外围萘修饰PAMAM树枝形聚合物的合成及其质子化过程研究

合成了外围修饰有萘基团的0～3代聚酰胺-胺树枝形聚合物GnN (n＝0～3), 化合物通过了IR, 1H NMR, 13C NMR和MALDI TOF的表征. 稳态光物理研究表明, 甲醇溶液中GnN外围萘基团与骨架胺之间发生电子转移过程, 形成最大发射峰在450 nm的激基复合物, 萘的荧光被明显猝灭; 当GnN骨架被质子化, 分子内光致电子转移过程和萘与骨架胺基间激基复合物的形成被抑制, 萘单体荧光发射大大增强; 由于质子化后树枝形聚合物骨架趋于伸展构象, 外围萘基团间相互作用增强, 部分形成最大发射峰在400 nm的激基缔合物.     

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.     

多足开链化合物的分子内光诱导电子转移及pH对其荧光的影响

本文合成了含有1～3个萘基取代的脲类柔性开链化合物.通过对该类化合物在溶液中的光物理行为以及受溶液酸度影响的比较研究,发现多足化合物的发光性质强烈地依赖于化合物本身存在的构象形式;同时观察到以叔胺为骨架的三足化合物存在分子内光诱导电子转移反应(PET),且这一过程强烈地依赖于介质的pH值;而叔胺基的氮原子质子化将会减弱这一PET过程.     

外围准轮烷形成对萘修饰PAMAM树枝形聚合物光物理性质的调控

合成了1~3代外围修饰萘的聚酰胺-胺(PAMAM)树枝形聚合物Gn-NA,化合物通过了1H NMR,13C NMR,MALDI-TOF MS,IR的鉴定.稳态和时间分辨光物理研究表明,水溶液(含DMSO 0.3%~0.5%,V/V)中Gn-NA分子内相邻萘基团形成激基缔合物,猝灭了萘单体的荧光发射,随代数增加,对萘单体荧光猝灭作用增强.向体系中加入葫芦[7]脲(CB[7]),CB[7]与萘形成的准轮烷结构1∶1的包结复合物,1~3代Gn-NA中萘与CB[7]的结合常数分别为768,887和823 mol-1?L.准轮烷结构的形成抑制了分子内激基缔合物的生成,使单体荧光发射大大增强.本工作为可调控发光树枝形聚合物的发展提供了一种新的策略.     

芘-对二氰基乙烯基苯的光诱导分子内电子转移及其盐效应的研究

本工作设计并合成了一系列以不同链长相连的芘-对二氰基乙烯基苯(Py-DCVB)化合物, 利用紫外可见吸收光谱、荧光光谱、核磁共振谱研究了Py-DCVB的光诱导分子内电子转移激基复合物的形成与基态构象的关系, 并且利用激光闪光光解开展了盐效应的研究, 瞬态吸收光谱的结果证实了Py-DCVB分子内光诱导电子转移反应经历激基复合物的中间过程。     

一种新型的分子内激基缔合物——双-β-萘基烷烃及其衍生物分子内激基缔合物的研究

本文报道几种双-β-萘甲酸多次甲基二醇酯及双-β-萘基烷烃次甲基链上被极性基团取代的衍生物的合成及其荧光谱。结果表明,它们都能形成分子内激基缔合物,对于双-β-萘甲酸多次甲基二醇酯来说,其分子内激基缔合物的荧光强度与链长有关,以三次甲基链为最大。对于双-β-萘基烷烃取代衍生物来说,由于吸电子基团的引入使两个萘环的电子云密度不等,它们所形成的分子内激基缔合物的荧光峰都比未取代的1,3-双-β-萘基丙烷有所蓝移。在极性溶剂乙腈中其分子内激基缔合物的荧光峰的位置虽然不变,但I_E/I₂值则有所降低,表现出既不完全与激基缔合物相同,又不完全与激基复合物相同的性质。     

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。     

双-β-萘甲基二胺及其衍生物的荧光光谱及分子内激发态复合物的形成

我们合成了N,N'-二甲基-二-β-萘甲基乙二胺(Ⅰ),N,N'-二甲基-二-β-萘甲基丙二胺(Ⅱ),N,N'-二-β-萘甲基哌嗪(Ⅲ)三个化合物,并测定了它们的荧光光谱。结果表明,它们既能形成分子内激基缔合物(excimer),又能形成分子内激基复合物(exciplex),与溶剂极性有关。在极性较大的溶剂如乙腈和甲醇中,由于激基复合物几乎完全解离因而不发射荧光,这时观察到的荧光峰蓝移而且强度增加,可以认为,这是激基缔合物存在的证明。这三个化合物的分子内激基缔合物形成的难易程度按Ⅱ>Ⅰ>Ⅲ的次序依次递降。     

用于识别金属离子的超分子荧光/磷光传感器*

本文总结了近年来用于金属离子识别的超分子荧光/磷光传感器的研究工作进展,着重介绍了光诱导电子转移及单体-激基缔合物体系在金属离子识别中的应用.     

