic acid is promoted on Au(111) covered with 0.2 ML of oxygen atoms. The estimated selectivity for styrene epoxide formation is approximately 53%. Total combustion to CO2 accounts for approximately 20% of the styrene reaction. We propose that styrene epoxide, benzoic acid, and benzeneacetic acid are produced via two possible oxametallacycle intermediates. Our work demonstrates that extended Au is an effective material for olefin oxidation, which has implications for understanding the activity of nanoscale Au catalysts.  相似文献   

14.
本文研究BMIPF6离子液体中Au(111)和Pt(111)表面Ge的电沉积行为. 循环伏安法测试结果表明,在含0.1 mol·L-1 GeCl4的BMIPF6溶液Au(111)和Pt(111)表面均有两个与Ge沉积过程相关的还原峰. 第一个还原峰包含了Ge4+还原成Ge2+及Ge的欠电位沉积,第二个还原峰对应Ge的本体沉积. 现场扫描隧道显微镜研究结果表明,Ge在Au(111)和Pt(111)表面均有两层欠电位沉积. 第一层欠电位沉积厚度约为0.25 nm、形貌平整、带有缝隙的亚单层结构. 第二层欠电位沉积形貌相对粗糙的点状团簇结构. 该欠电位沉积过程伴随表面合金化.  相似文献   

15.
Self-organized systems have attracted much at-tention due to their potential applications in nano- technology as a bottom-up?approach for the con-struction of molecule-scale devices and nanostruc-tures[1—4]. Beyond the self-assembly of small molecu-lar building blocks, Schnherr et al. recently suc-ceeded in arranging the rosette supramolecular nanos-tructures in two dimensions on HOPG[5,6]. Moreover, interest has tremendously increased in the su-pramolecular structures via coordination-dr…  相似文献   

16.
In order to elucidate electronic effects on the oxidation of CO on small Ru clusters, we investigated this reaction on well defined Ru/Au(111) model systems via parallel in-situ STM studies of the structure and electrochemical deposition of Ru on Au(111) in H2SO4 solution and cyclic voltammetry of CO monolayer oxidation on these surfaces. The Ru deposit consists of nanoscale islands, which coalesce with increasing coverage. The Ru saturation coverage depends on the deposition potential, resulting in Ru submonolayer (>0.1 V), (defective) monolayer (≥−0.1 V), and multilayer films (<−0.1 V). At potentials >0.6 V irreversible formation of Ru oxide/hydroxide species is observed, which can be partly reduced in the range 0.4 to 0.0 V. CO stripping commences at ≈0.1 V and occurs over a broad potential range. From the stripping charge a local CO coverage on the Ru monolayer islands of 0.7 ML was estimated. The observed influence of the morphology of the Ru deposit on the CO stripping voltammetry is explained by (local) variations in the CO adsorption energy due to electronic modifications of the Ru film.  相似文献   

17.
研究Au(111)和Au(100)表面非离子型氟表面活性剂FSN自组装膜的电化学行为.电化学扫描隧道显微术和循环伏安法测试表明,在0~0.8 V电位区间,FSN自组装膜未发生氧化还原,均一性好,可稳定地存在于电极表面,并显著抑制硫酸根离子在电极表面的吸附和Au单晶表面的重构.在FSN自组装膜Au单晶电极的初始氧化阶段,Au(111)表面有少量突起,而Au(100)表面呈现台阶剧烈变化,但FSN自组装膜的吸附结构没有改变.与Au(100)表面相比,Au(111)表面形成的FSN自组装膜可更有效地抑制Au表面的氧化.  相似文献   

18.
采用基于密度泛函理论的第一性原理方法和平板模型研究了CH3SH分子在Au(111)表面的吸附构型和电子结构. 系统地计算了S原子在不同位置以不同方式吸附的系列构型, 计算结果表明, CH3SH分子倾向于吸附在top位上, S-C键相对于Au表面法线的夹角为62°~78°|而S-H键断裂后CH3S_H则倾向于吸附在bri-fcc位上, S-C键相对于Au(111)表面法线的夹角为49°~57°. 比较分析CH3SH分子和CH3S_H的吸附, 发现CH3SH分子倾向于不解离吸附, 表面温度的提升和缺陷的出现可能促使S-H键的断裂. 通过比较S原子在独立的CH3SH分子和吸附状态下的局域态密度, 发现S-H键断裂后S原子和表面的键合强于S-H键未断裂时S原子和表面的键合. 扫描隧道显微镜(STM)图像模拟显示了CH3SH和CH3S_H在Au(111)表面吸附的3个典型的STM图像.  相似文献   

19.
The Cd underpotential deposition (UPD) process on Au(111) was analyzed by means of combined electrochemical measurements and in situ scanning tunneling microscopy (STM). In the underpotential range 300?ΔE (mV) ?400, 2D Cd islands are formed on the fcc regions of the Au(111)‐(√3 × 22) reconstructed surface without lifting the reconstruction. At lower underpotentials, the 2D Cd islands grow and, simultaneously, new 2D islands nucleate and coalesce with the previous ones forming a complete condensed Cd monolayer (ML). STM images and long time polarization experiments performed at ΔE = 70 mV demonstrate the formation of an Au? Cd surface alloy. At ΔE = 10 mV, the formation of the complete Cd ML is accompanied by a significant Au? Cd surface alloying and the kinetic results reveal two different solid‐state diffusion processes. The first one, with a diffusion coefficient D1 = 4 × 10?17 cm2 s?1, could be ascribed to the mutual diffusion of Au and Cd atoms through a highly distorted (vacancy‐rich) Au? Cd alloy layer. The second and faster diffusion process (D2 = 7 × 10?16 cm2 s?1) is associated with the appearance of an additional peak in the anodic stripping curves and could be attributed to the formation of another CdzAux alloy phase. Copyright © 2008 John Wiley & Sons, Ltd.  相似文献   

20.
甲硫醇在Au(111)表面不同覆盖度下吸附的第一性原理研究   总被引:1,自引:0,他引:1  
采用第一性原理方法研究了五种覆盖度下甲硫醇在Au(111)面的吸附构型和吸附能. 分别对于S-H解离前CH3SH和S-H解离后CH3S, 计算其在不同覆盖度下的吸附结构和能量. 结果显示各种覆盖度下CH3SH都优先吸附于top位, 倾斜角为70°±2°, 在低覆盖度(1/12, 1/9, 1/8)下的吸附能最大, 为0.33~0.35 eV; 而CH3S在各种覆盖度下稳定吸附于bri-fcc位, 倾斜角为48.3°~58.5°, 低覆盖度下的吸附能为2.08 eV. 对于CH3SH和CH3S的吸附, 吸附能均随覆盖度的增大而减小. 重点研究了范德华力对高覆盖度吸附的影响. 在覆盖度为1/3时, 采用DFT-D2方法, 分别计算了CH3SH和CH3S的吸附, 结果显示范德华力使吸附物和Au表面的距离减小, 同时使CH3SH和CH3S的吸附能分别增大为0.59 eV和2.27 eV. DFT-D2方法修正使CH3SH的结果更接近实验结论, 但使CH3S的结果偏离实验值.  相似文献   

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