水杨叉间溴缩苯胺的光发色和热消色反应过渡态

本文报道水杨叉间溴缩苯胺(1)的光致色变和热消色, 首次提出了它的光发色和热消色反应过渡态结构, 确认顺-反-反烯醇式水杨叉间溴缩苯胺(2)有光致色变性能, 而顺-顺-反式异构体则无此性能。选择1作为确定研究对象的另一个原因是由于激发态间位效应[9]的考虑, 1的氮原子将呈现更强的碱性, 降低热消色反应速率常数, 期望在较高的温度下观察到光致色变。     

光致变色双呋喃俘精酸酐的合成及其在平行图象存储中的应用

通过两步Stobbe缩合反应合成了一种双杂环俘精酸酐化合物, E,E-3,4-二[1-(2,5-二甲基-3-呋喃基)乙叉]-3,4-二氢呋喃-2,5-二酮(双呋喃俘精酸酐). 通过X射线单晶衍射, 对目标产物的分子结构进行了研究, 结果表明在该化合物中, 2个反应中心的距离分别是0.3394和0.3406 nm, 有利于光环合反应. 研究了该化合物在不同溶剂中的光致变色性行为, 并对目标产物在平行图象光信息存储中的应用进行了探索.     

吡咯取代的俘精酸酐及俘精酰亚胺的光致变色反应研究

对6个吡咯取代的俘精酸酐和1个俘精酰亚胺的光致变色行为进行了研究,发现取代基的不同对它们的光致变色过程有显著的影响.稳态动力学分析表明,呈色体(7,7a-二氢吲哚衍生物,II)的光消色反应遵循一级动力学反应规律.取代基对光消色反应的速率常数有一定的影响,对于呈色体(II)而言,2-3-位上有取代基的化合物,其光开环反应的速率常数明显大于2-或3-位无取代基的化合物.对于俘精酸酐的光反应而言,其反应比较复杂,不符合简单的动力学级数.在呈色体(II)的2-或3-位引入给电子基团可以使7,7a-二氢吲哚衍生物的吸收光谱发生红移,化合物II7的最大吸收波长在乙腈中可达720nm.溶剂极性的增大,可以使是色体的吸收光谱发生显著的红移,而对俘精酸酐本身的吸收光谱影响甚微.     

水杨叉间溴缩苯胺的光发色和热消色反应过渡态

亚稳态的可控转换是未来信息记录分子器件原理,因此,人们对光致色变化合物合成和光化学行为研究感到兴趣。水杨叉缩苯胺及其部份衍生物的固体、固相溶液和Lan-gmuir-Blodgett膜(LB膜)呈现光致色变性质。质子迁移是水杨叉缩苯胺的光致色变和热消色反应机理,反应按协同机理进行,反应     

(口恶)唑环取代的俘精酸酐的合成及其光致变色性能的研究

合成了含噁唑环的俘精酸酐,4-（5-甲基-2-对甲氧苯基-4-乙酰基嘿唑）乙叉（异丙叉）丁二酸酐,研究了该化合物在不同溶剂中的光致变色性能,进行了光成色和光消色过程的动力学研究,并考察了溶剂极性对该化合物吸收光谱的影响。稳态动力学分析结果表明,该化合物呈色体的光消色反应遵循一级动力学规律,俘精酸酐本身的光反应比较复杂,不符合简单的动力学级数。     

1,2-二甲基-3-吲哚甲叉(异丙叉)丁二酸酐(1)和1,2-二甲基-3-吲哚乙叉(异丙叉)丁二酸酐(2)的晶体结构

1.2-二甲基-3-吲哚甲叉(异丙叉)丁二酸酐(1)(C_(18)H_(17)NO_3)与1.2-二甲基-3-吲哚乙叉(异丙叉)丁二酸酐(2)(C_(19)H_(19)NO_3)同属于吲哚俘精酸类化合物,它们的分子结构非常类似,只是(1)中为吲哚甲叉,(2)中为吲哚乙叉.但它们的光色性却差别很大.化合物(1)无光致变色性,化合物(2)则表现为良好的光致变色性.其原因在于结构的不同。     

