层间阴离子对四元水滑石超分子作用力的影响

构建一价阴离子(X=F^?, Cl^?, Br^?, I^?, NO₃^?, OH^?)插层铜锌镁铝四元水滑石(CuZnMgAl-X)周期性计算模型, 采用密度泛函理论(DFT), 选取CASTEP程序模块, 对体系进行几何全优化, 从结合能、结构参数、Mulliken布居、氢键布居、态密度等角度研究了不同层间阴离子的分布形态以及其对主客体间超分子作用的影响. 结果表明, 随着CuZnMgAl-X体系层间阴离子电负性的减弱, 电子逐渐从层间阴离子向层板发生转移, 主客体间静电作用力逐渐减小, 氢键强度逐渐降低, 禁带宽度逐渐变窄, 体系电子更易向高能级发生跃迁, 稳定性逐渐下降. 此外, Cu的掺杂使得CuZnMgAl-X 体系的价带顶向高能量处发生偏移, 禁带宽度较传统水滑石体系更窄,稳定性更低, 进一步解释了含铜水滑石较难合成的原因.     

镍镁铝类水滑石的超分子结构、电子性质及稳定性

以Ni²⁺同晶取代Mg²⁺的方式构建镍镁铝类水滑石(HT)的周期性计算模型, 通过进行密度泛函理论计算,研究了含镍水滑石的的超分子结构、电子性质及稳定性. 结果表明, 随着镍离子逐渐取代镁离子, 金属离子之间的平均距离逐渐减小, 层间距逐渐增大, 与实验结果一致. 与此同时, 电子逐渐从主体层板向客体阴离子传递,导致主客体之间的静电作用力及整体超分子作用力逐渐增强, 结合能的绝对值逐渐增大, 体系的稳定性增加.在微观结构上, 电子传递行为使层板中平均金属―氧键键长逐渐减小, 且金属配位角的畸变情况得到一定程度的缓解, 这些变化都有利于形成更稳定的体系, 说明镍铝类水滑石在理论上比镁铝水滑石更稳定.     

层间水分子含量对铜铁水滑石超分子作用力的影响

构建铜铁水滑石[Cu₃Fe-LDHs-yH₂O(y=0-2)]周期性计算模型, 采用密度泛函理论(DFT), 选取CASTEP程序模块, 对体系进行几何全优化, 从结构参数、氢键布居、Mulliken电荷布居、逐级水合能等角度研究了层间NO₃^-和H₂O的分布形态及其与水滑石(LDHs)层板的超分子作用, 探究了水分子数目对体系姜-泰勒效应的影响. 结果表明, Cu₃Fe-LDHs-yH₂O主客体间存在着较强的超分子作用力, 主要包括氢键和静电作用, 其中氢键作用在水合过程中起主导作用, 氢键强度的顺序是层板-阴离子(L-A)型＞阴离子-水(A-W)型＞层板-水(L-W)型＞水-水(W-W)型; 随着层间水分子数的增加, 层间距先略微降低后显著升高, Cu₃Fe-LDHs体系的Cu—O八面体被逐渐拉长, 层板Cu²⁺的姜-泰勒畸变程度逐渐增大, 体系的逐级水合能绝对值逐渐降低, 说明Cu₃Fe-LDHs的水合程度不会无限增加, 而是具有一个饱和值. Cu₃Fe-LDHs-1H₂O构型接近理想六方晶胞, 层板金属畸变程度最小, 稳定性最高, 层间距与实验值较吻合, 推测其为实验上合成的Cu₃Fe-LDHs较稳定的构型.     

在空气下制备掺二价稀土的硼酸盐及二价稀土离子(RE2+=Sm,Eu,Tm,Yb)的光谱特征

本文讨论了Sm²⁺、Eu²⁺、Tm²⁺、Yb²⁺等二价稀土离子的光谱特征,特别是在一些含四面体硼酸根的硼酸盐如SrB₄O₇、SrB₆O₁₀和BaB₈O₁₃中它们的光谱性质。当以三价稀土离子取代化合物中的二价碱土离子时,利用不等价取代而产生的缺陷所带的电荷,可在高温的空气下使上述的稀土离子还     

1,10-邻啡啰啉取代的希夫碱配体及其双核配合物的合成(英)

