双核铜配合物[Cu2（pida）2（2,2′-bipy）2]的合成、表征及其结构

N-苯基亚氨基二乙酸,Cu2 离子和2,2′-联吡啶在溶液中组装得到标题配合物[Cu2(pida)2(2,2′-bipy)2](H2pida=N-苯基亚氨基二乙酸)。用元素分析、红外光谱、单晶衍射对配合物的组成和结构进行了表征,结果表明,该标题配合物为N-苯基亚氨基二乙酸根桥联的双核结构,配体pida中的N原子没有参与配位,中心铜离子为五配位畸变的四方锥构型。     

混配配合物[Co(cpida)(C7H5N2)2]·C7H5N2·5H2O

在溶液中用N-(邻苯甲酸基)-亚氨基二乙酸、苯并咪唑和Co(Ac)2·4H2O进行自组装合成了标题三元金属混配配合物.用元素分析、红外光谱、单晶衍射对配合物的组成和结构进行了表征,确定配体N-(邻苯甲酸基)-亚氨基二乙酸中的3个羧基为单齿形式与中心金属钴离子配位.     

Ni2+、联吡啶和N-苯基亚氨基二乙酸三元金属混配配合物的合成与表征

N-苯基亚氨基二乙酸、2 ,2′-联吡啶和 Ni Cl2 · 6 H2 O在溶剂中进行自组装形成了一种新的三元金属混配配合物。用元素分析、热重分析、红外和紫外光谱对配合物的组成和结构进行了表征 ,初步确定配体N -苯基亚氨基二乙酸中的 2个羧基为单齿形式与中心金属离子 Ni2 配位。     

离子对配合物[Cu(L)n][Ni(dmit)2]的合成与光谱表征

本文首先合成了三种以 Cu2 离子为中心离子的配位阳离子 ,然后将其与配位阴离子 [Ni(dmit) 2 ]2 -组装 ,合成了 3个新型 [Cu Ln][Ni(dmit) 2 ]离子对配合物 ,用元素分析、红外光谱、紫外 -可见吸收光谱对配合物的组成和结构进行了表征     

Cu+与N-[2-羟基-1(S)-甲基]-N-甲基甘氨酸间的C-H…Cu(Ⅰ)抓氢键

采用密度泛函B3LYP(Becke, three-parameter, Lee-Yang-Parr)/6-311G**理论水平研究了Cu+和Cu2+离子与N-[2-羟基-1(S)-甲基]-N-甲基甘氨酸根负离子配体（PT）形成的配合物的结构,重点讨论了配合物中的C-H Cu抓氢键结构. 计算表明, 当单个配体与Cu+结合时,配合物PT•••Cu(Ⅰ)结构中有C-H Cu抓氢键形成,C-H键伸缩振动频率显著红移,键长显著增大而被活化, 配体为三齿配体;当两个配体与Cu2+结合时,配合物PT•••Cu(Ⅱ)不存在C-H Cu抓氢键结构,配体为双齿配体. NBO及AIM理论分析均表明C-H Cu抓氢键属于一种较强的基团间相互作用,在强度和电子行为上与氢键弱相互作用有本质不同.     

金属配合物(pq)_2Ir(N-phMA)发光材料的合成及光谱性质

设计出一种酰胺类金属铱有机配合物磷光电致发光材料,该材料是以2-苯基喹啉(pq)为主配体,N-苯基甲基丙烯酰胺(N-phMA)为辅助配体的金属配合物(pq)2Ir(N-phMA)。该化合物的结构由核磁,红外表征确定,它在586nm处的强荧光发射,表明它是一种可用于OLED的黄光发光材料。     

钕4,4′-二甲基-2,2′-联吡啶配合物液体激光介质的合成及其光学特性(英文)

合成并用元素分析、红外光谱法表征了一种4,4′-二甲基-2,2′-联吡啶五氟丙酸钕配合物—Nd(C2F5COO)3·Dmbp(Dmbp:4,4′-二甲基-2,2′-联吡啶).将该配合物溶解在N,N-二甲基甲酰胺中获得了液体介质,依据液体介质的吸收和荧光光谱,通过Judd-Ofelt理论计算获得了钕离子的谱线强度参数(Ω2,Ω4,Ω6)和受激发射截面.计算得到该配合物中钕离子4F3/2→4I11/2跃迁的受激发射截面为5.2×10-20 cm2,表明该钕配合物在液体基质中具有较好的发光特性.通过荧光发射光谱分析可知,Nd(C2F5COO)3·Dmbp将是一种有前途的光学增益材料.     