硼化合物的研究Ⅹ。B10H102-、B10H122-及B3H8-双二茂铁季铵盐及环状二茂铁季铵盐的合成

众所周知,二茂铁类和硼氢类化合物都具有特殊的化学结构,并且有可能作为高能材料得到应用。作者通过B₁₀H₁₀^2-、B₁₂H₁₂^2-及B₃H₈^-与(N,N-二甲基胺甲基)二茂铁和1,1'-双(N,N-二甲基胺甲基)二茂铁卤化铵反应,曾合成了一系列新的化合物并研究了它们的反应性能和晶体结构^[1-4]。     

柄型金属有机化合物(Ⅰ)──硅桥联二(1-茚基)和四氢茚基钛化合物的合成及结构

通过1,3-二(1-茚基)四甲基二硅氧烷的双锂盐与TiCl₄·2THF反应制得硅桥联二(1-茚基)钛化合物(Me₂SiOSiMe₂)[Ind]₂TiCl₂(1),对其催化氢化得到相应的四氢茚基化合物(Me₂SiOSiMe₂)[IndH₄]₂TiCl₂(2).对化合物1和2的单晶进行了X射线衍射结构分析,它们的晶体都属单斜晶系,P2₁/n空间群.     

3-芳基-5-(呋喃-2-基)-4,5-二氢-1H-吡唑衍生物的合成及其生物活性评价

二氢吡唑类化合物是一类具有良好生物活性的五元杂环化合物。本文以2-呋喃甲醛和4-氟苯乙酮为原料,经羟醛缩合和取代反应生成4’-二甲氨基呋喃查尔酮(2)后,与水合肼环化得到二氢吡唑中间体(3),再酰化得到9个未见报道的3-芳基5-(呋喃-2-基)-4,5-二氢-1H-吡唑衍生物(4a~4i),其结构经IR、~1H NMR和~(13)C NMR确证。分别采用小鼠巨噬细胞Raw264.7模型和DHHP法初步测试了目标化合物的体外抗炎活性和抗氧化活性。结果表明,部分化合物具有潜在的抗炎活性和清除自由基活性,特别是化合物4b和4c的抗炎活性与阳性对照药地塞米松活性相当(IC_(50)值分别为7.84μmol/L和10.52μmol/L),而化合物3、4b、4c和4d在浓度为4mg/m L时对DPPH自由基的清除率均超过90%。     

含硝基二代光致变色液晶树枝状大分子的光化学研究

研究了树外围含36个硝基偶氮苯端基新型二代碳硅烷光致变色液晶树枝状大分子(G₂)在溶液中的最大吸收波长, 摩尔消光系数, 反-顺光异构化反应速率常数, 热回复异构化反应速率常数, 光化学回复异构化反应平衡常数及速率常数. G₂的光致变色反应速率常数的数量级为10^－1 s^－1, 而含偶氮端基侧链聚硅氧烷的光致变色反应速率常数的数量级为10^－8 s^－1, 因此, 液晶树枝状大分子的光响应速率比后者快10⁷倍. G₂的光化学回复异构化反应平衡常数k_t/k_c为1.77～1.97, 有作为光控开关材料的应用前景.     

1-二茂铁基-3-[(9-乙基)咔唑-3-基]丙烯酮的合成及三阶非线性光学性质

合成了一个新的非线性光学(NLO)有机材料1-二茂铁基-3-[(9-乙基)咔唑-3-基]丙烯酮(FCAK),并通过NMR、IR、MS和元素分析等技术手段进行了表征。 采用粉末Nd∶YAG激光技术测定了标题化合物的三阶非线性光学性质并确定了相关参数。 激光脉冲为4 ns时,非线性折射率n₂=-3.5×10^-18 m²/W,非线性吸收系数β=-2.7×10^-11 m/W,三阶非线性极化率χ⁽³⁾=2.04×10^-12 esu,三阶非线性分子超极化率γ=1.1×10^-30 esu。 激光脉冲为21 ps时,n₂=0.55×10^-18 m²/W,β=-0.6×10^-11 m/W,χ⁽³⁾=3.4×10^-13 esu,γ=0.13×10^-30 esu。     

