配位聚合物[HgI_2(btx)]_n的制备、晶体结构及性能研究(btx=对二(1,2,4-三氮唑基甲基)苯)

选择具有较强配位能力的多齿有机化合物作为桥连配体,通过与过渡金属离子自组装制备具有新型骨架结构的一维、二维、三维配位聚合物,并进一步研究其电学、磁学、光学和催化等物理和化学性质[1～4],已成为当今化学学科和材料学科中最为活跃的领域之一.含有三氮唑、咪唑等基团的有机桥联配体由于其配位能力强、配位原子数目多、易与过渡金属离子形成具有特殊结构的配位聚合物等特点[5～7],引起了人们对于该类配体的极大兴趣,成为近年来配位化学的研究热点之一.例如,Richard Robson等人合成了一个含有咪唑基团的配体一对二(咪唑基甲基)苯,并使之与Ag(Ⅰ)及Zn(Ⅱ)自组装,制备出了两个具有二维多聚轮烷结构的配位聚合物[8,9].最近,我们课题组合成了一个含有三氮唑基团的有机配体对二(1,2,4-三氮唑基甲基)苯(btx),并通过分子的自组装作用,得到了一例新的一维锯齿状的配位聚合物[HgI2(btx)]n.本文报导了该配位聚合物的晶体结构和室温下固体化合物的荧光性质,并通过元素分析、红外光谱和热分析对其进行了表征.     

[Cu3(μ10-bta)(μ2-C2O4)(H2O)2]n的水热合成与结构表征

有机-无机杂化材料因其在催化、化学吸附、磁性和电子导体等方面具有广泛的应用而成为人们的研究热点[1,2]. 通过过渡金属离子和特殊的有机配体之间的反应, 一系列具有独特结构的配位聚合物已被合成出来. 多齿有机配体可螯合两个或多个金属离子, 这些金属离子之间存在良好的电子交换[3], 可形成一维、二维或三维的配位聚合物. 均苯三甲酸和均苯四甲酸都是良好的桥连多齿配体, Chui等采用均苯三甲酸合成了具有吸附作用的大孔道的[Cu3(tma)2(H2O)]n[4] (tma=benzene-1,3,5-tricarb-oxylate)三维配位聚合物, 并且[Ni(C12H3ON6O2)]3(tma)*H2O[5], [M(tma)2]*12H2O(M=Co,Ni,Zn)[6], Na2[Co(H2O)6(bta)]*4H2O[7] (bta=benzene-1,2,4,5-tetracarboxylate)和[Co(phen)(md)][8] (phen=1,10-phenanthroline, md=benzene-1,3-dicarboxylate)等配位聚合物也先后被合成出来.     

配位聚合物M(H_2O)_2[Ni(CN)_4]·xH_2O的合成、晶体结构及性能研究

以[Ni(CN)4]2-为构筑基元,与过渡金属离子Mn2+通过溶液缓慢扩散法合成出二维Hofmann类氰基桥联配位聚合物Mn(H2O)2[Ni(CN)4]·4H2O(1),并解析了其晶体结构.配位聚合物1属正交晶系,空间群Cmcm,晶胞参数a=0.73080(5)nm,b=1.21372(8)nm,c=1.40875(9)nm,α=β=γ=90°,Ni和Mn中心通过氰桥交互连接构成二维波浪形层状结构.通过混合法得到系列Hofmann类配位聚合物M(H2O)2[Ni(CN)4]·xH2O(M=Mn,Fe,Co,Ni,Cd)的粉末样品,粉末XRD结果表明,系列配位聚合物具有与1相同的晶体结构;变温粉末XRD和热重分析结果表明,系列配位聚合物具有较高的热稳定性.以Mn(H2O)2[Ni(CN)4]·xH2O的脱水样品为构筑模块与柱状配体pyrazine组装构筑的三维多孔配位聚合物具有一定的储气性能.     

