照相光谱增感染料在溴化银沉淀表面的吸附及吸附热测量

用离心分离法得到25℃菁染料Ⅱ和Ⅲ分别在几种溶剂的溴化银分散系中的吸附等温线;记录了染料溶液的吸收光谱和吸附态染料的反射光谱。采用精密量热技术得到25±0.01℃溴化银从DMF-水溶液中吸附染料Ⅱ等位摩尔吸附热为-(3.18±0.09)KJ/mol(θ=0.87)。还对从DMF溶液中吸附染料Ⅱ的体系绘制了以单位溴化银表面的吸附热表示的吸附等温线,表明用精密量热技术可以研究染料的吸附过程。     

照相光谱增感染料及其组合在溴化银表面的吸附及吸附热测量

本文研究了三个光谱增感染料及其组合在一些溶液中的吸收光谱和吸附态染料的反射光谱,得到25℃在几种溶剂的溴化银分散系中的吸附等温线,并采用精密量热技术测量了微小吸附热效应,得到25±0.01℃染料Ⅰ在溴化银水悬浮液中被吸附的等位摩尔吸附焓△H₂₉₈-(335±2.5)kJ/mol(表面覆盖度θ=0.94)。结合对染料组合的光吸收、吸附以及吸附热等的测试结果,对照相乳剂生产中采用的先加入感绿染料Ⅱ、Ⅲ,后加入感红染料Ⅰ的步序,从吸附角度作了初步的理论探讨。研究结果也表明,精密量热技术与光吸收测量等手段相结合,将有助于在乳剂制备过程中分析研究染料的增感效果。     

溴化银中氯离子含量对增感染料吸附及增感作用的影响

本文研究了在氯溴化银上不同类型染料的吸附和不同氯离子含量的溴化银乳剂中染料的增感作用。证明在溴化银乳剂中加入氯离子以后,光谱增感的倍率增加了。不同类型的染料呈现出不同的增感规律。份菁染料在氯溴化银乳剂上具有最好的吸附能力和光谱增感作用。实验结果还表明,染料的吸附与乳剂光谱增感效果,有着良好的对应关系。证实了染料和卤化银所形成的吸附络合物是具有照相活性的。对不同类型染料的增感现象进行了讨论。     

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。     

循环伏安法研究光谱增感染料在溴化银上的吸附

用循环伏安法和电子显微镜研究了不同类型的染料在溴化银上的吸附,使用了电沉积在铂上的溴化银电极作为照相乳剂的模型,证明了由于染料电荷的不同,其在AgBr/Br^-表面上的吸附也不同,正性染料被吸附时,形成难溶的表面络合物,和负性染料相作用时,形成易溶的表面络合物,而当AgBr与非菁负性染料作用时,则由于负电排斥而不形成络合物。因此,利用循环伏安法可以判断不同染料的吸附情况。本文还研完了超增感及Riester提出的‘强色增感’中的吸附情况。实验结果表明在AgBr上染料的排列次序取决于其吸附强度。本工作还证明了Reister所提出的‘强色增感剂’的作用机理是可信的。     

N,N'-二乙基喹啉菁染料分子吸附在溴化银溶胶上的表面增强喇曼散射

N,N'-二乙基喹啉菁染料分子吸附在硫敏化过的溴化银溶胶上产生强的表面增强喇曼散射,这种散射实际上是在直晒银上产生的。N,N'-二乙基喹啉菁染料分子吸附在硫敏化过的溴化银溶胶和银溶胶上的喇曼谱基本相似。而未经硫敏化的溴化银溶胶和经硫敏化后再被高硫酸钠氧化的溴化银溶胶中测不到N,N'-二乙基喹啉菁染料的表面增强喇曼信号。本实验进一步表明,表面增强喇曼散射方法可以用于感光机理的研究。     

