伴随着分子内电荷分离的分子内转动模型的时间分辨荧光光谱研究

本文采用时间分辨荧光光谱方法,考查了两种7-胺基香豆类素衍生物分子在不同溶剂中的荧光辐射弛豫过程,研究了环境因素对伴随着分子内电荷转移的分子内转动激发态(TICT)弛豫过程的影响。结果说明TICT态是非刚性香豆素分子激发态无辐射弛豫路径之一,这一过程受到环境介质的极性、粘度和温度的影响。并指出了在考虑粘度影响时,须对DSE理论进行修正,同时提出了TICT态存在位垒的观点。     

4′-(对-胺苯基)-2,2′:6′,2′′-三联吡啶光物理性质

用稳态吸收和荧光光谱技术研究4′-(对-胺苯基)取代的三联吡啶配体(APT)分子在不同极性溶剂中的光谱和光物理性质. 在极性溶剂中APT分子存在着双荧光现象,它分别对应于局域激发态和分子内电荷转移态. APT分子的胺基N原子与醇类溶剂之间的氢键作用使该分子在质子性与非质子性溶剂中具有不同的线性关系. 此外,APT分子的三联吡啶部分与锌离子络合以及三联吡啶N4—N8—N14与甲醇分子形成氢键后,在低能区域出现新的吸收光谱带与荧光光谱带,表明在基态和激发态均形成了新的络合物. 时间分辨单光子计数技术测量的APT分子的荧光衰减过程,证明了APT分子的分子内电荷转移机制符合〝两态〞模型.     

香豆素—1的荧光介质效应

详细研究了香豆素－１在环己烷－醇、１，４－二氧六环－水二元溶剂及环糊精，表面活性剂溶液体系中的荧光光谱。通过溶剂－溶质分子间氢键作用及对其非荧光性的ＴＩＣＴ态形成的影响。讨论了这种荧光探针的荧光光谱对环境极性非常敏感的原因，测定了它与环糊精的包结常数和与表面活性剂胶束的结合常数。     

香豆素衍生物的光谱性质研究及痕量Fe^3＋的测定

对比考查了水与乙醇溶液中不同浓度下丁二酸(7-羟基香豆素)单酯(SCE)的荧光光谱特性,基于溶剂本身的性质及SCE在氢键溶剂中的二聚作用对其光谱进行了讨论.同时基于不同pH值水溶液中荧光光谱的变化,计算得到该试剂激发态分子的酸离解常数pK*a=2.03.研究发现在pH 3.3盐酸介质中,Fe3 可使SCE的荧光猝灭,且其荧光猝灭程度与Fe3 的加入量呈线性关系.该方法线性范围为0.66～6.59 μg·L-1,方法检测限为51 ng·L-1,对比母体7-羟基香豆素对Fe3 的检测,SCE测定的灵敏度提高了104倍,从而建立了荧光猝灭法测定痕量Fe3 的新方法.     

两种新香豆素分子的热力学和光谱性质

使用密度泛函理论方法在B3LYP /6-31++G**理论水平对两种香豆素a和b分子的几何结构、光谱、热力学性质进行理论计算研究,并基于Tomasi的极化统一场模型(PCM)讨论溶剂效应。结果显示,香豆素a和b分子在气相中的最低能量吸收波长分别为352和355 nm,溶剂及其极性大小对香豆素a最低能量吸收波长影响很小,但在溶剂作用下香豆素b分子的最低能量吸收波长红移7-10 nm,溶剂的极性对该波长影响较小。298 K标准压力下香豆素a和b分子的气态标准摩尔生成焓 分别为-1373.171和-1310.805 kJ.mol-1,标准摩尔生成自由能 分别为-1064.043和-1035.849 kJ.mol-1,标准摩尔熵 分别为763.910和742.150 J.mol-1.K-1.     

