新型一维麻花状超分子配合物的合成与结构

具有特殊结构及性能的超分子化合物由于其结构上的新颖性及潜在的应用价值而成为人们关注的热点 .以一个苯环为间隔基两端含两个吡啶基团的配体 L1与 Pd( ) ,Pt( )形成 2 -索烃 [1 ] ,与Cd( NO3) 2 则形成具有一维平面结构的聚合物 [2 ] .以联苯为间隔基的配体 L2在 4 ,4′-二联吡啶共同作用下与 Pd( )形成 2 -索烃 [3] .同样以一个苯环为间隔基两端含两个咪唑基团的配体 L3与 Zn( NO3) 2 ,Ag NO3反应得到新型多聚轮烷配合物 [4,5 ] .研究结果表明 ,配体或配位金属离子等的微小差别即导致形成结构不同的超分子化合物 .但这些超分子…     

5,7′-(亚甲胺基)-二-8-羟基喹啉及其金属有机配合物的密度泛函和自然键轨道及电子密度拓扑理论研究

采用密度泛函理论, 在B3LYP/6-31G水平上对5,7′-(亚甲胺基)-二-羟基喹啉及其3种金属M(M=Zn, Mg, Be)有机配合物M(5,7′-Iminomethylq2)2的结构进行了全优化, 并用TDDFT方法计算了吸收光谱. 同时, 利用自然键轨道理论(NBO)和电子密度拓扑分析(AIM)方法对分子内氢键进行了分析. 结果表明, 光谱计算值与实验值基本符合, 该类化合物均具有较大的电子亲和能, 改变中心金属原子对配合物吸收光谱性质的影响不大. 和5,7′-Iminomethylq2相比, M(5,7′-Iminomethylq2)2的吸收光谱产生明显红移. 5,7′-Iminomethylq2及其M(5,7′-Iminomethylq2)2分子内存在较强的氢键, 可形成三元环, 五元环和六元环. 分子内氢键的存在使分子的稳定性增加.     

MX2(AsH3)2(M=Pd,Pt;X=Cl,Br,I)的含时密度泛函理论研究

采用密度泛函方法(B3LYP)优化了MX2(AsH3)2[M=Pd；X=Cl(1)，Br(2)，I(3)和M=Pt；X=Cl(4)，Br(5)，I(6)]的基态结构，得到的几何参数与实验结果符合．以基态几何为基础，将TD-DFT方法用于计算标题配合物的电子吸收光谱．研究结果表明，金属的dx2-y2与配体所组成的反键轨道为LUMO轨道，从而该类配合物具有d-d跃迁属性的吸收带；在多数跃迁过程中，配体也有较大的贡献．     

联吡啶Ir(Ⅲ)配合物电子结构及光谱性质的理论研究

采用密度泛函理论(DFT)对配合物Ir(ppy)2(N^N)+ [ppy=2-phenylpyrine, N^N=bpy= 2,2’-bipyridine(1); N^N=H2dcbpy=4.4’-dicarboxy-2,2’-bipyridine(2), N^N=Hcmbpy=4-carboxy-4’-methyl-2,2’-bipyridine(3)] 的基态和激发态几何构型进行优化, 通过TDDFT/B3LYP方法得到这些化合物在乙腈溶液中的吸收光谱和磷光发射光谱及其跃迁性质. 研究结果表明, 化合物1 (384 nm), 2(433 nm)和3 (413 nm) 最低的吸收谱被指认为MLCT/LLCT[dIr+π(ppy)→π*(N^N)]电荷跃迁. 化合物1(486 nm), 2(576 nm)和3 (567 nm)最低的磷光发射可以描述为[dIr+π(ppy)]→[π*(N^N)]跃迁. 这是由于联吡啶配体上吸电子基团的引入, 稳定了相应的空轨道, 导致了化合物2和3的吸收和发射光谱红移. 同时, 化合物非线性光学性质的计算结果表明, 三种化合物均具有较大的一阶超极化率(β), 联吡啶配体中吸电子基团的增加, 使得分子内电子转移增强, 导致一阶超极化率增大.     

