H2O分子在Fe（100）, Fe（110）, Fe（111）表面吸附的第一性原理研究

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     

通过不同烷基链取代调控喹吖啶酮分子在Ag(110)表面上的自组织结构

采用低能电子衍射、扫描隧道显微镜、第一性原理密度泛函理论计算以及分子力学计算，分别对不同烷基链取代的喹吖啶酮（QA）分子在Ag（110）基底上的吸附和生长进行了研究．QA和Ag基底的相互作用主要来自分子中0原子和Ag基底的共价键，它决定了分子的取向和最优吸附位置；而烷基链决定了分子吸附层的取向，QA分子间的排列可以通过烷基链的长度来调节．由此借助调节烷基链的长度，能够可控地制备具有不同物理性质的单层分子薄膜．     

氢在Ni(511)台阶面的吸附与解离研究

应用EAM模型研究了氢在Ni(511)面的吸附和解离.首先计算了单个氢原子在Ni(511)面上的吸附能、吸附键长及吸附高度,发现氢在Ni(511)面上有三种相对稳定的吸附位,即台阶棱上的二重桥位B、台阶面上的三重洞位H3′以及平台面上的四重洞位H1和H2.与Ni(001)低指数面相比,明显的增加了台阶棱上的二重桥位B以及台阶面上的三重洞位H3′,并且H1位的吸附性也有所增强,说明台阶的存在影响了氢在Ni(511)表面的吸附性,使台阶附近的吸附位增多且吸附性增强;然后计算了氢分子在台阶表面上解离吸附时的活化势垒、吸附能、氢镍之间键长及氢氢之间的距离,计算结果表明台阶底部更易于使氢分子解离,台阶附近是氢吸附和解离的活性部位.     

H2O分子在Fe(100), Fe(110), Fe(111)表面吸附的第一性原理研究

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,而这与晶面原子的排列密度相关.吸附体系的电子结构计算结果也得出了相似的结论.同时电荷布居分析表明,H2O分子与Fe表面相互作用时,O原子与基底原子之间的电荷交换使基底Fe原子表面带负电,导致表面电位降低,也促使Fe表面更易于发生电化学腐蚀反应.     

咖啡酸分子表面增强拉曼光谱的理论与实验研究

咖啡酸（CA）是一种具有很高的医学价值的药物成分,在抗菌抗病毒方面应用广泛,尤其是咖啡酸及其衍生物在抗肿瘤方面有着巨大作用,现在对咖啡酸的相关研究越来越多,但大部分都是关于咖啡酸医学性质的研究,所以对咖啡酸分子的微观结构研究是非常有必要的。目前关于CA在Ag表面上的表面增强拉曼散射（SERS）光谱的理论与实验结合的研究尚未见报道,而对其振动光谱及表面增强机理的研究可以为咖啡酸的各种药学机理的研究提供一种科学的物理解释,所以有必要将密度泛函理论（DFT）方法与表面增强拉曼散射技术相结合,对咖啡酸在Ag纳米颗粒上的吸附性质及表面增强机理进行全面的研究,这对推进它们在医药学等领域的相关研究有着重要的参考价值。采用SERS与DFT技术对CA分子在Ag纳米颗粒表面上的表面增强拉曼光谱进行了研究。在实验方面,利用热还原反应原理,使用柠檬酸三钠和硝酸银在加热搅拌情况下制备Ag纳米颗粒,并使用激光共聚焦显微拉曼光谱仪测量了CA分子的常规拉曼散射（NRS）光谱及其表面增强拉曼散射（SERS）光谱。在理论计算方面,采用DFT的B3LYP方法,以6-31+G**和LANL2DZ分别作为C,H,O和Ag的计算基组来优化咖啡酸的分子构型,羟基与Ag₄的吸附构型,羧基与Ag₄的吸附构型,羟基与羧基共同与Ag₄吸附的构型,并以此为基础分析计算了CA分子的NRS光谱以及三种可能吸附模型的SERS光谱,并结合实验结果进行比较。同时对CA分子的振动模式进行了详细指认。根据实验数据和理论结果分析,在452 cm-1处的谱峰归属为环面外弯曲振动和O-H面外弯曲振动的耦合,这说明CA分子上的酚羟基是与Ag纳米颗粒表面作用的,不过相互作用较弱,推测CA分子平面可能与Ag基底表面不垂直;出现在1 338 cm-1处的谱峰归属于COO-伸缩振动,则可以说明CA分子上的羧基可能与Ag纳米颗粒垂直吸附。结果表明,CA分子是以羧基和酚羟基为吸附位吸附在Ag纳米颗粒表面上的。同时对CA分子的振动模式进行了详细指认。该工作对推进咖啡酸在生物医药等领域进一步的应用将起到重要作用。     

