一经式异构体[Co(N-(3-Aminopropyl)-1,3-propanediamine)(1,2-diamino-2-methylpropane)Cl][ZnCl4]·2H2O的合成及晶体结构

用过氧化物法合成了新体系［ Ｃｏ（ ３, ３－ｔｒｉ）（ ｉｂｎ） ＣＩ］［ ＺｎＣｌ４］（ ３, ３－ｔｒｉ＝ Ｎ－（ ３－Ａｍｉｎｏｐｒｏｐｙｌ）－ １, ３－ｐｒｏｐａｎｅｄｉａ－ｍｉｎｅ; ｉｂｎ＝１, ２－ｄｉａｍｉｎｏ－２－ｍｅｔｈｙｌｐｒｏｐａｎｅ）中的一经式异构体［Ｃｏ（３, ３ｔｒｉ）（ｉｂｎ）ＣＩ］［ＺｎＣｌ４］·２Ｈ２Ｏ,解析了其晶体结构。晶体学参数：三斜晶系,空间群Ｐ１（＃２）,ａ＝９９．５８（２）ｎｍ,ｂ＝１１４．８３（２）ｎｍ,ｃ＝９８．８１（１）ｎｍ,ａ＝９６．７９（２）°,β＝９７．２４３（１０）°,ｙ＝９６．８９（１）°,Ｖ＝１．１０５５（３）Ｘ １０６ｎｍ３,Ｄｅ＝１．６７８ｇ·ｃｍ－３,Ｚ＝２,Ｆ０００＝５７２．００,μ（ Ｍｏ Ｋａ）＝ ２４． ５９ｃｍ－１, Ｒ＝ ０． ０２５, Ｒｗ＝ ０． ０３４。晶胞中含 ２个配位阳离子, ２个 ［ＺｎＣｌ４］２－阴离子及 ４个水分子。     

螺噻唑并咪唑类化合物的合成

由螺［５．５］十一烷－３－酮与硫脲在碘的存在下反应，生成了４，５－二氢螺［苯并［ｄ］噻唑－６－（７Ｈ），１′－环己烷］－２－胺（３），３与溴甲基苯基甲酮在苯中缩合得到相应的酮４ａ～４ｃ，然后在醇中加热环化生成二氢螺［咪唑并［２，１－ｂ］苯并［ｄ］噻唑］化合物５ａ～５ｃ。新化合物５ａ～５ｃ的分子组成及结构经元素分析、１ＨＮＭＲ、１３ＣＮＭＲ证实，其中产物５ｂ的分子结构经Ｘ－射线衍射晶体分析确认。     

Synthesis and Structure of the Hexanuclear Diazenido－oxomolybdate ［（n－C_4H_9）_4N］_3［Mo_6O_（18）（N_2C_6H_4－p－NO_2）］

ＳｙｎｔｈｅｓｉｓａｎｄＳｔｒｕｃｔｕｒｅｏｆｔｈｅＨｅｘａｎｕｃｌｅａｒＤｉａｚｅｎｉｄｏ－ｏｘｏｍｏｌｙｂｄａｔｅ［（ｎ－Ｃ_４Ｈ_９）_４Ｎ］_３［Ｍｏ_６Ｏ_（１８）（Ｎ_２Ｃ_６Ｈ_４－ｐ－ＮＯ_２）］ＬｉＨａｉ－Ｌｉａｎ；ＹｏｕＸｉａｏ－Ｚｅｎｇ；...     

