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.     

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。     

取代基对双酞菁铥LB膜及光谱特性的影响

采用紫外-可见吸收光谱的方法研究了三种稀土夹心双酞菁铥化合物在溶液和LB膜中的聚集性和光谱特性。实验结果表明三种稀土双酞菁化合物在氯仿溶液中形成了H-聚集体,但当浓度比较低时,溶液中表现出单体的吸收。取代基OC₈H₁₇的加入使氯仿溶液中双酞菁铥化合物的聚集性减弱,而且使得吸收峰发生红移,对吸收峰的强度也有较大的影响,造成了Soret吸收带的分裂。另外,取代基OC₈H₁₇对LB膜中双酞菁分子的存在状态有较大的影响,在LB膜中,TmPc₂和TmPcPc*分子以H-聚集体的形式存在,而TmPc*₂分子以T-聚集体的形式存在。形成LB膜后,由于双酞菁分子之间排列紧密,相互作用加强,使得薄膜中分子聚集体的吸收峰相对于溶液中聚集体的吸收峰发生了一定的红移,薄膜中分子排列方向的不同对吸收光谱也有一定的影响。     

萘酞菁化合物的LB膜及光谱特性研究

研究了两种不对称取代萘酞菁化合物LB膜的制备,并采用线性吸收谱研究了萘酞菁化合物在溶液和LB膜中的聚集特性。三叔丁基萘酞菁和三叔丁基氰基萘酞菁两种化合物均能制备成很好的LB膜,它们在溶液和LB膜中也均能形成H-聚集体,但在溶液中主要是以单体的形式存在,而在LB膜中则主要是以聚集体的形式存在。两种化合物是倾斜的站立在亚相表面上,但由于氰基的作用,使三叔丁基氰基萘酞菁的倾角较小,几乎是直立在亚相表面上。     

中心对称萘酞菁分子的LB膜及其聚集特性研究

研究了三种中心对称的萘酞菁分子LB膜的制备及其聚集特性。三种萘酞菁化合物均能制成很好的LB膜。在稀溶液中,四叔丁基萘酞菁以单体为主要存在形式;对四叔丁基萘酞菁锌,由于金属锌原子的作用,在稀溶液中不仅能形成H-聚集体,而且还能形成J-聚集体,且主要以聚集体的形式存在。在LB膜中,这两种化合物均形成了H-聚集体。对于双四叔丁基萘酞菁铒不论在稀溶液中还是在LB膜中均主要以单体的形式存在。     

取代萘酞菁化合物LB膜的光谱特性研究

研究了四叔丁基萘酞菁和四叔丁基萘酞菁锌两种对称取代萘酞菁化合物LB膜的制备及其它们的聚集特性。两种萘酞菁化合物均能制成很好的LB膜。在稀溶液中，四叔丁基萘酞菁以单体为主要存在形式；而四叔丁基萘酞菁锌不仅能形成H-聚集体，而且还能形成J-聚集体，且主要以聚集体的形式存在。在LB膜中，两种化合物均形成了H-聚集体。     

温度对稀土夹心双萘酞菁LB膜光学性质的影响

 采用线性吸收谱和二次谐波产生技术研究了温度对具有中心对称结构的稀土夹心双萘酞菁化合物LB膜光学特性及其LB膜结构的影响。研究发现,加热可以使其LB膜的结构及分子间的相互作用发生变化,并形成J聚集体,从而使得吸收峰发生红移。稀土夹心双萘酞菁化合物约在40 ℃时其二次谐波信号有一个极小值,约在65 ℃时该化合物发生相变,使得二次谐波信号产生极大值,二次谐波信号最小时温度可高达180 ℃,说明该化合物的化学结构较为稳定。     