吸附在溴化银颗粒表面上的增感染料的ESR波谱研究

本文用电子顺磁共振技术研究了光照条件下三十八种增感染料与溴化银之间发生的电子转移过程。增感染料和溴化银无论在黑暗处还是在光照下,均不产生ESR信号。当增感染料吸附在溴化银颗粒表面上时,如不加光照,仍看不到ESR信号。只有在光照条件下,才有可能观察到ESR信号,这主要取决于增感染料分子的最高占有能级与溴化银价带的相对位置。若染料分子的最高占有能级比溴化银价带顶部高0.7 eV,就可以观察到ESR信号,反之则观察不到。顺磁性中心是由染料正空穴Dye^©形成的。根据ESR信号的强度可以判断增感染料是否有较强的减感作用。     

菁染料与溴化银相互作用性质的研究

本文用计时电位法及电位滴定研究了十六种不同染料与溴化银之间的相互作用,进一步证明了具有离域π-电子的菁染料才能与卤化银形成络合物的论点。从得到的平衡常数K表明,固体表面上的卤化银-染料与溶液中银离子-染料具有相同键性质,都是银离子与染料离域π-电子作用的结果。     

立方体溴化银颗粒光谱增感的电子转移超快动力学研究

本文利用皮秒时间分辨条纹相机技术检测了3种染料在立方颗粒溴化银上吸附后形成聚集体的荧光光谱,分析了3种染料在不同染料浓度下对染料聚集体到溴化银导带的超快电子转移过程的影响,进而分析其对增感效率的影响关系,并探讨了增感过程的微观机理.实验结果表明,荧光衰减的动力学曲线与一个双指数函数拟合得相当好,存在一快一慢两个衰减成分,快衰减成分占拟合较大比例,表明其源于与荧光衰减相竞争的从激发态染料聚集体到AgBr导带的电子转移.光致电子转移的速率及增感效率随着染料相对浓度的增加表现出一定的变化趋势,染料浓度增加,增感效率减小.     

计时电位法研究照相染料与溴化银晶体的相互作用

本文以电沉积在银电极上的溴化银为研究对象,用计时电位法研究了照相染料与溴化银晶体之间的相互作用。结果表明,染料对溴化银过渡时间、还原电位和电还原惰性物生成量均有显著影响,并且生成的电还原惰性物量的多少或平衡常数的大小与照相染料对溴化银乳剂感光度之间有一定的关系。     

水分散体系中AgBr比表面的测定及晶体习性的确定

The surface area and crystal hibit of an AgBr dispersion were determined by a in situ method. In this method, the difference of the absorption spectra of an cationic cyanine dye Ⅰ in adsorption and solution state was used for the measurement of AgBr surface area. It was 17.1 m~2/g AgBr. And the crystal habit was determined hased upon the absorption spectra of an other two cyanine dyes (Ⅱ and Ⅲ) in adsorption state. It showed a cubic crystal.     

Spectral properties of tetraanionic porphyrin in formamide colloids of layered double hydroxides

Formamide colloidal suspensions of layered double hydroxides (LDHs) with anionic dye, meso-tetrakis(4-sulfonatophenyl)porphine (TPPS) were prepared. Optical properties of these suspensions were investigated by means of absorption and fluorescence spectroscopies in the visible region. For more detailed characterization, second derivative curves of the spectra were calculated. The adsorption of the dye on LDH nanosheets led to partial molecular aggregation, reflected in significant changes of the dye optical properties. The Soret band in the absorption spectra was split into two peaks and decreased in intensity. Changes were observed also for the Q-bands. The molecular aggregation significantly quenched the emission of the dye. The low intensity emission from dye H-aggregates was identified at slightly longer wavelengths. The molecular aggregation increased with the dye/LDH ratio. At low dye loadings, the optical properties were very similar to the dye solution. The yields of the dye molecular aggregation increased with LDH surface charge.      

