元素电负性和硬度的密度泛函理论研究

应用密度泛函理论的DFT LDA、DFT LDA/NL和改进的Slater过渡态方法,把元素的电离能和电子亲合能的计算扩展到周期表的103种元素.并用有限差分方法计算了这103种元素的电负性和硬度.计算中考虑了相对论效应.计算结果比以前Robles等用密度泛函理论的XGL和Xα近似的交换相关泛函的计算结果有所改进,更接近实验值.     

HCN Adsorption on the Fe(100), Fe(111) and Fe(110) Surfaces: a Density Functional Theory Study

Twenty kinds of adsorptions of HCN on the Fe(100), Fe(111) and Fe(110) surfaces at the 1/4 monolayer coverage are found using the density functional theory. For Fe(100), the adsorption energy of the most stable configuration where the HCN locates at the fourfold site with the C-N bonded to four Fe atoms is 1.928 eV. The most favored adsorption structure for HCN on Fe(111) is f-η3(N)-h-η3(C), in which the C-N bond is almost parallel to the surface, and the adsorption energy is 1.347 eV. On Fe(110), the adsorption energy in the most stable configuration in which HCN locates at the two long-bridge sites is 1.777 eV. The adsorption energy of the parallel orientation for HCN is larger than that of the perpendicular configuration. The binding mechanism of HCN on the Fe(100), Fe(111) and Fe(110) surfaces is also analyzed by Mulliken charge population and the density of states in HCN. The result indicates that the configurations in which the adsorbed HCN becomes the non-linear are beneficial to the formation of the addition reaction for hydrogen. The nature that the introduction of Fe into the catalyst could increase the catalytic activity of the bimetallic catalyst in the addition reaction of hydrogen for nitriles is revealed.     

原子簇Ni2Fe2P结构稳定性的密度泛函理论研究

利用DFT(密度泛函理论)方法在B3LYP/Lan12dz水平下对原子簇模型Ni₂Fe₂P的二十余种可能构型分别在二、四重态下进行优化计算,分析比较了优化结果的能量、结合能、吉布斯自由能变化和过渡态.结果表明:原子簇Ni₂Fe₂P十种异构体没有虚频,有可能稳定存在于非晶态合金中;其中以具有二重态的构型1的能量最低,结合能、吉布斯自由能变化及过渡态能垒最大,最为稳定;四重态中异构体1',2',3'和4'共存的可能性比较大.     

The Surface Chemistry of Water on Fe(100): A Density Functional Theory Study

The formation of water by hydrogenation of atomic oxygen is studied using density functional theory. Atomic oxygen preferentially adsorbs at the four‐fold hollow site, the hydroxyl group prefers the bridge site in a tilted configuration, and water is most stable when adsorbed at the top site with the two O? H bonds parallel to the Fe surface. Water formation by the hydrogenation of oxygen is a highly activated process on the Fe(100) surface, with similar activation energies, in the order of 1.1 eV, for the first and second hydrogen additions. A more favourable route for the addition of the second hydrogen atom involves the disproportionation of hydroxyl groups to form water and adsorbed oxygen. Dissociation of the OH is also likely since the activation energy is similar to that for disproportionation of 0.65 eV. Furthermore, the results show that the dissociation of water on Fe(100) is a non‐activated process: 0.16 eV for the zero‐coverage limit and 0.03 eV when surface oxygen is present. Herein, adsorption energies, structures and vibrational frequencies are presented for several adsorption states at 0.25 ML coverage, as well as the potential energy surface for water formation on Fe(100).     

Ag在MgF2(010)表面吸附的密度泛函理论研究

基于密度泛函理论(DFT)的第一性原理赝势法, 对MgF2(010)面及吸附Ag的构型进行了优化, 并计算了MgF2(010)面吸附Ag体系的吸附能、 电子结构和光学性能. 结果表明, MgF2(010)面能隙低于体相, 态密度分裂, 出现表面态. Ag在MgF2(010)面的吸附属于稳定的化学吸附, 最佳吸附位为最外层F的四重穴位. 吸附机理主要表现为Ag的4p轨道与第二层的Mg的2p和3s轨道之间发生相互作用, 有少量电荷从Ag向Mg迁移. 吸附Ag后, 可见光波段的光吸收增加, Ag吸附后将使体系在可见光波段出现吸收峰.     