杂环化合物DADDCI在H2O/DMSO溶剂体系中的光谱及聚集行为

化合物6-苯胺基-5H-2,3-二硫杂-5,7-二氮杂环戊二烯并[c,d]茚-1,4-二甲酸二乙酯(DADDCI)是本实验室合成的新型硫氮杂环化合物.通过吸收、荧光光谱,结合理论计算,研究了该化合物在溶剂DMSO/H2O中的结构和聚集性质.结果表明,在DMSO中,化合物的苯环与并噻吩共平面,易形成H-聚集体致使荧光强度相对较弱,在H2O含量为66％-70％时,化合物形成J-聚集体,吸收峰明显红移,从390nm到444nm,伴随着荧光峰强度迅速增强至7倍以上,此时可明显观察到体系呈凝胶状.结构优化证实,化合物与H2O之间的氢键复合物取代与DMSO形成的复合物后,化合物的苯环与主平面之间发生扭转,二面角达86°.形成J-聚集体后,化合物的结构被固定,灵活性降低,分子中亚胺N接受质子的能力及胺N上的氢质子离域能力明显下降,化合物的吸收光谱受酸碱的影响程度明显降低.     

温度对萘酞菁LB膜光学特性的影响

本文采用线性吸收谱研究了温度对两种不同结构的萘酞菁分子LB膜光学特性的影响。研究发现,加热可以使它们在LB膜中的聚集体离解,四叔丁基萘酞菁锌的LB膜结构较三叔丁基氰基萘酞菁的LB膜要稳定。     

Effect of surfactants on the aggregation of pyronin B and pyronin Y in aqueous solution

Molecular dynamics of pyronin B (PyB) and pyronin Y (PyY) in aqueous solution containing different surfactants were investigated by using absorption and fluorescence spectroscopy techniques. First, the interactions of PyB and PyY with the negatively charged surfactant sodium dodecyl sulphate (SDS) were investigated in the below and above critical micelle concentration (cmc). The H-aggregate formation of the dye compounds was observed for below the cmc of SDS surfactant. The absorbance of H-aggregate absorption band of PyB and PyY decreased according to the aggregate-monomer equilibrium by increasing SDS surfactant concentration towards the cmc. Therefore, equilibrium constants of the aggregate formation and oscillator strengths of monomer and aggregate of the dye compounds were calculated from spectral studies. Moreover, aggregate formation dynamics was discussed in terms of thermodynamic functions by using temperature studies. The interactions of PyB and PyY with the positively charged hexadecyltrimethylammonium bromide (CTAB) and neutral Triton X-100 (TX-100) were also studied and it was observed that there was no aggregate formation on the absorption and fluorescence spectra for below and above the cmc.     

MOC染料单分子层薄膜聚集体的吸收光谱研究

用吸收光谱对染料的Langmuir-Blodgett(LB)膜的聚集体在不同条件下进行了研究.典型的染料1-methyl-1’-octadecy1-2,2’-cyaninperchlorate(MOC)LB膜聚集体的吸收峰(J带)在580nm附近,吸收为0.09.刚制备好的样品随时间而改变其吸收特性,表明聚集体的结构在2hr后才趋于稳定;测定了不同样品J带的参数;吸收峰值波长位置和峰的半宽度,以及这些参数随温度的变化.吸收随温度变化的可逆性是LB膜聚集体用作光记录介质的一个物理基础.温度超过100℃时,样品吸收的不可逆变化反映相变发生.     

基于紫外-可见光谱法研究叶黄素聚集体结构及其动力学

利用紫外-可见分光光度计,检测了乙醇/水溶液中,不同温度下叶黄素吸收谱,并探测了光谱随时间的变化。结果表明,在1∶1乙醇/水溶液中,高浓度和低浓度样品中,叶黄素H-聚集体随温度升高呈线性降低规律。1∶2溶液中,叶黄素聚集结构不随温度变化而变化,结构稳定。对其吸收光谱的动力学检测发现,1∶1溶液中,随着时间的推移,H-聚集体呈指数增加。分析认为,溶液中水分子的氢键是形成叶黄素聚集结构的决定因素,水分子和氢键数目的增加促使叶黄素形成稳定的H-聚集结构。     

