氢原子在Ti(0001)表面吸附的密度泛函理论研究

用密度泛函理论研究了氢原子的污染对于Ti(0001)表面结构的影响. 通过PAW总能计算研究了p(1×1)、p(1×2)、3^1/2×3^1/2R30[deg]和p(2×2)等几种氢原子覆盖度下的吸附结构, 以及在上述结构下Ti(0001)面fcc格点和hcp格点的氢原子吸附. 结果表明, 在p(1×1)-H、p(1×2)-H、3^1/2×3^1/2R30[deg]-H和p(2×2)-H几种H原子覆盖度下, 以p(1×1)-H结构的单个氢原子吸附能为最大. 在p(1×1)-H吸附结构下, 由于氢原子吸附导致的Ti(0001)表面Ti原子层收缩的理论计算数值分别为-2.85%(hcp吸附)和-4.31%(fcc吸附), 因此实际上最有可能的情况是两种吸附方式都有一定的几率. 而实验中观察到的所谓“清洁”Ti(0001)表面实际上是有少量氢原子污染的表面. 不同覆盖度和氢分压下, 氢原子吸附的污染对Ti(0001)表面结构有极大的影响, 其表面的各种特性都会随覆盖度的不同而产生相应的变化.     

氢原子在Be(0001)表面吸附的密度泛函理论研究

采用第一性原理的密度泛函理论研究单个氢原子和多个氢原子在Be(0001)表面吸附性质.给出了氢吸附Be(0001)薄膜表面的原子结构、吸附能、饱和度、功函数、偶极修正等特性参数.同时也讨论了相关吸附性质与氢原子覆盖度(0.06-1.33ML)的关系.计算结果表明:氢原子的吸附位置与覆盖度之间有强烈的依赖关系,覆盖度低于0.67ML时,氢原子能量上易于占据fcc或hcp的中空位置;覆盖度为0.78ML时,中空位与桥位为氢原子的最佳吸附位;覆盖度在0.89到1.00ML时,桥位是氢原子吸附能量最有利的位置;以上覆盖度中Be(0001)表面最外层铍原子的结构均没有发生明显变化.当覆盖度为1.11-1.33ML,高覆盖度下Be(0001)表面的最外层铍原子部分发生膨胀,近邻氢原子渗入到铍表面次层,氢原子易于占据在hcp和桥位.吸附结构中的氢原子比氢分子中的原子稳定.当覆盖度大1.33ML时,计算结果没有发现相对于氢分子更稳定的吸氢结构.同时从分析偶极修正和氢原子吸附垂直高度随覆盖度的变化关系判断氢覆盖度为1.33ML时,在Be(0001)表面吸附达到饱和.     

甲醇在Ru(0001)表面吸附的密度泛函研究

采用密度泛函理论(DFT)的B3LYP方法,以原子簇Ru15为模拟表面,对甲醇在理想的Ru(0001)面三种吸附位置(top,fcc,hcp)的吸附模型进行了几何构型优化,能量计算,Mu lliken布局分析以及振动频率计算,结果表明顶位为最有利的吸附位.这些变化与实验观察到的甲醇在过渡金属表面解离的结果相一致.同时通过对吸附过程的分析推测其可能的解离途径.     

Structure of Oxygen and CO Adsorption on Ru(0001) Electrode

It is important to understand the chemisorption of oxygen and CO on Ru(0001) surface. CO oxidation at oxygen precovered Ru(0001) surface at low oxygen coverages gave an extremely low CO oxidation rate, and it was also observed that, with a nominal oxygen coverage exceeding ca. 3 mL, rather high CO/CO2 conversion probabilities were achieved1. In the case of coadsorption of CO and oxygen on Ru(0001) surface under UHV conditions, a model comprising two CO molecules in an (22)-O unit cel…     

氢原子在Ru(0001)和Ru(1010)面上吸附扩散势能面的结构

本文构造了H-Ru相互作用的五参数Morse势,用经典的对势方法研究了氢原子在Ru(0001)和Ru(1010)面上的吸附和扩散,得到了氢原子在两个表面上的吸附位、吸附几何、结合能及本征振动等数据与实验结果符合得很好;同时研究了两个体系的吸附扩散势能面结构。     

钡原子对Ru（0001）表面氮分子吸附和解离过程的影响

采用密度泛函理论方法研究了钡原子对Ru（0001）表面氮分子解离过程的影响.计算结果表明：在Ru（0001）表面,钡原子失去电子后形成Ba（1＋δ）＋阳离子.表面转移电荷增强了衬底钌原子d轨道和氮分子π轨道间的杂化作用以及氮分子内的库仑排斥作用,减弱了氮分子键.在钡原子的作用下,γ态氮分子键键长从0.113 nm增加到...     