过渡金属纯簇和混合簇的密度泛函研究:Nb4,Co4和Nb2Co2

用密度泛函方法对过渡金属双原子Nb₂,Co₂和NbCo的电子态进行研究,得到三者的基态分别为³∑_g^-,⁵∑_g⁺和³△.并以此为基础,讨论四核簇Nb₄,Co₄和No₂Co₂的成键情况,发现稳定的单金属簇Nb₄具有高对称性的密堆结构,稳定的Co₄具有低对称性的变形封闭结构,两者都是典型的金属键;而Nb₂Co₂在封闭式结构中是一般的金属键,在线形结构中有强弱交替的定域键,Nb原子易相互靠近成键,Co原子趋于远离不成键.三种团簇的多重度以Nb₄＜Nb₂Co₂＜Co₄顺序依次升高.     

CN在 Pt(100)表面吸附的密度泛函研究

采用密度泛函方法,以原子簇Pt14为模拟表面,对CN自由基分子在Pt(100)表面上不同吸附位的吸附情况进行了研究.结果表明,CN分子吸附在Pt(100)面上时,通过原子C垂直吸附在表面顶位是其最佳吸附方式,CN键振动频率明显发生蓝移,与实验事实相吻合;而在桥位及四方穴位吸附时CN键振动频率均发生红移.吸附前后,CN分子的σ、π电子与底物间的电荷转移的差异决定了CN键振动频率的不同变化.     

密度泛函理论预测微量元素在Al(100)表面的偏聚

通过周期性层状模型, 利用密度泛函理论预测了微量杂质元素原子M(M=Fe, Si, Mg, Cu, Mn, Ga, In, Sn, Pb)在高纯铝箔(100)表面的偏聚趋势. 计算得到表面偏聚能与已有实验结果相吻合. 表面偏聚能由表面取代的微量元素原子M的位置、原子半径和金属的表面能决定. 当表面偏聚能为负时, 微量元素原子M在表面偏聚, 反之则杂质原子不发生表面聚集. 微量元素原子在铝箔表面偏聚可以使铝箔表面产生大量的缺陷和位错, 它们在铝箔腐蚀时容易成为腐蚀的形核起点, 进而增加铝箔的腐蚀发孔密度.     

复合添加合金元素对纳米双相Nd2Fe14B/α-Fe永磁体微观结构和磁性能的影响

采用正交实验法系统地研究了复合添加合金元素Ga ,Nb ,Zr,Hf和Pr对纳米双相Nd9-xPrxFe86 .5-y -z -m -nGayNbzZrmHfnB4 .5(x =0 ,2 2 5 ;y ,z ,m ,n =0 .5 ,1.0 )快淬带微观结构和磁性能的影响。结果表明 :复合添加合金元素可以大大地降低Nd2 Fe1 4B和α Fe相的晶粒尺寸 ,并促使快淬带在低辊速下非晶化 ;在退火后样品带中 ,没有发现晶粒的不均匀长大 ,但大量添加合金元素会导致晶粒形貌不够理想。另一方面 ,由于各元素间的交互作用 ,复合添加合金元素使磁性能的变化规律非常复杂。实验发现 ,当Nb的含量为 0 .5 %时 ,增加Pr和Ga的添加量并降低Zr和Hf的添加量可以明显地改善磁性能。成分为Nd2 .2 5Pr6 .75Fe84 .5Ga1 .5Nb0 .5B4 .5的合金 ,在 15m·s- 1 辊速下获得的最佳磁性能为Jr=1.0 5 3T ,iHc=5 3 0 .9kA·m- 1 ,(BH) max=12 4kJ·m- 3。     