A new ligand N, N′-Bis(salicyidene)-5,6-phenanthrolinenediamine (H₂L) 1 and its four binuclear complexes [M²⁺LM²⁺(B^-)₂]( M=Cu²⁺, B^-=Ac^-, 1a; M=Ni²⁺, B^-=Ac^-, 1b; M=Co²⁺, B^-=Cl^-, 1c; M=Ni²⁺, B^-=Cl^-, 1d) have been prepared by condensing 1 equiv. of 5,6-diamino-1,10-Phenanthroline with 2 equiv. of 2-hydroxybenzaldehyde and reaction of 1 with metal salts, and characterized by IR, ¹H and ¹³C NMR, UV-Vis and EI-MS analysis.     

球形微米镍颗粒的液相体系制备及应用

本研究采用液相还原法,选用六水合硫酸镍为镍源,水合肼为还原剂,在封端剂聚乙烯吡咯烷酮的辅助下,制备得到球形微米镍颗粒。所制备的球形微米镍颗粒粒径约为3 μm,粒径分布均匀,表面粗糙度较低。为了获得球形微米镍颗粒的最优工艺方案,分别探究了PVP浓度、氢氧化钠和水合肼用量及反应温度等工艺参数对产物形貌的影响。研究发现,PVP能够有效控制镍原子的排布和沉积,NaOH可调节反应的pH值,确保水合肼持续还原Ni₂₊^,温度会影响体系的还原反应速率。结果表明：当反应体系使用的PVP浓度为0.5 M、NaOH用量为2.5 mL、水合肼用量为5 mL时,在 60 ℃下水浴反应可获得表面粗糙度低的球形微米镍颗粒,其电导率为5×10₅ S.m_-1^,饱和磁化强度为49.34 emu.g_-1^{。通过添加去离子水、异丙醇和羧甲基纤维素的混合溶液},将球形微米镍颗粒配制成25 wt%的导电油墨,并在纸基表面绘制导电线路,经测试该线路的电导率为1.28×10₃ ^S.m_-1^,此电路在弯折条件下,呈现出良好的工作稳定性。     

α-Fe2O3/SiO2纳米颗粒混合体系表面的酸碱性质及其对重金属离子的吸附行为

以Fe(NO₃)₃·9H₂O和正硅酸乙酯(TEOS)为原料, 通过溶胶-凝胶法和辅助模板法分别制备了纳米α-Fe₂O₃和SiO₂, 并对所合成样品进行了粉末X射线衍射(XRD)和BET表征. 使用自动电位滴定仪测定了α-Fe₂O₃/SiO₂纳米颗粒混合体系的表面酸碱性质. 研究了在不同pH下α-Fe₂O₃/SiO₂混合体系对Cu²⁺、Pb²⁺、Zn²⁺离子的吸附行为. 基于上述实验数据, 用WinSGW软件计算了α-Fe₂O₃/SiO₂混合体系表面酸碱配位常数, 并得出结论: α-Fe₂O₃/SiO₂混合体系表面反应为单一脱质子反应≡XOH ⇔ ≡XO^-+ H⁺(lg K = -8.19±0.15), 明显区别于同时具有加质子和脱质子反应的α-Fe₂O₃/SiO₂/γ-Al₂O₃, α-Fe₂O₃/γ-Al₂O₃和SiO₂/γ-Al₂O₃等纳米颗粒混合体系. 在此基础上拟合得到α-Fe₂O₃/SiO₂混合体系吸附重金属离子Cu²⁺、Pb²⁺、Zn²⁺的表面络合反应平衡常数分别为:
≡XOH + M²⁺ ⇔ ≡XOM⁺+ H⁺ [lg K = -3.1, -3.6, -3.8 (M = Cu, Pb, Zn)].
≡XOH＋M²⁺＋H₂O ⇔≡XOMOH＋2H⁺[lg K = -8.8, -8.0, -10.5 (M = Cu, Pb, Zn)]     