甲酸及联吡啶配体构筑的三维网状镍(Ⅱ)/钴(Ⅱ)配位聚合物的合成及晶体结构(英文)

通过水热法合成两个混配的配位聚合物[M(bipy)(Metha)2]n·nH2O(M=Ni,1;Co,2;bipy=4,4′-联吡啶;Metha=甲酸),并对配合物进行了元素分析、红外光谱和X-射线单晶衍射测定。结果表明,2个配合物为单斜晶系,C2/c空间群。配合物1和2具有相似的三维网状结构。配体Metha以2种不同的类型与M2+离子配位,一种是Metha中的2个氧原子作为桥联配位原子,连接着由bipy作为双基配体连接2个不同的金属离子构成的链,另一个Metha中的羧基氧只有1个氧原子与金属离子配位,使配合物构成三维结构。     

新型三维配位聚合物[Fe(C_5H_4NCOO)_2]_n的可控合成、晶体结构和UV-VIS-NIR反射光谱研究

近年来，金属有机配位聚合物由于其独特的电学、磁学、催化和光学性能而受 到普遍关注。通过选择不同的多齿配体和金属离子，可以组装成具有各处新型骨架 结构和特殊物理化学性能的配位聚合物。异烟酸根可以通过吡啶环氮原子和羧基氧 原子与金属离子配位，生成配位聚合物。本文采用三氯化铁和4-氰基吡啶在水热条 件下的反应可控地合成具有三维骨架结构的配位聚合物[Fe(C_5H_4NCOO)_2]_n，并 进行元素分析、红外光谱表征，单晶结构测定和UV-VIS-NIR（紫外-可见-近红外） 反射光谱研究。     

基于4H-1,2,4-三氮唑-4-乙酸配体的两个新的过渡金属配位聚合物的合成、结构与性质(英文)

用水热方法合成了两个新的配位聚合物[Co(trza)](1)和[Ni(trza)(H2O)2](2)(Htrza=4H-1,2,4-三氮唑-4-乙酸).单晶X-射线衍射结构分析表明:化合物1和2具有二维(2D)层状结构.在1中,Co(II)离子采用六配位方式,分别与来自两个不同配体(trza)上的两个氮原子和四个羧基氧原子配位,形成八面体配位聚合物,每个羧基以二齿桥联方式连接两个Co原子,形成1D链,这些一维链进一步与唑环上的N原子形成2D层状结构.在2中,中心Ni(II)离子采用同样的配位模式形成八面体配位聚合物,与1不同的是:来自两个配体阴离子(trza)上的两个羧基氧原子分别被两个配位水分子所取代,且配体上的羧基氧原子采用的是单齿配位模式.化合物1的变温磁化率测定表明了金属间弱的反铁磁相互作用.此外,两个配位聚合物的IR光谱、热稳定性以及化合物1的磁性质也被测定.     

含二氢噻唑类卟啉配位聚合物自组装染料敏化太阳能电池

合成了两种不同类型(2+2型、A4型)含二氢噻唑基团的锌卟啉与Mn(Ⅱ)的配位聚合物(CPsx,x=1,2)。两种配位聚合物与锚定卟啉(ZnPA)通过金属-配体轴向配位自组装成染料敏化太阳能电池。通过电镜表征了其在TiO_2上的自组装结构。光伏性能测试表明,聚合物自组装体与单体相比具有较优的光电转换效率,特别是A4型结构(CPs2)具有较高的短路电流和转换效率。     