硝酸异丙酯与Cl原子、 OH和NO3自由基反应的机理及动力学

采用CCSD(T)//M06-2X/6-311++G(d,p)方法, 结合传统过渡态理论, 研究了硝酸异丙酯与Cl原子、 OH及NO₃自由基的反应机理和动力学. 两个反应物单体首先形成氢键复合物, 随后X(X=Cl原子、 OH和NO₃自由基)提取硝酸异丙酯中叔碳的α-H原子或甲基的β-H原子, 室温下, 以X提取α-H原子为主. 反应的主要历程为 Cl原子(OH或NO₃自由基)提取(CH₃)₂CHONO₂的α-H原子, 生成HCl(H₂O或HNO₃)分子和(CH₃)₂CONO₂自由基, 后者分解为丙酮和NO₂. 结果表明, 在200~500 K温度范围内, 随着温度的升高, 丙酮和NO₂的产率降低; 在室温下, 硝酸异丙酯与Cl原子、 OH和NO₃自由基反应的速率常数分别为3.933×10^-11, 1.182×10^-13和7.134×10^-19 cm³·molecule^-1·s^-1. 计算所得硝酸异丙酯与OH自由基反应的动力学数据与实验结论一致.     

Hydrogen peroxide photoproduction by the semicarbazide—tris(2,2′-bipyridine)ruthenium(II)—oxygen system

A light-driven system consisting of tris(2,2′-bipyridine)ruthenium(II) (Ru(bpy)₃²⁺) as the photosensitizer, semicarbazide as the electron donor and molecular oxygen as the electron acceptor has been employed for hydrogen peroxide production. The efficiency of this photosystem markedly depends on pH: while the peroxide yield is almost negligible at acid, neutral or slightly alkaline pH, it reaches significant values at high hydroxide concentrations, the initial rate of H₂O₂ formation drastically increasing from pH 12 to pH 14. In 1 M NaOH solutions containing Ru(bpy)₃²⁺ and semicarbazide at optimum concentrations, the number of catalytic cycles (or turnover number) undergone by the ruthenium complex over the complete course of the photochemical reaction is as high as 1.1 × 10⁴.

Spectrofluorometric and laser flash photolysis techniques were used to study the primary photochemical reactions involving the excited state of the ruthenium complex as well as the photochemically generated species Ru(bpy)₃³⁺ and Ru(bpy)₃⁺. It is proposed that at pH 14 a sequence of reactions leading to O₂ photoreduction by electrons from semicarbazide takes place, with the concomitant formation of H₂O₂; the excited state of Ru(bpy)₃²⁺ appears to react via oxidative quenching by oxygen rather than via reductive quenching by semicarbazide. At neutral pH, in contrast, there is no H₂O₂ formation owing to the fact that semicarbazide is unable to reduce (Ru(bpy)₃³⁺ to Ru(bpy)₃²⁺, although the photoexcited ruthenium complex is quenched equally by oxygen.     

1-(芘-1-基)-3-(4-甲氧基苯基)丙烯酮的合成及三阶非线性光学性质

合成了一种新的有机非线性光学(NLO)材料1-(芘-1-基)-3-(4-甲氧基苯基)丙烯酮(PMPAK),通过¹H NMR、IR、HR-MS和元素分析表征其结构。 以Nd:YAG-Laser System作为光源,激光波长450 nm,脉冲宽度4 ns(FWHM),采用4f相位相干成像技术测定了PMPAK的三阶NLO性质并确定了相关参数:非线性折射率n₂=-1.84×10^-16 m²/W,非线性吸收系数β=2.53×10^-9 m/W,非线性极化率χ⁽³⁾=1.137×10^-10 esu。     

