含Br…π及Br…Br相互作用的1-溴-3，5-二(1-咪唑基-亚甲基)苯-镉(Ⅱ)配合物的合成和晶体结构

利用双齿含氮有机配体1-溴-3,5-二(1-咪唑基-亚甲基)苯(bib)与不同的镉盐反应合成了2个配合物[Cd(bib)₂(NO₃)₂] (1)和[Cd(bib)Br₂] (2)。利用元素分析及X-射线衍射单晶结构分析对其进行了表征。晶体结构表明标题化合物1晶体属于三斜晶系,P1 空间群。化合物2晶体属于单斜晶系,P2₁/c空间群。在化合物1中,一维链状结构通过Br…π相互作用连接成为二维网状结构;而化合物2的二维结构通过卤素…卤素相互作用形成一个三维结构。     

基于4-(4-咪唑基-亚甲基氨基)苯甲酸配体配合物的合成及结构

利用不同的方法由配体4-(4-咪唑基-亚甲基氨基)苯甲酸(H₂L)和过渡金属盐反应合成了3个配合物[M(HL)₂(H₂O)₂](M(Ⅱ)=Mn(Ⅱ)(1),Cd(Ⅱ)(2),Cu(Ⅱ)(3)),进行了X-射线单晶衍射等表征。晶体结构解析结果表明：配合物1~3都属于三斜晶系,P1空间群,分子之间通过丰富的氢键相互作用最终形成了三维超分子结构。并且研究了配合物的热稳定性和电化学性质。     

二维网状配合物[Co(dimb)2(MeOH)2](ClO4)2的合成及晶体结构

设计并合成了一个含咪唑基团的柔性双齿配体:1,3-二(咪唑基-1′-甲基)-5-甲基苯(dimb)(1),并进行了 ¹H NMR和结构表征。通过dimb与高氯酸钴的反应,得到了一个新型的具有二维网状结构的配合物:[Co(dimb)₂(MeOH)₂](ClO₄)₂(2)。X-射线晶体结构测定表明,这两个化合物的晶体学参数分别为:配体(1)属单斜晶系, 空间群     

咪唑-芳香多羧酸金属有机骨架化合物的合成、结构及性质

以5-(1H-咪唑)异酞酸(H₂L)为配体,在水热条件下合成了3个金属有机框架化合物:[PrL(HL)(H₂O)2]·H₂O (1),Er(H_0.5L)₂ (2)和[CoL(H₂O)2]·H₂O (3)。单晶X-射线衍射测试结果表明,3个化合物都属于单斜晶系,P2₁/c空间群。化合物1中,Pr³⁺为九配位,而化合物2和3中,Er³⁺和Co²⁺均为六配位。在镧系配合物1和2中,配体中氮原子未参与配位。1为2D折叠形结构,2为3D框架结构。在过渡金属配合物3中,氮原子与Co²⁺配位,这有助于形成平面二维结构。化合物1和3通过分子间π-π堆积,进一步形成3D结构。3个化合物均展现出较好的热稳定性。     

2-乙酰基吡啶缩噻吩-2-甲酰腙的铜和镍配合物:水热合成、晶体结构及量化计算

采用水热法制备了两种结构类似的金属配合物M(Ls)₂(M=Cu(1),Ni(2)),其中HLs是2-乙酰基吡啶缩噻吩-2-甲酰腙Schiff碱。通过元素分析、红外光谱、紫外光谱和X射线单晶衍射对它们进行了表征,结构分析表明,Ls以烯醇式与金属配位形成畸变的八面体单核配合物,化合物的分子结构被分子间弱的相互作用所稳定。配合物1通过C-H…π作用形成二维层状结构,而配合物2则通过C-H…π作用和C-H…O与C-H…N类型氢键形成三维超分子网络。     

基于4-二苯基乙酸及1,3-二(4-吡啶基)丙烷的两个银配合物的结构和荧光

以同物质的量比例的4-二苯基乙酸(Hbpa)、1,3-二(4-吡啶基)丙烷(bpp)和[Ag(NH₃)](OH),在不同反应条件下制备了2个基于柔性配体的类三明治配合物[Ag₂(bpa)₂(bpp)₂]·2H₂O_n(1)和[Ag(bpa)(bpp)]·2H₂O_n(2),对其进行了单晶结构、元素分析、红外光谱、荧光光谱和粉末衍射表征。结构表明1是由T型配位的银离子和Ag…Ag超分子作用组装而成的二维配合物;配合物2则是由四面体构型银离子和π…π堆积作用组装的二维配位超分子。此外,1和2还可在可见光区的不同位置发射较强荧光。     

