聚苯乙炔LB多层膜及其光电导性能的研究

制备了聚苯乙炔（ＰＰＡ）ＬＢ多层膜，将其作为电荷产生层首次应用于机能分离型光电导体领域．从π Ａ曲线发现，ＰＰＡ单分子膜具有表面压力的各向异性和松弛特性．ＴＥＭ照片显示，ＰＰＡ分子链在ＬＢ膜中有序排列．转移比和ＸＰＳ的研究表明，复合膜沉积均匀．与ＰＰＡ涂膜相比，以ＰＰＡ ＬＢ多层膜作为电荷产生层的光电导体表面充电电位Ｖ０＝１３４５Ｖ，光照１ｓ后的光衰百分比ΔＶ１ｓ＝６５０５％，半衰时间ｔ１／２＝０５８ｓ，具有更优异的光电导性能．     

聚甲基丙烯酸甲酯Langmuir—Blodgett复合膜及其在光电导体中…

制备了聚甲基丙烯酸甲酯（ＰＭＭＡ）ＬＢ复合膜，将其作为阻挡层首次应用于机能分离型光电导体领域。从π－Ａ曲线发现ＰＭＭＡ单分子膜具有表面压力的各向异性和松弛特性。ＴＥＭ照片显示，ＰＭＭＡ分子链在复合膜中有序排列。转移比、ＵＶ和ＸＰＳ研究表明，复合膜沉积均匀。以ＰＭＭＡ－ＬＢ复合膜作为阻挡层的光电导体表面充电电位Ｖ０＝１５１８Ｖ，光照１ｓ后的光衰百分率△Ｖ１ｓ＝５０．１６％，半衰期ｔ１／２＝０．９３ｓ     

新型水溶性大π共轭高分子——聚吡咯｛2,5-[双(对二甲氨基苯甲烯)]｝的合成

该研究合成了一种新型水溶性大π共轭高分子———聚吡咯 ｛２ ,５ ［ 二（ 对二甲氨基苯甲烯）］｝（ＰＰＤＭＡＢ） ,它能溶于强酸的水溶液,在１ｍｏｌ／Ｌ 的盐酸中溶解度为０－５ ～１－０ｇ／１００ｍＬ．通过ＥＡ、ＸＰＳ、ＦＴ ＩＲ、ＵＶ Ｖｉｓ ＮＩＲ、Ｉｎ ｓｉｔｕ ＵＶ Ｖｉｓ ＮＩＲ 对ＰＰＤＭＡＢ进行了结构表征．通过质子化、碘掺杂、浓硫酸（９８ ％ ） 掺杂等处理,ＰＰＤＭＡＢ的电导率提高２～４ 个数量级（δ＝ １０ － ７ ～１０－ ５Ｓ／ｃｍ） ．在质子化、去质子化的过程中ＰＰＤＭＡＢ发生了可逆的颜色变化,本征态（ 综色） 质子态（ 墨兰色） ．     

修饰微带金电极上细胞色素C电极过程的热力学研究

研究了细胞色素Ｃ（Ｃｙｔ．Ｃ）在一种新的电子转移促进剂４，６－二甲基－２－巯基嘧啶修饰微带金电极（ＤＭＭＰ／Ａｕ）上的氧化还原热力学；求得Ｃｙｔ．Ｃ在ＤＭＭＰ／Ａｕ电极上反应的标准电极电位Ｅ＾ｏ，熵变△Ｓ＾ｏ，焓变△ＩＩ＾ｏ及Ｇｉｂｂｓ自由能的改变△Ｇ１０值分别为：０．２７２Ｖ（ｕｓ．ＮＨＥ），－１２３．７Ｊ．ｍｏｌ＾－＾１，－６３．１ｋＪ．ｍｏｌ．ｍｏｌ＾－＾１和－２６．２ｋＪ．ｍｏｌ＾－＾１（     