氢原子在Pd（n（100）×（111））—（011）台阶面上的吸附和扩散

采用氢－钯表面的５参数Ｍｏｒｓｅ势，用对势方法研究了氢原子在Ｐｄ（ｎ（１００）×（１１１））－（０１１）台阶面上的吸附和扩散，获得了氢原子在该台阶面上的吸附位，吸附几何，结合能和本征振能，并给出氢原子在台阶下四重位的吸附优先于台阶面上的三重位吸附，计算结果与实验结果符合很好，理论分析给出台阶对氢原子表面扩散的影响。     

用分子模拟方法研究羟基乙叉二膦酸(HEDP)在方解石表面的吸附行为

建立了基于分子力学计算方法的分子模拟手段,用于研究羟基乙叉二膦酸(HEDP)在方解石{104}表面的吸附特性.分子模拟三维吸附图像显示,HEDP中的膦酸基团中的氧原子具有强烈的负电性,能与晶体表面的阳离子产生强烈的静电吸引作用,形成“立体匹配”吸附结构.计算结果显示,HEDP在方解石面上、台阶和扭折点位置的平均吸附能依次约为-5.2eV,-7.0eV和-23.5eV,表明HEDP强烈地吸附到扭折点位置上,从而影响和抑制台阶的生长. 关键词： 分子模拟 方解石 阻垢剂 表面吸附     

有机分子PTCDA在P型Si单晶(100)晶面的生长机理

对PTCDA的分子结构及其化学键的形成进行了分析,并讨论了晶面指数（100）Si单晶的晶格结构。在此基础上,评述了PTCDA分子在P-Si单晶（100）晶面上生长的机理,并制备了样品PTCDA/P-Si（100）。利用XRD对样品测试得出,在P-Si（100）晶面上沉积的PTCDA薄膜中仅存在α物相。利用XPS对样品测试得出,在其界面层中PTCDA酸酐中的4个羟基O原子与C原子结合,其结合能为532.4 eV;苝核基团外围的8个C、H原子以共价键结合,其结合能为289.0 eV;在界面处,悬挂键上的Si原子与PTCDA酸酐中的C、O原子结合,形成C-Si-O键及C-Si键,构成了界面层的稳定结构。     

PTCDA分子基态的飞秒激光控制研究

将优化控制理论和多组态含时Hartree（MCTDH）方法相结合,建立了适合于MCTDH方法的计算具有平面结构的PTCDA分子的多自由度振动量子模型,研究了在PTCDA分子激发后从分子激发态回落至分子基态的动力学过程.在理论上分析了约化目标态产生率与激发脉冲、分子的演变时间及优化场的有效能量之间的关系,对分子在各个振动坐标下波函数的振动分布做了分析与比较.研究发现,增加分子的回落演变时间在提高目标态产生率的同时可以使优化激光控制场的强度降低,这为实验上用低能量激光最大程度地实现目标态提供了有效手段. 关键词： PTCDA 多组态含时Hartree方法 飞秒激光控制     

小分子在Pd(100)面上的共吸附

本文应用紧束缚模型和单电子理论研究了几种小分子在Pd(100)面上的共吸附特性,结果表明:在Pd(100)面上两个吸附分子(或吸附原子)间的间接相互作用随吸附质与衬底之间的耦合强度的减小呈现振荡性衰减的趋势,并且,当O₂或H₂存在时,NO在Pd(100)面上的解离将受到影响,此外,根据两吸附质之间的间接相互作用,推断出一些吸附层结构,这些结果与实验结果作了比较。 关键词：     

Selective nontemplated adsorption of organic molecules on nanofacets and the role of bonding patterns

A key element of functionalizing nanocrystals with organic molecules is the nontemplated selective adsorption of different molecules on different facets. Here we report scanning-tunneling-microscopy images of perylene-3,4,9,10-tetracarboxylic-dianhydride and 2,5-dimethyl-N,N'-dicyanoquinonediimine on silver, demonstrating selective adsorption on different facets. We also report first-principles calculations that account for the data and show that bonding, which controls selectivity, occurs via the end atoms, while the molecule's midregion arches away from the substrate. The results are also consistent with data that have been interpreted in terms of bonding via the midregion.     

