反胶束笼对纳米氯化银反应性能的微环境限定

研究了反映束中直径为１０￣１７ｎｍ的ＡｇＣｌ微料与亚甲基蓝之间的作用，比较了阴离子型和非离子型表面活性剂组成的反胶束微环境的影响，讨论了亚甲基蓝在粒子上的吸附，二聚体形成的钠米ＡｇＣｌ粒子对亚甲基蓝荧光猝灭机制。     

锰(Ⅱ)-邻菲罗啉-曙红-Triton X -100 体系荧光熄灭法测定痕量锰

在ＰＨ８．２的Ｈ３ＢＯ３－ＫＣｌ－ＮａＯＨ缓冲溶液中及非离子表面活性剂ＴｒｉｔｏｎＸ－１００存在下,锰（Ⅱ）与１,１０－邻菲罗啉及曙红反应生成无荧光的的使曙红的荧光熄灭,据此建立了一个荧光熄灭法测定痕量锰的新方法。方法的检出限为２μｇ／Ｌ,线性范围为０．２０－３．５０μｇ／２５ｍＬ,本方法已用于铝合金、面粉、小麦、麸皮中锰的测定     

荧光和动态光散射方法研究两性表面活性剂胶束的聚集和相互作用

以芘为荧光探针、二苯酮为猝灭剂，利用荧光方法测定了两性表面活性剂Ｎ－十二烷基－Ｎ，Ｎ－二甲基氨基丙磺酸盐（ＤＤＡＰＳ）胶束在不同温度和不同ＮａＣｌ浓度下的聚集数．利用动态光散射方法得到了胶束的水力半径Ｒｈ．结果表明，ＤＤＡＰＳ的胶束聚集数和Ｒｈ值随ＮａＣｌ浓度的升高略有增大；随温度的升高而稍有下降．ＤＤＡＰＳ胶束之间的作用力以排斥力为主．     

荧光和动态散射方法研究两性表面活性剂胶束的聚集和相互 …

以芘为荧光探针，二苯酮为猝灭剂，利用荧光方法测定了两性表面活性剂Ｎ十二烷基－Ｎ，Ｎ－二甲基氨基丙磺酸盐（ＤＤＡＰＳ）胶束在不同温度和不同ＮａＣｌ浓度下的聚集数，利用动态光莠射方法得到了胶束的水力半径Ｒｈ，结果表明，ＤＤＡＰＳ的胶束聚集数和Ｒｂ值随ＮａＣｌ浓度的升高略有增大，随温度的升高而稍有下降，ＤＤＡＰＳ胶束之间的作用力以排斥力为主。     

激光烧蚀金属氯化物的发光光谱和飞行时间质谱研究

测定了３５５ｎｍ紫外线光烧蚀ＡｇＣｌ，ＣｕＣｌ和ＣｕＣｌ２产生的等离子体发光光谱顺３００～５００ｎｍ范围内的发光谱线可归属为激光态金属原子的发射线，飞行时间质谱测定表明激光烧蚀产生的正，负离子主要有Ａｇ，Ｃｕ，Ｃｕ２Ｃｌ＾＋，Ｃｕ２Ｃｌ２＾＋，Ｃｕ３Ｃｌ２及Ｃｌ，ＡｇＣｌ，ＡｇＣｌ２，Ａｇ２Ｃｌ３，ＣｕＣｌ，ＣｕＣｌ２，Ｃｕ２Ｃｌ３等，对激光烧蚀机理也进行了讨论。     

聚乙烯醇存在下以硝酸铁代替铁铵矾用Volhard法测定银和氯离子

１引言Ｖｏｌｈａｒｄ法以铁铵矾作指示剂，终点不够敏锐。尤其是直接滴定Ａｇ＋时，ＡｇＳＣＮ沉淀易吸附Ａｇ＋而导致终点提前；返滴定Ｃｌ－时ＡｇＣｌ沉淀易转化为ＡｇＳＣＮ，使终点颜色闪而褪去难于观察，分析结果偏低。虽用有机溶剂（如硝基苯）可促进ＡｇＣｌ沉淀凝聚与溶剂化而减缓ＡｇＣｌ的转化，但有机溶剂多数有毒使测定条件恶化．作者提出以聚乙烯醇（ＰＶＡ）化学修饰ＡｇＳＣＮ、ＡｇＣｌ沉淀的结构，阻止ＡｇＳＣＮ对Ａｇ＋的吸附与ＡｇＣｌ的转化，用硝酸铁代替铁铵矾指示滴定终点测定Ａｇ＋、Ｃｌ－的方法。本法比经典Ｖ…     