基于阴离子调控策略的Co(Ⅱ)配位聚合物的合成、晶体结构及荧光性质

以三键桥联吡啶类配体2,6-二(3′-吡啶乙炔基)-4-甲基苯胺(L)为配体,在常温混合溶剂(二氯甲烷-甲醇)中分别与CoCl_2、Co(SCN)2通过自组装反应,获得了一维及二维配位聚合物[Co(L)Cl_2]_n(1)及[Co(L)_2(SCN)_2]_n(2),通过红外、元素分析、X射线单晶衍射等检测手段对所合成的配合物进行了结构表征。对比1和2的单晶结构可以发现,配体L在配位聚合物1和2中的配位取向及结构相似,不同的是Co(Ⅱ)离子的配位数受配位阴离子的影响而不同:配位聚合物1中四配位的Co(Ⅱ)通过2个配体的相互连接呈现一维的弯曲链状结构,而配位聚合物2中六配位的Co(Ⅱ)则通过4个配体的相互连接得到二维的平面结构。2个配合物中均存在氢键及π-π相互作用。通过粉末衍射证明了配位聚合物1和2为单一晶相,其固态下的荧光测试显示,二者的荧光均减弱,并相对于配体L有红移(1)及蓝移(2)。     

具有氢键假想孔道结构的[M(en)3][GeF6](M=Ni,Co)的合成与表征

描述了两个具有管状氢键假想孔道结构的化合物[Ni(en)3][GeF6][JLG-1(Ni)]和[Co(en)3].[GeF6][JLG-1(Co)].在这两个结构中,[GeF6]2-阴离子与手性金属配合物阳离子[M(en)3]2+(M=Ni,Co)通过F…N之间复杂的弱氢键相互作用,在沿着63螺旋轴方向形成六方蜂窝状排布的管状氢键假想孔道.结构研究发现,配对的[GeF6]2阴离子和手性[M(en)3]2+阳离子同属于D3点群,这是JLG-1(Ni)和JLG-1(Co)形成管状氢键假想孔道的关键.这一研究成果对设计合成氢键假想孔道体系具有一定的指导意义.     

新型手性金属-有机配位聚合物的合成、结构与性质

在水热条件下, 分别用过渡金属离子Zn(Ⅱ)和Co(Ⅱ)与混合手性羧酸和含氮配体反应, 合成了2个手性金属-有机配位聚合物[M(D-cam)(H₂mbdpz)]_n[M=Zn(1), Co(2); D-H₂cam=D-(+)-樟脑酸; H₂mbdpz=4,4'-亚甲基二(3,5-二甲基吡唑)]. 通过单晶X射线衍射、粉末X射线衍射、元素分析、热重分析及荧光分析对其结构、组成和性质进行了表征. 单晶结构分析表明, 配合物1和2是异质同晶的手性三维开放骨架结构, 具有单节点三连接的ThSi₂型网络拓扑结构.     

Synthesis, structure, and multi-NMR studies of (Me4N)[A(M(SC(O)Ph)3)2] (A = Na, M = Hg; A = K, M = Cd or Hg)

The compounds (Me4N)[A(M(SC(O)Ph)3)2] (A = K, M = Cd (2); A = Na, M = Hg (3); and A = K, M = Hg (4)) were synthesized by reacting the appropriate metal chloride with A+PhC(O)S- and Me4NCl in the ratios 1:3:1 and 2:6:1. The structures of these compounds were determined by single-crystal X-ray diffraction methods. All the compounds are isomorphous, isostructural, and crystallized in the space group P1 with Z = 1. Single-crystal data for 2: a = 106670(2) A, b = 111522(2) A, c = 119294(2) A, alpha = 71782(1) degrees, beta = 85208(1) degrees, gamma = 69418(1) degrees, V = 126140(4) A3, Dcalc = 1528 g cm-3. Single-crystal data for 3: a = 10840(2) A, b = 10946(4) A, c = 12006(3) A, alpha = 7218(2) degrees, beta = 8675(2) degrees, gamma = 6743(2) degrees, V = 12493(6) A3, Dcalc = 1756 g cm-3. Single-crystal data for 4: a = 104780(1) A, b = 112563(2) A, c = 119827(2) A, alpha = 71574(1) degrees, beta = 85084(1) degrees, gamma = 70705(1) degrees, V = 126523(3) A3, Dcalc = 1755 g cm-3. In the [A(M(SC(O)Ph)3)2]- anions, each M(II) atom is bonded to three thiobenzoate ligands through sulfur atoms, giving a trigonal planar MS3 geometry. The carbonyl oxygen atoms from the two [M(SC(O)Ph)3]- anions are bonded to the alkali metal atom, providing an octahedral environment. Solution metal NMR studies showed the concentration-dependent dissociation of the alkali metal ions in the trinuclear anions.     