Micellar effects on photoinduced redox reactions of Fe(bpy)2(CN)2

Excitation of solutions of Fe(bipy)₂(CN)₂ by a 266-nm laser pulse produces a hydrated electron and the oxidized complex, Fe(bipy)₂ (CN)₂⁺, in the primary photochemical step, in homogeneous aqueous solution as well as in aqueous solutions containing cetyltrimethylammonium bromide (CTAB) or sodium dodecyl sulfate (SDS) micelles. In all cases nascent hydrated electrons react with ground state Fe(bipy)₂(CN)₂ to form Fe(bipy)₂(CN)₂⁻, and comparison of the decay constants in the three media (H₂O: k = 2.8 × 10¹⁰ M⁻¹ s⁻¹; CTAB: k = 2.9 × 10¹⁰ M⁻¹ s⁻¹; SDS: k = 5.5 × 10⁹ M⁻¹ s⁻¹), shows that the reaction is essentially unaffected by CTAB micelles but is much slower in SDS solution. Similar micellar effects were found for the back reaction between e_aq⁻ and Fe(bpy)₂(CN)₂⁺. Rate constants for the scavenging of the photogenerated hydrated electrons by methyl viologen (MV²⁺) cations and NO₃⁻ anions were measured in the three systems, and the results indicate that for scavenging by MV²⁺ the rate constants are decreased in the micelle systems (k in H₂O, 8.4 × 10¹⁰; CTAB, 3.5 × 10¹⁰ and SDS, 1.58 × 10¹⁰ M⁻¹ s⁻¹), whereas for NO₃⁻ the CTAB micelle decreases while the SDS micelle enhances the scavenging compared to water solution (k in H₂O, 8.3 × 10⁹; CTAB, 7 × 10⁸; and SDS, 2.05 × 10¹⁰ M⁻¹ s⁻¹). For the comproportionation reaction between Fe(bipy)₂(CN)₂⁺ and Fe(bipy)₂(CN)₂⁻ both micelles reduce the rate (k in H₂O, 3.3 × 10¹⁰; CTAB, 2.3 × 10¹⁰; and SDS, 1.05 × 10¹⁰ M⁻¹s⁻¹), but while the reaction of Fe(bipy)₂(CN)₂⁺ with MV⁺ is increased in CTAB compared to water, it is slowed in SDS (k in H₂O, 2.4 × 10¹⁰; CTAB, 8.9 × 10¹⁰; and SDS, 1.8 × 10¹⁰ M⁻¹s⁻¹). All effects observed in these microheterogeneous systems can be uniformly interpreted in terms of Coulombic interactions between the actual reactants and the charged surface of the micelles.     

Photoactivation of dichloro(ethylenediamine)platinum(II)

Photolysis of dimethylsulfoxide (dmso) solutions of the compound Pt(en)Cl₂, where en=ethylene-1,2-diamine, leads to solvolysis of the complex and formation of Pt(en)(dmso)Cl⁺. The reaction follows clean pseudo-first-order kinetics with parallel photolytically activated and thermally activated paths. Both paths are first-order in both Pt(en)Cl₂ and solvent. Eyring analysis of the rate constants for 25 °C≤T≤55 °C yielded a Gibbs energy of activation of 96 kJ mol⁻¹ for the thermal pathway and no measurable activation barrier for the photochemical pathway. The quantum yield for the photochemical path is 0.22, as determined using ferrioxalate actinometry.     

