阴阳离子菁染料超快荧光动力学特性研究

采用飞秒荧光上转换技术,研究了阴阳离子菁染料及对应的阴离子和阳离子菁染料吸附在立方型和T型溴碘化银表面上形成J-聚集体的荧光衰减时间分辨特性,分析了几种菁染料增感体系的超快电子转移动力学过程及其对增感效率的影响.通过比较几种菁染料增感体系的荧光衰减特性,两种阴阳离子染料要明显快于阴离子染料、阳离子染料及二者的加合,说明阴阳离子染料聚集体到溴碘化银的电子注入速率较快,增感效果更好.对两种阴阳离子染料聚集体荧光衰减特性的比较,可以看出染料在T型颗粒溴碘化银上形成聚集体的荧光寿命更短,因而对T型颗粒的增感效果更好.染料Dye2的荧光衰减要快于染料Dye1,说明染料Dye2到溴碘化银的电子注入速率更快,增感效率更高.     

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11～14nm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.     

不同取代基的噻碳菁和吲哚碳菁染料对其在溴化银微晶上吸附能力及形成J-聚集体尺寸分布的影响

本文研究了5-位不同取代基的噻碳菁和吲哚碳菁染料对其在立方型颗粒和T-颗粒溴化银微晶上吸附能力的影响,并采用ACFEM(Analytical Color Fluore scence Electron Microscopy)研究了上述结构染料对其吸附在溴化银微晶所形成的J-聚集体尺寸分布的影响。实验结果表明,对吲哚碳菁染料来说,立方体溴化银微晶表面的吸附能力较T-颗粒溴化银微晶表面的吸附能力强;但对噻碳菁染料来说则相反,它们在T-颗粒溴化银微晶表面的吸附能力较立方体溴化银微晶表面的吸附能力强。另外,对5-位不同取代基的噻碳菁染料而言,无论是在立方型颗粒或T-颗粒溴化银微晶上的吸附能力来说,含取代基(无论4-取代基是吸电子型还是推电子型)的噻碳菁染料较未取代的噻碳菁染料强;而5-位取代基是吸电子型的噻碳菁染料更有利于其吸附在T-颗粒溴化银微晶表面。此外,本文还进一步证明了溴化银微晶表面上染料J-聚集体的生长过程是符合奥斯瓦尔特成熟过程的。吲哚碳菁染料在T-颗粒溴化银微晶上形成的J-聚集体的平均尺寸明显大于在立方体溴化银微晶上形成的J-聚集体的平均尺寸。吸附在立方体溴化银微晶上的5-不同取代基的噻碳菁染料对其形成J-聚集体尺寸分布的影响的研究结果表明,含取代基(-CH₃,-Ph,-Cl)的噻碳菁染料形成的J-聚集体的尺寸分布几乎相同,但与未取代的噻碳菁染料形成的J-聚集体的尺寸分布明显不同;5-位含取代基的噻碳菁染料形成的J-聚集体平均尺寸大于未取代的噻碳菁染料的。     

水溶液中一种离子菁J-聚集体引起相反电荷离子菁形成J-聚集体的影响因素

水溶液中的聚电解质可引起离子菁生成聚集体,考虑到离子菁J-聚集体与聚电解质的一些相似性,我们研究了其对相反电荷离子菁J-聚集体生成的引发作用。本文分析了离子菁J-聚集体引起相反电荷离子菁生成J-聚集体的影响因素,讨论了引发聚集与被引发聚集的离子菁的电性、它们本身的结构之间的相互关系及外加无机盐对引发聚集效应产生的影响。     

桥环菁染料——Ⅱ.1-(N-烷基-4-吡啶鎓基)-3-(N-烷基-4-吡啶亚基)-4,5-二取代-1,4-环戊二烯菁染料的合成和质子化及荧光性质研究

本文报道带有疏水长链的桥环菁染料的合成.并研究这类菁染料的质子化过程和平衡常数、取代效应,以及胶束、糖淀粉和环糊精对染料的可见光谱及质子化过程的影响,本文也考察了桥环菁染料的荧光光谱,这些研究在理论上和实际应用有一定意义.     

水溶性菁染料与类脂物混合单分子膜中J-聚集体形成的研究

报道了具有相同发色团,并有不同电荷的二种菁染料单分子膜中J-聚集体的形成。测定了单分子膜的π/A,△V/A曲线,反射光谱及吸收光谱。从实验结果得出:带正电荷的染料与花生酸混合形成单分子膜后,膜中染料的二聚体与J-聚集体随着表面压力改变存在着一个平衡。而带负电荷的染料与二十烷基胺成膜后,即使在很低的表面压下也有J-聚集体形成。同时染料分子在水面上的取向是各向异性。     