4’-（3-甲氧基-4-羟基苯基）-2，2’：6’，2″-三联吡啶及其铜、锌配合物的合成、结构和性质

通过一锅反应制备了4’-（3-甲氧基-4-羟基苯基）-2,2’：6’,2″-三联吡啶（L）,通过重结晶的方法得到了其醋酸盐单晶体（HL）（CH₃COO）（1）,并以L为配体组装了过渡金属配合物[Cu（NO₃）（CH₃OH）L]（NO₃）（2）和[Zn（NO₃）₂L]（C₂H₅OH）（3）,通过元素分析、IR光谱和单晶X-射线衍射等表征了3个化合物的结构。结果表明,化合物1中,三联吡啶环呈反-反构型,而在2和3中,三联吡啶环呈现出顺-顺构型,然后采取三齿螯合模式连接金属离子形成单核单元。3个化合物中,三联吡啶分子之间以及它们与溶剂分子之间形成的氢键、π-π堆积和范德华力等相互作用将化合物1~3的单核单元连接形成三维网状结构。     

咪唑-芳香多羧酸金属有机骨架化合物的合成、结构及性质

以5-(1H-咪唑)异酞酸(H₂L)为配体,在水热条件下合成了3个金属有机框架化合物:[PrL(HL)(H₂O)₂]·H₂O(1),Er(H_0.5L)₂(2)和[CoL(H₂O)₂]·H₂O(3)。单晶X-射线衍射测试结果表明,3个化合物都属于单斜晶系,P2₁/c空间群。化合物1中,Pr³⁺为九配位,而化合物2和3中,Er³⁺和Co²⁺均为六配位。在镧系配合物1和2中,配体中氮原子未参与配位。1为2D折叠形结构,2为3D框架结构。在过渡金属配合物3中,氮原子与Co²⁺配位,这有助于形成平面二维结构。化合物1和3通过分子间π-π堆积,进一步形成3D结构。3个化合物均展现出较好的热稳定性。     

由V-型双咪唑和芳香羧酸根配体共同构筑的Zn(Ⅱ)配位聚合物的合成,结构与性能

在溶剂热条件下,将一个V-型双咪唑配体1,1'-(5-甲基-1,3-亚苯基)二(1H-咪唑)(Bim)与其它V-型辅助配体(具有不同的对称性和功能基团的芳香羧酸)一起与金属盐ZnSO₄·6H₂O进行反应,分别得到2个新的配位聚合物{[Zn(Bim)(Bra)₂]·CH₃OH}_n(1)和{[Zn(Bim)(Mpa)]·H₂O}_n(2)(Bra^-=5-溴烟酸根,Mpa^2-=5-甲基间苯二甲酸根)。采用红外光谱、元素分析、X射线粉末衍射、X射线单晶衍射和热重分析对配合物进行了表征。配合物1是由配体Bim桥联形成的一维链状结构并进一步通过链间的π…π、C-H…π和Br…π作用堆积成一个三维超分子。在2中,Zn(Ⅱ)离子通过Mpa^2-桥联形成左手和右手螺旋链,这些具有不同手性的螺旋链进一步通过Bim联接形成具有(4,4)拓扑结构的内消旋的二维层。相邻的二维层之间的交错对插、层间配体分子Bim的咪唑环和苯环的双重π…π作用最终形成了三维超分子。固态荧光测试结果表明:在室温条件下,配体Bim和配合物1~2均出现了有趣的多重发射峰,而且在配合物1中四配位的Zn(Ⅱ)离子中心能显著地敏化配体Bim的高强度发射峰。     