基于二茂铁的两个查尔酮衍生物的合成及超快三阶非线性光学响应

二茂铁是合成新颖有机功能材料的基本单元之一。 本文设计并合成了两个基于二茂铁的同分异构查尔酮衍生物:1-二茂铁基-3-(噻吩-2-基)丙烯酮(a)和1-二茂铁基-3-(噻吩-3-基)丙烯酮(b)。 采用超快激光Z-扫描技术(脉宽180 fs,波长532 nm)测定了化合物a和b的三阶非线性光学性质。 结果表明,化合物a吸收系数β=-2.1×10^-12 m/W,折射率n₂=1.9×10^-19 m²/W,分子超极化率γ=5.37×10^-32 esu;化合物b:β=-1.2×10^-13 m/W,n₂=2.0×10^-19 m²/W,γ=4.48×10^-32 esu。 说明在飞秒激光激发下,电荷转移能够在化合物a和b分子内部快速进行,二者均具有优异的超快三阶非线性光学响应。 在B3LYP/6-311+G(d,p)理论水平下,计算了化合物a和b分子轨道能量、极化率和各基团在前线分子轨道中的占有率。 理论计算结果显示,二茂铁基团在化合物a和b前线分子轨道中占有率分别为97%和98%,对两化合物的非线性光学性能起主导作用。     

Flow Injection Chemiluminescence Method for Nalbuphine Hydrochloride in Pharmaceutical Formulations Using Tris(2,2'-bipyridyl)ruthenium(II) Chloride-diperiodatocuprate(III) Reaction

Asensitive and selective method employing chemiluminescence(CL) coupled with flow injection(FI) is reported for nalbuphine hydrochloride(NAL) assay in pharmaceutical formulations. The enhancement effect of NAL on the CL reaction between tris(2,2'-bipyridyl)ruthenium(II) chloride-diperiodatocuprate(III) {Ru[(bpy)₃]²⁺-Cu(III) complex} in acidic medium is used as analytical measurement. The optimal conditions of the CL reaction were sulfuric acid 1.0×10^-3 mol/L, Ru[(bpy)₃]²⁺ 7.5×10^-5 mol/L, Cu(III)/Ag(III) complexes 4.0×10^-4/5.0×10^-4 mol/L, sample loop volume of 120 μL and flow rate of 2.5 mL/min. The sensitivities of the method in terms of detection(S/N=3) and quantification(S/N=10) limits are 5×10^-4 and 0.001 ppm(1 ppm=1 mg/L), respectively. The linear response of the instrument in the form of CL intensity with respect to NAL concentration is over the range 0.001-15.0 ppm(R²=0.9999) with relative standard deviation from 0.8% to 3.2% and injection throughput of 120 injection/h. The applications of the method include the quantitative analysis of NAL in pharmaceutical injection samples. Variations and the average results of the proposed method are not signi-ficantly different from the results of a reported method by applying F- and paired student t-test. The most likely CL reaction mechanism is written in accordance with spectrophotometric and CL studies.     

Theoretical study of the visible photodissociation spectrum of Ar3

The six A′ potential energy surfaces were computed by a DIM-like method involving a valence-bond quasidiabatic basis. Transition dipole moments were also determined using a similar method. The 4D dynamics of this system (restricted to a molecular plane fixed in space) was obtained with the HWD method (hemiquantal dynamics with the whole DIM basis) and the visible photoabsorption spectrum was determined with the help of a 1D full quantum mechanical program applied to each normal mode. The photoabsorption spectrum of Ar₃⁺ was calculated in the range 440–710 nm. It corresponds to photodissociation since the excited Ar₃⁺ ions almost all dissociate into the Ar⁺ +Ar+Ar channel by a rapid explosion of the cluster, and only very few into Ar₂⁺ +Ar. It is dominated by a transition to the second excited state along with a symmetric stretching motion. We found a prominent 80 nm wide peak centered at 530 nm, with a maximum cross section of 4.2 × 10⁻¹⁶cm². The Ar₂⁺ formation results from a transition to the first excited state under low-energy laser excitation and is controlled by non-adiabatic transitions.     

溶液中三价稀土Ho3+、Nd3+的脉冲激光光声光谱研究及其测定

采用自制的液体光声传感器,研究了在620～665nm波长范围不同溶剂中稀土Ho³⁺的光谱精细结构;探讨了入射激光脉冲能量、测试温度以及各种与水混溶的有机溶剂对光声信号强度的影响。在乙腈水溶液中测定稀土Ho³⁺、Nd³⁺检测限分别为5×10^-8mol/L和1.0×10^-7mol/L,相应的吸光度为1.5×10^-7和6.3×10^-7。