C60分子间相互作用的Morse势函数及应用

利用C60晶体的升华焓、晶胞参数等性质,得到C60分子间相互作用的Morse势函数，其解析表达式为 u(r)=30.05 exp[－24.96(r－1.005)]－60.10 exp[－12.48(r－1.005)] 采用该作用势研究了C60及其晶体的一些性质, 如计算得到C60晶体(100)面的表面能为7.46×10－2 J•m－2, 在650～4500 K温度范围内计算了C60分子的第二维里系数, 研究了C60面心立方晶体的晶格振动, 并计算得到了晶格振动的态密度分布,还利用该作用势研究了不同晶型时C60晶体的稳定性.     

簇合物Co6(μ3-E)8(CO)6(E:-S,-Se)的电子结构及相关性能探讨

标题簇合物分子中所含的Co6为八面体结构，这一主干结构从化学上开始合成以来，已历经十余年[1]．由于硫族元素的钻原子簇合物具有如下两方面的作用：它与一些多相钻一硫催化剂的表面结构相当类似，因而可作为其研究模型．另外该簇合物分子可以进行可逆的氧化还原反应且不改变本身结构，依此特性又可作为电子库材料和生物酶电子传递研究的模拟物．所以人们对它的研究兴趣渐趋强烈．大量这些簇合物的合成、结构测定等见诸报道[1－3]．主要的分子类型为Co6（μ3－E）8（PR3）6（E：－S，－Se；R：－Et，－Ph．）．对于它们的研究，详细了…     

用可解的六次势研究9-羟基苯嵌萘酮的基态能级劈裂

质子转移（PT）得到了理论和实验方面广泛的研究［1-10],9－羟基苯嵌萘酮（9－HPO）是一个典型体系．在荧光光谱中,观测到氖化的9－HPO的基态能级劈裂,结合其它光谱和X射线衍射数据,提出用四次函数V（R）=A（R4-BR2）作为势能函数［1]．迄今,这一势能函数对应的Schr dinger方程还不能精确求解,且得到的结果与实验值[4]有较大差异．本文用可解的六次势V（R,γ）＝C[R6＋2γR4+(γ2＋μ）R2] 来描述该体系质子转移时的势能面,得到这一势能对应的Schr dinger方程的解析解,再用变分法并结合得到的解析解可计算9－HPO的基态能级劈裂．     

甲基化的β-环糊精与十六烷基三甲基溴化胺的相互作用

环糊精与表面活性剂的相互作用已有许多研究,但多局限于β－环糊精（β－CD）,而修饰的β－环糊精与表面活性剂的相互作用研究较少[1－3]．分子内扭转电荷转移（TICT）激发态对介质极性高度敏感性,已成功地用于探针环糊精与表面活性剂的相互作用[4]．研究表明,β－CD能够诱     

混合价配合物的振动偶合模型及进展

本文讨论了混合价二聚配合物的振动偶合模型，并应用Ｃｒｅｕｔｚ－Ｔａｕｂｅ（Ｃ－Ｔ）离子－（μ－吡嗪）二（五氨合钌）（５＋），计算其势能函数，混合价跃迁带的形状及ＥＰＲｇ值等性质，还指出了混合价三聚物，四聚物的振动偶合模型的新进展。     

预测[Si, C, S]＋和[Si, C, S]－体系的稳定异构体

采用DFT, QCISD及CCSD(T)方法分别对二重态的[Si, C, S]＋和[Si, C, S]－体系势能面进行理论计算, 用QCISD/6-311＋G(d)方法, 在[Si, C, S]＋和[Si, C, S]－体系中, 我们分别得到了2个过渡态连接的3个稳定体和2个过渡态连接的4个稳定体, 经热力学及动力学分析发现, [Si, C, S]＋体系只有二重态线性的离子[Si—C—S]＋可能稳定存在, 而[Si, C, S]－体系有二重态线性的离子[Si—C—S]－和三元环c-[SiCS]－可能稳定存在.     

PdH_2和YH_2分子热力学稳定性的理论研究

由于纯钯的渗氢速率较低,关于钯合金渗氢材料[1-3]的研究引起广泛关注,如钯钇合金.已有研究报道[3,4]PdH2和YH2分子可能的电子结构、势能函数与光谱性质,并提供了可靠的研究方法.     

