H2S、HCN、PH3在FeO（100）表面吸附的密度泛函理论研究

基于密度泛函理论研究了H2S、HCN、PH3 在FeO(100)表面的吸附行为,其吸附位点主要考虑四个：Fe-top(铁顶位)、O-top(氧顶位)、Hollow(空位)、Bridge(桥位)。结果表明H2S吸附在O-top吸附位点的吸附能最小,为-1.02ev,即在该位点的吸附体系最稳定。当HCN吸附在FeO(100)表面时,各吸附位点的稳定顺序为Hollow>Fe-top>Bridge>O-top。PH3 的最稳定的吸附位点与H2S的一致,为O-top吸附位点,其吸附能为-1.11ev。当H2S吸附在O-top吸附位点时,H2S与FeO（100）表面的电荷转移量最多,说明该吸附构型最稳定,而HCN吸附在FeO(100)表面,在Hollow吸附位点的电荷转移量最多,也即该吸附位点属于最稳定吸附位点。PH3与FeO（100）表面之间的电荷转移量最多的吸附位点与H2S的相同。当H2S和PH3吸附在O-top吸附位点时,吸附后的态密度曲线整体向低能级移动,峰值降低,其吸附结构变得更加稳定。而HCN吸附在Hollow位点时,吸附后的HCN态密度曲线向能量更低的区域移动,吸附体系变得更稳定。     

BTA在铜表面吸附的密度泛函理论研究

本文基于密度泛函理论(DFT)的第一性原理研究了苯并三氮唑(BTA)分子吸附于铜表面的反应活性特征及其吸附在三种不同取向晶面时的电荷转移以及成键情况,结果表明：BTA分子的亲电和亲核活性中心为N(1)、N(2)和C(5),在铜表面垂直吸附时为化学吸附,Cu原子的最外层价电子转移到N(2)原子上,两者形成配位键;BTA分子在三种不同取向的铜表面吸附时的吸附能大小为：Cu(110)_x>Cu(100)_x>Cu(111)_x(x=T、B、H),T表示顶位,B表示桥位,H表示空位;BTA吸附在Cu(111)面的转移电荷量：T(顶位)>B(桥位)>H(空位).     

密度泛函理论研究KA油在氧化钨表面上的吸附分离

环己烷氧化生成环己酮和环己醇(产物合称KA油)是重要的工业反应,其产物环己酮可作为化学工业中重要的中间体,广泛的用于生产尼龙-6.然而,环己醇和环己酮沸点接近难以分离,因此开发有效分离KA油的材料受到科学工作者的广泛关注.本文基于密度泛函理论计算,研究KA油在干净和有机物修饰的氧化钨材料上的吸附能和吸附构型;通过差分密度电荷和态密度计算,揭示了主-客体吸附过程中的电荷转移特性;研究结果发现使用硅烷修饰后的氧化钨材料对环己醇吸附性能更好;而使用硅醚修饰后对环己酮有更强的吸附能力.该理论研究工作为实验提供了理论依据,缩短了研发分离KA油新材料的时间,节省了人力和资源等成本.     

密度泛函理论研究碱金属原子在完美氧化镁(001)表面的吸附

基于平面波赝势法的密度泛函理论系统地研究了孤立碱金属原子(锂、钠、钾、铷、铯)在完美氧化镁(001)表面的吸附. 锂在氧位表面上的吸附能是0.72 eV,大约是其它碱金属的3倍. 锂和表面氧之间较强的相互作用主要是来源于共价键的作用,这可由态密度和差分电荷密度的分析所证实. 讨论碱金属在MgO(001)表面吸附的成键机理.     

密度泛函理论研究草甘膦在纯的, 金属原子掺杂石墨烯表面的吸附机理

本研究采用密度泛函理论方法详细讨论了纯的石墨烯及Ti, Fe, Al, Ca原子掺杂石墨烯吸附草甘膦的机理.通过它们之间的吸附能,差分电荷密度,布居电荷,态密度分析发现草甘膦可以被纯的石墨烯及金属原子掺杂石墨烯不同程度地吸附.纯的石墨烯对草甘膦的吸附作用远不及掺杂石墨烯,其中,草甘膦在Ca掺杂石墨烯表面有最强相互作用.这是因为草甘膦与纯的石墨烯之间主要形成了-P=O…π,-COOH…π和-OH…π非共价的相互作用,而与掺杂石墨烯之间主要形成了Metal-O“单齿”和O-Metal-O“双齿”共价相互作用.本研究结果希冀为石墨烯在环境保护方面的应用提供有价值的理论指导.     