吨染料与反胶束体系中CdS的光敏电子转移

用ＡＯＴ／异辛烷／水反胶束体系制备出了不同尺寸大小的纳米ＣｄＳ,并以曙红（ＥＯ）和孟加拉玫瑰红（ＲＢ）为探针分子,研究了它们与硫化镉微粒间的光致电荷转移相互作用,用光照实验和ＥＳＲ技术研究了这些染料向ＣｄＳ的导带注入电子的过程并讨论了作用机理     

阳离子表面活性剂与曙红Y的荧光反应及其分析应用

研究阳离子表面活性剂(CSAA)在水溶液中与曙红Y的荧光反应, 发现当CSAA单体与曙红Y形成离子缔合物时, 荧光发生猝灭, 而CSAA胶束与曙红Y作用又会出现一个新的、更强的荧光。荧光猝灭反应具有很高的灵敏度, 对于不同的CSAA, 其检测限在6.6-12.0ng/mL之间, 可用于痕量CSAA的测定。此外, 荧光猝灭和新荧光的产生也为研究表面活性剂和荧光染料在溶液中的存在状态提供了新的途径。还研究了反应体系的荧光特征、适宜条件并讨论了反应机理。     

阳离子表面活性剂与曙红Y的荧光反应及其分析应用

研究阳离子表面活性剂(CSAA)在水溶液中与曙红Y的荧光反应,发现当CSAA单体与曙红Y形成离子缔合物时,荧光发生猝灭,而CSAA胶束与曙红Y作用又会出现一个新的、更强的荧光.荧光猝灭反应具有很高的灵敏度,对于不同的CSAA,其检测限在6.6～12.0ng/mL之间,可用于痕量CSAA的测定.此外,荧光猝灭和新荧光的产生也为研究表面活性剂和荧光染料在溶液中的存在状态提供了新的途径.还研究了反应体系的荧光特征、适宜条件并讨论了反应机理.     

ICP—AES间接法连续测定混合物中的氯和碘离子的研究

本文研究了在Ｃｌ和Ｉ＾－的混合物中，加入过量Ａｇ＾＋使Ｃｌ＾－和Ｉ＾－分别以ＡｇＣｌ和ＡｇＩ沉淀后，用ＩＣＰ－ＡＥＳ测定剩余的Ａｇ＾＋，然后用ＮＨ３．Ｈ２Ｏ溶解ＡｇＣｌ沉淀，测定溶解液中的Ａｇ＾＋，间接得到Ｃｌ＾－的含量，以差减法求得Ｉ＾－量，实现Ｃｌ＾－和Ｉ＾＿的间接法连续测定。本文探讨了有关的化学条件和光谱测定条件，对方法的适用性进行了考察－共存离子的干扰情况，方法的精密度，检出限和试样中加入     

反胶束笼对纳米氯化银反应性能的微环境限定

研究了反胶束中直径为10～17nm的AgCl微粒与亚甲基蓝之间的作用，比较了阴离子型和非离子型表面活性剂组成的反胶束微环境的影响，讨论了亚甲基蓝在粒子上的吸附，二聚体形成和纳米AgCl粒子对亚甲基蓝荧光猝灭机制．     

反胶束中菁染料与AgCl粒子相互作用的光谱研究

在阴离子型和非离子型表面活性剂组成的反胶束体系中研究了直径为1 1～ 1 4nm的AgCl微粒子与菁染料之间的作用 ,讨论了AgCl纳米粒子对菁染料的吸附及荧光猝灭现象 .     

Photochemistry of a cyanine dye in reversed micelles

The effect of microenvironment on the existing state and spectral properties of a cyanine dye in different systems were investigated. Due to the space limitation and the polarity evolution of the water cell of reversed micelles, the optical behavior of the dye in reversed micelles was very different from in water and alcohol. The effect of surfactants with different charge on the interaction of a cyanine dye with AgCl nanoparticles in reversed micelles were also researched. The adsorption state of the dye on AgCl nanoparticles in reversed micelles was discussed.     

Fluorescence quenching of eosin upon adsorption by colloidal silver mediated in aqueous solution and reverse micelles

The optical effects of the adsorption of eosin on the colloidal silver particle have been investigated in aqueous solutions. It was found that upon adsorption the fluorescence of eosin was effectively quenched. This was explained as the photoinduced interfacial electron transfer from the excited singlet state of eosin to the silver particle. Decreasing pH of the solution favors the adsorption of eosin and so enhances the fluorescence quenching. For comparison, the fluorescence quenching in reverse micelles was also investigated. The quenching behavior was much different from that mediated in aqueous solution. This was attributed to the unique microenvironment of reverse micelles.     