炔基配体对2, 6-双(N-乙基苯并咪唑)吡啶炔基铂(Ⅱ)配合物与G-四链体作用及抗癌活性的影响

合成了三种2, 6-双(N-乙基苯并咪唑)吡啶炔基铂(Ⅱ)配合物(2-4),其中配合物2的炔基配体为抗癌药物埃罗替尼.利用紫外-可见(UV-Vis)吸收光谱,圆二色(CD)光谱,荧光共振能量转移(FRET)等方法研究了铂(Ⅱ)配合物与人体端粒(Hetelo)和c-myc原癌基因(c-myc)G-四链体的相互作用.实验结果表明,所合成的铂配合物与G-四链体具有较强的相互作用(K_a > 10⁶ L·mol^-1),在无碱金属离子存在条件下能诱导G-四链体的形成.含苯乙炔基团的配合物2、3能使c-myc G-四链体的熔解温度上升24 ℃以上,而含丙炔基团的铂配合物4仅使c-mycG-四链体的熔解温度升高9.0 ℃,表明炔基结构对铂(Ⅱ)配合物与G-四连体的作用有较大影响.配合物2对人肺癌细胞A549的细胞毒性明显高于埃罗替尼及其他两种配合物3、4.     

Push-pull effects and emission from ternary complexes of platinum(II), substituted terpyridines, and the strong-field cyanide ion

As part of an effort to develop new lumaphors involving late transition metal ions, this report describes the synthesis and characterization of the first platinum(II) derivatives containing 2,2':6',2'-terpyridine (trpy) and cyanide as co-ligands. According to existing models, including cyanide in the coordination sphere should raise the energies and minimize the influence of short-lived d-d excited states that otherwise compromise the excited-state lifetime. Both [Pt(trpy)(CN)]+ and the 4'-cyano-2,2':6',2'-terpyridine analogue [Pt(CN-T)(CN)]+ are emissive in dichloromethane solution, but the signals are weak. Part of the problem is that the d-pi* charge-transfer excited states also rise in energy, so that the emission actually originates from a (3)pi-pi* state with a relatively low radiative rate constant. However, another member of the series, the 4'-dimethylamino-2,2':6',2'-terpyridine (dma-T) derivative [Pt(dma-T)(CN)]+, proves to be a very promising platform with an emission quantum yield of phi= 0.26 and an excited-state lifetime of tau = 22 micros in room-temperature, deoxygenated dichloromethane solution. In the dma-T complex the electron-rich dimethylamino substituent provides the basis for an emissive, but largely ligand-based, charge-transfer excited state. The orbital parentage is such that the photoluminescence persists in donating solvents like dimethylformamide, which ordinarily quenches d-pi* excited states in complexes of this type.     

Theoretical study on the influence of ancillary ligand on the spectroscopic properties and electronic structures of phosphorescent Pt(II) complexes

The geometries, energies, and electronic properties of a series of phosphorescent Pt(II) complexes including FPt, CFPt, COFPt, and NFPt have been characterized within density functional theory DFT calculations which can reproduce and rationalize experimental results. The properties of excited‐states of the Pt(II) complexes were characterized by configuration interaction with singles (CIS) method. The ground‐ and excited‐state geometries were optimized at the B3LYP/LANL2DZ and CIS/LANL2DZ levels, respectively. In addition, we also have performed a triplet UB3LYP optimization for complex FPt and compared it with CIS method in the emission properties. The datum (562.52 nm) of emission wavelength for complex FPt, which were computed based on the triplet UB3LYP optimization excited‐state geometry, is not agreement with the experiment value (500 nm). The absorption and phosphorescence wavelengths were computed based on the optimized ground‐ and excited‐state geometries, respectively, by the time‐dependent density functional theory (TD‐DFT) methods. The results revealed that the nature of the substituent at the phenylpyridine ligand can influence the distributions of HOMO and LUMO and their energies. Moreover, the auxiliary ligand pyridyltetrazole can make the molecular structure present a solid geometry. In addition, the charge transport quality has been estimated approximately by the predicted reorganization energy (λ). Our result also indicates that the substitute groups and different auxiliary ligand not only change the nature of transition but also affect the rate and balance of charge transfer. By summarizing the results, we can conclude that the NFPt is good OLED materials with a solid geometry and a balanced charge transfer rate. © 2009 Wiley Periodicals, Inc. Int J Quantum Chem, 2010     

Theoretical Studies on Structural and Spectroscopic Properties of Photoelectrochemical Cell Ruthenium Sensitizers-the Derivatives of N3

