α、ω-双香豆素长链化合物激基缔合物的研究

通过α、ω－双香豆素长链化合物详细研究了香豆素激基缔合物的荧光行办，通过吸收光谱、荧光光谱和激发光谱，考察了香豆素激基缔合物的发光位置与激发波长，借助单光子技术确定了形成的是分子内的激基缔合物，通过1HNMR谱研究了不同双香豆素长链化合物的构象分布，揭示了在水溶液中由于疏水相互作用促进了长链化合物分子内激基缔合物的形成．     

疏水作用对光化学和光物理过程的影响 Ⅹ. 非平面分子2,2’-联萘在促簇性溶剂中的簇集和激基缔合物的形成

激基缔合物是由一个激发态分子和一个基态分子形成的复合物,组成激基缔合物的两个分子平面必须彼此平行呈夹心面包式构型^[1]。在某些情况下,两个芳香环在基态时就呈激基缔合物的构型并有很强的相互作用,形成基态复合物一二聚体^[2,3]。人们对平面结构的芳香化合物分子形成的激基缔合物已经进行了大量研究,并且注意到非平面的芳香化合物分子很难形成激基缔合物^[4]。     

新型三嗪桥连的双1,8-萘酰亚胺衍生物的合成及其光物理行为

以1,8-萘酰亚胺和三聚氯氰为主要原料, 合成了两种由三嗪环桥连的双1,8-萘酰亚胺化合物3 和5. 采用紫外-可见光谱和荧光光谱等手段考察了两种化合物在不同溶剂中的光物理行为. 与参比化合物N-丁基-1,8-萘酰亚胺相比, 在二氯甲烷、三氯甲烷和甲醇等极性溶剂中, 化合物3和5除了在短波区(λ<400 nm)存在1,8-萘酰亚胺的特征荧光发射峰外, 在长波区(>450 nm)均产生一个较强的新荧光发射峰, 表现出分子内激基缔合物的光物理行为. 与化合物5相比, 由于化合物3特殊的构象异构, 其荧光强度发生严重的猝灭. 在非极性溶剂甲基环己烷中, 化合物5 由于存在较强的分子间氢键作用而聚集, 受激后形成了较稳定的分子间激基缔合物, 但未观察到明显的分子内激基缔合物的形成. 在甲苯溶剂中, 化合物3和5与甲苯分子形成了激基复合物, 并未形成分子内激基缔合物. 进一步研究3和5的固态激发态性质, 发现化合物3和5的固体薄膜受激后分别在465和469 nm处出现激基缔合物的特征荧光发射峰.     

α、ω-双发色团长链化合物在不同环境中的光物理光化学行为研究

在对α、ω-双香豆素长链化合物的研究中,我们发现,由于链的束缚使其光化学行为不同于香豆素单体,其光二聚反应的产物不随溶剂的极性变化与敏化剂存在与否而有所不同,通过二维核磁、核磁碳谱等技术,对二聚产物进行了详细表征,证实得到的均是分子内顺式头一头二聚体,同时由于链的束缚使其分子内激基缔合物易于形成,在室温水溶液中首次明确地观察到香豆素的激基缔合物.     

核苷磷酸盐对含双芘侧链荧光敏感器化合物的荧光猝灭与分子识别

合成了一种在水溶液中对核苷磷酸盐ATP,ADP,AMP阴离子具有识别能力的荧光化学敏感器分子---化合物1。通过检测化合物1在水溶液中芘激基缔合物荧光发射强度随核苷磷酸盐、腺嘌呤等的加入而引起的变化,求出不同核苷磷酸盐及腺嘌呤对芘激基缔合物荧光发射的猝灭常数,并进行了比较研究。利用荧光发射强度随不同核苷磷酸盐引入而发生的变化计算出化合物1对不同核苷磷酸盐进行配位的配位稳定常数。结果表明所合成的化合物1对ATP有着良好的识别力选择功能。此外,还利用分子力学的计算方法对化合物1及其与核苷磷酸盐形成配合物后的分子构象及几何尺寸作了计算,并结合实验结果进行了初步讨论。     