不对称烷氧基取代聚对苯乙炔的合成及电致发光性能

利用强碱诱导的去卤缩合聚合法，合成了不对称烷氧基取代的聚（２－甲氧基－５－十二烷氧基－１，４－对苯乙炔）（ＰＭＤＰＶ）．其溶解性和成膜性能优于对称取代的聚（２，５－双十二烷氧基－１，４－对苯乙炔）．以ＰＭＤＰＶ为发光层质的聚合物电致发光器件，其发光峰值波长为６０５ｎｍ．并用ＩＲ、ＵＶ－Ｖｉｓ、ＴＧＡ、１ＨＮＭＲ、ＧＰＣ等对所合成的聚合物进行了表征．     

新型大溶性大π共轭高分子—聚吡咯—{2,5—[双（对二甲氨基苯甲烯）]}？…

该研究合成了一种新型水溶性大π共轭高分子－聚吡咯－｛２,５－〔二（对二甲氨基苯甲烯）〕｝（ＰＰＤＭＡＢ）,它地强酸的水溶液,在１ｍｏｌ／Ｌ的盐酸中溶解度为０．５～１．０g／１００mＬ,通过ＥＡ、ＸＰＳ、ＦＴ－ＩＲ、ＵＶ－Ｖｉｓ－ＮＩＲ、Ｉｎ－ｓｉｔｕＵＶ－Ｖｉｓ－ＮＩＲ对ＰＰＤＭＡＢ进行了结构表征。通过质子化、碘掺杂、浓硫酸（９８％）掺杂等处理,ＰＰＤＭＡＢ的电导率提高２～４个数量组（＆＝１－＾－７     

苯乙烯—二乙烯苯自由基共聚反应动力学研究

本文用气相色谱、激光拉曼、激光散射、ＧＰＣ以及粘度等方法研究了苯乙烯—二乙烯苯的自由基交联共聚反应．求得聚合反应初期的表现速率常数Ｋｓｔ、Ｋｍ－ＤＶＢ及Ｋｐ－ＤＶＢ分别为１．６８×１０－２（小时－１）、３．４３×１０－２（小时－１）及５．５４×１０－２（小时－１）；从悬挂双键含量变化解释分子内环化推迟了凝胶化点；由跟踪检测反应中分子重量、尺寸变化指出宏观尺寸分子的出现使重均分子量（）在凝胶化点发散；讨论了多分散、支化对分子尺寸Ｒｇ（均方旋转半径）、Ｒｈ（流体力学半径）的影响，定量关系为：δ＝Ｒｇ／Ｒｈ＝０．００６１ｅｘＰ（１．４３２ｔ）；拟合了Ｒｈ对反应时间的指数依赖性ＲＡ＝５．１９５ｅｘｐ（０．８７２ｔ），这证实了凝胶化点前属反应控制机理。     

8—氮鸟嘌呤的极谱伏安行为

用循环伏安法（ＣＶ）、电流采样极诸法（ＳＣＰ，即ＴＡＳＴ）、常规脉冲极谱法（ＮＰＰ）、微分脉冲极谱法（ＤＰＰ）、线性扫描伏安法（ＬＳＶ）、Ｏｓｔｅｒｙｏｕｎｇ方波伏安法（ＯＳＷＶ）和计时库仑法（ＣＣ）等电化学技术研究了抗癌药物８－氮鸟嘌呤（８－ａｚａｇｕａｎｉｎｅ，ｇｕａｎａｚｏｌｏ，简称８－ＡＧ）的极谱伏安行为．在 ０． １ｍｏｌ／Ｌ Ｈ２ＳＯ４底液中，８－ＡＧ有一良好的还原峰，峰电位（Ｅｐ）在－０． ９５Ｖ（ｖｓ．Ａｇ／ＡｇＣｌ，下同）附近，８－ＡＧ浓度在４×１０－６～８×１０－４ｍｏｌ／Ｌ范围内．峰高与浓度有良好的线性关系，线性相关系数ｒ＝０．９９９９～０．９９１０，检出限为１× １０－６ｍｏｌ／Ｌ．实验证明了该峰具有吸附性．本文提出了电极反应机理，它包括：酸性介质中８－ＡＧ的质子化、质子化的８－ＡＧ在汞电极上吸附以及完全不可逆的两电子还原过程．同时用量子化学计算方法（全略微分重叠法即ＣＮＤＯ／２）对８－ＡＧ和鸟嘌呤的各原子的净电荷以及Ｗｉｂｅｒｇ键级进行了计算，从理论上解释了８－ＡＧ的电化学还原机理。     