两个含2-(2-吡啶基)咪唑衍生物的铜(Ⅱ)配合物的合成、晶体结构及发光性质

通过自然挥发法,合成了2个配合物[Cu(DMPM)₂(Bz)][Cu(DMPM)(Bz)₃]·H₂O(1)和[Cu(PMA)Cl₂](2)(DMPM=4,5-二甲基-2-(2-吡啶基)咪唑,PMA=[2-(2-吡啶基)咪唑-1-基]乙酸乙酯,Bz=苯甲酸根),并对其荧光、热稳定性及电子自旋共振光谱进行了研究。结构分析结果表明化合物1属于三斜晶系,P1空间群;化合物2属于单斜晶系,P2₁/c空间群。化合物1通过氢键的作用形成了三维超分子框架,化合物2通过氢键作用形成了二维层状结构。     

Dinuclear Silver（Ⅰ） Complex Based on 1-Picolyl-3-propylbenzimidazolium Salt： Crystal Structure and Weak Interactions

1-Picolyl-3-propylbenzimidazolium bromide (LBr) was prepared from benzimida- zole by alkylation with 2-chloromethyl-pyridine in the presence of NaH, followed by quaternization with 1-bromopropane. Ligand LBr was treated with AgBr in CH2Cl2 to afford a dinuclear silver(I) complex L2Ag2Br4 (1). In complex 1, a 2-D supramolecular layer is formed through two types of π-π stacking interactions. Fluorescent emission spectra of ligand LBr and complex 1 are described.     

基于1-(1′，3′-苯并噁唑-2′-甲基)苯并咪唑的钴(Ⅱ)配合物：晶体结构、弱相互作用和荧光发射光谱

配体1-(1′,3′-苯并恶唑-2′-甲基)苯并咪唑(L)是通过苯并咪唑与2-(氯甲基)-1,3-苯并恶唑烷基化制备而来。配体L与CoCl2.2H2O反应得到了配合物[CoCl2L2](1)。配合物1通过π-π堆积作用和C-H…Cl氢键形成了三维超分子框架结构。测定了L和1的荧光发射光谱。     

吲哚乙酸及邻菲啰啉的锌(Ⅱ)配合物的晶体结构及荧光性质

利用3-吲哚乙酸(IAA)、邻菲啰啉(o-phen)和氯化锌在水-乙醇体系合成了一种金属配合物[Zn(IAA)2(o-phen)](1),并对其进行了X-射线单晶衍射分析、热重分析、元素分析、红外光谱、紫外光谱、荧光光谱表征。结构分析表明,该配合物中,锌离子处于四配位的四面体构型中,分别与2个IAA阴离子的羧基氧原子及1个邻菲啰啉的2个氮原子配位。通过超分子作用力:氢键和面对面式的π…π堆积作用力的自组装作用使这些分子形成二维的超分子层结构,继而这些层层间通过边对面式的π…π堆积作用力进一步的组装成三维的超分子结构。热重分析显示,该配合物具有较高的热稳定性。配合物的液态及固体荧光性质研究表明,此配合物具有一定荧光性质。     

New N-heterocyclic carbene mercury(II) and silver(I) complexes

The complexes [1-(9-anthracenylmethyl)-3-octylimy]₂Hg[HgCl₄] (2a) (imy = imidazol-2-ylidene) and [1-(9-anthracenylmethyl)-3-butylbimy]₂AgPF₆ (2b) (bimy = benzimidazol-2-ylidene) have been prepared and characterized. Crystal packing of complex 2a revealed that 1D polymeric chains are formed by [1-(9-anthracenylmethyl)-3-octylimy]Hg and [HgCl₄]²⁻ through weak Hg…Cl bonds. The packing diagram of 2b showed that 1D supramolecular chains are formed by both benzimidazole ring head to tail π–π stacking interactions and anthracene ring face-to-face π–π stacking interactions.     

A New Cobalt(Ⅱ)Polymer Based on 1-Butylben-zimidazole and Terephthalate Mixed-ligands:Crystal Structure and Weak Interactions

<正>A new cobalt(Ⅱ)polymer with quasi-rectangular cavities,[Co(L)_2(TP)·H_2O]_n 1(L =1-butylbenzimidazole,TP=terephthalate ion)has been prepared by means of self-assembly of 1-butylbenzimidazole,terephthalic acid and Co(NO_3)_2·6H_2O.The structure of 1 was characterized by X-ray diffraction analysis.In the crystal packing,2-D supramolecular layers are formed viaπ-πstacking interactions.The fluorescence emission spectra of L and 1 are described.     

