铌和过氧铌取代Dawson结构钨磷杂多配合物的氧化还原性质研究

本文用电化学方法研究了铌和过氧铌一、三取代Ｄｗｓｏｎ结构杂多配合物：ａ２－ＭａＨｂＰ２Ｗ１５ＮｂＯ６２．ｘＨ２Ｏ，ａ－１，２，３－ＭａＨｂＰ２Ｗ１５Ｎｂ３Ｏ６２．ｘＨ２Ｏ，ａ２－ＭａＨｂＰ２Ｗ１７（ＮｂＯ２）Ｏ６１．ｘＨ２Ｏ，ａ－１，２，３－ＭａＨｂＰ２Ｗ１５（ＮｂＯ２）３Ｏ５９．ｘＨ２Ｏ（Ｍ＝Ｋ，ＴＭＡ，ＴＥＡ和ＴＢＡ）共十六种盐的氧化还原性质。     

镧系四元混配化合物[Ln（BA）2（NO3）（phen）]2的合成,晶？…

在酸性介质,含水溶剂中合成了四元混配化合物「Ｌｎ（ＢＡ）２（ＮＯ３）（ｐｈｅｎ）」（ＢＡ＝苯甲酸根;Ｌｎ＝Ｌａ,Ｃｅ,Ｐｒ,Ｎｄ,Ｓｍ,Ｅｕ,Ｄｙ,Ｇｄ,Ｔｂ,Ｅｒ）,用元素分析、ＩＲ、ＤＴＡ＿ＴＧ等方法对配合物进行了珠征,研究服配合物的顺磁性能和荧光性能,镨配合物的单晶衍射结果表明,配合物属三斜晶系,双核,Ｐｒ＾３＋的配位数为９,４个ＢＡ呈二种配位方式,丰富了四元配合物的结构表现形式。     

5，14－二氢－6，8，15，17－四甲基二苯并［b，i］［1，4，8，11］四氮杂［14］轮烯金属配合物的合成和反应性研究

合成了二苯并四氮杂［１４］轮烯金属配合物ＴＭＴＡＡＮｉ（Ⅱ），ＴＭＴＡＡＣｕ（Ⅱ）和ＴＭＴＡＡＶ＝Ｏ，通过ＴＭＴＡＡＭ（Ⅱ）分子中金属离子Ｍ（Ⅱ）对位碳原子上发生酰化反应，获得了十个酰化产物，用元素分析，ＩＲ，ＵＶ，１￣ＨＮＭＲ，（１９）￣ＦＮＭＲ和ＥＰＲ等进行了表征。酰化反应的发生说明了这类金属配合物具有类芳香性，并为改善这类大环金属配合物的光－电性能提供了良好的途径。     

配合物C30H58O4N2·Cu(Ⅱ)的合成与表征

ＥＤＴＡ与金属离子络合时 ,一般只有二个羧基和两个Ｎ原子参加配位 ,另两个羧基没参加配位。ＥＤＴＡ二钠盐及其与金属的配合物均能溶于水 ,在有机溶剂中溶解性差不利于萃取。本文将十二烷基引入ＥＤＴＡ二钠分子 ,制备了配体Ｎ ,Ｎ′-二 (十二烷基 )乙二胺二乙酸二钠盐 ,它作为铜的萃取剂 ,萃取率高。用红外光谱、元素分析、核磁共振、紫外光谱及摩尔电导对其铜配合物进行了表征。1　实验部分1 1　主要仪器和试剂美国ＮＩＣＯＬＥＴ360 -ＰＴ型红外光谱仪 ,ＫＢｒ压片 ;岛津ＵＶ -紫外分光光度计 ;ＤＤＳ - 1 2数字电导率仪 ;德国Ｂｒａ…     

铍（Ⅱ）—均三溴偶氮胂配合物吸附波的研究

在ｐＨ９．２０的ＮＨ３．Ｈ２Ｏ－ＮＨ４Ｃｌ介质中，铍与均三溴偶氮胂（ＴＢＡ）的形成配合物，于－０．５５Ｖ（ｖｓ．ＳＣＥ）处产生一灵敏的配合物吸附波，峰电流与Ｂｅ浓度在８．０×１０＾－８～２．０×１０＾－６ｍｏｌ／Ｌ范围内呈线性关系。测得铍与均三溴偶氮胂的配合比为Ｂｅ（Ⅱ）：ＴＢＡ＝１：１，稳定常数β＝３．０×１０＾，电子转移数ｎ＝２，峰电流由配合物中配位体ＴＢＡ还原产生。可不经分离直接测定矿样中铍     