两种新香豆素分子的热力学和光谱性质

使用密度泛函理论方法在B3LYP/6-31++G**理论水平对两种香豆素a和b分子的几何结构、光谱、热力学性质进行理论计算研究,并基于Tomasi的极化统一场模型(PCM)讨论溶剂效应.结果显示,香豆素a和b分子在气相中的最低能量吸收波长分别为352和355 nm,溶剂及其极性大小对香豆素a最低能量吸收波长影响很小,但在溶剂作用下香豆素b分子的最低能量吸收波长红移7-10 nm,溶剂的极性对该波长影响较小.298 K标准压力下香豆素a和b分子的气态标准摩尔生成焓Δ_fH_m~Θ分别为-1373.171和-1310.805 k J·mol~(-1),标准摩尔生成自由能Δ_fG_m~Θ分别为-1064.043和-1035.849 kJ·mol~(-1),标准摩尔熵S_m~Θ分别为763.910和742.150 J·mol~(-1)·K~(-1).     

多孔硅镶嵌C102的蓝绿发光特性

利用多孔硅(PS)独特的微孔结构、非常大的比表面积、很强的吸附能力和灵敏的表面光学性质等特点,将激光染料香豆素102(C102)镶嵌在多孔硅中,得到多孔硅镶嵌C102的复合膜。研究复合膜的荧光特性,我们发现：镶嵌在多孔硅中的C102荧光光谱与其在无水乙醇溶液中的荧光光谱相似,主要呈现单体发光特性;通过比较镶嵌在不同孔隙率中的C102荧光光谱,得知镶嵌在不同多孔硅中的染料分子主要以同种形式存在。另外还发现,放置一段时间后的镶嵌复合膜,荧光强度明显增强,对称性提高,保留了激光染料发光的很多优点。多孔硅镶嵌C102的荧光特性展示了多孔硅在发展固体激光器方面有一定的应用,并为实现硅基蓝绿发光打开新的途径。     

兼具三线态-三线态湮灭上转换与单光子吸收上转换特性的氮杂蒽衍生物发光性能研究

弱光上转换是将低能量光子转换为高能量光子的过程,在三维荧光显微成像、太阳能电池、光催化等领域具有广泛的潜在应用,因而成为有机荧光材料领域的热点课题。目前基于三线态-三线态湮灭机制有机弱光上转换材料（TTA-UC）的研究已较为深入,有关发光机理及应用研究均有较多报道;然而针对另一种有机弱光上转换机理——基于单光子热带吸收的弱光上转换（OPA-UC）的研究目前还较为少见。氮杂蒽衍生物由于具有良好的结构刚性和平面性,高的荧光量子产率,是研究TTA-UC和OPA-UC两种有机上转换发光的理想模型分子结构。通过研究比较三种氮杂蒽衍生物：酚藏花红（PSF）、藏红T（SFT）、亚甲基紫（MTV）各自TTA-UC和OPA-UC的发光性能差异,分析探讨了分子结构对OPA-UC发光性能及TTA-UC敏化效率的构效关系。实验发现酚藏花红和藏红T由于具有较高的荧光量子产率,同时辐射衰减常数较大,其主要衰减过程为辐射衰减;而亚甲基紫具有较高的分子内电荷转移能力(ICT),因而非辐射衰减部分更多。研究三种分子的TTA-UC性能,发现亚甲基紫的三线态能级过低无法进行三线态-三线态能量转移过程,而藏红T由于拥有更高的三线态寿命而具有更高的上转换发光效率(9.69%),是酚藏花红体系(3.16%)的3倍。进一步研究酚藏花红和亚甲基紫的OPA-UC性能差异,发现相同浓度条件(10-3 mol·L-1)下亚甲基紫(0.12%)的OPA-UC发光效率相较于酚藏花红(0.059%)更高,且随着浓度的升高,亚甲基紫的OPA-UC发光增强效应更大。进一步研究表明,在TTA-UC发光过程中,敏化剂的敏化效率主要受分子三线态寿命以及系间窜跃能力影响,寿命越长,系间窜跃能力越强,敏化效率越高;而在OPA-UC发光过程中,湮灭剂分子的发光学率主要受ICT影响,ICT能力越大,分子发光效率越高。使用氮杂蒽分子廉价易得,对未来高性能TTA-UC和OPA-UC发光分子的设计具有一定的实际意义。     

香豆素C1F和C2F在醇类溶剂中的激发态溶剂效应

本文在Grabowski模型基础上,提出了一种描述TICT态生成动力学的理论模型,并采用时间相关单光予计数荧光光谱方法,测量了香豆素C1F和C2F在醇类溶剂中的荧光寿命,考察了各种溶剂效应(极性、粘度和温度)对TICT态生成速率的影响,并将结果与DSE关系比较,指出在醇类溶剂中,氢链效应的影响是十分重要的.     