Synthesis and Crystal Structure of a Coordination Polymer [Zn（p-pdoa）（bbp）]n with a One-dimensional Helical Chain

The coordination polymer [Zn（p-pdoa）4（bbp）]n 1 （p-pdoa = p-phenylenedioxydiacetate dianion and bbp = 2,6-bis（benzimidazol-2-yl）pyridine） has been synthesized by hydrothermal method and characterized by elemental analysis, IR and X-ray single-crystal diffraction. The title complex crystallizes in the triclinic system, space group P1^- with a = 7.8383（2）, b = 12.6610（4）, c = 13.1792（5）A, a = 84.433（2）,β = 74.2980（1）, γ = 87.4290（1）°, V = 1252.93（7）A^3, Z = 2, Dc = 1.593 g/cm^3,/z = 1.038 mm^-1, F（000） = 616, the final R = 0.0361 and wR = 0.1139. The Zn（Ⅱ） atom assumes a distorted trigonal bipyramidal geometry, involving two carboxyl O atoms from two different p-pdoa ligands and three N atoms from the bbp ligand. The Zn（Ⅱ） atom is alternately interlinked by p-pdoa ligands in a bismonodentate mode into a helical chain with a long pitch of 12.661 A and the adjacent Zn…Zn distance of 11.056 and 12.245 A. There exists a 2D supramolecular framework linked by π-π stacking （3.312 A） between adjacent benzimidazoles of bbp ligands and intermolecular hydrogen-bonding interactions between the uncoordinated carboxylate oxygen atoms （O（2）, 0（5）） and the uncoordinated imidazolyl N atoms （N…O distances 2.706 and 2.786 A）. There also exist two interlayer π-π stacking interactions of 3.299 A between adjacent central pyridines of bbp ligand and 3.176 A between the phenyl groups of p-pdoa ligand. Such π-π stacking interactions extend the two-dimensional layers into a 3D supramolecular network.     

Preparation,Structure and Properties of 3D Supramolecular Architecture,on the Basis of Hydrogen Bonds and π-π Stacking Between 2D Layers,with Windmill Building Blocks

A novel three-dimensional（3D） supramolecular architecture, {[Nd（OH-BDC）（OH-HBDC）（H2O）2]·2HaO）n（1） （OH-H2BDC=5-hydroxyisophthalic acid）, which was formed through hydrogen bonds and π-π stacking between two-dimensional（2D） layers, was hydrothermally synthesized and characterized by single-crystal X-ray diffraction. Windmill building blocks, which consist of two nine-coordinated metal centers and four OH-H2BDC groups are connected through two carboxyl groups, to lead to a one-dimensional infinite inorganic chain（… M--O--C--O--M…） along the [100] direction. An observed intense blue luminescence with an emission band peaked at 390 nm for compound 1 may results from ligand-to-metal charge transfer（LMCT）. Variable-temperature magnetic susceptibility of compound 1 was investigated and the value was deviated from the Curie-Weiss law.     

Luminescence enhancement and tuning via multiple cooperative supramolecular interactions in an ion-paired multinuclear complex

[(3,5-(CF(3))(2)Pz)(AgL)(2)](+)[Ag(5)(3,5-(CF(3))(2)Pz)(6)(CH(3)CN)](-) (L = 2-(N,N-diethylanilino-4-yl)-4,6-bis(3,5-dimethylpyrazol-1-yl)-1,3,5-triazine) shows bright and tunable emissions influenced by its supramolecular structure. Columnar stacks are assembled via cooperative interactions that include Ag(I)···Ag(I) argentophilic bonding, π···π stacking and Ag(I)···π interactions.     

Synthesis, structures, and magnetic properties of transition metal compounds with 2,2'-dinitrobiphenyl-4,4'-dicarboxylate and N,N'-chelating ligands

