乙腈-水和乙二醇-水均相溶液中光诱导杜醌激发三重态与色氨酸、酪氨酸的氢原子转移反应

本文用激光闪光光解技术研究了光诱导生物醌杜醌激发三重态(³DQ^*)和色氨酸(Trp)与酪氨酸(Tyr)在乙腈-水(MeCN-H₂O)及乙二醇-水(EG-H₂O)均相溶液中的光化学反应,分析了反应的机理,并基于Stern-Volmer方法测量了反应速率常数. 光解DQ体系可以生成³DQ^*,³DQ^*与Trp、Tyr发生的氢原子转移反应占主导地位. 对于DQ/Trp/MeCN-H₂O和DQ/Trp/EG-H₂O溶液,³DQ^*与Trp反应生成杜醌中性自由基DQH^·、以碳为中心的色氨酸中性自由基Trp^·/NH和以氮为中心的色氨酸中性自由基Trp/N^·. 对于DQ/Tyr/MeCN-H₂O和DQ/Tyr/EG-H₂O溶液,³DQ^*与Tyr反应生成DQH^·和酪氨酸中性自由基Tyr/O^·. ³DQ^*与Trp、Tyr的氢原子转移反应速率常数都在10⁹ L·mol^-1·s^-1量级,反应近似受扩散控制. MeCN/H₂O均相溶液中³DQ^*与Trp、Tyr的反应速率常数要明显高于EG/H₂O均相溶液中的反应速率常数,这与Stokes-Einstein方程定性一致.     

乙二醇均相溶液中苊醌三重激发态淬灭反应的TR-ESR研究

利用时间分辨电子自旋共振（TR-ESR）方法,研究了乙二醇（EG）均相溶液中稳定自由基TEMPO和生物抗氧化剂维生素C（VC）对苊醌（ACQ）激发三重态3ACQ*的淬灭反应。光解ACQ/EG体系,观察到苊醌中性自由基ACQH•和乙二醇烷基自由基的发射/吸收+发射（E/A+E）的CIDEP信号,ACQH•和CH2(OH)C•HOH由3ACQ*从EG上夺氢生成。光解ACQ/TEMPO/EG体系,3ACQ*与TEMPO相互作用将极化转移给TEMPO。光解ACQ/VC/EG体系,3ACQ*除了从EG上夺氢外,还从VC上夺氢生成VC负离子基As•-。较强的As•-的CIDEP信号表明VC对3ACQ*有明显的淬灭作用。     

乙二醇均相溶液中苊醌三重激发态淬灭反应的TR-ESR研究

利用时间分辨电子自旋共振(TR-ESR)方法,研究了乙二醇(EG)均相溶液中稳定自由基TEMPO和生物抗氧化剂维生素C(VC)对苊醌(ACQ)激发三重态3ACQ*的淬灭反应.光解ACQ/EG体系,观察到苊醌中性自由基ACQH*和乙二醇烷基自由基的发射/吸收+发射(E/A+E)的CIDEP信号,ACQH*和CH2(OH)CHOH由3ACQ*从EG上夺氢生成.光解ACQ/TEMPO/EG体系,3ACQ*与TEMPO相互作用将极化转移给TEMPO.光解ACQ/VC/EG体系,3ACQ*除了从EG上夺氧外,还从VC上夺氢生成VC负离子基As*-.较强的As*-的CIDEP信号表明VC对3ACQ*有明显的淬灭作用.     

二元混合体系Gemini表面活性剂G12-6-12和CTAB相互作用的NMR研究

运用NMR方法探讨了298 K时N,N'-双(十二烷基二甲基)-1,6-己烷溴化铵(G12-6-12)和十六烷基三甲基溴化铵(CTAB)在D₂O溶液中的相互作用. 测得G12-6-12和CTAB的临界胶束浓度cmc值分别约为0.773和0.668 mmol/L. 在不同G12-6-12摩尔分数下,混合体系的临界胶束浓度实验值cmc_*小于理想值CMC^*,相互作用参数β_M<0,但是当α≤0.3时,cmc^*比CMC^*小很多,同时 满足|β_M|>ln(cmc₁/cmc₂)条件. 表明G12-6-12和CTAB之间存在协同效应,可以形成混合胶束,在2D NOESY谱中可以看到G12-6-12与CTAB分子间的交叉峰,扩散实验也表明混合溶液中的胶束半径比纯溶液中的G12-6-12胶束半径大,都预示混合胶束的形成. 当α>0.3 时,cmc^*≈CMC^*,β_M≈0, 根据假相分离模型和规则溶液理论,G12-6-12和CTAB近似于理想混合.     