二茂铁双核铜配合物Cu2(dmaf)2(CH3COO)4(Ⅰ)和Cu2(dmaf)2(C6H5COO)4(Ⅱ)的光谱研究

室温下合成了含有二茂铁基的双核铜配合物Cu2 (dmaf) 2 (CH3 COO) 4 (Ⅰ )和Cu2 (dmaf) 2 (C6H5COO) 4(Ⅱ ) [dmaf=(dimethylaminomethyl)ferrocene]。采用扫描电镜半定量测定标题化合物成分 ,用X射线衍射法测试 ,并确定两者的晶胞参数 ,发现两者有相似的晶体结构。最后对标题物的红外、远红外、固体漫反射电子光谱、循环伏安法 (CV)等谱学性质进行深入研究。结果表明 ,两个配合物紫外吸收波段分别为 2 34～2 6 9nm和 2 4 5～ 2 80nm ,在可见光区出现了一个d d跃迁宽域带 ,其循环伏安曲线表明 ,两个化合物的氧化还原电位分别为 0 5 3,0 37和 0 6 2 ,0 36V。     

N,N''''-二(邻氧乙酸)苄叉乙二胺和Cu(Ⅱ)固体配合物的合成及其结构研究

在水溶液中, 无论是控制一定的pH值(约5及8.5 )把N,N'-二(邻氧乙酸)苄叉乙二胺(H2L3)和三水合硝酸铜混合后回流--直接法, 还是把邻氧乙酸苯甲醛、三水合硝酸铜、乙二胺混合后回流--模板法, H2L3都能与铜离子形成1∶1的单核配合物, 经分离后得到固体配合物. 本文测定了配合物的元素组成、差热曲线、在水溶液中的最大吸收波长及其红外特征吸收峰值, 并据此推断了配合物的可能结构. 结果表明: (1)端基羧酸根离子要与中心Cu(Ⅱ)离子配位只能从轴向配位; (2)在这一类配体中, 芳基醚氧原子对形成稳定的固体Cu(Ⅱ)配合物有重要作用; (3)H2L3和Cu(Ⅱ)形成的配合物是六配位的畸形八面体的构型.     

配合物[Co(PBSP)2(H2O)2]·CH3OH的合成、晶体结构和热重分析

由对氨基苯磺酸、吡啶-2-甲醛、KOH和Co(Ac)2.4H2O在甲醇和水的混合溶剂中反应得到了标题配合物[Co(PBSP)2(H2O)2]·CH3OH(KPBSP=对氨基苯磺酸缩吡啶-2-甲醛席夫碱的钾盐),并进行了元素分析、红外光谱、X-射线衍射和热重分析等表征.结果表明:标题配合物属三斜晶系,空间群为P-1,晶体学参数为:a=1.0188(4)nm,b=1.1079(5)nm,c=1.3243(5)nm,α=98.371(5)°,β=102.324(5)°,γ=106.419(4)°,V=1.3664 (10)nm3,Z=2.配合物中的金属钴离子位于非对称中心,分别与两分子脱质子的PBSP-配体中的吡啶氮原子、亚氨基氮原子及两个水分子的O原子配位,形成变形的八面体结构.     

Infrared Spectra of Morfolonium (mpH)2Mo2Cl6(H20)2(I),(mpH)2Mo2ClxBr6-x(H2O)2(II)/ (mpH)2Mo2Br6(H2O)2(III) and the Pyridinium (PyH)2Mo2I6(H2O)2(IV)Hexahalo-di(aquo): dimolybdate(II) Complexes,Containing Quadruple Metal-Metal Bounds

Abstract

The electronic (800–400 nm), infrared (4000–200,400–20 cm^?1), ordinary Raman (400–200 cm^?1) spectra of morpholinium and the pyridium hexahalo-di(aquo) dimolybdate(II) complexes, containing quadruple metal-metal bonds were investigated. The electronic spectra of the solid compounds at various temperatures (25,100 and 300K) demonstrate intense and structured bands in the visible region (510–582 nm) attributed to the expected δ→δ? transitions.

