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.     

一维双链4-氧-1(4H)-吡啶氮乙酸桥联铜配位聚合物[Cu(4-OPA)2]n的合成、结构及性能研究

A novel coordination polymer of [Cu(4-OPA)₂]_n (4-OPA^-=4-oxo-1(4H)-pyridineacetate anion) was synthesized and characterized by elemental analysis, IR, TG, fluorescence and X-ray single crystal diffraction. The title complex crystallizes in triclinic with space group P1, a=0.713 17(14) nm, b=0.739 81(15) nm, c=0.753 02(15) nm, α=91.46(3)°, β=109.14(3)°, γ=111.31(3)°. V=0.344 92(17) nm³, Z=1, R=0.028 6, wR=0.080 3. The Cu atom occupies an inversion site in an octahedral environment, defined by two carbonyl O atoms and four carboxyl O atoms from different 4-OPA^- ligands. Adjacent Cu(Ⅱ) atoms are bridged by the 4-OPA^- ligands, forming a one-dimensional double chain structure. The closest Cu…Cu distance is 0.850 6(3) nm. The results of TG and fluorescent analysis show that the title coordination polymer is stable under 262.8 ℃ and has two emission peaks at 422 and 484 nm. CCDC: 287038.     

Anomalous Freezing of Nano‐Confined Water in Room‐Temperature Ionic Liquid 1‐Butyl‐3‐Methylimidazolium Nitrate

Non‐crystal formation of ice is investigated by simultaneous X‐ray diffraction and differential scanning calorimetry measurements upon cooling to ?100 °C. At room temperature, size‐tunable water confinement (≈20 Å size) in a room‐temperature ionic liquid (RTIL, 1‐butyl‐3‐methylimidazolium nitrate, [C₄mim][NO₃]) exists in a water‐rich region (70–90 mol % D₂O). The confined water (water pocket) is characterized by almost monodispersive size distribution. In [C₄mim][NO₃]‐x mol % D₂O (70<x<94), the absence of sharp Bragg reflections and a distinct exothermal peak indicate that crystallization/cold crystallization both of [C₄mim][NO₃] and D₂O is suppressed, even upon slow cooling and heating.     

Synthesis,Crystal Structure,and Magnetic Properties of a New 2D Twofold Interpenetrated Coordination Polymer [Cu(3,4‐pybz)2]n

A new coordination polymer, [Cu(3, 4‐pybz)₂]_n ( 1 ) [3,4‐Hpybz = 3‐pyridin‐4‐yl‐benzoic acid], was synthesized by hydrothermal reaction of CuCl₂ · 2H₂O and 3,4‐Hpybz, and characterized by elemental analysis, IR spectroscopy, PXRD, and single‐crystal X‐ray diffraction. The structure determination reveals that 1 exhibits a 2D twofold interpenetrated 4‐connected (4,4) network topology, these 2D layers are further enlarged to form the final 3D supramolecular edifice via aromatic π–π stacking interactions. In addition, the magnetic behavior and thermogravimetric analysis of 1 were also studied.     

1‐Butyl‐3‐methylimidazolium Hydrogen Sulfate [Bmim]HSO4: An Efficient Reusable Acidic Ionic Liquid for the Synthesis of 1,8‐Dioxo‐Octahydroxanthenes

1‐Butyl‐3‐methylimidazolium hydrogen sulfate [bmim]HSO₄ as an acidic ionic liquid was prepared and used as a catalyst for the synthesis of 1,8‐dioxo‐octahydroxanthenes in excellent yields and short reaction times at 80 °C. The ionic liquid was easily separated from the reaction mixture by water extraction and was recycled four times without any loss in activity.     

Crystal Structures and Melting Behaviors of 2D and 3D Anionic Coordination Polymers Containing Organometallic Ionic Liquid Components

Although coordination polymers generally do not melt, several that do melt have been synthesized recently and have drawn much attention. In this study, two- and three-dimensional coordination polymers that melt were synthesized, [Ru(Cp)(C₆H₅R)][M{C(CN)₃}₂] (R=H, Me, Et; M=K, Rb; Cp=C₅H₅), which are complex salts comprising M[C(CN)₃] and organometallic ionic liquids [Ru(Cp)(C₆H₅R)][C(CN)₃]. They have anionic [M{C(CN)₃}₂]_n⁻ coordination polymer frameworks, whose dimensionalities depend on the size of the organometallic cation inside. Their melting points decreased with increasing cation substituent length and size of the alkali metal ion (T_m=102–239 °C), and these low-melting-point coordination polymers exhibited incongruent melting, forming mixtures of solid M[C(CN)₃] and ionic liquid upon melting. Using the same method, coordination polymers were synthesized with various bridging ligands, [Co(Cp)₂][MX₂] (X=B(CN)₄, C(CN)₃, N(CN)₂; M=K, Na), as well as a paramagnetic coordination polymer, [Fe(Cp)₂][K{C(CN)₃}₂].     