吡啶离子液体与水混合体系中蒽醌-2-磺酸钠的激光闪光光解机理

利用激光闪光光解技术研究了蒽醌-2-磺酸钠(AQS)在吡啶离子液体N-丁基吡啶四氟硼酸盐([BPy][BF₄])与水(H₂O)混合体系中的光化学反应过程. 实验结果表明,AQS的激发三重态(³AQS^*) 会与H₂O快速反应,不断增加[BPy][BF₄]在混合体系中的体积比(V_IL),瞬态吸收光谱发生了很大变化. 510 nm附近的瞬态吸收带变化最大,在0< V_IL< 0.1时,吸光度会随着[BPy][BF₄]的增加而增加;而在V_IL>0.1时,吸光度则随着比例的增加而减小. 然而380 nm附近吸收带的吸光度却一直在增加. 通过拟合近似地得到了瞬态物种B和³AQS^*的表观动力学参数. 另外还讨论了³AQS^* 与阳离子之间的夺氢反应,通过对350~420 nm处光谱图的分析,推断出这一范围的瞬态吸收光谱是³AQS^*与AQSH^·的叠加谱. 在混合体系中,³AQS^*分别与H₂O和[BPy][BF₄]的反应是一对竞争反应. 还发现在高浓度的离子液体环境下,体系的整体反应速率会减弱.     

硫酸催化乙二醛气体相水化反应机理和速率常数理论计算研究

采用M06-2X和CCSD(T)高阶量化计算和传统过渡态理论研究硫酸催化乙二醛气体相水化反应.对HCOCHO+H₂O, HCOCHO+H₂O+H₂O, HCOCHO+H₂O+H₂O, HCOCHO+H₂O...H₂SO₄和HCOCHO+H₂O+H₂SO₄五个路径的反应机理和速率常数进行了研究.计算结果表明硫酸具有较强的催化能力,能显著减小乙二醛水化反应的能垒,在CCSD(T)/6-311++G(3df,3pd)//M06-2X/6-311++G(3df,3pd)理论水平,当硫酸分子参与乙二醛水化反应时,反应能垒从37.15 kcal/mol减少至7.08 kcal/mol.在室温条件下,硫酸催化乙二醛水化反应的反应速率1.34×10^-11 cm³/(molecule.s),是等量水分子参与乙二醛水化反应的速率的10¹²倍,大于乙二醛与OH自由基反应的反应速率1.10×10^-11 cm³/(molecule.s).这表明大气条件下,硫酸催化乙二醛水化反应可以发生,同乙二醛与OH自由基反应相竞争.     

利用交流阻抗谱揭示Ir(111)电极在酸性溶液中的氢吸附动力学

本文利用阻抗谱研究Ir(111)电极在HClO₄和H₂SO₄中溶液中的氢吸附行为. 在HClO₄溶液中,随着施加电位从0.2 V降到0.1 V(vs RHE),Ir(111)电极上氢吸附速率从1.74×10^-8 mol·cm^-2·s^-1增大到 3.47×10^-7 mol·cm^-2·s^-1 . 与相同条件下Pt(111)电极上的氢吸附速率相比,Ir(111)上的氢吸附速率要小1∽2个数量级,这是由于Ir(111)电极与H₂O结合能力更强,因此位于水合氢键网络中的氢离子需要克服更高的能垒才能重新定向进而发生欠电位沉积. 在H₂SO₄溶液中,氢吸附电位负移了200 mV,吸附速率也下降了一个数量级,这是由于Ir(111)电极表面强吸附的硫酸根/硫酸氢根物种的阻碍作用. 结果表明,在电化学环境下,位于电极表面附近的水分子的取代和重新定向在很大程度上影响了氢吸附过程.     