甲氧基在Ir(111)表面吸附的密度泛函理论研究

本文采用第一性原理和周期平板模型相结合的方法,对甲氧基在Ir(111)表面top,bridge,fcc和hcp位的吸附模型进行了构型优化、能量计算、Mulliken电荷布居分析以及差分电荷密度计算.结果表明,甲氧基通过氧原子与金属表面相互作用时,垂直吸附在fcc位是最有利的吸附构型,吸附能为2.26eV,此时电子从金属表面向甲氧基转移.吸附过程中C-O键振动频率发生红移,表明在该表面C-O键容易被活化.结合差分电荷密度分析表明,吸附时CH3O中氧的2p原子轨道和铱的dz2原子轨道相互作用形成σ键.     

锑烯吸附金属Li原子的密度泛函研究

锑烯(antimonene)是继石墨烯和磷烯之后出现的新型二维材料,在锂离子电池等领域受到关注.本文基于第一性原理的密度泛函理论,计算研究了锑烯对Li原子的吸附特性,包括Li原子的最稳定吸附构型、吸附密度以及吸附Li原子的扩散路径.结果表明:Li原子最稳定的吸附位置位于谷位,即底层Sb原子之上、顶层三个Sb原子中心位置,吸附能为1.69 eV,吸附距离为2.81?;能带计算发现,锑烯为带隙宽度1.08 eV的间接带隙半导体,吸附Li原子后费米能级上升进入导带,呈现出金属性;原子分波态密度分析发现, Sb原子的p电子态和Li原子的p和s电子态形成明显的共振交叠,表现出杂化成键的特征;随着吸附Li原子数量增加,锑烯晶格结构和电子结构发生较大变化.通过微动弹性带方法计算发现, Li原子在锑烯表面的扩散势垒为0.07 eV,较小的势垒高度有利于快速充放电过程.     

Cu13团簇几何和电子结构的密度泛函研究

利用遗传算法结合Gupta原子间相互作用势,采用密度泛函理论,系统研究了带电 团簇的基态与低激发态的几何结构和电子结构并与中性Cu13团簇进行了对比．计算结果表明：对 Cu13（中性及带电）团簇,高对称性几何构型在众多异构中无能量竞争性优势,团簇基态结构皆为非紧致低对称性结构,对 负电Cu13找到一种新的低对称性最低能结构;带电明显影响团簇结构稳定性,带电Cu13团簇与中性Cu13团簇的结构稳定性序列显著不同;基态 Cu13（中性及带电）团簇的具有磁矩最小化效应,而其高对称性结构则有较大磁矩;计算所得Cu13团簇电离能及电子亲和势与实验结果相符．     

Ba和Sr原子在ZnO(0001)表面吸附的密度泛函理论研究

我们采用密度泛函理论下的平面波赝势方法研究Ba和Sr原子在ZnO(0001)表面的吸附结构和性质,仔细研究了三个吸附位（T4, H3 and Top）。发现Ba和Sr吸附在表面的H3和T4位时,他们之间的结合能相差很小,且这两种金属更易于吸附在表面的T4位,我们把计算的结果与贵金属在ZnO(0001)表面的吸附行为及前人的实验结果进行了比较,理论上发现Ag和Au易于吸附在ZnO(0001)表面的H3位,而实验上观察到即使在很小吸附比的条件下ZnO(0001)表面上也能形成Cu的团簇结构,这主要是由于Cu和ZnO(0001)表面衬底强的相互作用所致。     

Ni(111)表面C原子吸附的密度泛函研究

基于密度泛函理论的第一性原理计算,对过渡金属Ni晶体与Ni (111)表面的结构和电子性质进行了研究, 并探讨了单个C原子在过渡金属Ni (111)表面的吸附以及两个C原子在Ni(111)表面的共吸附. 能带和态密度计算表明, Ni晶体及Ni (111)表面在费米面处均存在显著的电子自旋极化. 通过比较Ni (111)表面各位点的吸附能,发现单个C原子在该表面最稳定的吸附位置为第二层Ni原子上方所在的六角密排洞位, 吸附的第二个C原子与它形成碳二聚物时最稳定吸附位为第三层Ni原子上方所在的面心立方洞位. 电荷分析表明,共吸附时从每个C原子上各有1.566e电荷转移至相邻的Ni原子, 与单个C原子吸附时C与Ni原子间的电荷转移量(1.68e)相当. 计算发现两个C原子共吸附时在六角密排洞位和面心立方洞位的磁矩分别为0.059μ_B和 0.060μ_B,其值略大于单个C原子吸附时所具有的磁矩(0.017μ_B).     