A series of dye molecules was designed theoretically. Particularly, azoles and their derivatives were chosen as the modifying groups linking to ancillary ligands of [Ru(dcbpyH₂)₂(NCS)₂](N3, dcbpy=4,4′-dicarboxy- 2,2′-bipyridine; NCS=thiocyanato). Density functional theory(DFT) based approaches were applied to exploring the electronic structures and properties of all these systems. The dye molecule with 1,2,4-triazole groups which exhibits a very high intensity of absorption in visible region, was obtained. Time-dependent DFT(TD-DFT) results indicate that the ancillary ligand dominates the molecular orbital(MO) energy levels and masters the absorption transition nature to a certain extent. The deprotonation of anchoring ligand not only affects the frontier MO energy levels but also controls the energy gaps of the highest occupied MO(HOMO) to the lowest unoccupied MO(LUMO) and LUMO to LUMO+1 orbital. If the gap between LUMO-LUMO+1 is small enough, the higher efficiency of dye-sensitized solar cell(DSSC) should be expected.     

Crystal structure and luminescence property of ternary terbium p-aminobenzoic acid complexes with different second ligands

Ternary terbium complexes with p-aminobenzoic acid (HL), [TbL₃(DMSO)(H₂O)]₂ (1), [TbL₃(DMF)(H₂O)]₂ (2) and [TbL₃(Bpy)(H₂O)]₂·2H₂O (3) (DMSO=dimethyl sulfoxide, DMF=N, N- dimethylformamide, Bpy=2, 2′- bipyridyl) have been synthesized, and their crystal structures determined. The luminescence properties of these complexes, including both the emission quantum yield and the fluorescence lifetime, have been investigated. The effect of a second ligand on the crystal structure and luminescence property of the ternary terbium p-aminobenzoic acid complexes, and the relationship between luminescence properties and crystal structure, including coordination mode of the L⁻ ligand and the characteristics of a second ligand, are discussed.     

Experimental and quantum-chemical studies of 1H, 13C and 15N NMR coordination shifts in Pd(II) and Pt(II) chloride complexes with methyl and phenyl derivatives of 2,2'-bipyridine and 1,10-phenanthroline

1H, 13C and 15N NMR studies of platinide(II) (M=Pd, Pt) chloride complexes with methyl and phenyl derivatives of 2,2'-bipyridine and 1,10-phenanthroline [LL=4,4'-dimethyl-2,2'-bipyridine (dmbpy); 4,4'-diphenyl-2,2'-bipyridine (dpbpy); 4,7-dimethyl-1,10-phenanthroline (dmphen); 4,7-diphenyl-1,10-phenanthroline (dpphen)] having a general [M(LL)Cl2] formula were performed and the respective chemical shifts (delta1H, delta13C, delta15N) reported. 1H high-frequency coordination shifts (Delta1Hcoord=delta1Hcomplex-delta1Hligand) were discussed in relation to the changes of diamagnetic contribution in the relevant 1H shielding constants. The comparison to literature data for similar [M(LL)(XX)], [M(LL)X2] and [M(LL)XY] coordination or organometallic compounds containing various auxiliary ligands revealed a large dependence of delta1H parameters on inductive and anisotropic effects. 15N low-frequency coordination shifts (Delta15Ncoord=delta 15Ncomplex-delta15Nligand) of ca 88-96 ppm for M=Pd and ca 103-111 ppm for M=Pt were attributed to both the decrease of the absolute value of paramagnetic contribution and the increase of the diamagnetic term in the expression for 15N shielding constants. The absolute magnitude of Delta15Ncoord parameter increased by ca 15 ppm upon Pd(II)-->Pt(II) transition and by ca 6-7 ppm following dmbpy-->dmphen or dpbpy-->dpphen ligand replacement; variations between analogous complexes containing methyl and phenyl ligands (dmbpy vs dpbpy; dmphen vs dpphen) did not exceed+/-1.5 ppm. Experimental 1H, 13C, 15N NMR chemical shifts were compared to those quantum-chemically calculated by B3LYP/LanL2DZ+6-31G**//B3LYP/LanL2DZ+6-31G*, both in vacuo and in DMSO or DMF solution.     