Microwave Assisted Synthesis of a New Triplet Iridium(III) Pyrazine Complex

采用微波辅助加热方法,2,3-二苯基吡嗪(DPP)与水合三氯化铱(IrCl₃·3H₂O)反应制备了[Ir(DPP)₃],通过¹H NMR、元素分析和质谱方法对配合物结构进行了表征,并研究了配合物的吸收光谱和光致发光光谱. 结果表明,配合物Ir(DPP)₃在382和504 nm处存在单重态¹MLCT(金属到配体的电荷跃迁)和三重态³MLCT的吸收;在573 nm 处有较强的金属配合物三重态的磷光发射.     

Synthesis and photoluminescence properties of Nd2O3 nanoparticles modified by sodium bis 2-ethylhexyl sulfosuccinate

This paper reports that Nd₂O₃ nanoparticles modified by AOT(sodium bis(2-ethylhexyl) sulfosuccinate) were prepared using microemulsion method in the system of water and propanol/AOT/toluene. Transmission electron microscopy shows that the Nd₂O₃ nanoparticles take the shape of sphere with 18\,nm and 31nm with different preparation. The organic sol of Nd₂O₃ nanoparticles is very stable at room temperature. X-ray diffraction results show that the product has hexagonal phase structure. Two ultraviolet emission band at 344\,nm and 361\,nm corresponding to the transition of ⁴D_3/2→4I_9/2 and 2P_3/2→⁴I₁₁₂ or ⁴D_3/2 →⁴I_13/2 were observed.     

4-硝基联苯酚三重态质子化和去质子化过程中瞬态物种的指认

近年利用超快光谱技术对于4-硝基联苯酚(HO-Bp-NO₂)的研究发现，其在单重态和三重态时均会发生光致质子耦合电子转移(PCET)反应. 其瞬态吸收光谱450 nm处有一个独特的尖锐吸收带，但无羟基取代的对硝基联苯(Bp-NO₂)未观察到此现象. 本文利用酸性溶液作为外加可控质子供体，通过在强酸(∽10^-1 mol/L)和弱酸(∽10^-4 mol/L)溶液中的光谱和动力学结果，指认这个新吸收带为开壳层单重态O-Bp-NO₂H. 它是HO-Bp-NO₂的互变异构体，由三重态HO-Bp-NO₂中硝基氧得质子后羟基快速去质子产生. 动力学分析表明，非质子极性溶剂中三重态HO-Bp-NO₂与基态母体间还会发生PCET或先质子后电子转移生成自由基·O-Bp-NO₂. 这一反应与O-Bp-NO₂H竞争，导致其产率较低. 这些结果阐明了三重态HO-Bp-NO₂在非质子极性溶剂中的失活机制.     

杜醌自由基光化学路径的CIDEP研究

用自制的高时间分辨电子自旋共振波谱仪,测量得到了酸性、碱性和胶束环境下的光解杜醌/乙二醇(DQ/EG)溶液瞬态自由基的化学诱导动态电子自旋极化(CIDEP)谱.在光解均相DQ/EG溶液时,观察到了以增强发射的的中性杜半醌自由基(DQH.)的CIDEP信号;在碱性环境下(pH=9)和TX-100胶束环境下光解DQ/EG体系时得到杜醌负离子自由基(DQ-.)的CIDEP信号;在酸性环境下(pH=2.5)光解DQ/EG体系时,出现的又是中性杜半醌自由基(DQH.)的CIDEP信号.实验结果显示,DQH.由3DQ*与EG之间的氢原子转移反应生成,DQ.-由DQH.的去质子化反应生成,反应中伴随着极化转移.     