配位聚合物[HgI2(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)

A novel one-dimension coordination polymer [HgI₂(btx)]_n was synthesized through the reaction of alpha, alpha’-dichloro-p-xylene and HgI₂ in mixed MeOH-THF (1∶1) solution. The compound was characterized by X-ray crystallography and crystallizes in orthorhombic with space group Pnma. The cell parameters of the title compound are: a=0.936 3(2) nm, b=1.769 4(4) nm, c=1.032 2(2) nm, α=90°. Attractive I…I interactions link HgI₂(btx) chains directly resulting in the formation of three-dimensional network structure. In addition, the compound shows better luminescence spectroscopic property in the solid state, and is thermally stable below 126 ℃. CCDC: 233053.     

两个含有平行交替链的新型二氰胺配位高聚物: {Mn(dmpz)[N(CN)2]2}2和{Cu(dmpz)[N(CN)2]2}2

Two new dicyanamide coordination polymers, {Mn(dmpz)[N(CN)2]2}2 (1) and {Cu(dmpz)[N(CN)2]2}2 (2)(dmpz=3,5-dimethylpyrazole), were synthesized and characterized by single crystal X-ray diffraction analysis and IR spectroscopy. In 1 and 2 the metal ions have two different coordination modes, where one is coordinated to four dicyanamide anions and two monodentate dmpz molecules to form a slightly distorted octahedral geometry, while the other adopts octahedral geometry, surrounded by four nitrile N atoms and two amide N atoms of the dicyanamide anions. Both complexes contain two alternating chains that are parallel to each other.     

Encapsulated Ionic Liquids for CO2 Capture: Using 1‐Butyl‐methylimidazolium Acetate for Quick and Reversible CO2 Chemical Absorption.

The potential advantages of applying encapsulated ionic liquid (ENIL) to CO₂ capture by chemical absorption with 1‐butyl‐3‐methylimidazolium acetate [bmim][acetate] are evaluated. The [bmim][acetate]‐ENIL is a particle material with solid appearance and 70 % w/w in ionic liquid (IL). The performance of this material as CO₂ sorbent was evaluated by gravimetric and fixed‐bed sorption experiments at different temperatures and CO₂ partial pressures. ENIL maintains the favourable thermodynamic properties of the neat IL regarding CO₂ absorption. Remarkably, a drastic increase of CO₂ sorption rates was achieved using ENIL, related to much higher contact area after discretization. In addition, experiments demonstrate reversibility of the chemical reaction and the efficient ENIL regeneration, mainly hindered by the unfavourable transport properties. The common drawback of ILs as CO₂ chemical absorbents (low absorption rate and difficulties in solvent regeneration) are overcome by using ENIL systems.     

Copper(I) and Silver(I) Bis(trifluoromethanesulfonyl)imide and Their Interaction with an Arene,Diverse Olefins,and an NTf2−‐Based Ionic Liquid

The chemistry of coinage metal bis(triflyl)imides of technological interest, CuNTf₂ and AgNTf₂, their synthesis and complexes with excess of comparatively weakly coordinating NTf₂^? as well as with ether, olefins, and the arene mesitylene are described. The existence of the solvent‐free pure phase [CuNTf₂]_∞ has not been evidenced so far. Contrary to the literature, in which the preparation of [CuNTf₂]_∞ is supposed to be carried out by reacting mesityl copper, [Cu(Mes)]₅, and HNTf₂, we found that in fact this reaction leads reproducibly to the interesting copper diarene sandwich complex [Cu(η³‐MesH)₂][Cu(NTf₂)₂] ( 1 ) (MesH=1,3,5‐trimethylbenzene). The unexpectedly stable molecular etherate [Cu(Et₂O)(NTf₂)] ( 2 ) turned out to be the best precursor for CuNTf₂ having only an inert and easily exchangeable solvent ligand. The coordination mode of NTf₂^? in 1 and 2 as well as in the hitherto unknown crystalline phase of [AgNTf₂]_∞ ( 3 ) is described. The complex formation, which takes place when dissolving 2 or 3 in the room temperature ionic liquid (RTIL) [emim]NTf₂ ([emim]⁺=1‐ethyl‐3‐methylimidazolium), has been studied. Furthermore, the reaction of 1 – 3 towards the diolefins 1,5‐cyclooctadiene (COD), 2,5‐norbornadiene (NBD) and isoprene (2‐methylbuta‐1,3‐diene) and towards ethylene has been investigated. The products 4 – 13 of these conversions have been isolated and fully characterized by NMR‐ and IR spectroscopies, mass spectrometry, and elemental‐ and XRD analyses. The potential of [Cu(η³‐MesH)₂][Cu(NTf₂)₂] ( 1 ), [Cu(Et₂O)(NTf₂)] ( 2 ) and [AgNTf₂]_∞ ( 3 ) as well as of [emim][M(NTf₂)₂] (M=Cu 4 , Ag 5 ) as chemisorbers for ethylene was studied by NMR spectroscopy.     