配位滴定法连续测定铁铝钛的研究及应用：5Br—PADAP作指示剂

以５－Ｂｒ－ＰＡＤＡＰ作指示剂，ＰＨ１．８－２．２ＥＤＴＡ滴定铁（Ⅲ）；用过量的ＥＤＴＡ在ＰＨ３煮沸下与钛和铝生成稳定的配合物，再以苦杏仁酸，氟化钾分别置换Ｔｉ－ＥＤＴＡ，Ａｌ－ＥＤＴＡ配合物中的ＥＤＴＡ，用硫酸铜回滴法于ＰＨ４．８分别测定钛和铝。     

噻吩甲酰三氟丙酮和4,5-二氮芴-9-酮及4,5-二氮芴-9-酮连氮铕(Ⅲ)三元配合物的合成和表征

合成了Ｅｕ（ＴＴＡ）３Ｌ１（Ⅰ）和［Ｅｕ（ＴＴＡ）３］２Ｌ２（Ⅱ）二种新的铕（Ⅲ）三元配合物（ＴＴＡ＝噻吩甲酰三氟丙酮一价阴离子、Ｌ１＝４，５－二氮芴－９－酮、Ｌ２＝４，５－二氮芴－９－酮连氮）。用元素分析、ＩＲ、ＵＶ和溶液荧光光谱对配合物进行了表征。探讨了溶剂对Ｅｕ（Ⅲ）三元配合物荧光光谱的影响，发现在ＣＨ３ＣＮ中Ｅｕ（Ⅲ）三元配合物发光效果最好，而溶剂ＤＭＦ会使配合物荧光减弱     

EDTA—Cu配合物用于还原糖的测定

首次报道了应用ＥＤＴＡ（乙二胺四乙酸二钠盐）－铜配合物（ＥＣ）测定还原糖的分光光度法，结果表明，ｐＨ４～１１时ＥＣ的最大吸收波长为７３２ｎｍ，在ＨＣＯ－３ＣＯ２－３缓冲介质中，配合物ＥＣ的吸光度与还原糖在０７７～１６１ｍｇ（六碳糖）范围内有很好的线性关系，相关系数大于０９９８，样品测定回收率在９５％～１０５％之间。该法试剂易得、性质稳定，操作方便，灵敏度较高，取样量少于５ｍＬ。     

1—羟基—2（1H）—吡啶硫酮及其甲基衍生物与Au（Ⅲ）配合物的合成和性质

合成了１－羟基－２－（１Ｈ）－吡啶硫酮及其甲基衍生物［ＡｕＬ２］ＯＨ型配合物（Ｌ＝ＰＴ＾－，３－ＣＨ３－ＰＴ＾－Ｔ ４－ＣＨ３－ＰＴ＾－）。用元素，紫外光谱，外红光谱，＾１ＨＮＭＲ谱，摩尔电导，ＴＧＤＴＡ－ＤＴＧ进行了表征，用循环伏安法研究其氧化还原性质，含甲基的配合物有较强的抑菌活性     

铕离子在乙二醇低聚物中的配合作用与电化学行为

研究了乙二醇低聚物（ＰＥＧ）与Ｅｕ（２＋）及Ｅｕ（３＋）所形成配合物的结构，荧光性质和电化学行为．Ｅｕ（３＋）的配合物是由ＥｕＣｌ３溶于具有不同摩尔质量的ＰＥＧ而成的．它们在３９４ｎｍ和６１４ｎｍ处分别有很强的激发和发射光谱峰，并且这两峰的强度随着ＰＥＧ的摩尔质量的增大而加强．Ｅｕ（２＋）的配合物是通过用涂布有氧化铟及氧化锡的玻璃板作为工作电极，在氮气气氛下，加－２Ｖ（ｖｓＡｇ）电压还原ＥｕＣｌ３的ＰＥＧ溶液来制备的．它们的荧光性质和１８—Ｃ—６冠醚与Ｅｕ（２＋）所形成配合物的性质非常接近，从而表明ＰＥＧ的化学环境与大环聚醚配体的很相似．进一步的红外与荧光谱实验结果表明：铕离子不但与聚乙二醇的末端－ＯＨ基团结合，而且亦能与链中间的氧原子作用．随着聚合物分子量的增大，铕离子的点对称性不断下降．Ｅｕ（３＋）在聚合物中的氧化还原很不可逆．添加支持盐对其电化学行为有很大影响．     