Mononuclear Pt(II) and Pd(II) 1,4-dithiolato complexes. Crystal structures of [Pt((−) DIOS) (PPh3)2] and [Pd(S(CH2) 4S)(Ph2P(CH2) 3PPh2)]. Application in styrene hydroformylation

Addition of 1,4-dithiols to dichloromethane solutions of [PtCl₂(P-P)] (P-P = (PPh₃)₂, Ph₂P(CH₂)₃PPh₂, Phd₂P(CH₂)₄PPh₂; 1,4-dithiols = HS(CH₂)₄SH, (−)DIOSH₂ (2,3-O-isopropylidene-1,4-dithiol-l-threitol), BINASH₂ (1,1′-dinaphthalene-2,2′-dithiol)) in the presence of NEt₃ yielded the mononuclear complexes [Pt(1,4-dithiolato)(P-P)]. Related palladium(II) complexes [Pd(dithiolato)(P-P)] (P-P=Ph₂P(CH₂)₃PPh₂, Ph₂P(CH₂)₄PPh₂; dithiolato = ⁻S(CH₂)₄S⁻, (−)-DIOS) were prepared by the same method. The structure of [Pt((−)DIOS)(PPh₃)₂] and [Pd(S(CH₂)₄S)(Ph₂P(CH₂)₃PPh₂)] complexes was determined by X-ray diffraction methods. Pt—dithiolato—SnC1₂ systems are active in the hydroformylation of styrene. At 100 atm and 125°C [Pt(dithiolate)(P-P)]/SnCl₂ (Pt:Sn = 20) systems provided aldehyde conversion up to 80%.     

Strongly luminescent palladium(0) and platinum(0) diphosphine complexes

The synthesis, structure, and photoluminescence of palladium(0) and platinum(0) complexes containing biarydiphosphines, biphep (biphep = 2,2'-bis(diphenylphosphino)-1,1'-biphenyl) and binap (binap = 2,2'-bis(diphenylphosphino)-1,1'-binaphthyl) have been studied. X-ray structure analysis of [Pt(biphep)(2)] revealed the distorted-tetrahedral geometry of the complex. The photophysical properties of the three complexes [Pd(biphep)(2)], [Pt(biphep)(2)], and [Pd(binap)(2)] were investigated and compared with that of the previously reported [Pt(binap)(2)] complex. The [Pd(biphep)(2)] complex shows the strongest luminescence with a high quantum yield (38%) and a long lifetime (3.2 micros) in a toluene solution at room temperature. The luminescence should be due to metal-to-ligand charge transfer excited states. At room temperature, radiative rate constants of the four complexes show similar values. The difference in the luminescent properties should reflect the different nonradiative rate constants of the complexes. The temperature-dependence of the luminescence spectra and lifetime of the complexes were also discussed.     

Theoretical investigations of the substituent effect on the absorption and emission properties for a series of platinum (II) complexes supported by tetradentate N2O2 chelates

The photophysical properties, which vary as R is varied, of a series of [Pt(N₂O₂)] complexes bearing bis(phenoxy)bipyridine auxiliaries with different substituents R=H (Pt-H) (1), 4,4′-2NH₂ (Pt-NH₂) (2), 4,4′-2tBu (Pt-tBu) (3), 4,4′-2CN (Pt-CN) (4), and 4,4′-2NO₂ (Pt-NO₂) (5) are investigated using density functional theory (DFT) and time-dependent density functional theory (TDDFT). The solvent effects are discussed in CH₂Cl₂, CH₃CN and CH₃OH solutions, respectively, by polarizable continuum model (PCM). It is anticipated that compared with σ-donor substituents, π-acceptors have more dramatic effects on the electronic and optical properties in this series of complexes. Introduction of π-electron withdrawing substituents on bipyridine ligand will benefit the LLCT (or MLCT) and prohibit the non-radiative pathways via d–d transitions by increasing the energy gap between the HOMO–LUMO and d–d transitions. The results also reveal that the lowest-energy excitations of all complexes show blue-shifts in the polarized solution and when the polarity of the solvent increases from CH₂Cl₂, CH₃CN and CH₃OH, the low-energy broad absorption band exhibit blue-shifts. The lowest-energy excitations and photoluminescence of all complexes are dominated by π(phenoxy)→π^*(bpy/NO₂) (LLCT) excited state mixed with some energetically dπ (Pt)→π^*(bpy/NO₂) (MLCT) transition.     

