聚苯乙烯负载多吡啶铂(Ⅱ)炔基络合物的合成

通过自由基共聚成功地将具有高磷光发光效率的-苯基-2,2’-二联吡啶(C^N^N)Pt(Ⅱ)苯乙炔络合物共价键合在聚苯乙烯高分子骨架上,得到了发射磷光的聚合物.实验表明,发光聚合物基本保持了多吡啶铂络合物单体的光谱性质.具有与小分子相当的光致发光效率.     

双希夫碱稀土络合物的荧光性质

采用荧光光谱、紫外吸收光谱及红外吸收光谱对稀土元素钐、铽与双希夫碱N ,N′ 二 (亚水扬基 ) 1 ,4 二氨基丁烷、N ,N′ 二 (亚水扬基 ) 1 ,5 二氨基戊烷以及还原希夫碱N ,N′ 二 (水扬基 ) 1 ,4 二氨基丁烷合成的络合物进行了研究。双希夫碱和还原双希夫碱的N和O原子参与配位 ,形成络合物的荧光是以配体发光为主。当双希夫碱和TTA共存于同一络合物时 ,钐的络合物存在配体协同发光效应 ,表现为有较强Sm3+ 特征发光性能 (m →m型发光 ) ;而铽的络合物则以配体发光为主     

8-羟基喹啉基稀土络合物的近红外发光研究

以8-羟基喹啉(Q)作为配体,通过控制配位反应条件,制备了二配体(ErQ2),三配体(ErQ3)和四配体(ErQ4,NdQ4和YbQ4)的8-羟基喹啉基稀土络合物,并用元素分析、红外光谱、紫外-可见吸收光谱和荧光光谱对其结构和性能进行了研究。通过激发配体,络合物均发射稀土离子的特征近红外光;随着配体数目的增加,络合物的近红外发光效率和寿命均增加,非辐射衰减速率常数减少。研究结果表明,稀土离子的近红外发光是通过8-羟基喹啉敏化产生的,并且8-羟基喹啉对铒离子的敏化不如对钕离子和镱离子的有效。     

铕、铽2,6-二甲酸吡啶、α-甲酸吡啶络合物的研究

近年来,稀土络合物的发光引起了人们的重视。Yamazoe等报道了R-CH=CH-COO~-类及β-羧酸吡啶铕、铽络合物的发光性能。山添等报道了α-甲酸吡啶铕、铽络合物的摩擦发光。本文制备了铕和铽的2,6-二甲酸吡啶络合物Na_3[Ln(DPA)_3]·NaCl·_3H_2O和α-甲酸吡啶络合物Ln(DPA)(PA)·1.5NaCl·3H_2O(Ln=Eu、Tb;DPA=2,6-二甲酸吡啶酸根;PA=α-甲酸吡啶酸根),并测定了络合物的红外光谱和荧光光谱。     

三蝶烯衍生大三环主体与π-延展双吡啶盐之间络合性质的研究

描述了三蝶烯衍生大三环主体与π-延展双吡啶盐在溶液中与固态下的络合性质,表明由于客体中两个吡啶盐之间连接单元的不同及端基官能团的不同,大三环主体与π-延展双吡啶盐能够形成1∶1或1∶2络合物,也可以在固态下形成梯状聚准[3]轮烷型超分子组装体.络合物的形成得到了核磁共振氢谱、质谱以及X衍射单晶结构证明.     

一种新型的铕络合物/TiO2发光薄膜

研究了Eu(DBM)3(DiBut-bpy)/TiO2/AA 单分子膜的表面压－分子面积(π－A)曲线和稳定性,单层膜中的TiO2纳米粒子是经TBT（tetrabutyloxyltitanium ,钛酸四丁酯）二维溶胶-凝胶法得到的.TiO2纳米粒子和铕络合物都被成功地转移到固体基片上，得到了具有良好的机械和热稳定性的新型发光薄膜.小角度X射线衍射结果证明这种复合膜具有层状有序的周期性结构.讨论了TiO2基质对复合膜发光机理的影响.     

卤素-三-(三苯基膦)合铜的~(31)P NMR研究

XCu(PP?h_?)_3,(X为卤素、硼氢阴离子等)是一类稳定的亚铜络合物,对一些有机反应和聚合反应有催化作用,曾用于多种成像过程,因而吸引人们对这一类化合物的结构和性质进行了广泛的研究。Lippard等测定了这类化合物在溶液中的表观分子量表明,在溶液中这类化台物的配体可以离解,并与络合物形成动态平衡。本文用 FX-90Q NMR 谱仪研究了四种络合物(PPh_3)_3CuX(X=Cl~-、Br~-、I~-和CN~-)在氯仿溶液中的~(32)PNMR谱及加入不同浓度的PPh_3对其~(35)P     

会议消息

中国化学会第三届全国多元络合物光度分析法学术会议于1987年9月15—21日在浙江省宁波市召开。会议共录用论文208篇。本次会议论文内容涉及:1.出现了许多新的多元络合物光度显色体系,在灵敏度的提高和选择性的改善方面有了明显的改进;2.多元络合物的机理研究有了进一步的深化;3.多元络合物在其它领域中的应用,如发光分析,色谱,原子吸收,电分析,分离技术等     

Gatifloxacin-铕荧光探针测定DNA

在pH 7.0±0.1的Tris-HCl缓冲溶液中,Eu3 与加替沙星形成的络合物受270 nm紫外光激发发出Eu3 的特征荧光峰,加人脱氧核糖核酸(DNA)能大大增强体系的荧光强度,由此建立GFLX-Eu3 络合物探针测定核酸的方法.与GFLX-Eu3 二元络合物相比.GFLX-Eu3 -DNA三元体系荧光强度显著增强,且最大吸收波长紫移5 nm,表明形成三元络合物.研究了反应的最佳条件,并初步探讨了GFLX-Eu3 络合物探针和DNA结合机制.     