Studies on Phosphate Effect of Cytosine and Its Novel Photoproduct

ＩｎｔｒｏｄｕｃｔｉｏｎＩｎ１９６３，ＭｏｏｒＡ．Ｍ．［１］ｆｉｒｓｔｌｙｒｅｐｏｒｔｅｄｔｈｅｐｈｏｓｐｈａｔｅｅｆｅｃｔ，ｉ．ｅ．，ｉｎｔｈｅＵＶｉｒｒａｄｉａｔｉｏｎ（２５３．７ｎｍ）ｏｆａｑｕｅｏｕｓｓｏｌｕｔｉｏｎｓｏｆ４－ａｍｉｎｏ－２－...     

氢化物发生—冷阱捕获—色谱分离—原子吸收法测定天然水中坤的形态

研究建立了氢化物发生－冷阱捕获－色谱分离－原子吸收方法测定天然水中四种主要砷形态，测试系统自行组装，色谱柱填料采用ＣｈｒｏｍｏｓｏｒｂＧＡＷ－ＤＭＣＳ（粒径０．３～０．４５ｍｍ），其上涂布３％ＯＶ－１０１。方法的检出限以砷计分别为：Ａｓ（Ｖ）０．５１ｎｇ，Ａｓ（Ⅲ）０．４３ｎｇ，ＭＭＡ０．３８ｎｇ，ＤＭＡ０．６７ｎｇ；１２ｎｇ砷标准偏差为Ａｓ（Ⅴ）４．２１％，Ａｓ（Ⅱ）３．５６％，ＭＭＡ３．２３％     

ClInPc-(TPD-PVK)光电导体性能的研究

本文以氯化酞菁铟(ClInPc)为载流子发生层(CGL),四苯基联苯胺(TPD)与聚乙烯咔唑(PVK)复合为载流子传输层(CTL),形成双层结构的功能分离型有机光电导体(P/R),研究了它的静电感光性能。结果表明,ClInPc/PMMA(30%)与TPD/PVK(1:1)两者匹配时的P/R具有良好的光电导性能,其电荷接受能力V_max≈800V,光电导率△V_t(ls)>70%,暗衰小(<50V/s),残余电位低(30V/s).由真空蒸镀成膜(CGL)所研制的P/R的光电导性能更为优异。     

A solid-state spectral effect in eclipsed tetracyanonickelates: X-ray crystal structure, polarized specular reflectance spectroscopy, and ZINDO modeling of Sr[Ni(CN)4].5H2O, Rb2[Ni(CN)4].H2O, and Na2[Ni(CN)4].3H2O