钛,锆和铪羰基化合物M(CO)_n(M=Ti,Zr,Hf;n=4～7)的理论研究

利用密度泛函方法对标题化合物的平衡几何、热化学及振动频率进行了理论预测,发现这3种金属原子都有相似的M(CO)n(n=4～7)结构.全局最低构型对M(CO)7都是单态C3v戴帽八面体7S-1,对M(CO)6都是三重态D3d畸变八面体6T(而对应的单重态M(CO)5仅比它低不到21 kJ·mol-1).对M(CO)n(n=5,4)都是三重态6S-1,其构型分别为从6T中移去1个或2个CO基的衍生物5T和4T.此外,五重态的D3h的三角双锥M(CO)5和单态的Td四面体M(CO)4以及能量更高的含有C和O同时与金属成键的独特配位CO基的M(CO)6和M(CO)3也被发现.最后,给出M(CO)7→M(CO)6+CO反应的离解能.并讨论了金属18价电子的Ti(CO)7存在的可能性.     

Theoretical study of M(+)-RG complexes (M = Ga, In; RG = He-Rn)

We present potential energy curves calculated at the CCSD(T) level of theory for Ga(+)-RG and In(+)-RG complexes (RG = He-Rn). Spectroscopic parameters have been derived from these potentials and compared to previously calculated parameters for the Al(+)-RG and Tl(+)-RG complexes. Additionally, for some cases, we compare these parameters with those obtained from electronic spectroscopic studies on excited states of the neutral species, arising from atomic-based d ← p excitations. The Ga(+)-RG and In(+)-RG potentials have also been used to calculate the transport coefficients for M(+) traveling through a bath of RG atoms.     

Synthesis and characterization of (smif)2M(n) (n = 0, M = V, Cr, Mn, Fe, Co, Ni, Ru; n = +1, M = Cr, Mn, Co, Rh, Ir; smif =1,3-di-(2-pyridyl)-2-azaallyl)

A series of Werner complexes featuring the tridentate ligand smif, that is, 1,3-di-(2-pyridyl)-2-azaallyl, have been prepared. Syntheses of (smif)(2)M (1-M; M = Cr, Fe) were accomplished via treatment of M(NSiMe(3))(2)(THF)(n) (M = Cr, n = 2; Fe, n = 1) with 2 equiv of (smif)H (1,3-di-(2-pyridyl)-2-azapropene); ortho-methylated ((o)Mesmif)(2)Fe (2-Fe) and ((o)Me(2)smif)(2)Fe (3-Fe) were similarly prepared. Metatheses of MX(2) variants with 2 equiv of Li(smif) or Na(smif) generated 1-M (M = Cr, Mn, Fe, Co, Ni, Zn, Ru). Metathesis of VCl(3)(THF)(3) with 2 Li(smif) with a reducing equiv of Na/Hg present afforded 1-V, while 2 Na(smif) and IrCl(3)(THF)(3) in the presence of NaBPh(4) gave [(smif)(2)Ir]BPh(4) (1(+)-Ir). Electrochemical experiments led to the oxidation of 1-M (M = Cr, Mn, Co) by AgOTf to produce [(smif)(2)M]OTf (1(+)-M), and treatment of Rh(2)(O(2)CCF(3))(4) with 4 equiv Na(smif) and 2 AgOTf gave 1(+)-Rh. Characterizations by NMR, EPR, and UV-vis spectroscopies, SQUID magnetometry, X-ray crystallography, and DFT calculations are presented. Intraligand (IL) transitions derived from promotion of electrons from the unique CNC(nb) (nonbonding) orbitals of the smif backbone to ligand π*-type orbitals are intense (ε ≈ 10,000-60,000 M(-1)cm(-1)), dominate the UV-visible spectra, and give crystals a metallic-looking appearance. High energy K-edge spectroscopy was used to show that the smif in 1-Cr is redox noninnocent, and its electron configuration is best described as (smif(-))(smif(2-))Cr(III); an unusual S = 1 EPR spectrum (X-band) was obtained for 1-Cr.     