Cu(100)表面吸附HCN和HNC的密度泛函研究

采用密度泛函方法，以原子簇Cul4为模拟表面，对氢氰酸(HCN)和异氰酸(HNC) 在Cu(100)表面上不同吸附位的吸附情况进行了研究．结果表明：HCN和HNC分别通 过原子N和C垂直吸附在表面上时，顶位是其最佳吸附位，且是吸附能为18．5kJ· mol^-1和42．6kJ·mol^-1的弱吸附，计算结果与实验相符．C—N(HCN)键或N—C (NHC)键偏离垂直的分子轴线的吸附体系均不稳定．顶位吸附时HCN和HNC分子的C- N键振动频率均发生蓝移．     

Ni(100)表面吸附SO2的密度泛函研究

以原子簇Ni14为模拟表面,采用DFT/B3LYP方法研究了二氧化硫(SO2)分子在Ni(100)表面的吸附构型、能量、电荷及态密度。结果表明,SO2分子通过S原子平铺吸附在Ni(100)的桥位最有利,计算结果与实验相符。电荷密度及态密度分析表明,Ni原子的d轨道与SO2分子的空p轨道之间存在明显的s-p作用和电荷转移,这一作用可能导致SO2分子发生解离。     

Density Functional Theory Study on the Adsorption of HCNH and CNH2 on Cu（100） Surface

The HCNH and CNH2 adsorption on different coordination sites of Cu（100） was theoretically studied considering the cluster approach. The present calculations show that the bridge site is the most favorite for CNH2 perpendicularly adsorbed on the Cu（100） surface via the C atom. For HCNH absorbed on the Cu（100） surface, the parallel adsorption mode with the C and N atoms nearly directly above the adjacent top sites of Cu（100） surface is the most favored. Both CNH2 and HCNH are strongly bound to the Cu（100） surface with CNH2 which is lightly stable （2.51 kJ·mol^-1）, indicating that both species may be co-adsorbed on the Cu（100） surface.     

甲醛在CeO2(111)表面吸附的密度泛函理论研究

采用基于第一性原理的密度泛函理论和周期平板模型, 研究了甲醛在以桥氧为端面的CeO2(111)稳定表面上的吸附行为. 通过对不同覆盖度, 不同吸附位的甲醛吸附构型、吸附能及电子态密度的分析发现, 甲醛在CeO2(111)表面存在化学吸附与物理吸附两种情况. 化学吸附结构中甲醛的碳、氧原子分别与表面的氧、铈原子发生相互作用, 形成CH2O2物种; 吸附能随着覆盖度的增加而减小. 与自由甲醛分子相比, 物理吸附的甲醛构型变化不大, 其吸附能较小. 利用CNEB(climbing nudged elastic band)方法计算了甲醛在CeO2(111)表面的初步解离反应活化能(约1.71 eV), 远高于甲醛脱附能垒, 这与甲醛在清洁CeO2(111)表面程序升温脱附实验中产物主要为甲醛的结果相一致.     

2-氯噻吩在 Rh(111) 表面吸附的密度泛函理论研究

 采用密度泛函理论探讨了 2-氯噻吩分子在 Rh(111) 表面上吸附行为. 结果表明, 平行的 hol 位及 bridge 位上的吸附最稳定. 吸附后, 2-氯噻吩键长发生明显变化, 分子平面被扭曲, 分子中 C–H(Cl, S) 相对于金属表面倾斜上翘. 垂直吸附模式不如平行吸附模式稳定, 但吸附后噻吩环未发生变形. hol 及 bridge 吸附模式下 2-氯噻吩的芳香性已遭破坏, 噻吩环上的碳原子呈现准 sp3 杂化. 在平行的 hol 位吸附后, 2-氯噻吩环累计得到 0.77 个电子, 而 Rh(111) 表面累计失去 1.19 个电子.     