内含式化合物X@(HBNH)12的结构与稳定性

采用B3LYP/6-31++G(d,p)方法，对内含式化合物X@(HBNH)₁₂ (X = Li^0/+, Na^0/+, K^0/+, Be^0/2+, Mg^0/2+, Ca^0/2+, H和He)的不同对称性构型进行计算，讨论其最稳定构型的几何参数、包含能、平衡常数、自然电荷、自旋密度、电离势和HOMO-LUMO能隙。发现在X@(HBNH)₁₂化合物中，客体Na^0/+, K^0/+, Mg^0/2+, Ca^0/2+, H和He几乎处在笼的中心，Li⁺处在中心附近0.021 nm的半径内，Li和Be^0/2+很大程度上偏离笼的中心位置。Li⁺, Be²⁺, Mg²⁺和Ca²⁺与其它离子相比，更易嵌入笼内形成稳定的内含式化合物。而且，M@(HBNH)₁₂ (M = Li, Na,K)的第一电离势比Cs(3.9 eV)原子小，是超碱金属。     

以[M(DETA)2)]n+(M=Cu2+, Ni2+, Co3+)为客体的MnPS3夹层化合物的合成、结构表征与磁性研究

将过渡金属配合物阳离子([M(DETA)₂]ⁿ⁺(M=Cu²⁺,Ni²⁺,Co³⁺;DETA=Diethylenetriamine,二乙烯三胺)作为客体插入层状MnPS₃层间得到了相应的3个夹层化合物。通过X-射线粉末衍射、元素分析和红外光谱对夹层化合物的结构进行了表征。结果表明,与主体MnPS₃ 0.65 nm的层间距相比较,夹层化合物(Mn_0.88PS₃[Cu(DETA)₂]_0.12)的层间距扩大了0.32 nm,由此推测客体[Cu(DETA)₂]²⁺在层间以平面四方的配位形式存在,而另2个夹层化合物(Mn_0.79PS₃[Ni(DETA)₂]_0.21和Mn_0.74PS₃[Co(DETA)₂]_0.17)的层间距扩大了0.48 nm,说明客体[(M(DETA)₂]ⁿ⁺,M=Co³⁺,Ni²⁺) 在主体层间以八面体配位形式存在。磁性测试结果表明过渡金属离子[(M(DETA)₂]ⁿ⁺(M=Cu²⁺,Co³⁺)的插入能引起主体MnPS₃的磁性在35~40 K发生由顺磁向亚铁磁性的转变并表现自发磁化,而客体[Ni(DETA)₂]²⁺却使夹层化合物的反铁磁相互作用增强,抑制了自发磁化的发生。     

三核钼钨簇合物的电化学性质研究

合成了四种三核钼钨簇合物(［Mo₃L］²⁺, ［Mo₂WL］²⁺, ［MoW₂L］²⁺, ［W₃L］²⁺, 其中L=［(μ₃-O)₂(μ-CH₃COO)₆(H₂O)₃］)。并研究了四种簇合物在铂电极上的电化学特性，结果表明：在0.01 mol/L簇合物的水溶液中，［Mo₃L］²⁺, ［Mo₂WL］²⁺出现两个氧化峰，两个还原峰。［W₃L］²⁺, ［W₂MoL］²⁺则出现三个氧化峰和两个还原峰，四种簇合物的电化学性质不同，主要是由于钼钨的外层电子排布不同造成的。     

类水滑石主体层板与客体CO2-3、H2O间的超分子作用

通过构建类水滑石双层计算模型, 采用混合密度泛函B3LYP/6-31G(d)//B3LYP/3-21G方法计算类水滑石(LDHs-CO3-yH2O)的结构与能量, 探讨LDHs限域空间中客体阴离子及水分子的分布形态以及主客体超分子作用. 计算结果表明, 客体阴离子与水分子以平行层板的方式存在于水滑石层间. 主客体发生作用时, CO2-3的HOMO轨道向层板的LUMO轨道转移电子. 所形成的LDHs-CO3主客体作用要强于LDHs-F以及LDHs-Cl, 与其离子交换性能相一致. 水滑石去水结构(LDHs-CO3)水合过程, 氢键作用较静电作用更占优势, 并且layer-water型氢键要强于anion-water 型氢键. 此外, 水合能计算表明LDHs水合具有一定的饱和量.     