阻光染料对氯化银乳剂光谱增感的影响

增感染料在卤化银微晶上吸附并形成J-聚集体是染料光谱增感和超增感的关键步骤.本文利用紫外-可见吸收光谱研究了增感染料和阻光染料在氯化银微晶上的吸附,并考察了阻光染料对增感染料J-聚集体的形成及乳剂感光性能的影响.结果表明:不同阻光染料在氯化银微晶表面的吸附程度不同,对增感染料J-聚集体形成的影响也有差异.其中,吸附较小的不影响增感染料J-聚集体的形成,而吸附较大的阻碍增感染料J-聚集形成,特别是阻光染料在增感染料之前加入乳剂中时.在氯化银微晶上吸附很小的阻光染料基本不影响增感染料对乳剂的光谱增感,而吸附较强的阻光染料不仅吸收入射光,还抑制或破坏增感染料的光谱增感.因此,在氯化银微晶表面没有吸附的阻光染料才是优良的阻光染料.     

桥环菁染料II:1-(N-烷基-4-吡啶基)-3-(N-烷基-4-吡啶亚基)-4,5-二取代-1,4-环戊二烯菁染料的合成和质子化及荧光性质研究

本文报道带有疏水长链的桥环菁染料的合成。并研究这类菁染料的质子化过程和平衡常数、取代效应, 以及胶束、糖淀粉和环糊精对染料的可见光谱及质子化过程的影响, 本文也考察了桥环菁染料的荧光光谱, 这些研究在理论上和实际应用有一定意义。     

桥环菁染料II:1-(N-烷基-4-吡啶基)-3-(N-烷基-4-吡啶亚基)-4,5-二取代-1,4-环戊二烯菁染料的合成和质子化及荧光性质研究

本文报道带有疏水长链的桥环菁染料的合成。并研究这类菁染料的质子化过程和平衡常数、取代效应, 以及胶束、糖淀粉和环糊精对染料的可见光谱及质子化过程的影响, 本文也考察了桥环菁染料的荧光光谱, 这些研究在理论上和实际应用有一定意义。     

阴离子碳菁染料的合成与聚集动力学研究

自从1938年,Scheibe^[1]发现了菁染料聚集体中的能量传递现象,人们对菁染料的聚集行为展开了大量的研究^[2,3].由于菁染料聚集体对乳剂具有特殊的增感作用,人们主要研究聚集体在乳剂中的增感机理^[4,5]以及菁染料聚集的溶剂效应与浓度效应^[6]等,而对于菁染料聚集的动力学行为研究较少.     

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.     

卤化银乳剂颗粒上不对称菁染料J-聚体荧光的研究

光谱增感机理的研究是感光科学中的一个重要课题Gilman^[1]和Kuhn等^[2]曾经提出光谱增感的电子转移和能量传递理论。随着现代谱学手段的出现,为人们了解光谱增感的初始过程提供了条件。近年来,电子转移的机理已被广泛接受,并用来解释与光谱增感有关的各种现象。但在ns~ps范围内的光谱增感动力学方面的研究还不多见。Dahne认为光谱增感不仅决定于染料与卤化银的能级关系,而且是由动力学控制的^[3],激发态染料向卤化银导带注人电子的电子转移过程与辐射及其他无辐射去活过程是竞争的^[4]我们通过对两种不对称的苯并咪哇唾碳著染料在AgBrI乳剂颗粒上吸附形成的J一聚体的荧光性质的研究,以求深人了解光谱增感的电子转移机理及其动力学过程,无疑是有重要意义的。     

Specifics of the formation of J-aggregates of cyanine dyes in solutions of AOT/water/hexane reverse micelles

The behavior of a cyanine dye (3,3′-di-(gamma-sulfopropyl)-4,5,4′,5′-dibenzo-9-ethylthiacarbocyanine betaine pyridinium salt) was studied in AOT/water/hexane reverse micelles over a wide range of W at various concentrations of the dye, AOT, and reverse micelles. The processes occurring during the formation of the AOT/water/hexane micellar solution were studied in detail. It has been shown that, before the formation of the stable microemulsion, the dye aggregation processes occur by virtue of the interaction of the dye with the AOT anion. The amount of J-aggregates is proportional to the logarithm of the ratio of the amount of AOT molecules to the amount of dye molecules. The time behavior of J-aggregates after the formation of a micellar structure depends on the concentration of reverse micelles, thereby indicating an important role of intermicellar exchange.     

Surfactant-induced aggregation patterns of thiazole orange: a photophysical study

The aggregation behavior of the DNA marker dye thiazole orange (TO), has been investigated in two types of surfactant assemblies, namely, premicelles/micelles of sodium dodecyl sulfate (SDS) and pre reverse micelles/reverse micelles of sodium bis(2-ethylhexyl) sulfosuccinate (AOT). In the case of an SDS/water system, absorption spectral changes of TO signify the formation of H-aggregates and H-dimers of the dye at premicellar concentrations, which subsequently convert to the monomeric form beyond the critical micellar concentration (cmc). Interestingly, the observed changes in the absorption and emission characteristics due to the surfactant-induced formation of H-aggregates/dimers of TO are found to be useful to estimate the surfactant concentration parameters for premicellar aggregation of SDS. In the case of an AOT/n-heptane system, similarly, H-aggregates/dimers are observed at low AOT concentrations, below the cmc. However, in this case, the H-dimers persist even beyond the cmc. This is attributed to the strong tendency of TO for self-aggregation and its favorable electrostatic interactions with the AOT head groups. With increasing water content in the AOT reverse micelles, the hydration of the dye leads to the conversion of H-dimers to the monomeric form. The steady-state fluorescence results are nicely corroborated with those from time-resolved fluorescence studies and demonstrate the interesting behavior of the surfactant-induced aggregation of TO dye.     