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．     

Photophysical Properties of Intramolecular Charge Transfer in a Tribranched Donor–π–Acceptor Chromophore

The photophysical properties of intramolecular charge transfer (ICT) in a novel tribranched donor–π–acceptor chromophore, triphenoxazine‐2,4,6‐triphenyl‐1,3,5‐triazine (tri‐PXZ‐TRZ), with thermally activated delayed fluorescence character was investigated in different aprotic solvents by steady‐state spectroscopy and femtosecond and nanosecond transient absorption spectroscopy measurements. Increasing the solvent polarity led to a significant increase in the Stokes shift. The large Stokes shift in highly polar solvents was attributed to ICT properties upon excitation; this resulted in a strong interaction between the tri‐PXZ‐TRZ molecule and the surrounding solvent, which led to a strong solvation process. Quantum‐chemical calculations and changes in the dipole moment showed that this compound has a large degree of ICT. Furthermore, an apolar environment helped to preserve the symmetry of tri‐PXZ‐TRZ and to enhance its emission efficiency. The femtosecond and nanosecond transient absorption spectroscopy results indicated that the excited‐state dynamics of this push–pull molecule were strongly influenced by solvent polarity through the formation of a solvent‐stabilized ICT state. The excited‐state relaxation mechanism of tri‐PXZ‐TRZ was proposed by performing target model analysis on the femtosecond transient absorption spectra. In addition, the delayed fluorescence of tri‐PXZ‐TRZ was significantly modulated by a potential competition between solvation and intersystem crossing processes.     

取代苄叉亚胺类化合物溶液电子光谱的研究

研究了二甲氨基苄叉亚胺类化合物溶液的电子光谱。结果表明一端为电子给体另一端为电子受体的共轭型取代苄叉对硝基苯胺3,在基态下发生了分子内电荷转移,其跃迁吸收波长比化合物1,2(315 nm)红移90 nm。以乙撑基联接的非共轭型苄叉亚胺奥化合物4,5,6未观察到基态时的电荷转移现象,但在激发条件下可明显的发生分子内的电荷转移而使荧光强度大大减弱。MMA等对1的荧光有明显的猝灭作用,表明其间发生了电荷转移。丙烯酸则因会引起西佛碱的水解,而使荧光减弱。     

阳离子荧光敏感器的器件化问题研究

通过对石英玻片表面修饰, 制作了联有多氨基链萘基的超薄膜荧光敏感器件, 研究了它在镍、铜等金属离子水溶液及有机溶剂中的荧光猝灭现象. 发现其荧光光谱无论在水或其他有机溶剂中都存在着单体和激基缔合物(ex-cimer)的发射峰, 当处于镍离子水溶液中时, 其单体峰随离子浓度的增大出现了先增强后减弱的现象, 而激基缔合物的发光峰则仅略有减弱但变化不大. 在铜离子水溶液中其荧光的变化情况和镍离子有所不同, 对单体荧光只能观察到强度减弱的趋势, 而激基缔合物则变化不大. 比较了未联结的敏感器化合物分子在有机溶剂中荧光被铜离子猝灭的行为, 发现与其在器件表面时有很大的差别, 表明其分子结构和构象也有很大的不同.     

Review: fluorescent cyclodextrins for molecule sensing

Cyclodextrins (CDs), which are spectroscopically inert, were converted into fluorescent CDs by modification with one or two fluorophores. Many fluorescent CDs changed the fluorescent intensities upon addition of guest compounds, causing the locational change of the fluorophore mostly from inside to outside of the CD cavities. On this basis, the fluorescent CDs were used as fluorescent chemosensors for molecule recognition. Modified CDs bearing two naphthalene or pyrene moieties exhibit intramolecular excimer emission and their guest-responsive excimer intensity variations were used for molecule sensing. Fluorescent CDs bearing a dansyl moiety decreased the fluorescence intensity upon guest addition, reflecting the environmental change around the fluorophore from the hydrophobic interior of the CD cavities to bulk water solution. Modified CDs bearing a p-N,N-dimethylaminobenzoyl (DMAB) moiety exhibit dual emissions from nonpolar planar (NP) and twisted intramolecular charge transfer (TICT) excited states, and the TICT emission intensity was useful for sensing molecules. A biotin-bound DMAB system was also constructed, and the presence of the protein (avidin) was found to enhance the NP fluorescence. This avidin-bound DMAB system showed higher sensitivities and stronger binding ability for guest species than the system without avidin.     