空气-乙炔火焰原子吸收光谱法测定烟草中锌、铜、镉

空气 -乙炔火焰原子吸收法测定烟草样品中的锌、铜、镉 ,探讨了烟草样品的前处理与试液制备。方法快速、简便 ,干扰少 ,测定结果令人满意。     

Density functional theory study of water adsorption on FeOOH surfaces

Using density functional theory (DFT) calculations with an on-site Coulomb repulsion term, we study the composition, stability, and electronic properties of the most common FeOOH surfaces goethite(101), akaganeite(100), and lepidocrocite(010), and their interaction with water. Despite the differences in surface structure, the trends in surface stability of these FeOOH polymorphs exhibit remarkable similarities. We find that the reactivity and the binding configuration of adsorbates depend strongly on the coordination of surface iron: at the fourfold coordinated Fe2 site water is chemisorbed, whereas at the fivefold coordinated Fe1 water is only loosely bound with hydrogen pointing towards the surface. Our results show that the oxidation state of surface iron can be controlled by the surface termination where ferryl (Fe^4 +) species emerge for oxygen terminated surfaces and ferrous iron (Fe^2 +) at iron and water terminations leading to a reduced band gap. In contrast, the fully hydroxylated surfaces, identified as stable surface configurations at standard conditions from the surface phase diagram, show electronic properties and band gaps closest to bulk FeOOH with ferric surface iron (Fe^3 +). Only in the case of goethite(101), a termination with mixed surface hydroxyl and aquo groups is stabilized.     

ICP-MS测定土壤样品中的有效锰、铜和锌

以DTPA提取土壤中的有效锰、铜、锌,不经分离富集,电感耦合等离子体质谱直接测定土壤样品中的有效锰、铜和锌,方法检出限分别可达0.042μg/L、0.039μg/L、0.028μg/L.通过对国家土壤有效态一级标准物质测试,测定结果基本一致;GBW 07412标准物质11次测定锰、铜和锌的相对标准偏差(RSD)分别为3.49%、3.72%、5.65%.     

Density functional slab model studies of water adsorption on flat and stepped Cu surfaces

Density functional and periodic slab model calculations are performed to study adsorption of water on various Cu surfaces, focusing on monomers and dimers at the planar Cu surfaces and monomers at stepped ones. Single water molecules tend to weakly bind to atop positions with the molecular plane basically parallel to the substrate surface on the planar surfaces or the step plane on the stepped surfaces with negligible structural deformation of water. The experimental adsorption energies of water on the (1 1 1) and (1 0 0) surfaces are about twice as large as the theoretical values of monomerically adsorbed water. This phenomenon is demonstrated to be due to formation of water clusters and/or existence of surface defects. It is revealed that the most favorable hexagonal ring superstructure on Cu(1 1 0) is a four-layer structure, not the commonly accepted bi-layer configuration. We found that the adsorption energy of monomeric water correlates linearly with following quantities, respectively: the bond length and the stretching frequency of the Cu-O bond, the coordination number of the surface Cu atom, the surface work function of the clean surface and the 1b₁ MO energy shift with respect to the value in the gas phase.     

Density functional study of the adsorption of K on the Cu(111) surface

The adsorption of potassium on the Cu(111) surface in a (2×2) pattern has been simulated with all-electron full-potential density functional calculations. The top site is found to be the preferred adsorption site, with the other highly symmetric adsorption sites being nearly degenerate. The bond length from potassium to the nearest copper atom is computed to be 2.83 ?. Population analysis and density of states indicate that there is no evidence for covalent bonding so that the binding mechanism appears to be a metallic bond. Received 11 April 2001     

X-ray absorption study of Cu,Zn SOD under high pressure

Abstract

We have investigated Cu, Zn Superoxide Dismutase (Cu, Zn SOD) metal sites at high pressure using X-ray absorption. XAS (X-ray Absorption Spectroscopy) gives information on local structure and it is particularly suited to metal site investigation. To the best of our knowledge, this is the first time that protein conformational states have been investigated using the high pressure XAS technique. Cu, Zn SOD catalyses the dismutation of toxic oxygen radicals produced in cells; this reaction occurs at the copper metal site. Structural changes around the copper, induced by pressure, can be directly related to protein substates. Their characterisation is thus important in the understanding of protein activity.

The high-pressure device was a Paris-Edinburgh large volume cell.

Experiments were performed on lyophilised Cu, Zn SOD between 0 and 48 kbar at the copper and zinc K-edges. The two metal local atomic environments have a different behaviour as pressure increases: copper exhibits a more flexible environment; on the contrary, zinc shows small structural modifications. We have identified a state, formed between 3 and 8 kbar, which is stable up to 48 kbar.     