四苯基[b,f,j,n][1,5,9,13]四氮杂环十六碳炔镍轴向氮碱加合物的合成、结构和性质研究

合成了3个四苯基[b,f,j,n][1,5,9,13]四氮杂环十六碳炔镍轴向氮碱加合物[Ni(TAAB)(L)_2](BF_4)_2(L为吡啶、咪唑、DMF)以及4,4′-联吡啶桥联配合物[Ni(TAAB)(μ-4,4′-bipy)]。[(ClO_4)_2·H_2O]_((??))。用元素分析、IR和热分析对标题化合物作了表征。双吡啶加合物的晶体结构显示,TAAB大环呈马鞍形结构,轴向配位的吡啶环平面相互垂直,轴向的2个Ni—N键长明显比赤道平面的4个Ni—N键长大,形成拉长的配位八面体。4,4′-联吡啶配合物的变温磁化率表明,镍(Ⅱ)离子间存在反铁磁性磁交换相互作用。     

Synthesis and structures of gallium amido imido phenyl clusters (PhGa)(4)(NH(i)Bu)(4)(N(i)Bu)(2) and (PhGa)(7)(NHMe)(4)(NMe)(5)

The phenylgallium-containing clusters constructed with bridging imido and amido ligands, (PhGa)(4)(NH(i)Bu)(4)(N(i)Bu)(2) (1) (51% yield) and (PhGa)(7)(NHMe)(4)(NMe)(5) (2) (31% yield), were synthesized from the room-temperature reactions of bis(dimethylamido)phenylgallium, [PhGa(NMe(2))(2)](2), with isobutylamine and methylamine, respectively. The reaction of [PhGa(NMe(2))(2)](2) in refluxing isobutylamine (85 degrees C) afforded (Ph(2)GaNH(i)Bu)(2) as one of the products, while the reaction of [PhGa(NMe(2))(2)](2) with methylamine at 150 degrees C afforded compound 2 in only 9% yield. Compound 1 possessed an admantane-like Ga(4)N(6) core, whereas compound 2 had a novel Ga(7)N(9) core constructed with both chair- and boat-shaped Ga(3)N(3) rings. The presence of several isomers of compounds 1 and 2 in solution is discussed along the structural similarities with other known gallium-nitrogen clusters and with gallium nitride.     

Rhenium-to-benzoylpyridine and rhenium-to-bipyridine MLCT excited states of fac-[Re(Cl)(4-benzoylpyridine)(2)(CO)(3)] and fac-[Re(4-benzoylpyridine)(CO)(3)(bpy)](+): a time-resolved spectroscopic and spectroelectrochemical study

The lowest allowed electronic transition of fac-[Re(Cl)(CO)(3)(bopy)(2)] (bopy = 4-benzoylpyridine) has a Re --> bopy MLCT character, as revealed by UV-vis and stationary resonance Raman spectroscopy. Accordingly, the lowest-lying, long-lived, excited state is Re --> bopy (3)MLCT. Electronic depopulation of the Re(CO)(3) unit and population of a bopy pi orbital upon excitation are evident by the upward shift of nu(CO) vibrations and a downward shift of the ketone nu(C=O) vibration, respectively, seen in picosecond time-resolved IR spectra. Moreover, reduction of a single bopy ligand in the (3)MLCT excited state is indicated by time-resolved visible and resonance Raman (TR(3)) spectra that show features typical of bopy(*)(-). In contrast, the lowest allowed electronic transition and lowest-lying excited state of a new complex fac-[Re(bopy)(CO)(3)(bpy)](+) (bpy = 2,2'-bipyridine) have been identified as Re --> bpy MLCT with no involvement of the bopy ligand, despite the fact that the first reduction of this complex is bopy-localized, as was proven spectroelectrochemically. This is a rare case in which the localizations of the lowest MLCT excitation and the first reduction are different. (3)MLCT excited states of both fac-[Re(Cl)(CO)(3)(bopy)(2)] and fac-[Re(bopy)(CO)(3)(bpy)](+) are initially formed vibrationally hot. Their relaxation is manifested by picosecond dynamic shifts of nu(C(triple bond)O) IR bands. The X-ray structure of fac-[Re(bopy)(CO)(3)(bpy)]PF(6).CH(3)CN has been determined.     