Photoinduced transient absorption within zinc sulphide phosphors in powder form detected by diffuse reflectance laser flash photolysis

Transient absorptions have been obtained in powdered samples of ZnS : Ag, ZnS : Cu and undoped ZnS at room temperature by the technique of diffuse reflectance laser flash photolysis. For the undoped material an absorption was detected that maximises at 400 nm and decays non-exponentially with an initial half-life of (6.8±1.0)×10^?6s. The absorption is assigned to a transition within a donor impurity. In the cases of ZnS : Ag and ZnS : Cu, broad featureless absorptions in the 500–850 nm region were recorded. These decays are non-exponential and have initial half-lives of (3.1±0.2) ms and (0.48±0.05) ms for the Ag- and Cu-doped phosphors, respectively. These transient absorptions are considered to occur from electron traps introduced by the metal dopant. Laser-induced emission was also studied, and only in the case of undoped ZnS was a correlation observed between the decay of the weak emission at 520 nm and the decay of the transient absorption.     

温度对鱼鳞胶原蛋白二级结构的影响

从草鱼鱼鳞中提取酶溶性胶原蛋白(PSC),通过SDS-PAGE电泳分析为典型Ⅰ型胶原蛋白且达到电泳纯。在此基础上利用傅里叶变换红外光谱(FTIR)、拉曼光谱(Raman)和圆二色谱(CD)研究了温度对鱼鳞胶原蛋白二级结构的影响。FTIR分析表明：鱼鳞胶原蛋白具有典型的胶原蛋白特征吸收带,酰胺Ⅰ、酰胺Ⅱ和酰胺Ⅲ带的特征吸收频率分别出现在1658,1552和1238cm-1处。随温度升高,酰胺A和酰胺B峰位向低波数移动,1658cm-1处吸收峰裂解成多个吸收峰;1552cm-1处的吸收峰在35℃微略红移,随后发生明显蓝移;1238cm-1处吸收峰随温度升高向低波数移动。在拉曼光谱中,胶原蛋白的酰胺Ⅰ、酰胺Ⅱ和酰胺Ⅲ带的特征吸收频率分别出现在1669,1557和1245cm-1处,都较红外光谱的波数高;此外,921和855cm-1处脯氨酸的特征谱峰在拉曼光谱中体现出来。圆二色谱分析表明,胶原蛋白溶液在221.6和204.4nm分别有一正、负峰,具有典型胶原蛋白三螺旋结构的特征圆二色谱峰型。胶原蛋白冻干品的FTIR光谱和Raman谱线大都在35～60℃时发生波数和强度改变,而胶原蛋白乙酸溶液的CD谱线在20～35℃之间发生剧烈改变。由此可以判断胶原蛋白在固态和溶液状态下,变性温度存在一定差异,胶原蛋白冻干品比其乙酸溶液更稳定。     

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.     

Spectroscopic and morphological investigation of conjugated photopolymerisable quinquethiophene liquid crystals