From the infrared and Raman spectra, the skeletal stretching modes in these complexes have been localized, and the charectenstic bands of these ions were observed in the expected regions.

Finally, the ionic interections were relatively weak, but the existance of phenomena was perceptible and the result was obtained in agreement with X-ray data.     

Isomeric Cl(2)O(2)(+) and Cl(2)O(2)(-) ions

Charged species structurally related to several isomers of Cl(2)O(2), of considerable importance in atmospheric chemistry, were obtained by chemical ionization (CI) and characterized by collisionally activated dissociation (CAD) mass spectrometry. The ClOClO(+) and [Cl(2)-O(2)](+) species were prepared by positive ion Cl(2)/CI of ClO(2) and O(2), respectively, whereas the ClClO(2)(+) isomer proved an elusive species of considerably lower stability. The ClClO(2)(-) anion was obtained from the negative ion Cl(2)/CI of ClO(2). The formation process, structure and stability of the ions are discussed in connection with available theoretical results and related to the recent preparation of (Cl(2)O(2))(+)SbF(6)(-) and (Cl(2)O(2))(+)Sb(2)F(11)(-) salts in the solid phase. Copyright 1999 John Wiley & Sons, Ltd.     

The 2(3)Delta(g) State of (7)Li(2)

Using pulsed perturbation-facilitated optical-optical double resonance (PFOODR) spectroscopy, the 2(3)Delta(g) state of (7)Li(2) (electronic configuration (varsigma(g)2s) (4ddelta(g)), effective principal quantum number n* = 4.101) has been observed and assigned. Molecular constants and a RKR potential energy curve were obtained. The major molecular constants are Copyright 2000 Academic Press.     

Isotope fractionation in aqua-gas systems: Cl(2)-HCl-Cl(-), Br(2)-HBr-Br(-) and H(2)S-S(2-)

We report calculated values of isotope fractionation factors between chlorine, bromine and sulphide hydrated anions and respective gaseous compounds: hydrogen chloride, hydrogen bromide, molecular chlorine and bromine and hydrogen sulphide. For the calculation of the reduced partition function ratios (β-factors) of hydrated Cl(-), Br(-) and S(2-) anions, we used a model of a cluster composed of the considered ion surrounded by two shells of H(2)O molecules. Only the electrostatic interaction between ion and water molecules treated as electric dipoles was taken into account. The β-factors for the gaseous compounds (HCl, Cl(2), HBr, Br(2) and H(2)S) were calculated from vibrational frequencies reported by Urey and Greiff [Isotopic Exchange Equilibria, J. Am. Chem. Soc. 57, 321 (1935)] and Schauble et al. [Theoretical Estimates Equilibrium Chlorine-Isotope Fractionation, Geochim. Cosmochim. Acta 67, 3267 (2003)]. Low-temperature isotope fractionation between chlorine-hydrated anion and hydrogen chloride attains 1.55-1.68‰ (this work), which is in good agreement with experimental data (1.4-1.8‰) [Z.D. Sharp, J.D. Barnes, T.P. Fischer and M. Halick, An Experimental Determination of Chlorine Isotope Fractionation in Acid Systems and Applications to Volcanic Fumaroles, Geochim. Cosmochim. Acta 74, 264 (2010)]. The predicted isotope fractionations for hydrated bromine and HBr, Br(2) gases are very small, 1000?ln α, do not exceed 0.8‰; thus, the expected variations of bromine isotope composition in aqua-gas systems will require enhanced precision for their detection. In contrast, the sulphur isotope fractionation between H(2)S( gas ) and S(2-) attains 6.0‰ at room temperature and drops nearly linearly to 3.1‰ at 350°C.     