钒离子与乙烷反应的理论研究

用量子化学方法在UB3LYP／6－311＋＋G（3df,3pd)水平上研究了一阶钒离子与乙烷的反应，找到了[VC2H6]^ 势能面上各驻点的结构，分析了反应过程中有关的电子转移性质，给出了CH4和H2的还原消队理。结果表明：CH4消除反应一般按加成－消除机理进行，在高能条件下也可按协同机理进行；H2分子消除反应，一般按1，2－H2分子消除机理进行，在高能条件下也可按1，1－H2分子消除机理进行。计算表明：能量最有利的反应通道是V^ C2H6→V(C2H4)^ H2，该反应放热11.82kJ/mol。     

紫外辐射诱导C60聚合的扫描隧道显微研究

C60的聚合反应是近年来C60研究的热点．Yeretzian等[1]首先在质谱中观察到了C60在激光作用下的聚合反应，我们也曾以激光真空溅射技术制备了丰富的C60与C70的聚合物[2]．进一步研究还发现，C60在紫外光照射下也能聚合成膜[3]．为更深入地了解C60的聚合过程，本文以扫描隧道显微（STM）技术跟踪观察了C60在紫外光辐射下所发生的形态变化．1实验部分C60吸附在Au（111）面上时能够铺展成单分子层[4]．因此，我们选择Au（111）面作基底，将C60配成一定浓度的甲苯溶液滴在金表面上，待甲苯挥发后制得C60的单分子层．实验所用的紫外光源为…     

二乙炔桥连苯并菲盘状液晶二聚体的合成及其介晶性

通过桥链将2个盘状介晶基元相连,不仅可以稳定盘状液晶柱状相,还有利于玻璃态柱状相的形成,提高盘状液晶作为有机半导体材料的实用性．为此,通过铜盐催化的Eglinton偶联反应合成了8个二乙炔桥连的苯并菲盘状液晶二聚体化合物[C18H6（OCnH2n＋1）4（OMe）O2C—C8H16-C--C-]2,3（n）,（n=4-8）,[C18H6（OC6H13）5O2C—C8H16-C-C-]2,（6）和[C18H6（oc6H13）5O-（CH2）m-C-=C-]2,8（m）,（m=1,3）．差示扫描量热法（DSC）和热台偏光显微镜（POM）对其介晶性进行研究发现：（1）苯并菲周边柔链长度对液晶二聚体化合物的介品性有影响;（2）二聚体化合物3（n）和6具有玻璃态柱状相,并且所有苯并菲二聚体化合物在降温至-50℃均未出现结晶现象;（3）与二聚体3（6）相比,分子对称性较高的化合物6具有较稳定的柱状相,及较宽的介晶温度范围;（4）连接基、中心桥链的长度和刚性对苯并菲盘状液晶二聚体介晶性有重要影响．     

立方面心C60晶体晶格振动的研究

采用C60分子之间相互作用势的Kihra形式,研究了立方面心C60晶体的晶格振动问题,得到了质心振动沿[111]、[110]及[100]方向的声子散射圆频率分布曲线及C60晶格振动频率的态密度分布.采用所得到的C60晶格振动频率的态密度分布,计算了晶体C60在298 K时的等压热容,所得数值与实验值相符.     

Topochemical 3D polymerization of C60 under high pressure at elevated temperatures

Fullerene C60 monomer crystals were compressed to a face-centered cubic (fcc) phase with a lattice parameter of a = 11.93(5) A and a micro-Vickers hardness of 4500 kg/mm2 using high-pressure and high-temperature conditions of 15 GPa at 500-600 degrees C. The hardness is compatible with that of cubic boron nitride (c-BN), suggesting the formation of a 3D C60 polymer. The single-crystal X-ray structural analysis revealed that each C60 molecule in the polymer was linked to the 12 nearest neighbors by [2+2] cycloaddition between the common pentagon-hexagon (56) edges. However, ab initio geometry optimization and molecular dynamics calculations suggested that the 3D polymer should have a rhombohedral structure with the space group of R containing [3+3] cycloaddition between the pentagons of C60 molecules within the plane perpendicular to the 3-fold axis. The higher apparent symmetry of fcc was observed as an averaged structure of different orientations of the rhombohedral structure. The R structure can be derived by only a slight rotation of each C60 unit in the (111) plane of the fcc structure. The band-structure calculation suggested that the 3D polymer (R) was a semiconductor; the activation energy for the electrical conductivity was experimentally determined to be 0.25 eV at 550 K.     