CeO2(110)表面上CO氧化反应的密度泛函理论研究

利用密度泛函理论系统研究了O2与CO在CeO2(110)表面的吸附反应行为. 研究表明, O2在洁净的CeO2(110)表面吸附热力学不利, 而在氧空位表面为强化学吸附, O2分子被活化, 可能是重要的氧化反应物种. CO在洁净的CeO2(110)表面有化学吸附与物理吸附两种构型, 前者形成二齿碳酸盐物种, 后者与表面仅存在弱的相互作用. 在氧空位表面, CO可分子吸附或形成碳酸盐物种, 相应吸附能均较低. 当表面氧空位吸附O2后(O2/Ov), CO可吸附生成碳酸盐或直接生成CO2, 与原位红外光谱结果相一致. 过渡态计算发现,O2/Ov/CeO2(110)表面的三齿碳酸盐物种经两齿、单齿过渡态脱附生成CO2. 利用扩展休克尔分子轨道理论分析了典型吸附构型的电子结构, 说明表面碳酸盐物种三个氧原子电子存在离域作用, 物理吸附的CO及生成的CO2电子结构与相应自由分子相似.     

Production and Characterization of Nanostructured Powders of Nd2Fe14B and Fe90Al10 by Mechanical Alloying

The objective of this work is to evaluate the applicability of exchange coupling between nanoparticles of Nd₂Fe₁₄B (hard magnetic material) and Fe₉₀Al₁₀ (soft magnetic material), as permanent magnets produced by surfactant-assisted mechanical alloying. The obtained powders were then mixed with 85% of the Nd₂Fe₁₄B system and 15% of the Fe₉₀Al₁₀ system and subsequently sintered at 300 °C, 400 °C and 500 °C for one hour. The results obtained by Mössbauer spectrometry (MS) show a ferromagnetic behavior with six magnetic sites represented by sextets (16k1, 16k2, 8j1, 8j2, 4c and 4e), characteristic of the Nd₂Fe₁₄B system. X-ray diffraction (XRD) results show a tetragonal and BCC structure for the Nd₂Fe₁₄B and FeAl systems, respectively. The results obtained by vibrating sample magnetometry (VSM), for mixtures of the Nd₂Fe₁₄B and Fe₉₀Al₁₀ sy stems sintered at 300 °C, 400 °C and 500 °C, allow for the conclusion that the coercive field (Hc) decreases drastically with temperature and the percentage of soft phase at values of Hc = 132 Oe compared to the coercive field values reported for Nd₂Fe₁₄B Hc = 6883 Oe, respectively. Images obtained by transmission electron microscopy (TEM), for the Fe₉₀Al₁₀ system, show a tendency for the nanoparticles to agglomerate.     

Density Functional Theory Study on the Structural and Electronic Properties of Ge（SiO_2）_n Clusters

The geometry,stability,binding energy and electronic properties of(SiO2)n and Ge(SiO2)n clusters(n = 7) have been investigated by Density functional theory(DFT).The results show that the lowest energy structures of Ge(SiO2)n are obtained by adding one Ge on the end site of the O atom or the Si near end site of the O atom in(SiO2)n.The chemical activation of Ge-(SiO2)n is improved compared with(SiO2)n.The calculated second-order difference of energies and fragmentation energies show that the Ge(SiO2)n clusters with n = 2 or 5 are stable.     

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.     

Density Functional Theory Study on Hydrogen Bonding Interaction of Catechin-(H2O)n

Density functional theory B3LYP method with 6‐31G* basis set has been used to optimize the geometries of the catechin, water and catechin‐(H₂O)_n complexes. The vibrational frequencies have been studied at the same level to analyze these complexes. Six and eleven stable structures for the catechin‐H₂O and catechin‐(H₂O)₂ have been found, respectively. Theories of atoms in molecules (AIM) and natural bond orbital (NBO) have been utilized to investigate the hydrogen bonds involved in all the systems. The interaction energies of all the complexes corrected by basis set superposition error, are from ?13.27 to ?83.56 kJ/mol. All calculations also indicate that there are strong hydrogen‐bonding interactions in catechin‐water complexes. The strong hydrogen‐bonding contributes to the interaction energies dominantly. The O–H stretching motions in all the complexes are red‐shifted relative to that of the monomer.