六聚同多酸阴离子M6On-19(M=Mo,W,n=2;M=Nb,Ta,n=8)电子结构和化学性质的密度泛函理论研究

采用B3LYP方法在Lanl2DZ水平上计算了六聚同多阴离子(M6On19^-(M=Mo和W，n=2；M=Nb和Ta，n=8)的电子结构，分析了它们的前线轨道、分子静电势(MEP)．计算结果表明，Nb6O19^8-和Ta6O19^8-是电子给体，而Nb6O19^2-和Ta6O19^2-则是电子受体，这与它们在溶液中具有不同的化学性质是一致的．     

Endohedral and Exohedral Metalloborospherenes: M@B40 (M=Ca,Sr) and M&B40 (M=Be,Mg)

The recent discovery of the all‐boron fullerenes or borospherenes, D_2d B₄₀^−/0, paves the way for borospherene chemistry. Here we report a density functional theory study on the viability of metalloborospherenes: endohedral M@B₄₀ (M=Ca, Sr) and exohedral M&B₄₀ (M=Be, Mg). Extensive global structural searches indicate that Ca@B₄₀ ( 1 , C_2v, ¹A₁) and Sr@B₄₀ ( 3 , D_2d, ¹A₁) possess almost perfect endohedral borospherene structures with a metal atom at the center, while Be&B₄₀ ( 5 , C_s, ¹A′) and Mg&B₄₀ ( 7 , C_s, ¹A′) favor exohedral borospherene geometries with a η⁷‐M atom face‐capping a heptagon on the waist. Metalloborospherenes provide indirect evidence for the robustness of the borospherene structural motif. The metalloborospherenes are characterized as charge‐transfer complexes (M²⁺B₄₀²⁻), where an alkaline earth metal atom donates two electrons to the B₄₀ cage. The high stability of endohedral Ca@B₄₀ ( 1 ) and Sr@B₄₀ ( 3 ) is due to the match in size between the host cage and the dopant. Bonding analyses indicate that all 122 valence electrons in the systems are delocalized as σ or π bonds, being distributed evenly on the cage surface, akin to the D_2d B₄₀ borospherene.     

噻吩在M(111)(M=Pd,Pt, Au)表面的吸附

采用密度泛函理论(DFT), 选取DMol³程序模块, 对噻吩在M(111) (M=Pd, Pt, Au)表面上的吸附行为进行了探讨. 通过对噻吩在不同底物金属上的吸附能、吸附构型、Mulliken 电荷布居、差分电荷密度以及态密度的分析发现, 噻吩在Pd(111)面上的吸附能最大, Pt(111)面次之, Au(111)面最小. 吸附后, 噻吩在Au(111)面上的构型几乎保持不变, 最终通过S端倾斜吸附于top 位; 噻吩在Pd(111)及Pt(111)面上发生了折叠与变形, 环中氢原子向上翘起, 最终通过环平面平行吸附于hollow 位. 此外, 噻吩环吸附后芳香性遭到了破坏, 环中碳原子发生sp³杂化, 同时电子逐渐由噻吩向M(111)面发生转移, M(111)面上的部分电子也反馈给了噻吩环中的空轨道, 这种协同作用最终导致了噻吩分子稳定吸附于M(111)面.     