钴(Ⅲ)—邻菲绕啉混配型配合物的合成及结构研究

在不同条件下合成了［Ｃｏ（ｐｈｅｎ）ｍＸｐ］Ｙ１·ｎＨ２Ｏ型配合物，（ｍ＝１，２；ｐ＝１，２；１＝１－３；ｎ＝０－４；ｐｈｅｎ＝邻菲绕啉；Ｘ＝Ｃｌ－，Ｈ２Ｏ，酒石酸（ｔａｒｔ），甘氨酸（ｇｌｙ），α－皮可林酸（ｐｉｃ）．ＤＬ－两氨酸（ａｌａ），Ｌ－亮氨酸（ｌｅｕ），Ｌ－脯氨酸（ｐｒｏ）；Ｙ＝Ｃｌ－，］并进行了元素分析，热重分析，电子光谱，红外光谱和磁化率测定，计算它们的１０Ｄｑ和Ｂ值．Ｘ－ｒａｙ单晶衍射实验证明：［Ｃｏ（Ｐｈｅｎ）２（Ｈ２Ｏ）２］（ＮＯ３）３·２Ｈ２Ｏ，［Ｃｏ（Ｐｈｅｎ）２（ｇｌｙ）］Ｃｌ２·４Ｈ２Ｏ均为顺式结构．［Ｃｏ（Ｐｈｅｎ）（ａｌａ）２］Ｃｌ·３Ｈ２Ｏ，［Ｃｏ（Ｐｈｅｎ）（ｐｒｏ）２］ＣｌＯ４·４／３Ｈ２Ｏ均为ｔｒａｎｓ（Ｎ）结构．在［Ｃｏ（ｐｈｅｎ）２Ｘ２］（ｎ＋）型配合物中，Ｘ反位的键长均长于顺位键长，其反位效应的顺序为：Ｃｌ－＞羧基，ＮＨ２＞Ｈ２Ｏ。     

Synthesis and Structure of [HOCH2CH2N（CH3）3]4[Cu4OCl10]

ＳｙｎｔｈｅｓｉｓａｎｄＳｔｒｕｃｔｕｒｅｏｆ［ＨＯＣＨ_２ＣＨ_２Ｎ（ＣＨ_３）_３］_４［Ｃｕ_４ＯＣｌ_（１０）］ＷｕＤｉｎｇ－Ｍｉｎｇ；ＨｕａｎｇＸｉａｏ－Ｙｉｎｇ；ＺｈｕａｎｇＨｏｎｇ－Ｈｕｉ（ＳｔａｔｅＫｅｙＬａｂｏｒａｔｏｒｙｏｆＳｔｒｕｃｔ?..     

新型六核钼原子簇化合物{[Mo3（μ3—S）（μ—S2）2（dtp）3]—（μ3—S）（η…

［Ｍｏ３（μ３－Ｏ）（μ－Ｓ）３（μ－ＯＡｃ（ｄｔｐ）３（ｐｙ）］和［Ｍｏ３（μ－Ｓ）３（μ－ＯＡｃ（ｄｔｐ）３－（ｐｙ）］（ｄｔｐ＝Ｓ２Ｐ（ＯＣ２Ｈ５）２＾－）族合物分别与金属化合物ＢｉＩ３和ＳｂＢｒ３进行原子簇反应均能获得意外产物｛［Ｍｏ３（μ３－Ｓ）（μ－Ｓ２）２（ｄｔｐ）３］（μ３－Ｓ）（η＾３－Ｓ２）［Ｍｏ２（μ３－Ｓ）（μ－Ｓ）３（μ－ＯＡｃ）（ｄｔｐ）２］｝六核钼簇。其结构实际上是由     

稠杂环化合物的研究（ⅩⅤⅠ）──1－芳基－1，2，3－连三唑［4，5－e］嘧啶酮及哌啶／氢化吖辛因［1，2－b］嘧啶酮类化合物的合成

研究了１－芳基－４－乙氧羰基－５－氨基－１，２，３－连三唑（１）同甲酰胺、异氰酸磺酰氯以及内酰亚胺醚等的反应，制得５－Ｈ－１－芳基－１，２，３－连三唑［４，５－ｅ］嘧啶－４－酮（２ａ－ｃ）、５－Ｎ－甲基－１－芳基－１，２，３－连三唑［４，５－ｅ］嘧啶－４－酮（３ａ－ｃ）、１－芳基－４－乙氧羰基－５－脲基－１，２，３－连三唑（４ａ，ｂ）、５－Ｈ－１－芳基－１，２，３－连三唑［４，５－ｅ］嘧啶－４，６－二酮（５＿（ａ，ｂ））、１－苯基－１，２，３－连三唑［４，５－ｅ］哌啶［１，２－ｂ］嘧啶－４－酮（６ａ）、１－苯基－１，２，３－连三唑［４，５－ｅ］氢化吖辛因［１，２－ｂ］嘧啶－４－酮（７ａ），并经元素分析、红外、核磁共振以及质谱等方法确认了它们的结构，初步筛选了其代表特的生物活性．     