Heteroleptic platinum(II) complexes of macrocyclic thioethers and halides: the crystal structures of [Pt(9S3)Cl2], [Pt(9S3)Br2], and [Pt(9S3)I2]

The synthesis, spectroscopic, and crystal structures of three heteroleptic thioether/halide platinum(II) (Pt(II)) complexes of the general formula [Pt(9S3)X₂] (9S3=1,4,7-trithiacyclononane, X=Cl⁻, Br⁻, I⁻) are presented. All three 9S3/dihalo complexes form very similar structures in which the Pt(II) center is surrounded by a cis arrangement of two halides and two sulfur atoms from the 9S3 ligand. The third sulfur from the 9S3 forms a long distance interaction with the Pt center resulting in an elongated square pyramidal structure with a S₂X₂+S₁ coordination geometry. The distances between the Pt(II) center and axial sulfur shorten with larger halide ions (Cl⁻=3.260(3) Å>Br⁻=3.243(2) Å>I⁻=3.207(2) Å). These distances are consistent with the halides functioning as π donor ligands, and their Pt---S axial distances fall intermediate between Pt(II) thioether complexes involving π acceptor and σ donor ligands. The ¹⁹⁵Pt NMR chemical shift values follow a similar trend with an increased shielding of the platinum ion with larger halide ions. The 9S3 ligand is fluxional in all of these complexes, producing a single carbon resonance. Additionally, a related series of homoleptic crown thioether complexes have been studied using ¹⁹⁵Pt NMR, and there is a strong correlation between the chemical shift and complex structure. Homoleptic crown thioethers show the anticipated upfield chemical shifts with increasing number of coordinated sulfurs. Complexes containing four coordinated sulfur donors have chemical shifts that fall in the range of −4000 to −4800 ppm while a value near −5900 ppm is indicative of five coordinated sulfurs. However, for S₄ crown thioether complexes, differences in the stereochemical orientation of lone pair electrons on the sulfur donors can greatly influence the observed ¹⁹⁵Pt NMR chemical shifts, often by several hundred ppm.     

2-(Phenyltelluromethyl)tetrahydrofuran (L) and 2-(2-{4-methoxyphenyl}telluroethyl)-1,3- dioxolane (L) and their palladium(II) and platinum(II) complexes

The nucleophile [ArTe⁻] generated in situ borohydride solution of Ar₂Te₂, reacts with 2-(chloromethyl) tetrahydrofuran and 2-(2-bromoethyl)-1,3-dioxolane resulting in L¹ and L², respectively. The complexes of palladium(II) and platinum(II) with L¹/L² having stoichiometries [MCl₂·L₂], [ML₂](ClO₄)₂, [(DPPE)ML₂](ClO)₄)₂, [(PPh₃)₂ML₂](ClO₄)₂ and [(phen)ML₂](ClO₄)₂ (where L = L¹/L² DPPE = Ph₂PC H₂CH₂PPh₂, PHEN = 1,10-phenanthroline and M = Pd/Pt) have been synthesized. IR, ¹H, ¹²⁵Te{¹H} and ³¹P{¹H} NMR and UV-vis spectral data of these species in conjunction with their molar conductance and molecular weight data have been used to authenticate the new species. In all complexes (1–20) the ligands L¹ and L² are coordinated through tellurium and in the complexes of formula [ML₂](ClO₄)₂ (M = Pd, Pt) the ligand is bidentate with the oxygen atom used in complexation. In solution, complexes PtCl₂L₂ exist as a mixture of cis and trans isomers whereas only the trans isomer was observed for the palladium analogues. The [(phen)PdL₂](ClO₄)₂(Q) quenches ¹O₂ readily. The plot of log [Q] vs time is linear. Mechanism compatible with the experimental observations is proposed.     

Synthesis and photochemistry of Ru(II) complexes containing phenanthroline-based ligands with fused pyrrole rings

Hydrolysis of 1,10-phenanthrolinopyrrole ethyl ester leads to the acid derivative which is unstable at room-temperature releasing CO(2) and forming 1,10-phenanthrolinopyrrole (php). The ligand reacts with ruthenium(II) to form a series of complexes of the general formula [Ru(php)(n)(bpy)(3-n)](2+), where bpy = 2,2'-bipyridine and n = 1-3. The photochemical properties reveal that the complexes have longer-lived excited states than the standard complex, [Ru(bpy)(3)](2+). Their emission lifetimes range from 9.04 micros (n = 1) to 35.5 micros (n = 3) at 77 K compared to 7.57 micros for the standard. Similarly, at room-temperature, emission lifetimes range from 1.20 micros (n = 1) to 1.70 micros (n = 3) relative to the standard (0.56 micros). The emission quantum yields also have higher values than the standard [Ru(bpy)(3)](2+) under similar conditions. The temperature-dependent studies for the complexes establish the distribution among the radiative, nonradiative, and (3)MLCT to (3)d-d decay channels and are in agreement with the energy gap law.     