Photo-induced structural changes of azobenzene Langmuir-Blodgett films

Structural changes of the Langmuir-Blodgett (LB) films of azobenzene accompanied by photoisomerization are described. First, photoisomerization is explained in terms of 'free volume'. In the polyion complex monolayers of amphiphiles having two azobenzene units at the air-water interface, the area per molecule depends on the polycation species. The fraction of cis-azobenzene in the LB films at the photostationary state under the illumination with UV light increased with increasing area per molecule, which is consistent with the concept of free volume. Second, a counter example of the concept of free volume is presented. Three-dimensional cone-shaped structures developed with trans-to-cis photoisomerization in the polyion complex LB film of a water-soluble amphiphilic azobenzene. These structures appeared and disappeared reversibly by alternate illumination with UV and visible light. The results indicate that the two-dimensional LB film structure exerts significant modification by photoisomerization. This is against the concept of free volume because this concept does not consider the possibility that the two-dimensional LB film structures may change into three-dimensional ones. Finally, photo-induced J-aggregate formation of non-photochromic and photochromic dyes is described. Two cyanine dyes were each mixed with an amphiphilic azobenzene in the LB films. These cyanine dyes are known to form J-aggregates in single-component LB films. In the mixed LB films, the J-aggregate formation was suppressed to some extent. The alternate illumination of the films with UV and visible light caused the photoisomerization of azobenzene in the mixed LB films, which triggered the J-aggregate formation of the cyanine dyes. The J-aggregate formation was accompanied by the development of three-dimensional cone-shaped structures from the film surface. When an amphiphilic merocyanine was mixed with the azobenzene in the LB films, J-aggregate formation was also induced by the alternate illumination with UV and visible light. This J-aggregate formation was also accompanied by a large morphological change: circular domains changed into fractal-like ones. The J-aggregate formation of the dyes and the concomitant morphological change were irreversible. In these cases, the photoisomerization of azobenzene served as a trigger to induce self-organization of the dye molecules.     

Controlling J aggregation in fluorescein by bile salt hydrogels

Aggregation of the well-known xanthene dye, fluorescein has been studied in the restricted environment of a bile salt hydrogel and in the bile salt micelles. It has been observed that the hydrogel can be used to some extent “control” the type of aggregation in fluorescein, since J-aggregate formation is favored at the expense of H-aggregates in the gel. In contrast to the hydrogel, the effect of normal bile salt micelles is less dramatic, i.e., bile salt micelles do not lead to significant change in the type of dye aggregation.     

J-聚集体生成中阴离子菁与外加盐反离子相互作用的量热瘀电化学活度测量

用量热和反离子活度测量法研究了阴离子菁(Ⅰ)在DMF-水(35%DMF, V/V)中生成J-聚集体时, 染料与外加盐反离子之间的相互作用。当外加盐为CdCl_2或LaCl_3时, 由量热曲线获得J-聚集焓△H_9, 分别为-42.6, -42.0 kJ·mol~(-1), 染料(Ⅰ)束缚的Cd~(2+), La~(3+)量与染料量之比分别为0.48:1和0.31:1。由反离子活度的电化学活度测量获得束缚的Cd~(2+)离子量与染料量之比为0.47:1, 这些结果表明J-聚集体中, 染料与其反离子形成了盐型的总体。     

Micellar characteristics of diblock polyacrylate-polyethylene oxide copolymers in aqueous media

The formation and structural features of micelles from low molecular weight diblock copolymers of poly(methylmethacrylate-b-ethylene oxide) PMMA-PEO (varying in total molecular weight) and poly(butylmethacrylate-b-ethylene oxide) PBMA-PEO in water, aqueous NaCl and urea solutions were examined by surface tension, dye spectral, cloud point, viscosity and small angle neutron scattering (SANS) measurements. The increasing concentrations of NaCl reduce the onset concentration of micellization and phase separation, while urea has reverse effect. The analysis of the SANS curves revealed the presence of prolate ellipsoidal micelles in diblock copolymers at various experimental concentrations and temperatures studied. The effect of temperature, NaCl and urea on the neutron scattering profiles are more or less the same which is well supported by viscosity and surface tension measurements. The diblock copolymers form spherical micelles of aggregation number in the range of 522-664. The micelles are very temperature stable.