Dependence of molecular recognition of fullerene derivative on the adlayer structure of zinc octaethylporphyrin formed on Au(100) surface

Adlayers of ZnOEP were prepared on reconstructed Au(100)-(hex) and unreconstructed Au(100)-(1 x 1) surfaces by immersing into a benzene solution containing ZnOEP molecules, and the adlayer structures were characterized by scanning tunneling microscopy (STM). A hexagonally arranged ZnOEP array was formed on an Au(100)-(hex) surface, whereas a rectangularly arranged ZnOEP array was found on an Au(100)-(1 x 1) surface. The adlayer structure of ZnOEP was dependent upon the underlying Au atomic arrangements. Furthermore, an investigation of the spuramolecular assembly for these modified surfaces was carried out by using an open-cage C(60) derivative (opened C(60)). A supramolecular assembled adlayer with a 1:1 composition of opened C(60)/ZnOEP was formed on Au(100)-(hex), whereas aggregates of opened C(60) were found on the ZnOEP-modified Au(100)-(1 x 1) surface. Electrochemical responses of opened C(60) were significantly influenced by underlying ZnOEP arrays. This finding suggests that precise control of underlying ZnOEP adlayers with the Au atomic structure is important to recognize the opened C(60) on them.     

Chemical imaging of terrace-based active sites on gold

Scanning tunneling microscopy data of a mixed monolayer comprised of a 40:60 ratio of H8Si8O12 and C6H13-H7Si8O12 clusters on gold are presented. The images display a composite monolayer surface with well-defined domain regions of the individual components. Holes present at face-centered cubic (fcc) sites of the starting Au/H7Si8O12 adsorbate layer indicate the location of active sites for impinging C6H13-H7Si8O12 clusters. Adsorption of a C6H13-H7Si8O12 cluster likely yields a mobile hydrogen atom available to recombine with and desorb an adjacent H8Si8O12 cluster. Hydrogen atom diffusion along substrate [121] directions is the proposed pattern formation mechanism of the mixed monolayer. Imaging of the spherosiloxane cluster domains identifies a novel terrace-based active site located in the fcc regions of the Au(111) 23 x square root3 surface reconstruction.     

Synthesis and characterization of fullerene nanowhiskers by liquid-liquid interfacial precipitation: influence of C60 solubility

Fullerene nanowhiskers (FNWs) composed of C(60) fullerene molecules were prepared using the liquid-liquid interfacial precipitation (LLIP) method in the carbon-disulfide (CS(2)) and isopropyl alcohol (IPA) system. The electron microscopic images reveal the formation of non-tubular FNWs. The X-ray diffraction (XRD) pattern studies indicate the presence of fcc crystalline structure and unusual triclinic structure in the FNWs. The selected area electron diffraction pattern (SAED) analysis demonstrates the existence of triclinic and electron beam assisted fcc to tetragonal crystalline phase transformation. The formation of triclinic structure might be validated due to the partial polymerization of FNWs at C(60) saturated CS(2)-IPA interface. The high solubility of C(60) in CS(2) solvent system results in partial polymerization of FNWs. The polymerization of fullerene molecules in the FNWs has been further confirmed using Raman spectroscopy.     

X-ray emission spectroscopy of (2 square root of 3 x 2 square root of 3)R30 degrees CO/Ru(0001): comparison to c(2x2)CO/Ni(100) and c(2x2)CO/Cu(100)

The atom specific electronic structure of (2 square root of 3 x 2 square root of 3)R30 degrees CO on hcp Ru(0001) has been determined with resonantly excited x-ray emission spectroscopy. We find that the general features of the local adsorbate electronic structure are similar to the situation of CO adsorbed on the fcc metals Ni(100) and Cu(100). The interpretation of the surface chemical bond of (2 square root of 3 x 2 square root of 3)R30 degrees CO/Ru(0001) based on the direct application of the local, allylic model from on-top adsorption on the fcc(100) surfaces Ni(100) and Cu(100) explains many aspects of the surface chemical bond. However, also nonlocal contributions like adsorbate-adsorbate interaction and the deviation from upright on-top adsorption on the Ru(0001) surface influence observables like the heat of adsorption and the Me-CO bond strength.     