等瓣置换反应的研究──手性簇合物［（η~5－MeO_2CC_5H_4）（CO）_2Mo］·［（η~5－MeO_2CC_5H_4）（CO）_2W］Fe（CO）_3（μ_3－S）的分子结构及晶体结构

用Ｘ射线衍射法测定了由η~５－ＭｅＯ_２ＣＣ_５Ｈ_４）（ＣＯ）_３ＭｏＮａ和［（η~５－ＭｅＯ_２ＣＣ_５Ｈ_４）（ＣＯ）_２Ｗ］Ｆｅ－（ＣＯ）_３Ｃｏ（Ｃｏ）_３（μ_３－Ｓ）的等瓣置换反应所生成的手性簇合物──［（η~５－ＭｅＯ_２ＣＣ_５Ｈ_４）（ＣＯ）_２Ｍｏ］－［（η~５－ＭｅＯ_２ＣＣ_５Ｈ_４）（ＣＯ）_２Ｗ］Ｆｅ（ＣＯ）_３（μ_３－Ｓ）的分子结构及晶体结构。晶体属Ｐ１空间群，晶胞参数α＝０．８７１６２（５）ｎｍ，ｂ＝０．７６２１８（４）ｎｍ，ｃ＝１．８７１１１（８）ｎｍ；α＝９４．１６４（４）°，β＝９７．９７９（２）°，γ＝９９．１０８（２）°，Ｚ＝２，μ＝５．９ｃｍ~（－１）。最终的一致性因子Ｒ＝０．０３６，Ｒｗ＝０．０３７．该簇合物含ＭｏＷＦｅＳ四面体簇核，其中Ｍｏ、Ｗ原子以１：１的比例无序地分占了四面体的２个顶点．     

Co3（CO）7（μ3—S）（μ,η^2—SCNR2）的合成和晶体结构

Ｃｏ２（ＣＯ）８与４个二硫代双（烷基硫代甲酰胺）类前配体［Ｒ２ＮＣ（Ｓ）Ｓ］２反应,得４个含烷基硫代甲酰胺基的三核钴羰基硫簇合物。通过元素分析、ＩＲ、＾１ＨＮＭＲ和ＭＳ等方法表征了它们的结构,用Ｘ射线衍射法测定了其中一个簇合物Ｃｏ３（ＣＯ）７（μ３－Ｓ）［μ,η＾２－ＳＣＮ（ｉ－Ｐｒ）２］（Ⅲ）的晶体结构。晶体属单斜晶系,Ｐ２１／ｎ空间群,晶胞参数ａ＝１．１４５２（２）ｎｍ,ｂ＝１．５０２８（３）     

Synthesis and Crystal Structure of［（n－Bu）_4N］_2［Mo_4O_（10）（OC_（10）H_6O）_2（OCH_3）_2］

ＳｙｎｔｈｅｓｉｓａｎｄＣｒｙｓｔａｌＳｔｒｕｃｔｕｒｅｏｆ［（ｎ－Ｂｕ）_４Ｎ］_２［Ｍｏ_４Ｏ_（１０）（ＯＣ_（１０）Ｈ_６Ｏ）_２（ＯＣＨ_３）_２］￥ＬｕＸｉａｏ－Ｍｉｎｇ；ＺｈｕＨｕｉ－Ｊｕ；ＹａｎｇＮｉｎｇ；ＬｉｕＳｈｕｎ－Ｃｈｅｎｇ；ＪｉｎＸ?..     

Fragmentation Behavior and Ionization Potentials of Lead Clusters Pb_n(n≤30)

The properties of Pbn(n=2―30) clusters including binding energies,second differences in energy,and HOMO-LUMO gaps,especially fragmentation energies and ionization potentials,have been studied by ab initio calculation.The main fragmentation products of Pbn+ are shown to be Pb+Pbn-1+ for n≤14 and two small cluster fragments for larger ones with n14.The Pb13+ appears frequently as the products in the fragmentations of large clusters.Also,the calculated ionization potentials of the clusters are consistent with the experiment data.     