Influence of the crystal field stabilization energy of metal(II) ions on the structural distortion of matrix-isolated SO4(2-) guest ions in selenate matrices

Infrared spectra of metal(II) selenate hydrates (MeSeO4.nH2O and Na2Me(SeO4)2.2H2O; n=6, 5, 4, 1; Me=Mg, Mn, Co, Ni, Cu, Zn, Cd) containing matrix-isolated SO42- guest ions are reported and discussed with respect to the S-O stretching modes 3 and 1. An adequate measure for the SO42- guest ion distortion is the site group splitting deltanuas (deltanuab and deltanuac in the case of a doublet and a triplet for 3, respectively; a, being the highest wavenumbered component of nu3) and deltanumax (the difference between the highest and the lowest wave numbered S-O stretching modes). It has been shown that the SO42- guest ion distortion depends on both the number of the sulfate oxygen atoms involved in coordinative bonds with the metal(II) ions and the electronic configuration of the metal(II) ions, i.e. their crystal field stabilization energy (CFSE) additionally to the site symmetry and the local potential at the lattice site of the host lattice. The SO42- guest ions matrix-isolated in MeSeO4.H2O (Me=Mn, Co, Zn) and in Na2Me(SeO4)2.2H2O (Me=Mn, Cu, Cd) exhibit three bands corresponding to the nu3 modes as deduced from the site group analysis and deltanuab approximately equal to deltanubc. When SO42- guest ions are incorporated in the triclinic Na2Me(SeO4)2.2H2O host lattices (Me=Co, Ni, Zn) the nu3 stretching region resembles a higher local symmetry of the SO42- guest ions (an approximate (A1 + E) splitting) than the crystallographic one (i.e. deltanuab>deltanubc instead of deltanuab approximately equal to deltanubc) and, hence, the ratio deltanuab/deltanubc has to be taken into account (the higher value of the ratio deltanuab/deltanubc, the weaker is the distortion of the SO42- guest ions). The SO42- guest ions incorporated in MeSeO4.nH2O (n=6, 5, 4) exhibit a higher local symmetry of the guest ions than that deduced from the site group analysis (D2d for the SO42- guest ions in MeSeO4.5H2O, MeSeO4.4H2O and in the monoclinic MeSeO4.6H2O host lattices and close to Td in the tetragonal MeSeO4.6H2O host lattices). The analysis of the infrared spectra of selenate host lattices containing SO42- guest ions reveals that the guest ions are stronger distorted when the adjacent metal(II) ions have CFSE not equal to 0. These ions are more resistant to angular deformations of the MeO6-octahedra (i.e. changes in the O-Me-O bond angles), thus facilitating the SO42- guest ion distortion as compared to those having CFSE=0 which allow stronger angular deformations of the respective metal octahedra. Infrared spectra of kieserite-type compounds MeSeO4.H2O (Me=Mn, Co, Zn) containing matrix-isolated SO42- guest ions and Me'2+ guest ions different from those of the host ions (i.e. Me'SO4.H2O in MeSeO4.H2O) are also presented and discussed (double matrix-spectroscopy).     

Laser ablation and secondary ion mass spectrometry of inorganic transition-metal compounds. Part I: comparison between static ToF-SIMS and LA-FTICRMS

Most of the first-row transition-metal oxides, M(A)O(B) (M = Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn) were examined by static secondary ion mass spectrometry (s-SIMS) and laser ablation/ionization Fourier transform ion cyclotron resonance mass spectrometry (LA-FTICRMS). Positive and negative ions show strong correlation between the studied oxide and the detected cluster ions. Specific M(x)O(y) (+/-) species were systematically observed with both MS techniques for each investigated M(A)O(B) transition-metal oxide. Moreover, the ion composition and ion distribution are greatly dependent on the ionization technique. Laser ablation (LA)/ionization leads to larger cluster ions (ionic species with nearly hundred atoms were in particular detected for Sc2O3 and Y2O3 oxides), whereas hydrogenated, dihydrogenated, and sometimes trihydrogenated species were observed in s-SIMS. However, the ion distribution for a given M(x)O(y) (+/-) ion series (i.e. ions including the same number of metal atoms M) generally presented important similarities in both techniques.Finally, it was demonstrated that the chemical state of metal atoms in the observed ionic species is closely dependent on the metal electronic valence shell. High valence states (+III, +IV, +V, and +VI) are favored for metals with a less-than-half full valence shell configuration, whereas for other first-row transition metals (manganese, iron, cobalt, nickel, copper and zinc) lower metal valence states (0, +I or, +II) are involved.     