Solvothermal reactions of Co(II), Ni(II), Zn(II) salts with 2,2'-dinitrobiphenyl-4,4'-dicarboxylate (dnpdc) and 2,2'-bipyridyl-like chelating ligands yielded five compounds formulated as [Co(dnpdc)(bipy)](n)·nH(2)O (1), [M(dnpdc)(phen)](n) (2, M = Co; 3, M = Ni; 4, M = Zn) and [Co(dnpdc)(biql)](n)·2nH(2)O (5) (bipy = 2,2'-bipyridine, phen = 1,10-phenanthroline and biql = 2,2'-biquinoline). With bipy or phen as coligands, compounds 1-4 exhibit isomorphous 3D M(dnpdc) metal-organic frameworks in which double carboxylate bridged chains are interlinked by the backbones of the dicarboxylate ligands. The bipy or phen ligands are involved in interchain hydrogen bonding or π-π interactions to form 1D zipper-like arrays in the rhombic channels of the frameworks, playing a templating role and determining the channel dimensions. The biql coligand is too bulky for the 1D double carboxylate bridged chain and the rhombic channel. Instead, in compound 5, the dnpdc ligands link metal ions into 1D zigzag metal-organic chains and the biql ligands are arranged into 2D (6,3) arrays through extensive π-π stacking interactions. In compounds 1-3, the double carboxylate bridges in the nonplanar syn-skew conformation mediate ferromagnetic interactions along the chains, while the chelating ligands provide supramolecular pathways for interchain antiferromagnetic interactions. The π-π interactions in 5 also evoke weak antiferromagnetic interactions.     

Constructing single-chain magnets by supramolecular π-π stacking and spin canting: a case study on manganese(III) corroles

A single‐chain magnet (SCM) was constructed from manganese(III) 5,10,15‐tris(pentafluorophenyl)corrole complex [Mn^III(tpfc)] through supramolecular π–π stacking without bridging ligands. In the crystal structures, [Mn(tpfc)] molecules crystallized from different solvents, such as methanol, ethyl acetate, and ethanol, exhibit different molecular orientations and intermolecular π–π interaction or weak Mn ??? O interaction to form a supramolecular one‐dimensional motif or dimer. These three complexes show very different magnetic behaviors at low temperature. Methanol solvate 1 shows obvious frequency dependence of out‐of‐phase alternating‐current magnetic susceptibility below 2 K and a magnetization hysteresis loop with a coercive field of 400 Oe at 0.5 K. It is the first example of spin‐canted supramolecular single‐chain magnet due to weak π–π stacking interaction. By fitting the susceptibility data χ_MT (20–300 K) of 1 with the spin Hamiltonian expression ${\overrightarrow{H}}A single-chain magnet (SCM) was constructed from manganese(III) 5,10,15-tris(pentafluorophenyl)corrole complex [Mn(III) (tpfc)] through supramolecular π-π stacking without bridging ligands. In the crystal structures, [Mn(tpfc)] molecules crystallized from different solvents, such as methanol, ethyl acetate, and ethanol, exhibit different molecular orientations and intermolecular π-π interaction or weak Mn???O interaction to form a supramolecular one-dimensional motif or dimer. These three complexes show very different magnetic behaviors at low temperature. Methanol solvate 1 shows obvious frequency dependence of out-of-phase alternating-current magnetic susceptibility below 2?K and a magnetization hysteresis loop with a coercive field of 400?Oe at 0.5?K. It is the first example of spin-canted supramolecular single-chain magnet due to weak π-π stacking interaction. By fitting the susceptibility data χ(M) T (20-300?K) of 1 with the spin Hamiltonian expression H = -2J Σ(i=1)(n-1) S(Ai) S(Ai+1) + D Σ(i) S((iZ)(2)), the intrachain magnetic coupling parameter transmitted by π-π interaction of -0.31?cm(-1) and zero field splitting parameter D of -2.59?cm(-1) are obtained. Ethyl acetate solvate 2 behaves as an antiferromagnetic chain without ordering or slow magnetic relaxation down to 0.5?K. The magnetic susceptibility data χ(M) T (20-300?K) of 2 was fitted by assuming the spin Hamiltonian H = -2JΣ(i=1)(n-1) S(Ai) S(Ai+1), and the intrachain antiferromagnetic coupling constant of -0.07?cm(-1) is much weaker than that of 1. Ethanol solvate 3 with a dimer motif shows field-induced single-molecule magnet like behavior below 2.5?K. The exchange coupling constant J within the dimer propagated by π-π interaction is -0.14?cm(-1) by fitting the susceptibility data χ(M) T (20-300?K) with the spin Hamiltonian H = -2J S(A) S(B) + β(S((A)g(A)) + S((B)g(B)))H. The present studies open a new way to construct SCMs from anisotropic magnetic single-ion units through weak intermolecular interactions in the absence of bridging ligands.