NFeN结构和性质及反应势能曲线

用B3LYP/6-311+G(d)方法对化合物NFeN弯曲型和直线型的不同自旋多重度多个电子态的几何结构、电子结构、能量和振动光谱进行了计算研究. 结果表明, 单重态中Fe―N键长普遍比三重态和五重态中的短, 在155 pm左右; NFeN三重态电子结构最丰富, 自然键轨道和Mulliken布居显示Fe―N键具有部分离子键特征; 两种结构的所有稳定态中能量最低的是1⁵A₂态, 能量相近的有1³B₁、1³A₂、1³B₂和1¹A₁态, 直线型中能量最低是³Δ_g态; 相对于分子基态反应物Fe(a⁵D)+N₂(X¹Σ_g⁺)所有电子态的能量都偏高, 该反应在热力学上是不利的, 但是对于原子态反应物Fe(a⁵D)+2N(⁴S)则是放热反应; 计算振动频率和强度与实验较吻合的是1³B₁态; 复合物FeN₂与化合物NFeN结构差异明显; Fe原子直接插入N₂分子的势能曲线表明该反应能垒很高, 在动力学上也是不利的.     

CH4, CO2和H2O在非金属原子修饰石墨烯表面的吸附

煤层气(矿井瓦斯)是一种有望替代传统化石燃料,如煤、石油和天然气的非常规气体. 作为可得的清洁能源,它的利用被认为是节能和经济的选择. 在本工作中,非金属原子X(X=H,O,N,S,P,Si,F,Cl)修饰的石墨烯(Gr)被用来代表具有结构异性的煤表面模型. 通过密度泛函理论系统地研究了煤层气组分Y(Y=CH₄,CO₂,H₂O)在非金属原子修饰石墨烯上的吸附作用. 结果表明Y在非金属原子修饰石墨烯上的吸附均为物理吸附. 态密度和差分电荷密度共同表明了这种弱的相互作用.其中,H和Cl对CH₄的作用较大; N、O、F、Cl对CO₂的作用较强; N,Cl对H₂O的影响不容忽视. 总的来说,吸附能大小依次为：H₂O>CO₂>CH₄. 因此,在CH₄富集的煤层里注入H₂O或CO₂可以与CH₄形成竞争吸附,进而提高煤层气采收率. 本工作提供了在分子水平下煤层气与非金属原子修饰石墨烯之间的相互作用的详情,并为煤层瓦斯的开采与分离提供了有用的信息.     

2-(2-羟基苯亚甲基胺)-4,6-二羟基-嘧啶的质子转移异构化反应

为了探索2-(2-羟基苯亚甲基胺)-4,6-二羟基-嘧啶(M1)分子醇式和酮式结构互变异构化的反应机理,利用密度泛函理论(DFT)方法,在B3LYP/6-311+G(d,p)基组水平上,对M1化合物异构化反应的势能面进行了研究,在探讨各种可能的反应途径中,发现单体至少有8种异构体和10种过渡态.结果表明:2-(2-羟基苯亚甲基胺)-6-羟基-4(3H)嘧啶酮(M6)不论是单体、与水形成的配合物,还是二聚体,比其相对应的异构体能量低,表明在通常情况下是以M6形式稳定存在的;在考察的可能反应途径中,直接进行的分子内质子转移过程需要的活化自由能为143.8 kJ· mol-1,水助催化时,反应的活化自由能为38.9 kJ· mol-1,二聚体双质子转移的活化自由能为0.6 kJ·mol-1,二聚体双质子转移所需活化自由能最低,在室温下就可以进行,由此可见氢键在降低反应活化能方面起着重要的作用.     

AuClx (x=1, 3)催化2-炔丙基苯酮与苯炔环化反应机理

对金属元素Au采用LanL2DZ基组,对非金属元素C,H,O,Cl采用6-31G*和6-311++G**基组,用密度泛函理论的B3LYP、B3PW91、UB3LYP方法和二阶微扰理论MP2方法研究了不同氧化态的金催化剂催化2-炔丙基苯酮与苯炔环化反应的机理.结果表明:在AuCl和AuCl3的作用下,反应均能通过[4+2]和[3+2]途径生成产物.但在AuCl催化下,[4+2]反应途径比[3+2]反应途径具有更低的活化自由能,反应主要通过[4+2]途径进行;而在AuCl3催化下,[4+2]反应途径与[3+2]反应途径的活化自由能相近,反应通过两条途径竞争生成产物.比较AuCl和AuCl3的催化效果发现,不同氧化态的金催化剂改变了反应的机理,该反应的活化自由能在AuCl作用下比在AuCl3作用下低11.18 kJ·mol-1.对于该反应,AuCl表现出了更好的催化活性.这些计算结果和实验现象相吻合.     