Atomic and electronic structures of neutral and charged Pbn clusters (n=2-15): theoretical investigation based on density functional theory

The geometric and electronic structures of the Pbn+ clusters (n=2-15) have been investigated and compared with neutral clusters. The search for several low-lying isomers was carried out under the framework of the density functional theory formalism using the generalized gradient approximation for the exchange correlation energy. The wave functions were expanded using a plane wave basis set and the electron-ion interactions have been described by the projector augmented wave method. The ground state geometries of the singly positively charged Pbn+ clusters showed compact growth pattern as those observed for neutrals with small local distortions. Based on the total energy of the lowest energy isomers, a systematic analysis was carried out to obtain the physicochemical properties, viz., binding energy, second order difference in energy, and fragmentation behavior. It is found that n=4, 7, 10, and 13 clusters are more stable than their neighbors, reflecting good agreement with experimental observation. The chemical stability of these clusters was analyzed by evaluating their energy gap between the highest occupied and lowest unoccupied molecular orbitals and adiabatic ionization potentials. The results revealed that, although Pb13 showed higher stability from the total energy analysis, its energy gap and ionization potential do not follow the trend. Albeit of higher stability in terms of binding energy, the lower ionization potential of Pb13 is interesting which has been explained based on its electronic structure through the density of states and electron shell filling model of spherical clusters.     

High-pressure investigation of Li2MnSiO4 and Li2CoSiO4 electrode materials for lithium-ion batteries

In this work, the high-pressure behavior of Pmn2(1)-Li(2)MnSiO(4) and Pbn2(1)-Li(2)CoSiO(4) is followed by in situ X-ray diffraction at room temperature. Bulk moduli are 81 and 95 GPa for Pmn2(1)-Li(2)MnSiO(4) and Pbn2(1)-Li(2)CoSiO(4), respectively. Regardless of the moderate values of the bulk moduli, there is no evidence of any phase transformation up to a pressure of 15 GPa. Pmn2(1)-Li(2)MnSiO(4) shows an unusual expansion of the a lattice parameter upon compression. A density functional theory investigation yields lattice parameter variations and bulk moduli in good agreement with experiments. The calculated data indicate that expansion of the a lattice parameter is inherent to the crystal structure and independent of the nature of the transition-metal atom (M). The absence of pressure-driven phase transformation is likely associated with the incapability of the Li(2)MSiO(4) composition to adopt denser structures while avoiding large electrostatic repulsions.     

Simulation of core-level binding energy shifts in germanium-doped lead telluride crystals

To simulate the changes in core-level binding energies in germanium-doped lead telluride, cluster calculations of the changes in the electrostatic potential at the corresponding centers have been performed. Different locations of the Ge atom in the crystal bulk have been considered: near vacancies, near another dopant site, and near the surface. For calculating the potential in the clusters that model the bulk and the surface of the lead telluride crystal (c-PbTe), the electron density obtained in the framework of the Hartree-Fock and hybrid density functional theory (DFT) methods has been used.     

Structure and electronic properties of PbnM (M=C, Al, In, Mg, Sr, Ba, and Pb; n=8, 10, 12, and 14) clusters: theoretical investigations based on first principles calculations

A systematic theoretical study of the PbnM (M=C, Al, In, Mg, Sr, Ba, and Pb; n=8, 10, 12, and 14) clusters have been investigated to explore the effect of impurity atoms on the structure and electronic properties of lead clusters. The calculations were carried out using the density functional theory with generalized gradient approximation for exchange-correlation potential. Extensive search based on large numbers of initial configurations has been carried out to locate the stable isomers of PbnM clusters. The results revealed that the location of the impurity atom depends on the nature of interaction between the impurity atom and the host cluster and the size of the impurity atom. Whereas, the impurity atoms smaller than Pb favor to occupy the endohedral position, the larger atoms form exohedral capping of the host cluster. The stability of these clusters has been analyzed based on the average binding energy, interaction energy of the impurity atoms, and the energy gap between the highest occupied and lowest unoccupied energy levels (HLG). Based on the energetics, it is found that p-p interaction dominates over the s-p interaction and smaller size atoms interact more strongly. The stability analysis of these clusters suggests that, while the substitution of Pb by C or Al enhances the stability of the Pbn clusters, Mg lowers the stability. Further investigations of the stability of PbnM clusters reveal that the interplay between the atomic and electronic structure is crucial to understand the stability of these clusters. The energy gap analysis reveals that, while the substitution of Mg atom widens the HLG, all other elements reduce the gap of the PbnM clusters.     