Crystal structures of three Ni(CN)(4)(2)(-) salts all with eclipsed ligands and varying axial stacking arrangements are presented. The absorption spectra of all three salts show a slight red shift in the x,y-polarizations and a large red shift in their z-polarizations upon crystallization from solution. Semiempirical ZINDO calculations provide a good model of the solid state, even with only a three-molecule segment, allowing reproduction of the red-shifting and intensity increase upon crystallization found experimentally. The modified nickel beta(s,p) bonding parameter of -5 found appropriate for Ni coordination in our previous studies of single Ni(CN)(4)(2-) planes and a helically stacked Cs(2)[Ni(CN)(4)].H(2)O crystal was changed to -3 for the more parallel-stacked Ni(CN)(4)(2-) planes in this case, while beta(d) was retained at -41. Crystal data are as follows: Na(2)[Ni(CN)(4)].3H(2)O, triclinic space group P1, a = 7.2980(10) A, b = 8.8620(10) A, c = 15.132(2) A, alpha = 89.311(5) degrees, beta = 87.326(5) degrees, gamma = 83.772(6) degrees, V = 971.8(2) A(3), T = 100 K, Z = 4, R = 0.024, R(w) = 0.064; Sr[Ni(CN)(4)].5H(2)O, monoclinic space group C2/m, a = 10.356(2) A, b = 15.272(3) A, c = 7.1331(10) A, beta = 98.548(12) degrees, V = 1115.6(3) A(3), T = 100 K, Z = 4, R = 0.024, R(w) = 0.059; Rb(2)[Ni(CN)(4)].1.05H(2)O, triclinic space group P1, a = 8.6020(10) A, b = 9.6930(10) A, c = 12.006(2) A, alpha = 92.621(6) degrees, beta = 94.263(6) degrees, gamma = 111.795(10) degrees, V = 924.0(2) A(3), T = 100 K, Z = 4, R = 0.034, R(w) = 0.067.     

Synthesis and Crystal Structure of 〔Co_3(CO)_9(μ_3-C)C(O)OCH_2〕_2

１ＩＮＴＲＯＤＵＣＴＩＯＮＩｎｒｅｃｅｎｔｙｅａｒｓ,ｈｉｇｈｅｒ ｎｕｃｌｅａｒｉｔｙｃｌｕｓｔｅｒｓｈａｖｅｒｅｃｅｉｖｅｄｃｏｎｓｉｄｅｒａｂｌｅａｔｅｎｔｉｏｎｂｅｃａｕｓｅｏｆｔｈｅｉｒｐｏｔｅｎｔｉａｌａｐｐｌｉｃａｔｉｏｎｓｉｎｍａｎｙ...     

Effect of 1,8-Diiodooctane Content on the Performance of P3HT:PC61BM Bulk Heterojunction Photodetectors

A series of polymer photodetectors with device configuration of ITO/PEDOT:PSS/P_3 HT:PC_(61) BM/C_(60)/Al were prepared by using P_3 HT as the donor material and PC_(61) BM as the acceptor material. By regulating the content of 1,8-diiodooctane(DIO)(V/V: 1%, 3%, 5%) as a processing additive, the morphology of the active layer can be greatly improved. With C_(60) as the hole blocking layer, the dark current density of the device can be reduced by about an order of magnitude. When employing 3% DIO(V/V) in the active layer processing, the photodetetcors present the best performance, and the detectivity of the device is 1.52×10~(12) Jones at 540 nm under a bias of-0.1 V. Moreover, it also has a wider linear dynamic range of 60 dB as well as faster response speed(τ_r/τ_f=0.53/0.71 μs) than those of devices with other content of DIO additives.     

Syntheses and Structures of Two New Coordination Polymers:[Cu(C_(14)H_9O_4)(C_(14)H_(10)O_4)(C_(12)H_(12)N_2)_2] and [Ag(C_(14)H_9O_4)(C_(13)H_(14)N_2)]·0.5H_2O

1 INTRODUCTION Supramolecular approaches to self-assembly of infinite molecular solids with novel structural topo- logies attract considerable attention for their po- tential applications as functional materials and their fascinating architectures[1]. In…     

Hydrocarbon-Soluble Mercuracarborands: Syntheses, Halide Complexes, and Supramolecular Chemistry