O与O2在Au团簇上吸附的密度泛函理论研究

采用基于密度泛函理论(DFT)的Dmol³程序系统研究了O原子与O₂在 Au₁₉与Au₂₀团簇上的吸附反应行为. 结果表明: O在Au₁₉团簇顶端洞位上的吸附较Au₂₀强; 在侧桥位吸附强度相近. O与O₂在带负电Au团簇上吸附较强, 在正电团簇吸附较弱. 从O―O键长看, 当金团簇带负电时, O―O键长较长, 中性团簇次之, 正电团簇中O―O键长较短, 因而O₂活化程度依次减弱. 电荷布居分析表明, Au团簇带负电时, O与O₂得电子数较中性团簇多, 而团簇带正电时, 得电子数较少. 差分电荷密度(CDD)表明, O₂与Au团簇作用时, 金团簇失电子, O₂的π^*轨道得电子, 使O―O键活化. O₂在Au₁₉^-团簇上解离反应活化能为1.33 eV, 较中性团簇低0.53 eV; 而在Au₁₉⁺上活化能为2.27 eV, 较中性团簇高0.41 eV, 这与O₂在不同电性Au₁₉团簇O―O键活化规律相一致.     

LiVPO4F电子结构及电化学性质的第一性原理研究

采用密度泛函理论(DFT)结合投影缀加波(PAW)方法,对LiVPO₄F的晶体结构,电子结构和电化学属性进行了研究。从理论上获得了脱Li前后具体的晶格参数的变化。通过对其态密度的计算,发现在放电过程中,V在化合物中呈现离子态,发生+3/+4价态的转变,电子转移主要发生在V原子上;而P原子的状态比较稳定,并不发生大的电子的转移,磷酸根的空间结构也变化不大。同时LiVPO₄F的禁带宽度仅为1.63 eV,说明其在一定情况下具有良好的导电性,有利于放电过程中电子的输运。LiVPO₄F是铁磁相,磁矩为2μ_B,而VPO₄F为反铁磁相。此外,通过计算获得了LiVPO₄F的平均嵌锂电压为4.0 eV。     

Synthesis and Structure Investigation of a Novel 3-Dimensional Potassium Supermolecular Compound Based on 2,4-Dinitro Resorcinol

A novel 3‐dimensional potassium supermolecular compound [K(HDNR)(H₂DNR)(H₂O)]_n (H₂DNR?2,4‐dinitro resorcinol) was synthesized and characterized by elemental analysis and FT‐IR spectroscopy. The crystal structure investigated by X‐ray single crystal diffraction shows that [K(HDNR)(H₂DNR)(H₂O)]_n crystallizes with a monoclinic unit cell in the space group P2(1)/c with unit cell dimensions of a=17.648(5) Å, b=12.527(3) Å, c=7.735(2) Å, β=94.33(2)°, V=1705.00(73) ų, Z=4. The structure was refined to the final R=0.0670 and wR=0.0722 for 2022 observed reflections with I>2σ(I). In the compound, potassium cation is assembled into one‐dimensional chains along c‐axis through oxygen atoms from water molecules, and the chains were connected by the bridged HDNR^? anions to form a two‐dimensional net structure. The two‐dimensional nets constructed a three‐dimensional supramolecular architecture via intermolecular hydrogen bonds and N–O···π interaction. Density functional theory (DFT) B3LYP was employed to optimize the structure and calculate energies for three tautomers of HDNR^? univalent anion. Three stable tautomers were located. It was found that the structure (I) with O(1) losing hydrogen atom is more stable than the structure (II) also with O(1) losing hydrogen atom and the structure (III) with O(4) losing hydrogen atom.     

The Rearrangement of 2,2‐Diphenyl‐1‐[(E)‐2‐phenylethenyl]cyclopropane to 3,4,4‐Triphenylcyclopent‐1‐ene: a DFT Analysis

A computational study on the rearrangement of 2,2‐diphenyl‐1‐[(E)‐2‐phenylethenyl]cyclopropane ( 1 ) is presented, using density functional theory (DFT), (U)B3LYP with the 6‐31G* basis set (DFT1) and (U)M05‐2X with the 6‐311+G** basis set (DFT2). In agreement with a biradical character of the transition structure (TS) or intermediate, the potential‐energy hypersurface is lowered by the influence of three conjugated Ph groups. Surprisingly, two conformations of the geminal diphenyl group (different twist angles) induce two different minimum‐energy pathways for the rearrangement. Independent of the functional used, the first hypersurface harbors true biradical intermediates, whereas the second energy surface is a flat, slightly ascending slope from the starting material to the TS. The functional (U)M05‐2X with the basis set 6‐311+G** provides realistic energies which seem to be close to experiment. The activation energy for racemization of enantiomers of 1 is lower than that of rearrangement by 2.5 kcal mol^?1, in agreement with experiment.     

Density functional study of AgnPd and AgnPdH clusters

Small Ag_nPd (n = 5) clusters and their hydrides Ag_nPdH (n = 5) have been studied by density functional theory calculations. For bare clusters, the structures in which the Pd atom has a maximum number of neighboring Ag atoms tend to be energetically favorable. Hydrogen prefers binding to Ag? Pd bridge site of Ag_nPd clusters except for Ag₅Pd. The binding energy has a strong odd–even oscillation. The electron transfers are from Ag atoms to Pd in bare clusters and are from metal clusters to H in cluster hydrides. © 2010 Wiley Periodicals, Inc. Int J Quantum Chem, 2011