磺化金属萘酞菁聚集倾向的光谱研究

在磺化金属萘酞菁的荧光光谱和电子吸收光谱的Q谱带上观察到激基缔合物的荧光光谱峰和基态聚集物的吸收光谱峰。荧光光谱和吸收光谱实验说明 ,溶液中聚体分子和单体分子同时存在 ;聚体放出或吸收光子后都解离为单体 ;在荧光光谱中金属萘酞菁的激基缔合物荧光峰相对于单体荧光峰发生红移 ,在吸收光谱中金属萘酞菁基态聚集体的吸收峰相对于单体吸收峰发生蓝移 ,聚集体的荧光光谱和吸收光谱有镜像对称关系。磺化萘酞菁钴浓度较大时 ,其荧光光谱的猝灭较大。     

LB薄膜中四新戊氧基酞菁锌和四壬基酞菁铜分子聚集体的吸收光谱的温度特性

本文制备了四新戊氧基酞菁锌(Tetra-neopentoxy phthalocyanine zine)(TNPPeZn)和四壬基酞菁铜(Tetra-nonyl phthalocyanine copper)(TNPeCu)两种酞菁衍生物的Langmuir-Blodgett(LB)薄膜.通过测量10～473K温度下的吸收光谱,研究了两种薄膜的分子聚集状态.TNPPeZn的LB薄膜中,存在着分子单体和分子二聚体,在吸收光谱中分别表现为680nm和620nm的吸收峰.随着温度的升高,分子单体逐渐转变为分子二聚体,这个过程是不可逆的.TNPeCu的LB薄膜中,除了分子单体和分子二聚体以外,还有吸收为740nm的分子J聚集体存在.随着温度的变化,J聚集体发生可逆变化.     

八丁氧基-2,3-萘酞菁铜(Ⅱ)的合成与UV光谱研究

采用分子碎片法合成了5,9,14,18,23,27,32,36-八丁氧基-2,3-萘酞菁铜,利用元素分析、红外及紫外可见光谱进行了表征。配合物的电子吸收光谱表明:新配制的氯仿溶液中萘酞菁铜的Q带H聚集体和单体的吸收峰在758、854nm处,5h后单体和H聚集体的吸收峰基本消失,出现了798和909nm的错位H/J聚集体以及960nm的J聚集体吸收,12h后主要以795nm的H聚集体形式存在。     

3-羟基黄酮在不同极性和酸碱度溶剂中的光谱研究

实验观测了3-羟基黄酮(3-HF)在不同极性溶剂中的吸收光谱和荧光光谱,发现在吸收光谱中有3个吸收带,峰值位于300和345 nm的两个吸收带较强,位于415 nm处的吸收带较弱。用345 nm作为激发光,观测到两个荧光带,其中峰值位于400 nm的荧光带为3-HF稀醇式构型的发射,随着溶剂极性的增大其强度增强,峰值位于526 nm的荧光带为3-HF互变异构体的发射,随着溶剂极性的增大其强度减弱,这表明溶剂极性阻碍质子转移的发生。用415 nm的光激发样品,在荧光光谱中发现了3个新荧光谱带,峰值分别位于440,471和515 nm,这3个荧光谱带归属至今未见报道。为了指认这3个荧光谱带,分别观测了3-HF在不同酸碱度溶液的荧光光谱及其吸收光谱,通过对这些光谱的分析研究,指认出荧光峰位于440和471 nm的荧光谱带为3-HF的两种阳离子的发射,峰值位于515 nm的荧光谱带为3-HF的阴离子的发射。     

轴向尼泊金甲酯取代的酞菁硅的合成、光谱性质和离体光动力活性

合成了一种轴向尼泊金甲酯取代的酞菁硅,即二(4-甲酯基苯氧基)酞菁硅,并通过IR,NMR,HPLC和元素分析等手段进行了表征。研究了该配合物在不同溶剂中的电子吸收光谱和荧光光谱。结果表明,它在含2%Cremophor EL,20%丙二醇的生理盐水中,以单体形式存在,Q带最大吸收位于683 nm附近,相应的摩尔吸光系数为7.47×104mol-1.L.cm-1,最大发射带位于690 nm附近,荧光量子产率为0.34,荧光寿命为4.7 ns。初步的离体光动力活性测试表明,该配合物对B16黑色素瘤细胞具有光动力灭活能力,半致死量LD50为1.2×10-4mol.L-1。     