低维原子/分子晶体材料的可控生长、物性调控和原理性应用

本文介绍了高鸿钧课题组在物理所20年来的部分代表性工作.研究的主要方向为低维纳米功能材料的分子束外延可控制备、生长机制、物性调控及其在未来信息技术中的原理性应用.从材料的可控制备入手,结合第一性原理的理论计算,阐明材料生长机制和结构与物性的关系,进而实现物性调控和原理性应用.主要内容有:1)纳米尺度"海马"分形结构的形成及其生长机制;2)STM分辨率的提高及最高分辨Si(111)-7×7原子图像的获得;3)固体表面上功能分子的吸附、组装及其机制;4)稳定、重复、可逆的纳米尺度电导转变与超高密度信息存储;5)固体表面上单分子自旋态的量子调控及其原理性应用;6)原子尺度上朗德g因子的空间分辨及其空间分布不均匀性的发现;7)晶圆尺寸、高质量、单晶石墨烯的制备及原位硅插层绝缘化;8)几种新型二维原子晶体材料的可控构筑及其物性调控;9)"自然图案化"的新型二维原子晶体材料及其功能化.这些工作为低维量子结构的构造、物性调控及其原理性应用奠定了基础.     

Facet‐Dependent Effect of Well‐Defined CeO2 Nanocrystals on the Adsorption and Dephosphorylation of Phosphorylated Molecules

CeO₂ nanocrystals (CN) with different morphologies (i.e., cube, octahedron, and rod) are prepared and the facet‐dependent effect of these CeO₂ nanocrystals on the adsorption and dephosphorylation of phosphorylated molecules is investigated for the first time using the model p‐nitrophenyl disodium orthophorphate (p‐NPP). Due to their different surface atomic configurations, the {111} and {110} facets have much higher adsorption capacity and kinetic catalytic activities than {100} facets. All the CeO₂ nanocrystals can intensely promote the dephosphorylation reaction owing to the strong interaction between Ce cations and phosphoryl oxygens resulting in the cleavage of phosphoester bonds. As was expected, the above facet‐dependent effect can be verified by the practical application results of the CeO₂ nanocrystals on the capture and dephosphorylation of phosphopeptides. Thus, surface engineering could be a useful and feasible strategy for not only fundamentally understanding the interaction between crystal facets and molecules but also effectively developing high‐performance functional materials.     

Surface electronic structure of polar NiO(111) films

The surface and electronic structure of polar NiO(111) films with or without facets, prepared on a Mo(110) substrate, were in situ studied using various surface analytical techniques. A new surface state located at 0.8–1.8 eV measured by electron energy loss spectroscopy was observed on faceted NiO(111) films, which is originated from surface Ni vacancies. This surface state is decreased by annealing or deposition of Ni atoms. The experimental results indicate that the charge transfer occurs between surface and bulk of the faceted NiO(111) films. Present work provides a model surface with polarity and facets, which can be used for further investigation on chemical adsorption of atoms or molecules as well as selective reaction.     

Theoretical study of hydrogen adsorption in Ti-decorated capped carbon nanotube

We present ab initio study using dispersion-corrected density functional theory calculations to investigate the hydrogen interaction with Ti-coated, one end closed, single-walled carbon nanotube (SWCNT). Our results demonstrate that a single Ti atom binds up to five hydrogen molecules on SWCNT cap top, whereas adsorption of four hydrogen molecules is energetically more favourable. The analyses from adsorption energy profile, highest occupied molecular orbital–lowest unoccupied molecular orbital gap and Mulliken charge distribution show contrast in first hydrogen molecule adsorption compared with the rest of four configurations. This is clearly due to the strongly different bonding nature of first hydrogen adsorption among others, between hydrogen molecules and Ti-coated SWCNT. These results not only support our understanding of adsorption nature of hydrogen in Ti-coated SWCNTs but also suggest new directions for smart storage techniques.     

Grand canonical Monte Carlo simulations of hydrogen adsorption in carbon cones

The Monte Carlo method in its grand ensemble variant (GCMC) is used in order to study the hydrogen adsorption (77 K) characteristics of novel carbon structures, namely Carbon Cones (CCs). CCs are conical shaped curved graphitic sheets, with five different apex angles. CC structures with correct bonding topology were developed via atomistic-molecular simulations, while GCMC simulations of hydrogen adsorption were carried out on the five different apex angle structures. Emphasis has been given on the adsorption properties inside the cones and it was found that cone tips are characterized by enhanced adsorbability. The results were also compared with similar calculations on carbon nanotubes.     