The syntheses of macrocyclic species composed of carborane derivatives joined via their carbon vertices by electrophilic mercury atoms are described. The reaction of closo-1,2-Li(2)[C(2)B(10)H(10)(-)(x)()R(x)()] with HgI(2) gives Li(2)[(1,2-C(2)B(10)H(10)(-)(x)()R(x)()Hg)(4)I(2)] [R = Et, x = 2 (5.I(2)Li(2)); R = Me, x = 2 (6.I(2)Li(2)); R = Me, x = 4 (7.I(2)Li(2))]. 6.I(2)(K.[18]dibenzocrown-6)(2) crystallizes in the monoclinic space group C2/m [a = 28.99(2) ?, b = 18.19(1) ?, c = 13.61(1) ?, beta = 113.74(2) degrees, V = 6568 ?(3), Z = 4, R = 0.060, R(w) = 0.070]; 7.I(2)(NBu(4))(2) crystallizes in the monoclinic space group P2(1)/c [a = 12.77(1) ?, b = 21.12(2) ?, c = 20.96(2) ?, beta = 97.87(2) degrees, V = 5600 ?(3), Z = 2, R = 0.072, R(w) = 0.082]. The precursor to 7, closo-8,9,10,12-Me(4)-1,2-C(2)B(10)H(8) (4), is made in a single step by reaction of closo-1,2-C(2)B(10)H(12) with MeI in trifluoromethanesulfonic acid. The free hosts 5, 6, and 7 are obtained by reaction of the iodide complexes with stoichiometric quantities of AgOAc. A (199)Hg NMR study indicates that sequential removal of iodide from 5.I(2)Li(2) and 6.I(2)Li(2) with aliquots of AgOAc solution leads to formation of two intermediate host-guest complexes in solution, presumed to be 5(6)ILi and 5(2)(6)(2).ILi. Crystals grown from a solution of 6.I(2)Li(2) to which 1 equiv of AgOAc solution had been added proved to be an unusual stack structure with the formula 6(3).I(4)Li(4) [tetragonal, I4/m, a = 21.589(2) ?, c = 21.666(2) ?, V = 10098 ?(3), Z = 2, R = 0.058, R(w) = 0.084]. Addition of 2 equiv of NBu(4)Br ion to 5 or 6 gives 5.Br(2)(NBu(4))(2) and 6.Br(2)(NBu(4))(2), respectively, while addition of 1 equiv of KBr to 6 forms 6.BrK. 5.Br(2)(NBu(4))(2) crystallizes in the triclinic space group P&onemacr;, [a = 10.433(1) ?, b = 13.013(1) ?, c = 15.867(2) ?, alpha = 91.638(2) degrees, beta = 97.186(3) degrees, gamma = 114.202(2) degrees, V = 1492 ?(3), Z = 1, R = 0.078, R(w) = 0.104]. The hosts 5 and 6 form 1:1 supramolecular adducts with the polyhedral anions B(10)I(10)(2)(-) and B(12)I(12)(2)(-) in solution.     

Imido transfer from bis(imido)ruthenium(VI) porphyrins to hydrocarbons: effect of imido substituents, C-H bond dissociation energies, and Ru(VI/V) reduction potentials

[Ru(VI)(TMP)(NSO2R)2] (SO2R = Ms, Ts, Bs, Cs, Ns; R = p-C6H4OMe, p-C6H4Me, C6H5, p-C6H4Cl, p-C6H4NO2, respectively) and [Ru(VI)(Por)(NTs)2] (Por = 2,6-Cl2TPP, F20-TPP) were prepared by the reactions of [Ru(II)(Por)(CO)] with PhI=NSO2R in CH2Cl2. These complexes exhibit reversible Ru(VI/V) couple with E(1/2) = -0.41 to -0.12 V vs Cp2Fe(+/0) and undergo imido transfer reactions with styrenes, norbornene, cis-cyclooctene, indene, ethylbenzenes, cumene, 9,10-dihydroanthracene, xanthene, cyclohexene, toluene, and tetrahydrofuran to afford aziridines or amides in up to 85% yields. The second-order rate constants (k2) of the aziridination/amidation reactions at 298 K were determined to be (2.6 +/- 0.1) x 10(-5) to 14.4 +/- 0.6 dm3 mol(-1) s(-1), which generally increase with increasing Ru(VI/V) reduction potential of the imido complexes and decreasing C-H bond dissociation energy (BDE) of the hydrocarbons. A linear correlation was observed between log k' (k' is the k2 value divided by the number of reactive hydrogens) and BDE and between log k2 and E(1/2)(Ru(VI/V)); the linearity in the former case supports a H-atom abstraction mechanism. The amidation by [Ru(VI)(TMP)(NNs)2] reverses the thermodynamic reactivity order cumene > ethylbenzene/toluene, with k'(tertiary C-H)/k'(secondary C-H) = 0.2 and k'(tertiary C-H)/k'(primary C-H) = 0.8.     