多足化合物的分子内激基缔合物形成及pH对其荧光的影响

研究了含萘脲基多足化合物溶液的稳态和瞬态光物理行为.由于分子内不同足间脲基的相互作用干扰了萘基的π-π叠合,使分子内萘基的激基缔合物生成受到影响.实验表明:由于三足化合物存在着给电子叔胺基团,因此当萘基被激发时、可因分子内的光诱导电子转移而导致荧光猝灭.正因如此,在三足化合物归一化后的稳态光谱中激基缔合物的发光强度很弱.用皮秒级单光子记数技术测得该化合物的瞬态荧光为三指数衰变过程.其中最长寿命的物种,即属于生成激基缔合物后再分解为萘激发态的部分仅占总量的4%,与稳态的结果相一致.工作表明对这类可用作荧光化学敏感器的三足化合物,如利用其激基缔合物的强度变化为其识别外来物种的敏感部位并不适合.相反,如引入的外来物种能影响化合物的分子内光诱导电子转移,进而影响萘基的发光强度,则是一较好的判别外来物种是否已进入主体的标志.     

基于二噻吩并[2,3-b:3′,2′-d]噻吩开环反应的二芘基四联噻吩的制备及其激基缔合物荧光行为

通过芘基锂对二(三甲基硅基)二噻吩并[2,3-b:3′,2′-d]噻吩开环产生碳负离子,再经氯化铜氧化偶联,获得二芘基四联噻吩化合物.考察了该化合物在溶液中的光谱行为,结果表明,该化合物在溶液相的部分分子可以发生基于分子构象折叠而形成的分子内激基缔合物;在THF-H2O二元体系中可以形成分子间的基于激基缔合物的聚集诱导发光现象.     

时间分辨荧光光谱研究聚2-乙烯基萘与对苯二甲酸二甲酯形成的三分子激基复合物

本文研究了在稀溶液中,聚2-乙烯基萘分子内不同生色团之间相互作用后先形成分子内激基缔合物,然后与受体分子相互作用后再生成三分子激基复合物的机理。测定了聚2-乙烯基萘分子内激基缔合物的荧光寿命的r_2=18.83ns;形成三分子激基复合物的速度常数k_7=4.18×10~9(mol/L)~(-1)S~(-1),受扩散速度反应控制。首次提出了激基缔合物或激基复合物可能是形成三分子激基复合物的中间体,并提出了由激基缔合物再形成三分子激基复合物的光物理过程的理论模型。     

聚甲基苯乙基硅烷的荧光光谱

本文研究了聚甲基苯乙基硅烷(PMPES)的荧光光谱。从浓度效应和猝灭规律证明了PMPES溶液中既有分子间激基缔合物又有分子内的激基缔合物。低温荧光光谱说明在基态时有部分生色团呈激基缔合物构象。     

磺甲基酚醛树脂激基缔合物的荧光光谱

本文研究了磺甲基酚醛树脂(SMP)在无盐和外加盐的水溶液中的荧光光谱.证实了生色团在主链上的聚电解质SMP分子间激基缔合物的形成.探讨用SMP分子间激基缔合物荧光作为研究SMP分子形态变化探针的可能性.     

Highly selective fluorescent sensing of Cu ion by an arylisoxazole modified calix[4]arene

A novel fluorescent chemosensor 1 with two anthraceneisoxazolymethyl groups at the lower rim of calix[4]arene has been synthesized, which revealed a dual emission (monomer and excimer) when excited at 375 nm. This chemosensor displayed a selective fluorescence quenching only with Cu²⁺ ion over all other metal ions examined. When Cu²⁺ ion was bound to 1, the fluorescence intensities of both monomer and excimer were quenched. Furthermore, the association constant for the 1:1 complex of 1·Cu²⁺ was determined to be (1.58 ± 0.03) × 10⁴ M⁻¹.     

含芘荧光化学敏感器化合物同小牛胸腺DNA分子间的相互作用

研究了含芘荧光化学敏感器分子被ctDNA猝灭的荧光光谱.ctDNA分子对该化学敏感器中芘的激发单体,激基缔合物都有猝灭作用.对激发单体的猝灭速度顺序为;化合物(2)>化合物(1)>芘丁酸>化合物(3);对激基缔合物的猝灭速度顺序为;化合物(2)化合物(3).由得到的荧光猝灭数据,可按公式(2)求得荧光化学敏感器分子与ctDNA分子相互作用的稳定常数.发现化合物(2)与ctDNA分子间有着最强的相互作用能力.按ctDNA和含芘荧光化学敏感器的分子结构、构型以及分子内原子-原子的间距等提出了ctDNA分子与该荧光化学敏感器的作用模型,并对上述结果进行了初步解释.     