Syntheses, structural determination, and electrochemistry of Ru(2)(Fap)(4)Cl and Ru(2)(Fap)(4)(NO)Cl

Ru(2)(Fap)(4)Cl and Ru(2)(Fap)(4)(NO)Cl, where Fap is the 2-(2-fluoroanilino)pyridinate anion, were synthesized, and their structural, electrochemical, and spectroscopic properties were characterized. Ru(2)(Fap)(4)Cl, which was obtained by reaction between Ru(2)(O(2)CCH(3))(4)Cl and molten HFap, crystallizes in the monoclinic space group P2(1)/c, with a = 11.2365(4) A, b = 19.9298(8) A, c = 19.0368(7) A, beta = 90.905(1) degrees, and Z = 4. The presence of three unpaired electrons on the Ru(2)(5+) core and the 2.2862(3) A Ru-Ru bond length for Ru(2)(Fap)(4)Cl are consistent with the electronic configuration (sigma)(2)(pi)(4)(delta)(2)(pi*)(2)(delta*)(1). The reaction between Ru(2)(Fap)(4)Cl and NO gas yields Ru(2)(Fap)(4)(NO)Cl, which crystallizes in the orthorhombic space group Pbca, with a = 10.0468(6) A, b = 18.8091(10) A, c = 41.7615(23) A, and Z = 8. The Ru-Ru bond length of Ru(2)(Fap)(4)(NO)Cl is 2.4203(8) A, while its N-O bond length and Ru-N-O bond angle are 1.164(8) A and 155.8(6) degrees, respectively. Ru(2)(Fap)(4)(NO)Cl can be formulated as a formal Ru(2)(II,II)(NO(+)) complex with a linear Ru-N-O group, and the proposed electronic configuration for this compound is (sigma)(2)(pi)(4)(delta)(2)(pi*)(3)(delta*)(1). The binding of NO to Ru(2)(Fap)(4)Cl leads to some structural changes of the Ru(2)(Fap)(4) framework and a stabilization of the lower oxidation states of the diruthenium unit. Also, IR spectroelectrochemical studies of Ru(2)(Fap)(4)(NO)Cl show that NO remains bound to the complex upon reduction and that the first reduction involves the addition of an electron on the diruthenium core and not on the NO axial ligand.     

Synthesis and properties of [Ru(2)(acac)(4)(bptz)](n+) (n=0,1) and crystal structure of [Ru(2)(acac)(4)(bptz)

The neutral complex [Ru(2)(acac)(4)(bptz)] (I) has been prepared by the reaction of Ru(acac)(2)(CH(3)CN)(2) with bptz (bptz = 3,6-bis(2-pyridyl)-1,2,4,5-tetrazine) in acetone. The diruthenium(II,II) complex (I) is green and exhibits an intense metal-ligand charge-transfer band at 700 nm. Complex I is diamagnetic and has been characterized by NMR, optical spectroscopy, IR, and single-crystal X-ray diffraction. Crystal structure data for I are as follows: triclinic, P1, a = 11.709(2) A, b = 13.487(3) A, c = 15.151(3) A, alpha = 65.701(14) degrees, beta = 70.610(14) degrees, gamma = 75.50(2) degrees, V = 2038.8(6) A(3), Z = 2, R = 0.0610, for 4397 reflections with F(o) > 4sigmaF(o). Complex I shows reversible Ru(2)(II,II)-Ru(2)(II,III) and Ru(2)(II,III)-Ru(2)(III,III) couples at 0.17 and 0.97 V, respectively; the 800 mV separation indicates considerable stabilization of the mixed-valence species (K(com) > 10(13)). The diruthenium(II,III) complex, [Ru(2)(acac)(4)(bptz)](PF(6)) (II) is prepared quantitatively by one-electron oxidation of I with cerium(IV) ammonium nitrate in methanol followed by precipitation with NH(4)PF(6). Complex II is blue and shows an intense MLCT band at 575 nm and a weak band at 1220 nm in CHCl(3), which is assigned as the intervalence CT band. The mixed valence complex is paramagnetic, and an isotropic EPR signal at g = 2.17 is observed at 77 and 4 K. The solvent independence and narrowness of the 1200 nm band show that complex II is a Robin and Day class III mixed-valence complex.     