Synthesis,Structure and Electrochemistry of Triruthenium Cluster Complex [Ru_3(μ_3- O)(μ-CH_3CO_2)_6(py)_2(PPh_2py)](PF_6)·CH_2Cl_2

1 INTRODUCTION The transition metal cluster complexes exhi- biting multistep redox processes have attracted more and more attention because of their potential applications in the areas of photonic and electronic devices[1～4]. The oxo-centered carboxyla…     

Synthesis and Crystal Structure of Bis(nitrate)- bis(N,N''''-dimethyl-N,N''''-dibenzenyl-urea)uranyl(Ⅱ)

1 INTRODUCTION Tri-butyl phosphate (TBP) has been widely used as the extraction reagent in U-Th fuel to separate uranium from thorium. But di-butyl phos- phate (DBP) and butyl phosphate (MBP), the radio- lytic products of TBP, exhibit some coordinated ability to the fission elements, such as Zr and Nb. The substitutes for TBP have being studied for several decades[1～4]. The physical and chemical properties of amides are similar to those of TBP and they selectively extract U(Ⅵ…     

M-M bond-stretching energy landscapes for M2(dimen)4(2+) (M = Rh, Ir; dimen = 1,8-diisocyanomenthane) complexes

Isomers of Ir(2)(dimen)(4)(2+) (dimen = 1,8-diisocyanomenthane) exhibit different Ir-Ir bond distances in a 2:1 MTHF/EtCN solution (MTHF = 2-methyltetrahydrofuran). Variable-temperature absorption data suggest that the isomer with the shorter Ir-Ir distance is favored at room temperature [K = ～8; ΔH° = -0.8 kcal/mol; ΔS° = 1.44 cal mol(-1) K(-1)]. We report calculations that shed light on M(2)(dimen)(4)(2+) (M = Rh, Ir) structural differences: (1) metal-metal interaction favors short distances; (2) ligand deformational-strain energy favors long distances; (3) out-of-plane (A(2u)) distortion promotes twisting of the ligand backbone at short metal-metal separations. Calculated potential-energy surfaces reveal a double minimum for Ir(2)(dimen)(4)(2+) (～4.1 ? Ir-Ir with 0° twist angle and ～3.6 ? Ir-Ir with ±12° twist angle) but not for the rhodium analogue (～4.5 ? Rh-Rh with no twisting). Because both the ligand strain and A(2u) distortional energy are virtually identical for the two complexes, the strength of the metal-metal interaction is the determining factor. On the basis of the magnitude of this interaction, we obtain the following results: (1) a single-minimum (along the Ir-Ir coordinate), harmonic potential-energy surface for the triplet electronic excited state of Ir(2)(dimen)(4)(2+) (R(e,Ir-Ir) = 2.87 ?; F(Ir-Ir) = 0.99 mdyn ?(-1)); (2) a single-minimum, anharmonic surface for the ground state of Rh(2)(dimen)(4)(2+) (R(e,Rh-Rh) = 3.23 ?; F(Rh-Rh) = 0.09 mdyn ?(-1)); (3) a double-minimum (along the Ir-Ir coordinate) surface for the ground state of Ir(2)(dimen)(4)(2+) (R(e,Ir-Ir) = 3.23 ?; F(Ir-Ir) = 0.16 mdyn ?(-1)).