二元类水滑石层板组成、结构与性能的理论研究

采用晶体学理论建立二元类水滑石(LDHs)微观结构模型与静电势能模型，将层板金属离子间距、层板电荷密度、层间阴离子间距等微观结构参数定量化，并将层间阴离子的静电势能表示成层板金属离子半径和物质的量之比、插层阴离子尺寸和电荷的函数。研究结果表明：LDHs层板金属离子间距应用离子紧密堆积来估算和孔径按阴离子平面六方点阵分布来计算是可行的；调变层板金属离子种类与物质的量之比影响层间阴离子的稳定性，势能计算值与文献报道的LDHs热稳定性次序一致。所以该模型可用于预测LDHs的微观结构参数以及热稳定性，为新型层状双羟基材料的定向合成提供思路。     

LDHs主体层板与卤素阴离子超分子作用的理论研究

构建了LDHs主客体作用模型, 采用混合密度泛函B3LYP方法, 在6-31G(d)水平上进行结构优化和频率分析, 然后分别用6-31G(d)和6-311++G(d, p)基组计算主客体相互作用能, 从几何参数、电荷布居、前线轨道、能量以及热力学参数等角度探讨LDHs主体层板与卤素阴离子(F?, Cl?)间的超分子作用. 计算结果表明, LDHs主体层板复合卤素阴离子是一个自发过程. LDHs主客体间存在着较强的超分子作用, 主要包括静电和氢键作用, 相互作用能分别为?592.45和?444.01 kJ·mol?1. LDHs主体层板与卤素阴离子的前线轨道发生作用, 电子容易从卤素阴离子的HOMO向层板的LUMO转移, 形成的组装产物Mg6Al(OH)14+?F?比Mg6Al(OH)14+?Cl?稳定.     

Magnetism tuned by intercalation of various metal ions in coordination polymer

Insertion of various metal ions have changed the ferromagnetic coordination frameworks into paramagnetic, superparamagnetic, or ferromagnetic. The net charge and radius of the ions determined the magnetism of the host frameworks.     

A hydrogen-bonding receptor that binds cationic monosaccharides with high affinity in methanol

A dicarboxylate host (1) binds cationic monosaccharides such as D-glucosamine HCl (2), D-galactosamine-HCl (3), and D-mannosamine-HCl (4) with high affinity (K1 = 8.0 x 10(4)-2.0 x 10(5) M(-1)) in methanol. In circular dichroism (CD) spectroscopy a positive exciton-coupling band was observed near 290 nm; this indicates that the saccharides are recognized by multiple point interactions. Since the corresponding neutral monosaccharides are not significantly bound, one may conclude that complex formation is primarily due to the electrostatic interaction between NH3+ in the guest and one carboxylate in the host and secondarily due to hydrogen-bonding interactions of OH groups with the other carboxylate and/or nitrogen bases. Molar ratio plots and Job plots indicate that host 1 and cationic monosaccharide guests form CD-active, pseudo-cyclic 1:1 complexes at low guest concentration followed by the formation of CD-silent, acyclic 1:2 1-saccharide complexes at high guest concentration. The possible binding modes are discussed in detail on the basis of molecular mechanics calculations and chemical shift changes in 1H NMR spectra. The results of competition experiments with several cationic reference compounds bearing fewer OH groups than 2-4 are consistent with the proposed binding model. Thus, the present study is a rare example of saccharide recognition in a protic solvent, where in general, hydrogen-bonding interactions are rarely useful because of strong solvation energy. These are apparently the strongest saccharide complexes involving noncovalent interactions between host and guest. We believe that the findings are significant as a milestone toward development of new saccharide recognition systems ultimately useful in aqueous solution.     

二茂金属共轭大环配体配合物的结构及性质

报道了配体Ｎ－（二茂铁基甲基）－１,４,７－氮杂－９－冠－３（Ｌ１）和Ｎ－（二茂钌基甲基）－１,４,７－氮杂－９－冠－３（Ｌ２）的Ｃｏ（Ⅲ）和Ｆｅ（Ⅲ）配合物１－４的合成及电化学性质,配合物「Ｃｏ（Ⅲ）（Ｌ１）２（ＡｃＯ）２（ＯＨ）」（ＣｌＯ４）（Ｉ）２（１）的晶体结构显示这些配合物具有线型排列的四金属中心结构,电化学研究表明：在这些配合物中,客体金属离子通过分子片断的电子传递作用使二茂金属的金属