Preparation and characterization of the fullerene diols 1,2-C(60)(OH)(2), 1,2-C(70)(OH)(2), and 5,6-C(70)(OH)(2)

The simple fullerene diols C(60)(OH)(2) and C(70)(OH)(2) were prepared by addition of RuO(4) followed by acid hydrolysis. The 1,2-C(60)(OH)(2) isomer was formed from C(60), and two isomers (1,2 and 5,6) of C(70)(OH)(2) were formed in the RuO(4) hydroxylation of C(70). These compounds are much more soluble in THF and dioxane than the parent fullerenes. More highly hydroxylated materials are formed as well.     

Transient mixed-valence character of Re(I)(4)(CO)(12)(4,4'-bpy)(4)Cl(4)

This study addresses, in detail, the orbital nature and the extent of metal-metal communication in the lowest emitting triplet state of Re(4)(CO)(12)(4,4'-bpy)(4)Cl(4) (where 4,4'-bpy = 4,4'-bipyridine) as well as the symmetry of the lowest (3)MLCT manifold in comparison to that of the ground state. All spectral evidence points to (1). a (3)MLCT excited manifold localized between a single Re(I) corner and an adjacent bridging ligand, (2). a transient mixed-valence state that is completely localized between a single transiently oxidized Re center and the adjacent metals, and (3). a second-order charge transfer from a localized transiently reduced bridging ligand to the adjacent Re(I) center to which it is attached, effectively lowering its oxidation state. The orbital nature of the lowest (3)MLCT manifold is fully corroborated by a molecular orbital diagram derived from quantum chemical modeling studies, while the existence of the localization, localized mixed valency, and second-order charge transfer rely on spectral evidence alone. This work makes use of low-temperature time-resolved infrared (TRIR) techniques as well as a luminescence study. Many of the nuances of the luminescence and TRIR data interpretation are extracted from statistical analysis and quantum chemical modeling studies. The relative concentrations of the dominant conformers that exist for Re(4)(CO)(12)(4,4'-bpy)(4)Cl(4) have also been estimated from Boltzmann statistics.     

Structure determination and infrared spectroscopy of K(UO2)(SO4)(OH)(H2O) and K(UO2)(SO4)(OH)

Two potassium uranyl sulfate compounds were synthesized, and their crystal structures were determined by single-crystal X-ray diffraction. K(UO2)(SO4)(OH)(H2O) (KUS1) crystallizes in space group P21/c, a = 8.0521(4) A, b = 7.9354(4) A, c = 11.3177(6) A, beta = 107.6780(10) degrees , V = 689.01(6) A3, and Z = 4. K(UO2)(SO4)(OH) (KUS2) is orthorhombic Pbca, a = 8.4451(2) A, b = 10.8058(4) A, c = 13.5406(5)A, V = 1235.66(7)A3, and Z = 8. Both structures were refined on the basis of F2 for all unique data collected with Mo Kalpha radiation and a CCD-based detector to agreement indices R1 = 0.0251 and 0.0206 calculated for 2856 and 2616 reflections for KUS1 and KUS2, respectively. The structures contain vertex-sharing uranyl pentagonal bipyramids and sulfate tetrahedra linked into new chains and sheet topologies. Infrared spectroscopy provides additional information about the linkages between the sulfate and uranyl polyhedra, as well as the hydrogen bonding present in the structures. The U-O-S connectivity is examined in detail, and the local bond angle is impacted by the steric constraints of the crystal structure.