FAAS法测定银杏胶囊中镁、锰、锌和铜

采用火焰原子吸收光谱法测定了银杏胶囊中Mg、Mn、Zn和Cu 4种金属元素的含量.结果表明,银杏胶囊中含有丰富的Mg、Mn、Zn、Cu元素,元素含量Mg＞Zn＞Mn＞Cu,测定结果为探讨中成药中金属元素与治疗心脑血管病之间的关系提供了有用的数据.     

基体改进-石墨炉原子吸收光谱法测定中药丹参中的铜和锌

以 NH4NO3 和 Se Triton X- 10 0作为铜和锌的基体改进剂 ,石墨炉原子吸收法测定丹参中铜和锌的含量。优化了实验条件 ,灰化温度分别提高到 12 0 0℃和 90 0℃ ,提高了方法的灵敏度。研究了不同测定波长对实验的影响 ,消除了基体干扰 ,提高了方法的重现性。用校准曲线法和标准加入法对试样分析结果一致 ,铜和锌的方法检出限分别为 0 .6 ng/ m L和 0 .9μg/ m L,RSD分别为 1.8%和 2 .3% ,回收率分别为 96 %和 10 1%。     

Ethylene adsorption on the Pt-Cu bimetallic catalysts. Density functional theory cluster study

The adsorption of ethylene on Cu₁₂Pt₂ clusters has been studied within the density functional theory (DFT) approach to understand the high ethylene selectivity of Cu-rich Pt-Cu catalyst particles in the reaction of hydrogen-assisted 1,2-dichloroethane dechlorination. The structural parameters for Cu₁₂Pt₂ clusters with D_4h, D_2d, and C_3v symmetry have been calculated. The relative stability of the isomeric Cu₁₂Pt₂ clusters follows the order: C_3v > D_2d > D_4h. Each isomer has an active site for ethylene adsorption that consists of a single Pt atom surrounded by Cu atoms. The interaction of ethylene with the active site yields a π-C₂H₄ adsorption complex. The strongest π-C₂H₄ complex forms with the cluster of C_3v symmetry; the bonding energy, ΔE_π(C₂H₄), is −15.6 kcal mol⁻¹. The bonding energies for the π-C₂H₄ complex with Cu₁₄ and Pt₁₄ clusters are −6.5 and −18.8 kcal mol⁻¹, respectively.The addition of Pt to Cu modifies the valence spd-band of the cluster as compared to a Cu₁₄ cluster. The DOS near the Fermi level increases when C₂H₄ adsorbs on the Cu₁₂Pt₂ cluster. As well, the center of the d-band shifts toward lower binding energies. Ethylene adsorption also induces a number of states below the d-band. These states correspond to those of gas-phase C₂H₄.The vibrational frequencies of C₂H₄ adsorbed on the clusters of D_4h and C_3v symmetry have been calculated. The phonon vibrations occur below 250 cm⁻¹. The intense bands around 200 cm⁻¹ are attributed to stretching vibrations of the Pt-Cu bonds normal to the cluster surface. The stretching vibrations of the Pt-C bonds depend on the local structure of the active site: ν_s(Pt-C) = 268 cm⁻¹ and ν_as(Pt-C) = 357 cm⁻¹ for the cluster of the D_4h symmetry; ν_s(Pt-C) = 335 cm⁻¹ and ν_as(Pt-C) = 397 cm⁻¹ for the cluster of the C_3v symmetry. Bands in the range of 800-3100 cm⁻¹ are attributed to vibrations of the adsorbed C₂H₄ molecule. The signature frequencies of the π-C₂H₄ adsorption complex are the δ_s(CH₂) deformation vibration at ∼1200 cm⁻¹ and the ν(C-C) stretching vibration at ∼1500 cm⁻¹. These vibration are absent for di-σ-C₂H₄ adsorption complexes.     

甲基和羟基在Ir(111)表面吸附的密度泛函理论研究

在超原胞近似和slab模型基础上,采用周期性密度泛函理论,在0.11覆盖度（ML）下,对甲基与羟基在Ir(111)表面的吸附进行了研究,得到了甲基和羟基在Ir(111)表面不同吸附位置的吸附能和吸附构型,计算了它们的振动频率,同时分析了甲基和羟基共吸附于Ir(111)表面的情况。结果表明,甲基和羟基在Ir(111)表面的最稳定吸附位置都是top位,甲基是碳端向下吸附,羟基是通过氧端向下倾斜吸附。通过频率分析发现吸附后CH3中C-H键的对称伸缩振动、反对称伸缩振动以及剪切振动频率均发生了红移,而羟基中的O-H键的振动频率发生蓝移现象。通过计算对比发现甲醇分解为甲基和羟基过程是一个放热反应,从热力学角度来说该反应是可行的。