酞菁锌掺杂二氧化硅凝胶基质的光谱学特征

利用溶胶凝胶技术将四磺化酞菁锌 (ZnPcS4)成功地引入到了二氧化硅凝胶基质中 ,制备了均匀掺杂的有机 /无机复合干凝胶。研究ZnPcS4分子在溶胶凝胶过程中紫外可见吸收光谱的变化规律以探索其在复合体系中的存在状态。实验表明 ,在溶胶阶段 ,随着时间的延长 ,紫外可见吸收光谱中单体的吸收峰强度增大 ,说明凝胶中酞菁单体的浓度增大 ;而形成凝胶后 ,随着时间的延长 ,紫外可见吸收光谱中单体的吸收峰强度减小 ,二聚体的吸收峰强度增大 ,说明由于体系结构和微化学环境的变化 ,酞菁分子趋向于聚合。     

一种轴向核苷修饰硅酞菁的合成与光动力抗癌活性

合成了一种轴向核苷修饰硅酞菁,即二[5′-(2′,3′-O-异丙基)-5-甲基胞苷氧基] 硅酞菁,并通过1H NMR和HR-MS等手段进行了表征。该化合物在N,N-二甲基甲酰胺和含1% Cremophor EL水溶液中以单体形式存在,Q带最大吸收波长分别位于676和679 nm,荧光发射峰分别位于685和689 nm。离体光动力抗癌活性表明,该化合物具有显著的光动力抗癌活性,对人肝癌细胞HepG2的半致死浓度(IC₅₀)低至7.8×10-8mol·L-1。荧光共聚焦显微镜研究显示,SiPcG可定位于细胞线粒体中。研究表明,SiPcG是一种有发展潜力的新型抗癌光敏剂。     

酞菁锌参杂二氧化硅凝胶基质的光谱学特征

利用溶胶-凝胶技术将四磺化酞菁锌（ZnPcS4）成功地引入到了二氧化硅凝胶基质中，制备了均匀掺杂的有机/无机复合干凝胶。研究ZnPcS4分子在溶胶-凝胶过程中紫外-可见吸收光谱的变化规律以探索其在复合体系中的存在状态。实验表明，在溶胶阶段，随着时间的延长，紫外-可见吸收光谱中单体的吸收峰强度增大，说明凝胶中酞菁单体的浓度增大；而形成凝胶后，随着时间的延长，紫外-可见吸收光谱中单体的吸收峰强度减小，二聚体的吸收峰强度增大，说明由于体系结构和微化学环境的变化，酞菁分子趋向于聚合。     

酞菁铜旋涂薄膜的形貌与光谱学性质研究

采用旋涂法制备了2,9,16,23-四-异丙氧基酞菁铜(CuPc(OC3H7-i)4)薄膜,利用AFM、UV-Vis和FT-IR对薄膜的表面形貌和光谱学性质进行了表征。薄膜表面结构是由约为216nm×55nm×4nm的清晰纳米畴组成,旋涂膜中酞菁铜分子是处于一种无序的状态,其Soret带吸收与氯仿溶液相比位置不变,而Q带的聚集体和单体的吸收峰红移约20nm。     

番茄红素的紫外可见光谱和荧光光谱分析

研究了番茄红素在不同溶剂中的紫外可见光谱图,对结果进行分析后发现番茄红素在正己烷、石油醚、丙酮、乙酸乙酯具有较低折光率的溶剂中的特征吸收带波长非常接近,但在较高折光率的溶剂苯、二硫化碳中的特征吸收带与以丙酮作为溶剂相比有不同程度的红移。番茄红素溶于丙酮与水的混合溶剂,当丙酮与水的体积比达到3∶2时,吸收光谱在紫外区出现一新的吸收峰,在可见区吸收光谱的精细结构消失。用荧光光度计采集不同溶液的番茄红素的荧光光谱,番茄红素的荧光峰位于580—590nm,在极性溶剂中荧光发射增强。     

磺化酞菁镓、钒、铝、锌在水、醇、胶束中的聚合行为的研究

采用分光光度法研究了四磺化酞菁镓,钒,铝和二磺化酞菁锌在水,醇－水,胶束体系中的聚合行为,测定了配合物的二聚常数。结果表明,ＡｌＴＳＰｃ形成二聚体是一个慢反应,而ＧａＴＳＰｃ,ＺｎＢＳＰｃ和ＶＯＴＳＰｃ的二聚体形成是快速过程。     