掺杂立方AgBr乳剂介电频谱的研究——Ⅲ.硫的影响

本文研究了用1×10^-5mol～1×10^-2mol Na₂S₂O₃/mol AgBr和1×10^-4mol～1×10^-2mol Na₂S/mol AgBr掺杂的立方AgBr乳剂的介电吸收频谱.发现在我们的实验条件下,当Na₂S₂O₃的加入量小于1×10^-4mol/mol AgBr时,Na₂S₂O₃,在AgBr微晶上吸附的影响占主要,样品介电吸收峰的f_max稍向低频方向位移,f_max位移量(△log f_max)的大小与AgBr微晶的表面状况有关.当Na₂S₂O₃的加入量大于1×10^-4mol/mol AgBr时,Na₂S₂O₃对AgBr微晶表面的溶蚀的影响逐渐占优势,使AgBr微晶表面的结构不均匀性增加,同时乳剂的pAg上升,结果样品的f_max逐渐向高频方向移动,介电吸收峰亦相应展宽.Na₂S的加入量小于1×10^-3mol/mol AgBr时,样品的f_max有稍向低频位移的趋势.当将掺Na₂S的样品干燥后在75℃和110℃下放置6小时后,f_max明显向高频方向移动.     

(AgBr)_核·(Ag)_壳纳米粒子的制备及其共振散射光谱研究

以 (AgBr) m 团簇作晶种 ,在柠檬酸钠存在条件下 ,(AgBr) m 团簇表面结合的Ag+被光化学还原而获得土红色的液相 (AgBr) 核·(Ag) 壳 纳米粒子 .研究了 (AgBr) 核·(Ag) 壳 纳米粒子的光谱特性 ,在 51 2nm处有最强共振散射峰 ,在41 0nm处产生一个吸收峰 .结果表明 ,(AgBr) 核·(Ag) 壳 纳米粒子的形成是导致51 2nm共振光散射的根本原因 .     

STRUCTURE OF DYE AGGREGATES AND THE MECHANISM(S) OF PHOTOSENSITIZATION OF AgBr*,†

Abstract— This paper reports the present conclusions of an extended investigation on photo-sensitization of silver bromide. A general molecular packing structure for dye aggregates on the AgBr (111) surface is proposed. This structure, along with the observed spectral absorption displacements of small aggregates, is used to elucidate the phenomena of antisensitization and supersensitization. Supersensitization is seen as a partitioning of large dye aggregates into small aggregates by a deliberately added second component or by gaps between the aggregates. This partitioning isolates antisensitizing dye in a small fraction of the aggregates and minimizes its effect. The smallest aggregates are least likely to contain an antisensitizer, and show the highest quantum efficiency for photoconductivity and photographic action. Photoconductivity measurements establish that supersensitization occurs before the electron appears in the AgBr phase.
The question of direct electron injection vs. energy transfer as mechanisms for AgBr photosensitization is examined in terms of radiationless transfer to surface Ag₂S on AgBr. The absorption of surface Ag₂S is shown to be adequate for acceptance of Förster transfer from the dye, and surface Ag₂S is known to be photographically active. However, this mechanism is inefficient, and inadequate to account for observed high efficiency infrared sensitization. Direct electron injection is seen as the more probable mechanism for efficient dye sensitization of AgBr.     

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。     

Effects of Dye‐Adsorption Solvent on the Performances of the Dye‐Sensitized Solar Cells Based on Black Dye

The effects of the dye‐adsorption solvent on the performances of the dye‐sensitized solar cells (DSSCs) based on black dye have been investigated. The highest conversion efficiency (10.6 %) was obtained in the cases for which 1‐PrOH and the mixed solvent of EtOH and tBuOH (3:1 v/v) were employed as dye‐adsorption solvents. The optimized value for the dielectric constant of the dye‐adsorption solvent was found to be around 20. The DSSCs that used MeOH as a dye‐adsorption solvent showed inferior solar‐cell performance relative to the DSSCs that used EtOH, 1‐PrOH, 2‐PrOH, and 1‐BuOH. Photo‐ and electrochemical measurements of black dye both in solution and adsorbed onto the TiO₂ surface revealed that black dye aggregates at the TiO₂ surface during the adsorption process in the case for MeOH. Both the shorter electron lifetime in the TiO₂ photoelectrode and the greater resistance in the TiO₂–dye–elecrolyte interface, attributed to the dye aggregation at the TiO₂ surface, cause the decrease in the solar‐cell performance of the DSSC that used MeOH as a dye adsorption solvent.