3′-methyl-(5,5′′-bis[3-ethyl-3-(6-phenyl-hexyloxymethyl)-oxetane])-2,2′:5′,2′′-terthiophene (5T(Me)Ox) is a solution processable small molecule semiconductor displaying smectic-C and nematic liquid crystal phases. The pendant oxetane group can be polymerized in situ in the presence of a suitable photoacid at concentrations ≥1% by weight. Spin-coated films of pure 5T(Me)Ox and 5T(Me)Ox doped with the soluble photoacid were characterized by absorption and photoluminescent spectroscopy. Thick pristine films showed absorption and emission from a crystalline phase. Thin monolayer (<5 nm) films, as well as thicker photoacid doped films, instead showed absorption from an H-aggregate phase and emission from an excimer. Optical microscopy showed a significant change in film structure upon addition of the photoacid; large and well-orientated crystals being replaced by much smaller domains which appear to vary in thickness. Grazing Incidence Wide Angle X-Ray Scattering (GIWAXS) was used to characterize the packing and orientation of molecules in the crystalline and doped samples. The results are consistent with the photoacid doped samples forming layers of H-aggregate phase monolayer sheets parallel to the substrate where the photoacid inhibits the transition into the three-dimensionally ordered crystalline phase. Field-effect transistors and light emitting diodes were constructed incorporating 5T(Me)Ox as the active layer. Pure 5T(Me)Ox field-effect transistors showed good, p-type device characteristics, but the morphological changes upon doping result in a loss of transistor action. In the diodes, curing through melting and exposure to UV light followed by photoacid removal resulted in an increase in current density but a decrease in light emission. These results indicate that the presence of the photoacid (≥1% by weight) can have a dramatic effect on the structure, morphology and device performance of ordered, photopatternable materials for organic electronics.     

1 053，527，351 nm倍频分离膜的制备与性能研究

 用电子束蒸发及光电极值监控技术在石英基底上沉积了三倍频分离膜，将部分样品置空气中于250 ℃温度下进行3 h热退火处理。然后用Lambda900分光光度计测量了样品的光谱性能；用表面热透镜技术测量了样品的弱吸收值；用调Q脉冲激光装置测试了样品分别在355 nm和1 064 nm的抗激光损伤阈值。实验结果发现，样品的实验光谱性能良好，退火前后其光谱性能几乎没有发生温漂，说明薄膜的温度稳定性好；同时弱吸收平均值从退火前的1.07×10^-4下降到退火后的6.2×10^-5，从而使对基频的抗激光损伤阈值提高，从14.6 J/cm²上升到18.8 J/cm²，但是三倍频阈值在退火后有显著降低，从7.5 J/cm²下降到2.5 J/cm²。     

开放光路非相干宽带腔增强吸收光谱技术测量大气NO2

采用蓝色发光二极管(LED)作为非相干宽带腔增强吸收光谱技术(IBBCEAS)系统光源,测量了436～470nm波段内NO2样气的吸收,验证IBBCEAS的高探测灵敏度。通过氮气和氦气两者瑞利散射截面的差异标定了镜片在430～490nm波段内的反射率,并利用纯氧中氧气二聚体(O2-O2)在477nm处的吸收验证了镜片反射率标定的准确性。镜片反射率在461nm处最大且为0.99937,光学腔长度为73.5cm时的最大有效光程为1.17km。当光谱采集时间为20s时,NO2的探测灵敏度(1σ)达到了0.25×10-9。进行了开放光路下环境大气中NO2和O2-O2在454～486nm波段内的吸收测量,结果表明大气中气溶胶等颗粒物的Mie散射消光降低了IBBCEAS仪器的探测灵敏度(1.04×10-9)。大气中O2-O2的测量为IBBCEAS吸收光程的在线标定提供了一种可行的途径。     

通过飞秒泵浦探测技术研究PbS纳米颗粒的激发态瞬态动力学过程

利用飞秒泵浦探测技术研究了PbS半导体纳米颗粒复合的SiO₂溶胶凝胶薄膜的瞬态动力学过程。通过改变激发探测波长和激发光强度,研究引起PbS半导体纳米颗粒的非线性吸收的两种机制。当激发探测波长选在激子吸收峰附近(620nm)时,由于激子的饱和吸收引起的光致漂白,当激发波长选在激子能态的低能侧(753,800nm),同时观察到激子的饱和吸收和双激子效应引起的光致吸收。研究了激子的饱和吸收和双激子效应引起的激发态吸收随激发态电子-空穴对浓度的变化关系,表明双激子效应与载流子浓度有很大关系。在高激发强度下,双激子效应引起的诱导吸收远远大于激子跃迁引起的光致漂白,双激子效应在非线性吸收中起着决定性作用。