基于ESIPT机理检测Al3+荧光探针分子结构和电子光谱的理论研究

本文应用密度泛函理论（DFT）和含时密度泛函理论（TD-DFT）方法，研究了具有激发态分子内质子转移（ESIPT）特性的3-羟基黄酮（3HF）及其两种氰基和氨基取代衍生物（3HF-CY和3HF-AM）作为水溶液中Al3+离子检测的荧光探针分子结构和电子光谱性质. 计算得到了与ESIPT过程相关的键长、键角以及势能曲线，模拟计算了单独分子和分子@Al3+复合物的吸收和荧光光谱. 结果表明，氰基或氨基的引入均会抑制3HF的质子在基态（S0）或激发态（S1）的转移. 而从得到的吸收光谱可以看出，在3HF中引入吸电子基团氰基可以引起其吸收光谱的红移，而给电子基团氨基的引入则出现相反现象. 此外，与3HF-AM的荧光光谱相比，3HF-AM@Al3+复合物发生了75.88 nm的蓝移，由此推测3HF-AM与水中的Al3+反应后，在光激发下溶液荧光会由绿色转变为紫色，表明3HF-AM分子可以作为有效检测水中Al3+的荧光探针.     

中草药猫人参与其同科同属植物的光谱分析与鉴别

本文用紫外光谱和荧光光谱等方法对猫人参与其同科同属的木天蓼、藤梨根进行了分析与鉴别。结果表明 :在 2 54nm紫外灯下 ,猫人参水溶液几无荧光 ,而木天蓼、藤梨根水溶液均显较强荧光 ;三种药材提取液的紫外光谱和荧光光谱存在明显差别。     

高分子添加剂对激光染料荧光的增强效应

本文研究以水作溶剂的Rh-6G激光染料中加入高分子添加剂——聚乙二醇(分子量为6000)引起的染料荧光的增强效应。通过荧光光谱,吸收光谱与染料浓度,添加剂含量的关系的实验研究,定量地给出了不同添加剂量对荧光的增强作用。表明了荧光增强效应的机理主要是添加剂抑制了二聚物的形成。     

Monomerization of photosensitizers by ultrasound irradiation in surfactant micellar solutions

The absorption and fluorescence properties of pheophorbide-a, Sodium salt of pheophorbide-a and its long chain (C₂₀H₃₉) ester (Pheophytine) were investigated in air-saturated micellar aqueous solutions before and after ultrasound irradiation (48 kHz, 10 min). The absorption spectra changed depending on the surfactant; cetyltrimethyl ammonium bromide (CTAB) or sodium dodecyl sulfate concentrations. The formation of different molecular species in various micellar solutions was estimated from the analysis of the absorption spectra. The absorption bands resulted from an aggregated form of the chromophore present in 50 mM phosphate buffer and in pre-micellar solutions. The specific bands of the aggregate disappeared with a simultaneous increase of the bands of monomer in normal micellar solution. The fluorescence spectra, the lifetimes and the fraction of each component (with a characteristic lifetime) of the chromophore in the micellar solutions changed significantly before and after ultrasound irradiation although the changes in absorption spectra were small. The fluorescence emission band at 710 nm due to the aggregate almost disappeared in the pre-micellar solution after ultrasound irradiation. The fraction of the short-lifetime component estimated for the aggregates decreased 55% in H₂O or 85% in 2 mM CTAB, however the long-lifetime components increased after the ultrasound treatment. From these fluorescence properties, it was concluded that the aggregated molecules were converted to a stable monomeric form by ultrasound. Extrapolation of these data to in vivo situations suggests that pretreatment of certain photosensitizers with ultrasound in micellar solutions may lead to increased efficiency of photodynamic therapy since only the monomers are photodynamically active.     