香豆素-3-甲酰氯修饰聚酰胺-胺大分子的荧光性能研究

用香豆素-3-甲酰氯对聚酰胺-胺树状大分子末端修饰合成了树状大分子PAMAM-CMAC,经FTIR,1H-NMR分析确证了其结构。荧光分析表明,PAMAM-CMAC树状大分子具有强的荧光发光,荧光强度比聚酰胺-胺树状大分子荧光强度增加很多。其荧光强度受pH值、溶液浓度和溶剂等各种因素的影响,在酸性条件下,荧光强度受溶液pH影响较大;但在强碱性介质中,氢键被完全破坏,荧光强度明显减弱。pH在7.00～10.00之间时,荧光发光比较稳定。溶液浓度对荧光强度也有影响,浓度太大或太小,荧光强度都相应减小,而且浓度大的溶液比浓度小的溶液荧光猝灭的快。这与理论相一致。同时,随着溶剂极性的增加,荧光发射向长波方向移动。     

具有电子推拉结构的多支化分子的光物理特性的研究

利用稳态光谱和飞秒时间分辨荧光亏蚀的技术,研究了不同溶剂中一系列有分子内电荷转移特性的分子的结构与光物理性质的关系,研究体系为三苯胺作为电子给体,2,1,3-苯并噻二唑作为受体的单支分子及其对应的两支和三支分子. 并结合TD-DFT计算进一步解释了实验中所观察到的现象. 三个分子相似的吸收和荧光光谱以及强的溶剂依赖光谱特性表明两支与三支分子激发态与单支分子相似,表明激发态都定域在其中一支上. 激发时多支分子内发生多维电荷转移,然后快速地定域到某一支上发射. 另一方面多支分子相对于单支分子吸收和发射光谱的红     

Solvatochromic and Fluorescence Behavior of Sulfisoxazole

The Fluorescence spectroscopic and solvatochromic behavior of Sulfisoxazole, a sulfa drug with antimicrobial activities, in various pure solvents of different polarity and hydrogen bonding capability is reported. The fluorescence emission spectrum of sulfisoxazole was found to be solvent polarity dependent, where a notable red shift in emission maximum was observed with increasing solvent polarity as well as hydrogen bonding capability. The effects of the latter two solvent parameters were quantitatively investigated using the methods of Lippert–Mataga and solvatochromic comparison method (SCM) that is based on the Kamlet-Taft equation. Particularly, the Lippert–Mataga method was applied to estimate the dipole moment of the excited state (μ_e) upon plotting Stokes shift versus solvent polarizability (Δf), where a value of 11.54 Debye was obtained. On the other hand, applying the multiple regression analysis to the SCM method revealed that solvent polarizability (π*) and hydrogen-bond donor capability (α) approximately equally stabilize sulfisoxazole in the excited state with minor destabilization contribution by the hydrogen-bond acceptor capability (β). These findings revealed that the excited state of sulfisoxazole is stabilized by polar solvents, indicating that this drug molecules exhibit larger dipole moment in the excited state than in the ground state, which in turn implies that a potential intramolecular charge transfer (ICT) occurs after excitation.     

Optimization in Solvent Selection for Chlorin e6 in Photodynamic Therapy

The photophysical properties of chlorin e6 (Ce6) in twelve different protic, aprotic and non-polar solvents were investigated using ultraviolet–visible and fluorescence spectroscopic methods. Solvatochromic effects were determined by the changes in quantum yield, Stokes shift, fluorescence half-life and excited state dipole moments of Ce6 in the different solvents. The absorption shifts observed in different solvents were further analyzed using the Kamlet-Abboud-Taft model and the nature of solute-solvent interactions between Ce6 and different protic and aprotic solvents was elucidated. The quantum yields were found highest in protic solvents (except water), followed by aprotic and non-polar solvents. Solvent polarity parameters showed a linear increasing trend with Stokes shift and fluorescence half-life, which indicated the presence of Ce6-solvent interaction. Using the Kamlet-Abboud-Taft model, a direct correlation between the solvent polarity parameters and absorption shift was observed, which substantiated the existence of Ce6-solvent interaction by hydrogen bond formation. The excited state dipole moments in specific protic and aprotic solvents were found to be higher than the ground state dipole moments, implying a more polar nature of Ce6 during excited state transition.     