Electroluminescence from Exciplex on the Interface Between TPD and La（PMIP）3（Bipy）

The bilayer organic light-emitting diode(OLED) with a blue fluorescent lanthanum complex, tris(1-phenyl-3-methyl-4-isobutyryl-5-pyrazolone)-(2,2′-dipyridyl) lanthanum [La(PMIP)3(Bipy)], as a light emitting material and N,N′-diphenyl-N,N′-bis(3-methylphenyl)-1,1′-biphenyl-4,4′-diamine(TPD) as a hole transporting material emits bright green light instead of blue light. The data of the absorption, the photoluminescence(PL) and the photoluminescence excitation(PLE) spectra of TPD, La(PMIP)3(Bipy) and the mixture of TPD and La(PMIP)3(Bipy)(molar ratio 1∶1) prove that the electroluminescent emission originates from the exciplex on the interface between TPD and La(PMIP)3(Bipy). By improving device configuration with tris(8-hydroxyquinoline) aluminum(ALQ) as an electron transporting material, a maximum luminance of 800 cd/m2 was obtained.     

双(对-氨基苯基)-2,3,7,8,12,13,17,18-八甲基卟啉及其金属衍生物的合成与表征

从3-甲基-2,4-戊二酮出发,经多步反应合成了3,3′,4,4′-四-甲基-2,2′-二吡咯基甲烷(TMDPM),改进了合成TMDPM的脱羧反应.研究了TMDPM与对-硝基苯甲醛反应合成meso-5,15-双-苯基-卟啉反应,发现对-甲基苯磺酸是卟啉原合成的良好催化剂,2,3-二-氯-5,6二氰基-1,4-苯醌是将卟啉原转化为卟啉的良好氧化剂;硝基卟啉经SnCl₂还原成氨基卟啉后,用固-液抽提进行氨基卟啉的纯化,得到了5,15-双(对-硝基苯基)-2,3,7,8,12,13,17,18-八甲基卟啉、5,15-双(对-氨基苯基)-2,3,7,8,12,13,17,18-八甲基卟啉及其金属衍生物,并表征了其结构     

Eu(III) Complex-doped PMMA with Fast Radiation Rate and High Emission Quantum Efficiency

Two Eu(III) complexes, (tris-4,4,4-trifluoro-1-phenyl-1,3-butanedione)(1,10-phenanthroline)europium(III) [Eu(tpb-H)₃(phen)] and (tris-4,4,4-trifluoro-1-phenyl-1,3-butanedione)(2,2′-bipyridine)europium(III)[Eu(tpb-H)₃-(bipy)] were synthesized from bi-dental oxygen and nitrogen ligands. Luminescent polymers were fabricated by incorporating deuterated Eu(III) complexes in poly(methylmethacrylate)(PMMA) matrixes. Luminescent PMMA containing Eu(tpb-D)₃(phen) exhibited relatively higher quantum yield[Φ, (48.7±4)%], faster radiation rate(k_r, 7.49×10² s^-1), sharper red emission[full width at half maximum(FWHM), 6.3 nm] and larger stimulated emission cross-section (SEC, 1.29×10^-20 cm²). The value of SEC is the same order as that of Nd-glass laser for practical use. Additionally, the thermal properties of Eu(tpb-H)₃(phen), Eu(tpb-H)₃(bipy), Eu(tpb-D)₃(phen)-PMMA, and Eu(tpb-H)₃(bipy)-PMMA were studied, indicating that the Eu(III) complexes and luminescent PMMA can be used for a long-term period in high temperature environment. Prepared luminescent polymers including Eu(tpb-D)₃(phen) have promising applications in novel organic Eu(III) devices, such as the high-power laser materials and optical fibers.     

氮杂大环双核铜锌金属配合物的合成结构及溶液中配位稳定性研究

在合成模型化合物之前 ,有必要先了解合成的大环配体在溶液中与金属离子的配位行为及其稳定性 ,以便选择不同结构的大环配体和控制反应的 p H值合成出结构和催化性能较好的模型化合物 [1～ 3] .本文报道了大环配体与 Cu( )和 Zn( )形成的配合物 ,对其结构和溶液中的配位稳定性进行了研究 .1　实验部分1 .1　试剂与仪器配体 L以 2 ,6-吡啶二甲醛和二乙烯三胺为原料 ,按文献 [4]报道的方法经 2 + 2合成得到 .其纯度经元素分析、红外光谱、核磁共振氢谱和质谱鉴定 .其它试剂均为分析纯 . p H滴定采用二次蒸馏水 .Perkin- Elmer 2 4 0型元…