Electric Spectra Study of Tetra-Hydrophenyl Porphyrin with Two Hexadecyl Chains in CTAB Micelle Aqueous Solutions

Abstract

UV-visible and fluorescence spectral studies shows that tetra-hydrophenyl porphyrin with two hexadecyl chains (P₂) could be solubilized in CTAB micelle, and that the hydrophilic ability of P2 increases with increasing bulk pH. The change in bulk pH lead to the changing of the solubilizing location of P₂ in the CTAB micelle. In neutral (pH 6.88) conditions, the hydrophilic head group of P₂ readily locates in the stern layer of CTAB micelle. However, the solubilizing location of P₂ takes a location change to the outer surface of the CTAB micelle with the bulk pH increasing up to 11.41. Furthermore, the CTAB micelle could provide a strong basic microenvironment (like 1.5 mol dm^?3 NaOH aqueous solution) to P₂ in mild basic conditions; resulting in the deprotonation of the pyrrole nitrogen of the porphyrin moiety in a mile basic CTAB micelle solution.     

Nitration of phenols in reversed micelle systems and enhanced oxidation ability of dilute nitric acid (less than 2.0 molarity) in concentrated salt solutions

In a previous paper, we have reported that dilute nitric acid in reversed micelle systems can oxidize the Br⁻ ion to Br₂ and proposed that the nitryl (or nitronium) ion NO₂⁺ should be the active species in the oxidation process. Nitration of phenol in reversed micelle systems with dilute nitric acid, CHCl₃/CTAC/H₂O (2.0 mol dm^− 3 HNO₃ in the 1.0% (v/v) H₂O phase), was performed at 35 °C to obtain 2- and 4-nitrophenols, where CTAC represents cetyltrimethylammonium chloride. In similar CTAC and AOT reversed micelle (CHCl₃ or heptane/AOT) systems, 4-methylphenol was converted to 2-nitro-4-methylphenol, where AOT stands for sodium bis(2-ethylhexyl) sulfosuccinate. In aqueous 2.0 mol dm^− 3 HNO₃ solution accompanied by 4.0 mol dm^− 3 LiCl (and a small amount of LiBr as the bromide resource), trans-1,4-dibromo-2-butene was successfully brominated to 1,2,3,4-tetrabromobutane. This result is a good evidence that the Br⁻ ion can be oxidized to Br₂ in dilute nitric acid (2.0 mol dm^− 3) provided that it contains concentrated salts. At 20-40 °C, the apparent oxidation-reaction rate constants (k/s^− 1) of Br⁻ to Br₂ were evaluated in 0.1-2.0 mol dm^− 3 HNO₃ solution accompanied by concentrated LiCl (3.5-9.0 mol dm^− 3). For chloride salts, the cation effects increased as Et₄N⁺ ? Na⁺ < Li⁺ < Ca²⁺ < Mg²⁺. Even the evolution of Cl₂ was demonstrated from < 2.0 mol dm^− 3 HNO₃ solution containing concentrated LiCl, MgCl₂, and CaCl₂ as well as AlCl₃, therefore, an indirect oxidation mechanism of the Br⁻ ion through Cl₂ was proposed as follows: 2Cl⁻ + NO₂⁺ → Cl₂ + NO₂⁻; 2Br⁻ + Cl₂ → Br₂ + 2Cl⁻.     

Investigations into the spectral and luminescent properties of methylphenols in neutral and ionic forms in aqueous micelle solutions

The special features of the absorption and fluorescence spectra of some substituted phenols (2-, 4-methylphenol and 2-amino-4-methylphenol) in aqueous micelle solutions are investigated on addition of an alkali and acid. A fluorescence band of 4-methylphenol in the anion form is detected in the presence of a cation surfactant. The fluorescence efficiency of 4-methylphenol in the presence of the triton X100 micelle decreases in comparison with aqueous solutions. It is established that the quantum yield of fluorescence of 2-methylphenol in the presence of N-cetyltrimethyl ammonium bromide (CTAB) increases in comparison with the aqueous solution (ϕ_fl = 0.25 and 0.17, respectively). The constant of fluorescence quenching for methylphenol in aqueous micelle solutions by the alkali is two orders of magnitude higher than by the acid. The proton-acceptor properties of 2-amino-4-methylphenol are higher than of 4-methylphenol. __________ Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 11, pp. 54–61, November, 2005.     