关于空间群判断失误的扎记 V.晶系不变情况下的非心群修正

我们发表胡盛志教授的“札记” ,一是想提醒晶体结构工作者们在晶体结构测定过程对空间群的指定应十分小心 ,尽量减少差错 ;同时也想借此透露一些国外同行在纠正空间群测定差错这一方面的工作 ,引起国内同行关注和响应。至于胡教授“札记”的论证方法的客观性 ,论据的充分性等 ,因纯系个人的见解 ,十分欢迎有不同意见者结合实例来稿进行讨论。     

Determination of the Real Surface Area of Palladium Electrode

Four methods, including voltammetric measurement of double layer capacitance, surface oxides reduction, under potential deposition of Cu and carbon monoxide (CO) stripping have been applied to evaluate the real surface area of a polycrystalline Pd (pc-Pd) electrode. The results reveal that the second and third methods lead to consistent results with deviations below 5%. And from the determined double layer capacitance and CO stripping charge, it is deduced that the double layer capacity unit area is 23.1±0.4 μF/cm² and the saturated CO adlayer should be ca. 0.66 ML in order to ensure that the real surface area as determined isconsistent with the other two techniques. The applicability as well as the attentions when applying these techniques for the determination of the real surface area of pc-Pd electrodes have been discussed.     

甲醇在Pt-Sn/Pb电极上的氧化行为——Ⅰ.电极催化特性的研究

采用欠电位沉积法,以铅电极作基体制备了负载型Pt-Sn双金属催化电极。应用循环伏安法和电位阶跃法研究了各种因素对该电极的催化活性和稳定性的影响,并应用XPS和AES技术分析了该电极的表面物性。该电极对酸性介质中的甲醇氧化反应显示出高于Pt-Sn/Pt电极的催化活性和稳定性。     

铅及铅锑合金阳极膜中硫酸铅的氧化过程

应用电位阶跃和交流阻抗法分别研究铅和Pb-5wt% Sb合金在4.5mol·dm^-^3H~2SO~4(30℃)中于1.3V(vs. Hg/Hg~2SO~4, 下同)生长20min后的阳极膜在0.9V还原5min后再在1.4V将膜中硫酸铅氧化的过程。实验结果表明在0.9V还原二氧化铅而得到的硫酸铅能在1.4V于1min内氧化为二氧化铅。这是由于此种硫酸铅处于硫酸铅颗粒表层的缘故。至于颗粒内部由铅直接生成的硫酸铅的氧化为二氧化铅就要缓慢得多。合金中的锑能使二氧化铅晶核形成和生长速率显著降低。     

The calcite/water interface II. Effect of added lattice ions on the charge properties and adsorption of sodium polyacrylate

The origin of the surface potential of calcium carbonate in aqueous dispersions and the dissolution of calcite in systems containing excess Ca(2+) and CO(3)(2-) have been the subjects of this study. In addition, stabilization of calcite particles with an anionic polyelectrolyte (sodium polyacrylate (NaPA)) and the effect on surface potential and dissolution of calcite have been studied. Preferential dissolution of either Ca(2+) or CO(3)(2-) from the surface, which is governed by the partial pressure of CO(2) in solution and the pH of the solution, mainly determines the surface potential. Both lattice ions (Ca(2+) and CO(3)(2-)) adsorb onto the surface and thus alter the surface potential. NaPA adsorbs strongly onto the calcite surface regardless of background electrolyte concentration, and reverses the surface potential to negative values. Chelation of the surface due to NaPA can be partly prevented by adding Ca(2+) to the dispersion.