电场作用下S修饰C24N24从CO2/N2混合气体中选择性吸附

在燃烧后气体中选择性捕获CO2,对减缓因CO2浓度过高引发的环境问题具有十分重要的意义。本文采用第一性原理计算的方法,研究了外加电场作用下S修饰C24N24富勒烯对CO2的选择性吸附性能。首先研究了S@C24N24的结构和性质,发现其具有良好的稳定性。其次,研究了无电场时S修饰C24N24富勒烯对CO2的吸附行为,发现其吸附为弱的物理吸附。另外,进一步研究了外加电场作用下S@C24N24对CO2的吸附行为。结果表明,结合距离（CO2与S）和CO2的键角（O=C=O）随电场的增大而减小;当电场增加到0.018 au时,物理吸附转变为化学吸附。关闭电场时,化学吸附又转化为物理吸附。此外,即使在相同的电场条件下,S修饰C24N24富勒烯对N2的吸附也为弱的物理吸附。这表明,通过控制外加电场的开/关,S@C24N24可以从CO2/N2混合气体中选择性捕获/释放CO2,可作为选择性捕获CO2的优良候选材料。     

电场作用下P掺杂硅烯选择性吸附CH_4的第一性原理计算

在煤层气中选择性吸附和捕捉甲烷分子,对提高煤矿安全具有十分重要的意义.本文采用第一性原理计算的方法,研究了外加电场作用下P掺杂硅烯对甲烷分子的选择性吸附性能.结果表明:正电场作用下,P掺杂硅烯与甲烷分子之间产生较强的化学吸附,能够快速捕获甲烷分子.当关闭外加电场时,P掺杂硅烯与甲烷分子之间则为微弱的物理吸附,甲烷分子很容易实现脱附.同时还发现,外加电场作用下,P掺杂硅烯与氮气、氧气及水之间的吸附均属于物理吸附,表明P掺杂硅烯可以在这些混合气体中实现甲烷气体的选择性吸附. P掺杂硅烯有望成为选择性好的甲烷传感、捕获新材料.     

Combined investigation of water sorption on TiO2 rutile (1 1 0) single crystal face: XPS vs. periodic DFT

XPS and periodic DFT calculations have been used to investigate water sorption on the TiO₂ rutile (1 1 0) face. Two sets of XPS spectra were collected on the TiO₂ (1 1 0) single crystal clean and previously exposed to water: the first set with photoelectrons collected in a direction parallel to the normal to the surface; and the second set with the sample tilted by 70°, respectively. This tilting procedure promotes the signals from surface species and reveals that the first hydration layer is strongly coordinated to the surface and also that, despite the fact that the spectra were recorded under ultra-high vacuum, water molecules subsist in upper hydration layers. In addition, periodic DFT calculations were performed to investigate the water adsorption process to determine if molecular and/or dissociative adsorption takes place. The first step of the theoretical part was the optimisation of a dry surface model and then the investigation of water adsorption. The calculated molecular water adsorption energies are consistent with previously published experimental data and it appears that even though it is slightly less stable, the dissociative water sorption can also take place. This assumption was considered, in a second step, on a larger surface model where molecular and dissociated water molecules were adsorbed together with different ratio. It was found that, due to hydrogen bonding stabilisation, molecular and dissociated water molecules can coexist on the surface if the ratio of dissociated water molecules is less than ≈33%. These results are consistent with previous experimental works giving a 10-25% range.     

Substrate-interaction,long-range order,and epitaxy of large organic adsorbates

Large and symmetric organic molecules (>200 amu) can form highly-ordered adsorbate layers and thin films when they are deposited by vacuum sublimation on clean reactive surfaces. In such cases covalent bonding often occurs via the molecular -system leading to a parallel orientation of the adsorbate as shown for oligothiophenes and PTCDA on Ag(1 1 1). A proper choice of the substrate and/or a preadsorbate may also cause an upright orientation with bonding via a reactive group of the molecule (example: NDCA/Ni(1 11)). Most of the used molecules yield long-range ordered monolayers with large, almost defect-free domains. The stronger the bonding and the smaller the molecule the more likely is the formation of commensurate superstructures which indicate site-specific adsorption even for such large molecules as PTCDA or EC4T. Organic epitaxy is discussed and shown for a particular system, PTCDA on Ag(1 1 1), for which the structure of the monolayer is nearly identical to that of the-modification of PTCDA crystals, whereas on other substrates (e.g. Si(1 1 1), Ge(1 0 0)) a disordered interface and hence no true epitaxy is found.