CO在Cs/Ru(1010)表面上吸附的ARUPS研究

CO adsorption on Ru(100) and Cs/Ru(10O) surfaces has been investigated using ARUPS, at low temperature 150K. The 5σ+1π and 4σ levels of CO molecule were　found in angle-rcsolved UP spectra showing that CO is in molecular adsorption states on clean and Cs precovercd Ru(1010). The dependence of CO 4σ intensity on incident angle suggests that adsorbed CO stands upright on clean Ru(1010) surface; But adsorbed CO, with a short-range interaction with Cs atom [15], does not stand upright and tilts in <1210> azimuth on a Cs-precovered Ru(1010) surface.     

氢原子与Fe(111)表面相互作用的理论研究

氢自由基在Fe表面的吸附是典型的表面吸附反应.本文首先对α-Fe体相开展研究,再对Fe(111)的周期性平板模型进行了参数测试,确定了7层模型可以有效表示Fe(111)表面.研究了氢原子在Fe的刚性表面和柔性表面上的吸附情况,发现弛豫效应主要集中在上3层表面,而底层4层原子几乎未发生驰豫.发现氢原子在Fe(111)表面...     

用同步辐射光研究CO在Cs/Ru(100)表面的吸附

(CO+Cs)/Ru(1010)共吸附的体系中,CO分子由于受CS原子强烈影响,分子轨道发生重新杂化组合.CO分子原来在清洁Ru(1010)表面上结合能位于7.5eV处相重叠的5σ和1π轨道对应谱峰分裂为两峰,结合能分别位于6.3和7.8eV处.其中6.3eV处的谱峰来自CO分子1π轨道的一支,它显示出该分子轨道沿衬底<0001>晶向的镜面反对称性.CO分子1π轨道的另一支和5σ轨道在结合能7.8eV处相重叠.     

水在石墨(0001)面簇模型桥位上吸附的量子化学研究

用从头计算方法对水在石墨(0001)面桥位上的吸附进行了研究.用C₆H₈原子簇模拟石墨表面,在6-31G^*水平上计算了水在不同方向和位置上的吸附能量.研究表明:水在石墨面上的吸附很弱,属于物理吸附;在中性或带负电荷的石墨表面,当水分子中的氢原子靠近石墨面时,体系存在能量最小值,而在带正电荷的表面,当氧原子靠近石墨面时存在稳定的吸附点;不论表面带正电荷还是带负电荷,均对水分子的吸附起增强作用.     

Adsorption of bisulfate on the Ru(0001) single crystal electrode surface

Adsorption of anions from sulfuric acid solutions has been studied on Ru(0001) single crystal and polycrystalline surfaces by electrochemical techniques and in-situ Fourier transform infrared spectroscopy. Infrared spectroscopy shows that bisulfate is the anion adsorbed on the Ru(0001) surface. The bisulfate adsorption is detected at the H₂ evolution potential and extends into the potential region where the Ru surface is oxidized. A method for extracting unipolar bands from bipolar bands has been presented. The tuning rate of adsorbed bisulfate in the double layer potential region of Ru(0001) was found to be significantly smaller than those observed for other platinum metals. This has been ascribed to a small change in bisulfate coverage on Ru(0001) in this potential range. Bisulfate vibration frequencies are higher on this surface than at any face-centered cubic metal with the (111) orientation. Oxidation of the Ru(0001) surface is limited to one electron per Ru atom, distinctly different from the high degree of oxidation seen in polycrystalline surfaces. For oxidized polycrystalline Ru, only solution phase sulfates and bisulfates are observed in the IR spectra.     