黄烷酮及其羟基衍生物的荧光性质研究

黄烷酮类化合物是天然药物的重要活性成分,也是有机合成的研究热点之一,但此类化合物的荧光性质尚缺乏研究。研究了黄烷酮及其6种羟基衍生物的荧光性质,发现黄烷酮(Flavanone,FV)、7-羟基黄烷酮(7-Hydroxyflavanone,7HF)和6-羟基黄烷酮(6-Hydroxyflavanone,6HF)的水溶液有荧光,而2’-羟基黄烷酮(2’-Hydroxyflavanone,2’HF)、4’-羟基黄烷酮(4’-Hydroxyflavanone,4’HF)、柚皮素(4’,5,7-三羟基黄烷酮,Naringenin)和乔松素(5,7-二羟基黄烷酮,Pinocembrin)的水溶液基本无荧光。在三维荧光图谱中,FV的荧光激发波长(λ_ex)为235,265和340 nm,发射波长(λ_em)为386 nm;7HF的λ_ex为230,276和315 nm,λ_em为391 nm;6HF的λ_ex为260和356 nm,λ_em为482 nm。研究了pH对FV,7HF和6HF荧光的影响,从分子结构的角度讨论了pH对荧光产生影响的原因。研究了7HF和6HF在不同pH条件下的紫外吸收光谱,用pH-光度法测得7HF和6HF的羟基质子电离常数pK_a分别为7.26±0.05和9.90±0.02。研究了溶剂(甲醇)对FV,7HF和6HF荧光光谱的影响,发现FV和7HF在甲醇溶液中的荧光比在水中减弱,而6HF在甲醇中的荧光显著增强。在有序介质(SDS,CTAB,β-CD)中,FV和7HF的荧光减弱,而6HF在β-CD或CTAB中的荧光增强。以硫酸奎宁或L-色氨酸为参比,测得FV和7HF水溶液的荧光量子产率分别为0.057和0.012;6HF在甲醇中和在β-CD浓度为1.62 mg·mL-1的水溶液中的荧光量子产率分别为0.064和0.012。     

The molecular aggregation of pyronin Y in natural bentonite clay suspension

The molecular aggregation and spectroscopic properties of Pyronin Y (PyY) in the suspension containing natural bentonite clay were studied using molecular absorption, steady-state and time-resolved fluorescence spectroscopy techniques. Interaction between the clay particles and the cationic dye compounds in aqueous solution resulted in significant changes in spectral properties of PyY compared to its molecular behavior in deionized water at the same concentration. These changes were due to the formation of dimer and aggregate of PyY in the clay suspension as well as the presence of the dye monomer. The H-type aggregates of PyY in the clay suspension were identified by the observation of a blue-shifted absorption band of the dye compared to that of its monomer. In spite of diluted dye concentrations, the H-aggregate of PyY in the clay suspension was formed. The intensive aggregation in the clay suspension attributed to the localized high dye concentration on the negatively charged clay surfaces. Adsorption sites of PyY on the clay particles were discussed by deconvulated absorption and excitation spectra. Fluorescence spectroscopy studies revealed that the fluorescence intensity of PyY in the clay suspension is decreased by H-aggregates drastically. Moreover, the presence of H-aggregates in the clay suspension resulted in the decrease of fluorescence lifetime and quantum yield of PyY compared to those in deionized water.     

IR absorption spectrum (4200–3100 cm) of H2O and (H2O)2 in CCl4. Estimates of the equilibrium constant and evidence that the atmospheric water absorption continuum is due to the water dimer

IR absorption spectra, 4200–3100 cm⁻¹, of water in CCl₄ solutions are presented. It is shown that for saturated solutions significant amounts of water are present as dimer (ca. 2%). The IR spectra of the monomer and dimer are retrieved. The integrated absorption coefficients of the monomer absorption are significantly enhanced relative to the gas phase values. The dimer spectrum consists of 5 bands, of which 4 were expected from data from cold beams and cold matrices. The origin of the “extra” band is discussed. In addition it is argued that the dimer absorption bands intensities must be enhanced relative to the gas phase values. Based on recent calculations of band strengths, and observed frequency shifts relative to the gas phase, the intensity enhancement factors are estimated as well as the monomer/dimer equilibrium constant in CCl₄ solution at T=296 K (K_c=1.29 mol⁻¹ L). It is noted that the observed dimer spectrum has a striking resemblance with the water vapour continuum determined by Burch in 1985 which was recently remeasured by Paynter et al. and it is concluded that the atmospheric water absorption continuum in the investigated spectral region must be due to water dimer. Based on the newly published spectral data a revised value of the gas phase equilibrium constant is suggested (K_p=0.035 atm⁻¹ at T=296 K) as well as a value for the standard enthalpy of formation, ΔH⁰=15.4 kJ mol⁻¹.