ENERGY TRANSFER FROM MICELLAR SODIUM PHENYLUNDECANOATE TO SOLUBILIZED NAPHTHALENE

Abstract— Excitation energy transfer from the phenyl groups of surface active phenylundecanoate ions to naphthalene molecules has been studied under conditions such that the naphthalene molecules have been solubilized by micelles of phenylundecanoate. From measurements of the naphthalene fluorescence intensity in solutions of varying surfactant concentration the critical micelle concentration has been determined as 0·0091 M. The product of the micellar aggregation number and the efficiency of energy transfer has been obtained as 75 from measurements of both the sensitized naphthalene fluorescence and the quenching of the phenylgroup fluorescence. In the evaluation of the experimental data it has been assumed that the partition of naphthalene between the micelles and the aqueous phase may be treated as a distribution equilibrium, and that the solubilized naphthalene molecules are partitioned among the micelles according to a Poisson distribution. With this model, the naphthalene fluorescence intensities may be accounted for over the whole range of surfactant concentrations.
At high naphthalene concentrations, emission from naphthalene excimers has been observed. The possibility of self-quenching via excimer formation is considered.
The experimental results point to a quantum efficiency near unity for the transfer of excitation energy from the phenyl groups of the surfactant ions that form a micelle to a single solubilized naphthalene molecule. The high efficiency suggests that the naphthalene molecule and the phenyl groups are present inside the micelles.     

Singlet-singlet intermolecular optical energy transfer from naphthalene to benzophenone in the vapor phase

By using the exothermic energy transfer as a function of pressure, the rate constant for diffusion was evaluated for benzophenone/naphthalene and naphthalene/benzophenone systems. In principle the optical energy absorbed by a complex molecule raises that molecule to one of its excited states, and afterwards this excitation energy decays through the different relaxation channels. Initially, electronically excited naphthalene "S1" state emits photons in the fluorescence band of naphthalene and these emitted photons, as a stream of particles, are absorbed by the acceptor molecule benzophenone, then excited benzophenone fluoresces. In this investigation, sensitized fluorescence decay times in different conditions were measured for naphthalene-benzophenone system in the vapor phase, and found to be 12+/-1 ns. The ultraviolet-visible spectra of the system in the vapor phase at room temperature conditions were broad and structureless.     

Photophysics of untethered ZnTPP-fullerene complexes in solution

The spectroscopy and dynamic behavior of the self-assembled, Soret-excited zinc tetraphenylporphyrin (ZnTPP) plus fullerene (C(60)) model system in solution has been examined using steady state fluorescence quenching, nanosecond time-correlated single photon counting, picosecond fluorescence upconversion, and picosecond transient absorption methods. Evidence of ground state complexation is presented. Steady-state quenching of the S(2) and S(1) fluorescence of ZnTPP by C(60) reveals that the quenching processes only occur in the excited complexes, are ultrafast, and proceed at different rates in the two states. Only uncomplexed ZnTPP is observed by fluorescence lifetime methods; the locally excited complexes are either dark or, more likely, rapidly relax to products that do not radiate strongly. Both short-range (Dexter) energy transfer and electron transfer relaxation mechanisms are evaluated. Picosecond transient absorption data obtained from the subtle differences between the spectra of Soret-excited ZnTPP with and without a large excess of added C(60) reveal the formation, on a subpicosecond time scale, of relatively long-lived charge-separated species. Soret excitation of ZnTPP···C(60) does not produce a quantitative yield of species in the lower S(1) excited state.     

Direct observation of excimer formation in anthracene and 9,9′-bianthryl

The existence of anthracene excimer in fluid solution was confirmed for the first time by observing the coincidence of the rise time of excimer fluorescence with the decay time of monomer fluorescence with the use of a picosecond laser, a streak camera, and a computer. The continuum model of diffusion theory is found to be applicable to the excimer formation and the encounter distance between anthracene in the excited state and that in the ground state is calculated to be 8 ± 2 Å. The anomalously broad featureless fluorescence observed for 9,9′-bianthryl in glycerol-methanol (9:1) solution was found to be emitted from the species formed only in the excited state and its rise time was found to be coincident with the decay time of fluorescence from anthracene moiety composing 9,9′-bianthryl, α,ω-9,9′-bianthrylpropane, -butane, -hexane, and -dodecane were found not to form excimer in the excited state.     

Etude comparative en luminescence UV-visible du 1,1′-binaphtyle et du 2,2′-binaphtyle

The modifications of emission spectra obtained in fluid and rigid media as a function of temperature show a conformation change for 1,1′-binaphthyl in the excited state. This change is facilitated in fluid medium by the rotation of the two naphthyl groups around the C₁C_1′ bond. The molecular twisting in this excited state explains the original results for 1,1′-binaphthyl where the intensity ratio of phosphorescence to fluorescence (I_ph/I_fluo) varies with excitation wavelength. This result agrees with the charge transfer (CT) character obtained by the excited state S*₂ due to the twist of this molecule.The emission spectra of 2,2′-binaphthyl, a molecule which is practically identical in its electronic structure to 1,1′-binaphthyl, do not undergo significant modification with effects of temperature variation, and as a function of the excitation wavelength. These different effects for 1,1′-binaphthyl and 2,2′-binaphthyl agree with the difference of twist for the naphthyl rings around the single bond between these rings.