Infinite period and Hopf bifurcations for the pH-regulated oscillations in a semibatch reactor (H(2)O(2)-Cu(2+)-S(2)O(2-) (3)-NaOH system)

Dynamic behavior of the pH-regulated oscillations has been studied for the hydrogen peroxide oxidation of thiosulfate ions in the presence of trace amounts of copper(II) ions in a semibatch reactor. A solution of 0.08 M Na(2)S(2)O(3) and 0.112 M NaOH was flowed at 0.160 mL/min into 300 mL of solution containing the H(2)O(2) and Cu(2+) in a vessel. There exists a critical value of the H(2)O(2) or Cu(2+) concentrations below which the system does not oscillate. The oscillations appear due to an infinite period bifurcation at low initial concentrations of the H(2)O(2). The initial concentration of Cu(2+) may be considered as a bifurcation parameter in this case. Increase of the initial hydrogen peroxide concentration causes the pH-regulated oscillations through a nondegenerate supercritical Hopf bifurcation. The classification of bifurcations is based on the analysis of the behavior of oscillation amplitude and period at different initial concentrations of the H(2)O(2) and Cu(2+). Our results show a possibility to distinguish different scenarios for the appearance of transient oscillations in semibatch experiments. (c) 1996 American Institute of Physics.     

Vortex fluctuations in underdoped Bi(2)Sr(2)CaCu(2)O(8+delta) crystals

Vortex thermal fluctuations in heavily underdoped Bi(2)Sr(2)CaCu(2)O(8+delta) (T(c)=69.4 K) are studied using Josephson plasma resonance. From the zero-field data, we obtain the c-axis penetration depth lambda(L,c)(0)=230+/-10 micrometer and the anisotropy ratio gamma(T). The low plasma frequency allows us to study phase correlations over the whole vortex solid state and to extract a wandering length r(w) of vortex pancakes. The temperature dependence of r(w) as well as its increase with dc magnetic field is explained by the renormalization of the vortex line tension by the fluctuations, suggesting that this softening is responsible for the dissociation of the vortices at the first order transition.     

The nu(2) Band of Formaldehyde-d(2)

High-resolution Fourier transform infrared spectrum of the nu(2) band (1590-1780 cm(-1)) of deuterated formaldehyde D(2)CO has been recorded. More than 2500 rovibrational transitions have been assigned up to J(max) = 52 and K(max)(a) = 17. The upper state v(2) = 1 (A(1)) was found to be perturbed by a DeltaK(a) = 2 interaction with the v(4) = 2 (A(1)) state. To explain the resonance perturbation in the v(2) = 1 state, some lines of the 2nu(4) band (the band center at about 1868 cm(-1)) have also been assigned. Both bands were fitted simultaneously to the Watson-type rotational Hamiltonian using I(r) representation in A reduction, and the mutual interaction was taken into account. As a result, the rotational parameters of the v(2) = 1 state up to eighth order and the interaction parameter have been obtained. Copyright 2001 Academic Press.     

Quasiparticles in the superconducting state of Bi(2)Sr(2)CaCu(2)O(8+delta)

Recent improvements in momentum resolution lead to qualitatively new angle-resolved photoemission spectroscopy results on the spectra of Bi(2)Sr(2)CaCu(2)O(8+delta) (Bi2212) along the (pi,pi) direction, where there is a node in the superconducting gap. We now see the intrinsic line shape, which indicates the presence of true quasiparticles at all Fermi momenta in the superconducting state, and lack thereof in the normal state. The region of momentum space probed here is relevant for charge transport, motivating a comparison of our results to conductivity measurements by infrared reflectivity.     

The (29)Si T(1) and T(2) NMR relaxation in porous paramagnetic material SiO(2)-MnO-Al(2)O(3)

The (29)Si spin-lattice relaxation in porous silica-based material 1, doped by ions Mn(2+) at a Si/Mn ratio of 3.5, is non-exponential, independent of magic-angle spinning (MAS) rates and governed by direct dipolar coupling between electron and nucleus where an electron relaxation time is estimated to be about 10(-8)s. In the absence of mutual energy-conserving spin flips (spin diffusion) in 1, the (29)Si T(2) time increases linearly with spinning rates. None was observed in diamagnetic porous system 2. The unexpected (29)Si T(2) dependence has been interpreted in terms of the large bulk magnetic susceptibility (BMS) effects. It has been shown that editing the (29)Si Hahn-echo MAS NMR spectra eliminates wide lines, belonging to (29)Si nuclei in the proximity of paramagnetic centers, and reduces the BMS broadenings in sideband patterns for nuclei remote from these centers.