豆荚型纳米材料C60@SWNTs的制备和表征

通过气相扩散的方法将C60填入单壁碳纳米管（SWNTs）,制备了豆荚型纳米材料C60@SWNTs,并利用高分辨电子显微镜（HRTEM）和拉曼光谱（Raman spectra）对其进行了表征.结果均证明C60以较高的比例填充入单壁碳纳米管中.HRTEM结果表明,填入单壁碳纳米管的C60之间的距离与面心立方C60晶体中C60之间的距离有细微的差别,说明C60分子与SWNTs间存在弱的范德华相互作用.此外,还观察到在电子束的照射下,C60在SWNT中两两聚合的现象.     

Catalytic effects of subsurface carbon in the chemisorption of hydrogen on a Mg(0001) surface: an ab-initio study

Ab initio density functional theory (DFT) calculations are performed to explore possible catalytic effects on the dissociative chemisorption of hydrogen on a Mg(0001) surface when carbon is incorporated into Mg materials. The computational results imply that a C atom located initially on a Mg(0001) surface can migrate into the subsurface and occupy an fcc interstitial site, with charge transfer to the C atom from neighboring Mg atoms. The effect of subsurface C on the dissociation of H2 on the Mg(0001) surface is found to be relatively marginal: a perfect sublayer of interstitial C is calculated to lower the barrier by 0.16 eV compared with that on a pure Mg(0001) surface. Further calculations reveal, however, that sublayer C may have a significant effect in enhancing the diffusion of atomic hydrogen into the sublayers through fcc channels. This contributes new physical understanding toward rationalizing the experimentally observed improvement in absorption kinetics of H2 when graphite or single walled carbon nanotubes (SWCNT) are introduced into the Mg powder during ball milling.     

Hypothetical C(60) Metal-Cluster Fullerides and General Aspects of Tetrahedral Cluster Bonding

It is geometrically feasible to insert metal-metal-bonded M(4) tetrahedra and M(6) octahedra into the tetrahedral and octahedral holes, respectively, of the fcc C(60) lattice. The electronic structure of the hypothetical tetrahedral variants C(60)(M(4))(2), M = Rh, Co, is analyzed with approximate molecular orbital methods and band structure calculations. These compounds feature M-M and M-C(60) bonding and a variable degree of electron transfer to or from C(60). The C(60)(M(4))(2) phases should be metallic, but we have no way of predicting if they will be superconducting. A number of discrete molecular tetrahedral cluster compounds which serve as models for the solid state materials are analyzed. There is a clear indication that tetranuclear and even mononuclear Rh, Ir, and Co arene complexes should be relatively unstable.     

Evolution of the Pt layer deposited on MgO(001) by pulsed laser deposition as a function of the deposition parameters: a scanning tunneling microscopy and energy dispersive X-ray diffractometry/reflectometry study

A combined ultrahigh vacuum scanning tunneling microscopy (STM-UHV) and energy dispersive X-ray diffractometry/reflectometry (EDXD/EDXR) study of the evolution of face-centered cubic (fcc) Pt layer growth on MgO(100) by pulsed laser deposition as a function of the process parameters such as deposition temperature and deposition duration has been carried out. The aim of this study is to define the best experimental conditions to obtain a controlled film deposition selective on the Pt growth direction (either [111] or [002]). The evolution of the Pt surface morphology as a function of the deposition temperature (T(dep)) from 300 to 700 degrees C has been studied with STM and ED techniques. Results show that the Pt surface, characterized at T(dep) = 300 degrees C by a 3D island morphology, evolves at higher temperatures to a morphology in which the original islands coexist with a distribution of orthogonal 2D stripes. The two features can be associated with the [111] and [002] Pt growth directions of the fcc phase, respectively. For T(dep) = 700 degrees C, the island morphology of the (111) face completely disappears, while the merging process of the (002) stripes reaches completion. The evolution of the morphology at T(dep) = 600 degrees C as a function of the deposition time and thickness has then been studied with STM-UHV, revealing an initial growth of mosaic-like 3D islands. These independent islands, already interconnected, expand along two orthogonal directions and, for longer deposition times, lead to the texture of orthogonal stripes. The EDXR characterization providing the morphological parameters of the films, i.e., thickness and roughness, confirms the above observation and quantifies the effect of such morphological changes on the surface roughness of the Pt film, an important parameter for applications of Pt films as underlayer in magnetic recording media.