脱氢枞酸基D-A型分子的合成、空间构型及光谱性能

对三苯胺进行溴代和C-N偶联反应合成4-萘基三苯胺(a),对脱氢枞酸进行酯化、溴代、硝化、还原和C-N偶联反应合成13-[N,N-(4-萘基苯基)-苯基]胺基-脱异丙基脱氢枞酸甲酯(b)及13-[N,N-双(4-萘基苯基)]胺基-脱异丙基脱氢枞酸甲酯(c)两个化合物,通过1H MNR,13C MNR及MS对化合物的结构进行表征。为了研究化合物结构与光谱性能之间的关系,首先利用Gaussian 09程序采用密度泛函DFT/B3LYP方法,对三个化合物的空间构型进行全优化,得到它们的键长、键角和二面角,对比发现脱氢枞酸骨架和萘环的引入会影响化合物的共平面性,而萘环的引入会增大化合物的共轭程度。光谱性能方面,研究了三种化合物在甲醇、二氧六环、四氢呋喃、二氯甲烷和环己烷这5种极性逐渐减小的溶剂中的荧光发射光谱和紫外吸收光谱。结果表明,在荧光光谱中,化合物a,b和c在不同极性溶剂中最大荧光发射波长均有不同程度位移,在甲醇中最大,在环己烷中最小,但是位移并非随着极性的增大而只发生红移,在二氯甲烷、四氢呋喃和二氧六环3种极性依次增大的溶剂中,a,b,c的荧光发射波长均随着溶剂极性的增大而发生较大程度的蓝移;在同一溶剂中,化合物b和c相对于a的荧光发射波长依次发生红移,c的红移程度与b差距不大。紫外吸收光谱中,三个化合物在不同极性溶剂中的最大吸收波长也有差异,在200～250 nm区间,三个化合物均在二氯甲烷中有较大位移,在300～350 nm区间,在甲醇中位移较大,而在250～300 nm区间,最大吸收波长差别不大;在同一溶剂中,它们在300～350 nm区间的最大吸收波长差别较大,化合物c较a红移26 nm。结合结构优化所得数据可以证明,化合物的共轭程度对荧光发射光谱和紫外吸收光谱均有影响,而共平面性对荧光发射光谱影响较大。化合物a,b和c在不同极性溶剂中荧光发射光谱和紫外吸收光谱的较大变化,表明它们有明显的溶致变色行为,具有作为分子探针探测外部环境极性大小的潜能。     

On the Photophysicochemical Properties of Selected Fluoroquinolones: Solvatochromic and Fluorescence Spectroscopy Study

The photophysicochemical properties of selected fluoroquinolones in different solvents of various physical properties, including polarity and hydrogen bonding ability, were investigated using steady state fluorescence spectroscopy. The solvent-dependant fluorescence emission spectra of selected fluoroquinolones, namely ciprofloxacin (CIPR) and enrofloxacin (ENRO), were employed to gain insights concerning its photophysicochemical properties of interests. Interestingly, fluorescence spectra of the selected drugs exhibited structured emission spectra in nonpolar solvents such as hexane, whereas unstructured spectra were observed in more polar solvents such as alcohols and water. Also, a notable bathochromic shift in $ \lambda_{{\max }}^{{em}} $ was observed in fluorescence spectra of both drugs with increasing solvent polarity that resulted in biphasic behavior upon applying the Lippert-Mataga correlation that correspond to general and specific solvent effects. Applying the Lippert-Mataga correlation to the fluorescence spectra of CIPR and ENRO in various solvents was employed to estimate the dipole moment difference between the ground and excited states of them, $ \Delta \mu \left( {{\mu_e} - {\mu_g}} \right) $ , where obtained results revealed the values of 9.4 and 16.2 Debye for the LE and ICT states of ENRO, respectively, and 8.0 and 16.2 Debye for the LE and ICT states of CIPR, respectively. Multiple linear regression analysis (MLRA) based on Kamlet-Taft equating was applied against absorption frequency (ν_abs), emission frequency (ν_em), Stokes shift (?ν), and fluorescence quantum yield (Φ_f), where obtained results revealed excellent correlation (R: 0.916–0.966) that are consistent with other results considering the effect of solvent polarizability, hydrogen bonding ability, and viscosity on the photophysicochemical properties of the studied fluoroquinolones.     