Characterization of TiO2 Nanoparticles in Langmuir-Blodgett Films

In this work we have synthesized TiO₂ nanoparticles, using either a sol–gel base catalysed process in the interior of CTAB reversed micelles (TiO₂ CTAB sol), or the neutralization of a TiO₂/H₂SO₄ solution in the interior of AOT reversed micelles. From the absorption and emission data of the TiO₂ nanoparticles it is possible to conclude that in the sol–gel route there remains alkoxide groups in the structure, originating transitions lower than the energy gap of TiO₂ semiconductor. These transitions disappear in the neutralization procedure, where the alkoxide groups are absent in the structure. We have assigned the observed indirect and direct optical transitions according to the anatase band structure. TiO₂ Langmuir-Blodgett (LB) films were prepared either by direct deposition of titanium isopropoxide or by deposition of the TiO₂ CTAB sol. These films showed photoluminescence, which was attributed to band-gap emission and to surface recombination of defect states.     

Fluorescence quenching of 3,7-diamino-2,8-dimethyl-5-phenyl phenazinium chloride by AgCl and Ag nanoparticles

Quenching of fluorescence of the dye 3,7-diamino-2,8-dimethyl-5-phenyl Phenazinium Chloride (Safranine T) has been investigated by AgCl nanoparticles in the W/O microemulsion medium at different [H₂O]/[AOT] ratios (ω) and with Ag nanoparticles and Ag⁺ in aqueous medium. A simple straightforward method has been introduced to prepare AgCl nanoparticles in well-characterized, monodispersed biomimicking nanocavities formed by sodium bis(2-ethylhexyl)sulfosuccinate (AOT) in heptane. Experimental results reveal that the size of the AgCl nanoparticles increases with increase in hydration. The results of the quenching experiment were analysed in the light of Stern Volmer equation. Quenching of fluorescence of the dye has been found to decrease with decrease in the size of the nanoparticles of AgCl and the variation of Stern Volmer quenching constants (K_SV) with particle size is different for two different size regimes.     

Phenol and anisol fluorescence quenching in aqueous micellar solutions

Phenol and anisol fluorescence quenching in aqueous micellar solutions is investigated on addition of H ₂ O ₂. It is established that the efficiency of interaction of the phenol molecule in water with hydrogen peroxide is higher than of anisol. In the phenol-H ₂ O ₂ system, the buildup of phenol fluorescence occurs in the presence of an anionic-reagent detergent. A decrease in the efficiency of phenol fluorescence quenching by hydrogen peroxide in aqueous solutions in the presence of CTAB and triton X-100 micelles is observed. The micellar media increase the efficiency of interaction of anisol with a quencher in comparison with phenol. __________ Translated from Izvestiya Vysshikh Uchebnykh Zavedenii, Fizika, No. 4, pp. 73–79, April, 2006.     

Fluctuation kinetics of the hopping fluorescence quenching in disordered solid solutions: A theoretical model and experimental evidence

Fluctuation kinetics of the hopping fluorescence quenching in disordered solid solutions is investigated for the first time. Measurements were made in the chelated complexes of rare-earth ions [Y_1−xTb_x(pyca)₃(H₂O)₂]nH₂O used as chromophore. The Tb³⁺ ions and the OH^--ions of unbounded water molecules appear as fluorescent donors and randomly distributed acceptors, respectively, with the dipole-dipole interaction between them. The measured fluctuation kinetics is the kinetics of the Förster type but with larger decay amplitude. It begins almost immediately after the initial static stage of quenching, and lasts for the entire interval of measurements leaving no room at all for the well-known exponential kinetics with constant rate. Proposed theoretical explanation of the phenomenon is based on the solution of the closed many-particle integral equation for the observable kinetics of hopping fluorescence quenching. The methods for determination of the energy transfer microparameters by the measured fluorescence quenching kinetics are discussed.