以甲酸为配体的无限三维配位聚合物[Zn(HCOO)2(H2O)2]∞的水热合成和热分析

The coordination polymer [Zn（HCOO）2（H2O）2]∞ has been synthesized using hydrothermal method and characterized by X-ray single crystal diffraction, elemental analysis, FTIR spectroscopy and TG-DTG analyses. The coordination polymer crystallizes in monoclinic, P21/c space group with crystal parameters of α=0.8688（1） nm, b= 0.7143（6） nm, c=0.9305（2） nm, β=97.61（5）°, V=0.5724（2） nm^3, Z=4, μ（Mo Kα）=42.50 cm^-1. The polymer features with two kinds of zinc centers： one is hexa-coordinated by four water ligands, two oxygen atoms of two formates and the other is coordinated by six oxygen atoms of six formates. By the formates as space linkers, three-dimensional frameworks were formed. Based on thermal analyses, thermal decomposition mechanisms were predicted that at the first step the polymer lost two coordination water molecules and at the second step lost two formates companied by the formation of some kinds of materials.     

Electrodeposition and Magnetic Characterization of Iron and Iron–Silicon Alloys from the Ionic Liquid 1‐Butyl‐1‐methylpyrrolidinium Trifluoromethylsulfonate

The electrodeposition of soft magnetic iron and iron–silicon alloys for magnetic measurements is presented. The preparation of these materials in 1‐butyl‐1‐methylpyrrolidinium trifluoromethylsulfonate, [Py_1,4]TfO, at 100 °C with FeCl₂ and FeCl₂+SiCl₄ was studied by using cyclic voltammetry. Constant‐potential electrolysis was carried out to deposit either Fe or FeSi, and deposits of approximately 10 μm thicknesses were obtained. By using scanning electron microscopy and X‐ray diffraction, the microstructure and crystallinity of the deposits were investigated. Grain sizes in the nanometer regime (50–80 nm) were found and the presence of iron–silicon alloys was verified. Frequency‐dependent magnetic polarizations, coercive forces, and power losses of some deposits were determined by using a digital hysteresis recorder. Corresponding to the small grain sizes, the coercive forces are around 950–1150 A m^?1 and the power losses were at 6000 J m^?3, which is much higher than in commercial Fe(3.2 wt %)Si electrical steel. Below a polarization of 1.8 T, the power losses are mainly caused by domain wall movements and, above 1.8 T, by rotation of magnetic moments as well as domain wall annihilation and recreation.     

One Dimensional Coordination Polymer Constructed by1,2—Bis（4—pyridinecarboxamido）ethane and Copper（Ⅱ）

The ligand [1,2‐bis(4‐pyridinecarboxamido)ethane] (L) and the coordination polymer |[Cu(L)₂(H₂O)]‐(NO₃)₂·6H₂O|·(1) haw been synthesized and characterized by ER and ¹H NMR spectra. Their molecular structures and the packing of 1 have been determined by single‐crystal X‐ray diffraction analysis. The Cu(n) in 1 is bridged by two ligands forming an infinite one‐dimensional chain like structure and L in 1 adopts a different conformation from its free state. 1 belongs to monoclinic, space group P2₁/n, a = 1.2896(3) nm, b = 1.2552(8) nm, c = 2.2903(19) nm, β = 93.04(5)°, Z = 4, V = 3.702(4) nm³. The TG and DTG experiments showed that the uncoordinated H₂O can be removed at low temperature by heating, and it does not decompose until 250 °C.     

亚乙基硫脲配位聚合物[Cu3(etu)3 Br3]n的合成与晶体结构

CuB r2和亚乙基硫脲反应生成Cu(I)配位聚合物[Cu3(etu)3B r3]n(etu=亚乙基硫脲),单晶X射线衍射测得该晶体为三斜晶系,Pī空间群.晶胞参数:a=0.762 46(6)nm,b=1.198 48(10)nm,c=1.224 52(7)nm,α=68.202(5),°β=74.607(6),°γ=87.652(7)°,V=0.999 61(13)nm3,Z=2,Mr=736.82,Dc=2.448 g.cm-3,μ=9.477 mm-1,F(000)=708,偏差因子R1=0.030 6,wR2=0.071 0.配合物由环状[Cu(etu)B r]3单元聚合而成,形成Cu4S2B r2和Cu2S4B r2聚合体,两聚合体通过μ2-S桥键交替连接,形成平行于晶胞b轴的[Cu3(μ3-etu)(μ2-etu)2(μ2-B r)2B r]n一维链.Cu(I)均为变形四面体配位,亚乙基硫脲以S原子与Cu(I)结合,形成μ2-S和μ3-S两种配位方式.     