Solvent-driven multiply configurable on/off fluorescent indicator of the pH window: a diethylenetriamine bearing two end pyrene fragments

Fluorescence behaviors of a simple-structured molecule (L), a diethylenetriamine bearing two end pyrene fragments, have been investigated in water. Effects of adding a less-polar organic solvent (acetonitrile: MeCN) on the emission behaviors have been studied by means of steady-state and time-resolved fluorescence measurements. L dissolved in water shows dual-mode fluorescence consisting of monomer and excimer emissions. The monomer emission shows an "on-off" intensity profile against the pH window (pH 2-12), whereas the excimer emission shows an "off-on" profile. Upon MeCN addition, the monomer emission maintains the "on-off" profile. In contrast, the "off-on" profile of the excimer emission is drastically changed: L shows two more types of profiles, "off-on-off-on" and "off-on-off", along with the MeCN concentration increase, thus behaving as a multiply configurable fluorescent indicator of the pH window. The MeCN-driven excimer emission switching of L is triggered by (i) the decrease in stability of the intramolecular ground-state dimer (GSD) formed between the end pyrene fragments, which suppresses the direct photoexcitation of GSD (suppression of the "static" excimer formation), leading to a decrease in the excimer emission intensity at basic pH; and (ii) the decrease in polarity of solution, which allows formation of a "dynamic" excimer via a monomer-to-excimer transition, resulting in an enhancement of the excimer emission intensity at acidic-neutral pH.     

Electric field effects on absorption and fluorescence spectra of trimethylsilyl- and trimethylsilylethynyl-substituted compounds of pyrene in a PMMA film

External electric field effects on absorption and fluorescence spectra of 1,3,6,8-tetrakis(trimethylsilyl)pyrene and 1,3,6,8-tetrakis(trimethylsilylethynyl)pyrene (TMSPy and TMS(E)Py, respectively) have been examined in a poly(methyl methacrylate) (PMMA) film at various concentrations at various temperatures. TMS(E)Py preferentially forms an aggregate in a PMMA film, as the concentration increases, indicating that the acetylenic groups enhance the pi-pi interactions between pyrene molecules. The change in molecular polarizability following excitation has been determined both for the monomer and for the aggregate, based on the electroabsorption spectra. The change in molecular polarizability following emission has also been determined in both compounds, based on the electrofluorescence spectra. TMSPy exhibits two excimer fluorescence emissions at high concentrations which are ascribed to the partially overlapping excimer and the sandwich-type excimer, respectively, besides the monomer fluorescence emitted from the locally excited state. The sandwich-type excimer fluorescence as well as monomer fluorescence is quenched by an electric field, whereas the fluorescence of the partially overlapping excimer is enhanced by an electric field. Excimer fluorescence of TMS(E)Py, which arises from the sandwich-type excimer, is quenched by an electric field at any temperature. Only one species of the partially overlapping excimer is confirmed in TMSPy, while no partially overlapping excimer is confirmed in TMS(E)Py.     

Guest‐responsive excimer emission in an α‐helix peptide bearing γ‐cyclodextrin and two naphthalene units

An α‐helix peptide (17 amino acids) bearing γ‐cyclodextrin (γ‐CD) and two naphthyl units (γ‐N₂17) was designed and prepared as a new type of chemosensor. The α‐helix peptide with γ‐CD sandwiched between two naphthyl moieties exhibits excimer emission by inserting the two naphthalene moieties into the γ‐CD cavity from the opposite sides in the side chain of the peptide. The two reference peptides, which have one naphthalene moiety and one γ‐CD unit, exhibit only monomer fluorescence and have larger binding constants for the examined guests than γ‐N₂17.     

EXCITED STATES OF DNA AND ITS COMPONENTS AT ROOM TEMPERATURE—III. SPECTRA, POLARISATION AND QUANTUM YIELDS OF EMISSIONS FROM ApA AND poly rA*

Abstract— Corrected normalised emission spectra from 300 to 480 nm and their polarisation are reported for neutral and poly rA at room temperature. Yields are 4 times (ApA) and 6 times (poly rA) greater than the monomer. Comparison of emission spectra and polarisation spectra demonstrates heterogeneity of emission and, following attempts at spectral synthesis, comparison with experimental reference spectra allows the observed total emission spectra to be resolved into four components assigned as I monomer-like emission, II excimer fluorescence, HI monomer phosphorescence, IV excimer phosphorescence; the polarisation of the excimer fluorescences of ApA and poly rA are deduced. The observations can be understood quantitatively using a simple stacking model with excimer emissions originating in the stacked components. Quantitative differences between ApA and poly rA are due to their different hypochromism and extent of stacking. Differences of polarisation are attributed to different stacking geometries, and the directional properties of the transition moment suggest that the excimer fluorescence is largely charge-resonance in nature.     