Endohedral and Exohedral Metalloborospherenes: M@B40 (M=Ca,Sr) and M&B40 (M=Be,Mg)

The recent discovery of the all‐boron fullerenes or borospherenes, D_2d B₄₀^?/0, paves the way for borospherene chemistry. Here we report a density functional theory study on the viability of metalloborospherenes: endohedral M@B₄₀ (M=Ca, Sr) and exohedral M&B₄₀ (M=Be, Mg). Extensive global structural searches indicate that Ca@B₄₀ ( 1 , C_2v, ¹A₁) and Sr@B₄₀ ( 3 , D_2d, ¹A₁) possess almost perfect endohedral borospherene structures with a metal atom at the center, while Be&B₄₀ ( 5 , C_s, ¹A′) and Mg&B₄₀ ( 7 , C_s, ¹A′) favor exohedral borospherene geometries with a η⁷‐M atom face‐capping a heptagon on the waist. Metalloborospherenes provide indirect evidence for the robustness of the borospherene structural motif. The metalloborospherenes are characterized as charge‐transfer complexes (M²⁺B₄₀^2?), where an alkaline earth metal atom donates two electrons to the B₄₀ cage. The high stability of endohedral Ca@B₄₀ ( 1 ) and Sr@B₄₀ ( 3 ) is due to the match in size between the host cage and the dopant. Bonding analyses indicate that all 122 valence electrons in the systems are delocalized as σ or π bonds, being distributed evenly on the cage surface, akin to the D_2d B₄₀ borospherene.     

噻吩在M(111)(M=Pd,Pt,Au)表面的吸附(英文)

采用密度泛函理论(DFT),选取DMol3程序模块,对噻吩在M(111)(M=Pd,Pt,Au)表面上的吸附行为进行了探讨.通过对噻吩在不同底物金属上的吸附能、吸附构型、Mulliken电荷布居、差分电荷密度以及态密度的分析发现,噻吩在Pd(111)面上的吸附能最大,Pt(111)面次之,Au(111)面最小.吸附后,噻吩在Au(111)面上的构型几乎保持不变,最终通过S端倾斜吸附于top位;噻吩在Pd(111)及Pt(111)面上发生了折叠与变形,环中氢原子向上翘起,最终通过环平面平行吸附于hollow位.此外,噻吩环吸附后芳香性遭到了破坏,环中碳原子发生sp3杂化,同时电子逐渐由噻吩向M(111)面发生转移,M(111)面上的部分电子也反馈给了噻吩环中的空轨道,这种协同作用最终导致了噻吩分子稳定吸附于M(111)面.     

Structure determination and relative properties of novel cubic borates MM'4(BO3)3 (M = Li, M' = Sr; M = Na, M' = Sr, Ba)

A series of novel borates, MM'4(BO3)3 (M = Li, M' = Sr; M = Na, M' = Sr, Ba), have been successfully synthesized by standard solid-state reaction. The crystal structures have been determined from powder X-ray diffraction data. They crystallize in the cubic space group Iad with large lattice parameters: a = 14.95066(5) A for LiSr4(BO3)3, a = 15.14629(6) A for NaSr4(BO3)3, and a = 15.80719(8) A for NaBa4(BO3)3. The structure was built up from 64 small cubic grids, in which the M' atoms took up the corner angle and the BO3 triangles or MO6 cubic octahedra filled in the interspaces. The isolated [BO3]3- anionic groups are perpendicular to each other, distributed along three 100 directions. The anisotropic polarizations were counteracting, forming an isotropic crystal. Sr and Ba atoms were found to be completely soluble in the solid solution NaSr(4-)xBax(BO3)3 (0 < or = x < or = 4). The photoluminescence of samples doped with the ions Eu2+ and Eu3+ was studied, and effective yellow and red emission was detected, respectively. The results are consistent with the crystallographic study. The DTA and TGA curves of them show that they are chemically stable and congruent melting compounds.