Molecular Reorientational Dynamics of the Neat Ionic Liquid 1‐Butyl‐3‐methylimidazolium Hexafluorophosphate by Measurement of 13C Nuclear Magnetic Relaxation Data

The reorientational dynamics of the ionic liquid 1butyl‐3‐methylimidazolium hexafluorophosphate ([BMIM]PF₆) were studied over a wide range of temperatures by measurement of ¹³C spin–lattice relaxation rates and NOE factors. The reorientational dynamics were evaluated by performing fits to the experimental relaxation data. Thus, the overall reorientational motion was described by a Cole–Davidson spectral density with a Vogel–Fulcher–Tammann temperature dependence of the correlation times. The reorientational motion of the butyl chain was modelled by a combination of the latter model for the overall motion with a Bloembergen–Purcell–Pound spectral density and an Arrhenius temperature dependence for the internal motion. Except for C2 in the aromatic ring, an additional reduction of the spectral density by the Lipari–Szabo model had to be employed. This reduction is a consequence of fast molecular motions before the rotational diffusion process becomes effective. The C2 atom did not exhibit this reduction, because the librational motion of the corresponding C2? H vector is severely hindered due to hydrogen bonding with the hexafluorophosphate anion. The observed dynamic features of the [BMIM]⁺ cation confirm quantum‐chemical structures obtained in a former study.     

Synthesis,Structure, and Physico‐optical Properties of Manganate(II)‐Based Ionic Liquids

Several ionic liquids (ILs) based on complex manganate(II) anions with chloro, bromo, and bis(trifluoromethanesulfonyl)amido (Tf₂N) ligands have been synthesized. As counterions, n‐alkyl‐methylimidazolium (C_nmim) cations of different chain length (alkyl=ethyl (C₂), propyl (C₃), butyl (C₄), hexyl (C₆)) were chosen. Except for the 1‐hexyl‐3‐methylimidazolium ILs, all of the prepared compounds could be obtained in a crystalline state at room temperature. However, each of the compounds displayed a strong tendency to form a supercooled liquid. Generally, solidification via a glass transition took place below ?40 °C. Consequently, all of these compounds can be regarded as ionic liquids. Depending on the local coordination environment of Mn²⁺, green (tetrahedrally coordinated Mn²⁺) or red (octahedrally coordinated Mn²⁺) luminescence emission from the ⁴T(G) level is observed. 1 The local coordination of the luminescent Mn²⁺ centre has been unequivocally established by UV/Vis as well as Raman and IR vibrational spectroscopies. Emission decay times measured at room temperature in the solid state (crystalline or powder) were generally a few ms, although, depending on the ligand, values of up to 25 ms were obtained. For the bromo compounds, the luminescence decay times proved to be almost independent of the physical state and the temperature. However, for the chloro‐ and bis(trifluoromethanesulfonyl)amido ILs, the emission decay times were found to be dependent on the temperature even in the solid state, indicating that the measured values are strongly influenced by nuclear motion and the vibration of the atoms. In the liquid state, the luminescence of tetrahedrally coordinated Mn²⁺ could only be observed when the tetrachloromanganate ILs were diluted with the respective halide ILs. However, for [C₃mim][Mn(Tf₂N)₃], in which Mn²⁺ is in an octahedral coordination environment, a weak red emission from the pure compound was found even in the liquid state at elevated temperatures.     

Mass Distribution and Diffusion of [1‐Butyl‐3‐methylimidazolium][Y] Ionic Liquids Adsorbed on the Graphite Surface at 300–800 K

The structure and diffusion behavior of 1‐butyl‐3‐methylimidazolium ([bmim]⁺) ionic liquids with [Cl]^?, [PF₆]^?, and [Tf₂N]^? counterions near a hydrophobic graphite surface are investigated by molecular dynamics simulation over the temperature range of 300–800 K. Near the graphite surface the structure of the ionic liquid differs from that in the bulk and it forms a well‐ordered region extending over 30 Å from the surface. The bottom layer of the ionic liquid is stable over the investigated temperature range due to the inherent slow dynamics of the ionic liquid and the strong Coulombic interactions between cation and anion. In the bottom layer, diffusion is strongly anisotropic and predominantly occurs along the graphite surface. Diffusion perpendicular to the interface (interfacial mass transfer rate k_t) is very slow due to strong ion–substrate interaction. The diffusion behaviors of the three ionic liquids in the two directions all follow an Arrhenius relation, and the activation barrier increases with decreasing anion size. Such an Arrhenius relation is applied to surface‐adsorbed ionic liquids for the first time. The ion size and the surface electrical charge density of the anions are the major factors determining the diffusion behavior of the ionic liquid adjacent to the graphite surface.