Factors affecting the formation in the solid state of the metastable complex between naphthalene and dimethyl-β-cyclodextrin

An equimolar mixture of naphthalene and amorphous heptakis-(2,6-di-O-methyl)--cyclodextrin (DMCD) was heated at 70 or 90°C in a sealed container. After heating ffor 15 min at 90°C, the mixture was crystallized to show an excimer fluorescence of naphthalene, and the fluorescence spectrum changed to a monomer emission by further prolongation of heating time, accompanied by a slight change in its powder X-ray diffractogram. It is suggested that a metastable complex showing the excimer emission of naphthalene was transformed to a stable complex showing the monomer emission. The mixing molar ratio of naphthalene to DMCD was also found to affect the transformation temperature of the complex.     

Ratiometric determination of Hg2+ ions based on simple molecular motifs of pyrene and dioxaoctanediamide

A new podand-type dioxaoctanediamide-based chemosensor having two pyrene moieties was prepared, and its fluoroionophoric behaviors toward transition-metal ions were investigated. Pyrene-appended dioxaoctanediamide 1 showed a selective fluorescence quenching toward Hg2+ ions over other transition-metal ions in an aqueous methanol solution. Unique responses in pyrene monomer and excimer emissions allowed selective ratiometric determination of Hg2+ ions in aqueous environments, and the detection limit was found to be 1.6 x 10(-6) M. [structure: see text]     

Determination of the excited state dipole moment of fluorenone using the method of solvatochromism

The absorption spectra and steady state fluorescence spectra of fluorenone have been obtained at room temperature for various concentrations in a series of non polar and polar solvents. The concentration effect shows two fluorescence bands, one at shorter wavelength due to monomer and another at longer wavelength due to excimer formation by triplet-triplet annihilation process. The excited state dipole moments of both monomer and dimer are calculated by the method of solvatochromism. A reasonable agreement has been observed between the values obtained by the method of solvatochromism and electrochromism.     

Dynamics and energetics of the self-assembly of a hydrophobically modified polyelectrolyte: Naphthalene-labeled poly(acrylic acid)

Steady-state and time-resolved fluorescence studies were performed on aqueous solutions of poly(acrylic acid) hydrophobically modified with two very different levels of naphthalene (Np). It is demonstrated that unique information on association phenomena involving hydrophobe-modifed polymers can be obtained from an extended fluorescence study by using data for a less-modified polymer as a reference. For the more highly modified polymer, the presence of excited-state (as well as ground-state) dimers in addition to monomer emission due to locally excited naphthalene gives evidence for hydrophobic association between naphthalene groups. This association becomes, as expected, much less important at higher pH due to the electrostatic repulsion between different chain segments. However, it is noted that even at high pH there is a significant self-association. The coexistence of static and dynamic quenching phenomena of the Np monomer label was also revealed in the time-resolved fluorescence data. The data are compatible with the existence of two types of monomers and one excimer and suggest that the essential contribution to the monomer emission comes from isolated chromophores, whereas excimer formation arises from both a dynamic route (excited Np chromophores able to produce a dynamic excimer) and a static route (excitation of ground-state Np dimers). At room temperature, the dissociative reaction, excimer-to-monomer, can be neglected, and thus the rate constant for excimer formation and decay could be obtained with and without considering the influence of preformed dimers. Temperature has shown to induce different behavior in the polymer photophysics. In the case of the less-labeled polymer, the decays were found to be single-exponential with the fluorescence lifetime decreasing with increasing temperature. From the temperature dependence of the steady-state fluorescence data, the activation energy for excimer formation and the binding energy of the excimer were evaluated at different pH values, through the Stevens-Ban-type plots of the excimer-to-monomer intensity ratio. With the time-resolved data, measured in the temperature range of 5-60 degrees C, it was possible to extract the intrinsic activation energies for excimer formation. The thermodynamic driving force for the intrapolymeric association was found to be dependent on a balance between hydrophobic and electrostatic interactions, which are dependent on the pH, temperature, and hydrophobic content of the polymer.