Fluorescence Properties of Donor–Acceptor-Substituted Pyrazoloquinolines

The photophysical properties of three newly synthesized pyrazoloquinolines, composed of N,N-dimethylaniline as donor subunit and various substituted forms of the acceptor pyrazoloquinoline (DPPQ), were investigated by absorption as well as by stationary and time resolved fluorescence spectroscopy. These compounds show generally highly efficient emission in nonpolar and medium polar solvents; the dipole moment of the emitting state increases and the quantum yield decreases with solvent polarity. These results are explained by state reversion in polar solvents: At low polarities emission originates from a state localized on the DPPQ moiety, whereas in the high-polarity regime the next excited state of charge transfer character, in which an electron is promoted from the amino nitrogen lone pair into an excited orbital of the DPPQ moiety, becomes the fluorescent state. This view is corroborated by semiempirical calculations including the solvent reaction field, low-temperature fluorescence measurements, and the observation of effects of protonation on the spectroscopic and photophysical properties.     

激发态质子转移分子2-(2'-羟基苯基)苯并噻唑在不同溶剂中的光谱特性

观测了2-(2’-羟基苯基)苯并噻唑(HBT)在不同极性溶剂中的吸收光谱和荧光光谱,详细研究了溶剂极性对HBT发生激发态分子内质子转移(ESIPT)影响的机制。吸收光谱表明在常态条件下,HBT在各种溶剂中都以烯醇式构型和酮式构型共同存在,但以烯醇式构型占绝大多数。荧光光谱表明在纯环己烷溶剂中,HBT被紫外光激发时,绝大多数烯醇式构型发生ESIPT转变为酮式构型,分子的ESIPT效率最大。在含有乙醇的极性溶剂中,HBT烯醇式会形成溶剂化的烯醇式构型,阻碍分子发生ESIPT反应。溶剂中乙醇含量愈多极性愈强,溶剂化烯醇式的成份就愈多,HBT的ESIPT效率就愈低。以400 nm光激发HBT溶液时,在510 nm处发现酮式构型荧光,从而确认了400 nm处的弱吸收是酮式构型的吸收;且在436和456nm处还有新的荧光峰,分析其可能来源于酮式构型去质子化阴离子的发射。     

激发态质子转移分子2-（2′-羟基苯基）苯并噻唑在不同溶剂中的光谱特性

观测了2-（2′-羟基苯基）苯并噻唑（HBT）在不同极性溶剂中的吸收光谱和荧光光谱,详细研究了溶剂极性对HBT发生激发态分子内质子转移（ESWT）影响的机制。吸收光谱表明在常态条件下,HBT在各种溶剂中都以烯醇式构型和酮式构型共同存在,但以烯醇式构型占绝大多数。荧光光谱表明在纯环己烷溶剂中,HBT被紫外光激发时,绝大多数烯醇式构型发生ESIPPT转变为酮式构型,分子的ESIPT效率最大。在含有乙醇的极性溶剂中,HBT烯醇式会形成溶剂化的烯醇式构型,阻碍分子发生ESIPT反应。溶剂中乙醇含量愈多极性愈强,溶剂化烯醇式的成份就愈多,HBT的ESIPT效率就愈低。以400nm光激发HBT溶液时,在510nm处发现酮式构型荧光,从而确认了400nm处的弱吸收是酮式构型的吸收;且在436和456nm处还有新的荧光峰,分析其可能来源于酮式构型去质子化阴离子的发射。     

Ultrafast S1 and ICT state dynamics of a marine carotenoid probed by femtosecond one- and two-photon pump-probe spectroscopy

Ultrafast relaxation kinetics of fucoxanthin in polar and non-polar solvents have been studied by femtosecond pump-probe spectroscopy. Transient absorption associated with S₁ or intramolecular charge transfer (ICT) excited state has been observed following either one-photon excitation to the optically allowed S₂ state or two-photon excitation to the symmetry-forbidden S₁ state. The results suggest that the ICT state formed after excitation of fucoxanthin in a polar solvent is a distinct excited state from S₁.