含有BaMoO4纳米粒子的反胶束溶液与罗丹明B的相互作用

在三种带有不同电荷的表面活性剂构建的反胶束体系中(AOT/异辛烷、Oπ-10，环已烷、CTAB／正已醇)合成了BaMoO4的纳米粒子，采用透射电镜(TEM)观察其粒子呈球形，粒径在17-46 nm范围内，分布均匀；使用染料罗丹明B作为探针，采用紫外-可见光谱(UV-vis)和荧光光谱研究反胶束水池中罗丹明B与BaMoO4纳米粒子的相互作用；由于反胶束水池的空间和极性的限定，染料的光谱特征与其在纯水中发生很大变化，不同的反胶束体系中，由于染料分子所处的微观环境不同，导致其光谱特征也有较大区别。     

反胶束体系中水团的笼效应

在反胶束体系中研究了菁染料的吸收光谱以及ω值对菁染料荧光光谱的影响．讨论了不同粒径的AgCl纳米粒子对反胶束体系中菁染料的吸附状态及J-聚集体形成的影响．特别研究了反胶束水团空间限定效应对菁染料荧光量子产率及J-聚集体的影响．     

含有BaMoO4纳米粒子的反胶束溶液与罗丹明B的相互作用

在三种带有不同电荷的表面活性剂构建的反胶束体系中(AOT/异辛烷、Oπ-10/环已烷、CTAB/正已醇)合成了BaMoO₄的纳米粒子, 采用透射电镜(TEM)观察其粒子呈球形, 粒径在17～46 nm范围内, 分布均匀; 使用染料罗丹明B作为探针, 采用紫外-可见光谱(UV-vis)和荧光光谱研究反胶束水池中罗丹明B与BaMoO₄纳米粒子的相互作用; 由于反胶束水池的空间和极性的限定, 染料的光谱特征与其在纯水中发生很大变化, 不同的反胶束体系中, 由于染料分子所处的微观环境不同, 导致其光谱特征也有较大区别.     

Fluorescence quenching of bovine serum albumin.

The fluorescence emission spectra and 3D fluorescence spectra of bovine serum albumin (BSA) in cetyltrimethylammonium bromide (CTAB) reversed micelles were affected by the microenvironment. Blue shifts of the fluorescence emission peaks were found when BSA was present in CTAB reversed micelles. The fluorescence intensity changed with the water content. Similar changes in the peak regions of the 3D fluorescence spectra were also observed. CdS nanoparticles prepared in CTAB reversed micelles quenched the fluorescence of BSA significantly. The fluorescence of BSA was more effectively quenched by negative CdS nanoparticles than by positive or neutral CdS ones. The quenching degree increased linearly with increasing the concentration of negative CdS nanoparticles over the range of 5.0 x 10(-6) - 3.0 x 10(-5) mol L(-1). The quenching mechanism is discussed and the quenching constant is 1.32 x 10(4) L mol(-1).     

Effects of the water content on the growth rate of AgCl nanoparticles in a reversed micelle system

The effects of water content on the growth rate and the final particle size of AgCl nanoparticles in a reversed micelle (RM) system of polyoxyethylene (6) nonylphenyl ether (NP-6)/water/cyclohexane were investigated using a double-jet technique, in which RM solutions of AgNO(3) and KCl were added concurrently to a RM solution containing the excess concentration of chloride ion. As a result, the particle growth rate and the final particle size at a constant Rw ( identical with[water]/[surfactant]) below 5 were found to be in excellent agreement with our theoretical prediction based on a dynamic Ostwald ripening mechanism governed by the overall solubility of the solid and the diffusivity of the reversed micelles, whereas the final particle size was far beyond the size of the water pool of a reversed micelle. Thus, the dramatic reduction of the particle size in the RM system can be explained by the drastic reduction of the overall solubility of the solid and the small diffusivity of the bulky reversed micelles as a carrier of silver ion, and not by the size of the water pool of a reversed micelle as conventionally explained. Some additional contribution of a coagulation process was also suggested in a high Rw range above 5. Significant coagulation of AgCl particles was observed in a RM system with AOT in place of NP-6 even under the standard conditions for the NP-6 system.