Electrooxidation of CO on Ru（0001） and RuO2（ 100） Electrode Surfaces

The electrooxidation of CO on Ru(0001) and RuO2(100) electrode surfaces were characterized by cyclic voltammetry,AES and RHEED,The CO adlayer was first partially oxidized at 0.8 V, which is controlled by the attack of oxygen species toward the Ru(0001) surface. The remaining CO aldayer oxidation at 0.55 V is related to the combination of CO molecules with oxygen species already located on the surface,In contrast,successive peaks on RuO2(100) at 0.4 V and 0.72 V are observed ,which shows that CO molecules can directly react with two different lattice-oxygen on the surface to carbon dioxide.     

Supported Ru catalysts: a study of the influence of supports, promoters and preparative variables on the catalytic activity and selectivity

The influence of some preparative variables, of the metal loading and of the support on the activity of Ru catalysts for the selective hydrogenation of benzene to cyclohexene has been studied. The reaction has been carried out in a tetraphase reactor (in the presence of an aqueous solution of ZnSO₄) at 423 K and 5 MPa pressure. The effect of hydrogen diffusion on the reaction kinetics and on cyclohexene selectivity was studied. The hydrophilicity of the support was related to the observed selectivity. Hydrogen chemisorption indicates that the catalyst activity is not influenced by the Ru dispersion, but mainly by the weakly chemisorbed species on the catalyst surface. This revised version was published online in August 2006 with corrections to the Cover Date.     

氧化铈负载钌催化剂中钌表面密度对氨合成活性和氢中毒的影响

氨是关系国计民生的大宗化学品,也是氢能源的重要载体.目前,世界合成氨工业每年消耗约2％的世界总能源,并排放超过1％的CO2,节能降耗需求十分迫切,其中的关键在于高性能氨合成催化剂的开发.传统观点认为,B5活性位是钌催化剂上氮解离和氨合成的活性位,当钌粒子尺寸在1.8～2.5 nm时催化剂的B5活性位数量最多,而钌尺寸较小(0.7～0.8 nm)的催化剂几乎没有氨合成活性.本文通过改变钌负载量调变了氧化铈负载钌催化剂的钌表面浓度,证实钌粒子尺寸低于2.0nm时,氧化铈负载钌催化剂也具有较高的氨合成活性.XPS等表征结果证实:钌表面密度低于0.68 Ru nm-2时,钌主要以层状形式存在于氧化铈表面,层状钌与氧化铈紧密接触,电子从氧化铈的缺陷位传递给钌物种,在这种情况下,Ru 3d5/2的结合能有所下降,氮解离能力增强,这有利于提高催化剂的氨合成活性;当钌表面密度约为0.68 Ru nm-2时,钌金属传递电子给氧化铈,此时Ru 3d5/2结合能有所增加;当钌表面密度高于1.4 Ru nm-2后,钌物种优先在层状钌表面聚集成大尺寸钌纳米粒子,此时催化剂中同时存在钌团簇和钌纳米粒子,氧化铈载体对钌粒子电子性质的影响减弱,因此大尺寸钌金属颗粒Ru 3d5/2结合能又有所下降.另一方面,氢分子会在氧化铈表面形成均裂产物(两个OH基团)或异裂产物(Ce-H和OH).同时氢分子还会在0价钌金属表面解离形成氢原子,并进一步溢流到氧化铈表面与氧原子作用形成羟基.钌活性位上的氢物种比氧化铈中的氢更容易脱附,因此氧化铈中钌的存在不仅可以增强其氢吸附量,还降低了氢物种的吸附强度.当钌表面密度低时,氧化铈与钌的相互作用较强,催化剂中的氢物种容易溢流到氧化铈中形成羟基基团,此时催化剂的氢吸附能力增强,氢中毒问题较显著.当钌表面密度较高时,氢原子在大尺寸钌颗粒上移动、反应和脱附,因此催化剂的氢中毒问题也得到显著缓解.总之,对于氧化铈负载钌催化剂,氧化铈与钌金属之间的电子相互作用以及其吸附性质都会影响催化剂的氨合成活性,因此钌表面密度低于0.31 Ru nm-2以及约为2.1 Ru nm-2时,催化剂都展现出了较高的氨合成活性.本文将为设计制备高性能钌基氨合成催化剂提供理论指导.