两种新型2,2′:6′,2″-三吡啶配体的合成与表征

2,2′:6′,2″-三吡啶类化合物是一类具有良好配位能力的多齿配体,有关其金属络合物的报道近年来每年都有上百篇之多.以往的研究大多集中在该类配体以及所形成的金属络合物的发光性能,最近也有文献报道利用三吡啶配体与金属卤化物来合成一维配位聚合物,并研究其结构特性和非线性光学性质[1～3].     

Synthesis and photophysical studies of phthalocyanine-gold nanoparticle conjugates

This work reports on the synthesis, characterization and photophysical studies of phthalocyanine-gold nanoparticle conjugates. The phthalocyanine complexes are: tris-(5-trifluoromethyl-2-mercaptopyridine)-2-(carboxy)phthalocyanine (3), 2,9,17,23-tetrakis-[(1, 6-hexanedithiol) phthalocyaninato]zinc(II) (8) and [8,15,22-tris-(naptho)-2(amidoethanethiol) phthalocyanato] zinc(II)(10). The gold nanoparticles were characterized using transmission electron microscopy, X-ray diffraction, atomic force microscopy and UV-vis spectroscopy where the size was confirmed to be ～5 nm. The phthalocyanine Au nanoparticle conjugates showed lower fluorescence quantum yield values with similar fluorescence lifetimes compared to the free phthalocyanines. The Au nanoparticle conjugates of 3 and 10 also showed higher triplet quantum yields of 0.69 to 0.71, respectively. A lower triplet quantum yield was obtained for the conjugate compared to free phthalocyanine for complex 8. The triplet lifetimes ranged from 70 to 92 μs for the conjugates and from 110 to 304 μs for unbound Pc complexes.     

Photohydroxylation of 1,4-benzoquinone in aqueous solution revisited

In water, photolysis of 1,4-benzoquinone, Q gives rise to equal amounts of 2-hydroxy-1,4-benzoquinone HOQ and hydroquinone QH(2) which are formed with a quantum yield of Phi=0.42, independent of pH and Q concentration. By contrast, the rate of decay of the triplet (lambda(max)=282 and approximately 410 nm) which is the precursor of these products increases nonlinearly (k=(2-->3.8) x 10(6) s(-1)) with increasing Q concentration ((0.2-->10) mM). The free-radical yield detected by laser flash photolysis after the decay of the triplet also increases with increasing Q concentration but follows a different functional form. These observations are explained by a rapid equilibrium of a monomeric triplet Q* and an exciplex Q(2)* (K=5500+/-1000 M(-1)). While Q* adds water and subsequent enolizes into 1,2,4-trihydroxybenzene Ph(OH)(3), Q(2)* decays by electron transfer and water addition yielding benzosemiquinone (.)QH and (.)OH adduct radicals (.)QOH. The latter enolizes to the 2-hydroxy-1,4-semiquinone radical (.)Q(OH)H within the time scale of the triplet decay and is subsequently rapidly (microsecond time scale) oxidized by Q to HOQ with the concomitant formation of (.)QH. On the post-millisecond time scale, that is, when (.)QH has decayed, Ph(OH)(3) is oxidized by Q yielding HOQ and QH(2) as followed by laser flash photolysis with diode array detection. The rate of this pH- and Q concentration-dependent reaction was independently determined by stopped-flow. This shows that there are two pathways to photohydroxylation; a free-radical pathway at high and a non-radical one at low Q concentration. In agreement with this, the yield of Ph(OH)(3) is most pronounced at low Q concentration. In the presence of phosphate buffer, Q* reacts with H(2)PO(4) (-) giving rise to an adduct which is subsequently oxidized by Q to 2-phosphato-1,4-benzoquinone QP. The current view that (.)OH is an intermediate in the photohydroxylation of Q has been overturned. This view had been based on the observation of the (.)OH adduct of DMPO when Q is photolyzed in the presence of this spin trap. It is now shown that Q*/Q(2)* oxidizes DMPO (k approximately 1 x 10(8) M(-1) s(-1)) to its radical cation which subsequently reacts with water. Q*/Q(2)* react with alcohols by H abstraction (rates in units of M(-1) s(-1)): methanol (4.2 x 10(7)), ethanol (6.7 x 10(7)), 2-propanol (13 x 10(7)) and tertiary butyl alcohol ( approximately 0.2 x 10(7)). DMSO (2.7 x 10(9)) and O(2) ( approximately 2 x 10(9)) act as physical quenchers.     

Time resolved fluorescence spectroscopy of quercetin and morin complexes with Al3+.

The association process of Al3+ with quercetin and morin in methanol was studied by electronic absorption and emission spectroscopies. The number of species in solution with different absorption spectra were determined by the method of Rank analysis of the absorbance matrix, and the stoichiometries of the complexes were evaluated using the Job method. The number of fluorescent species in solution were calculated from the Rank analysis method of the time resolved emission spectra (TRES), and compared with a global analysis of the decay surface using a proper multi-exponential decay model. The association of Al3+ with morin gives rise to two complexes with 1:1 and 2:1 (morin: Al3+) stoichiometries, but in both species the association of the cation involves the carbonyl and 3-hydroxyl groups of the pyrone ring. The fluorescence decay surface of this system is biexponential and the lifetimes of the 1:1 and 2:1 complexes are 4.3 and 2.0 ns, respectively. The association of Al3+ with quercetin forms preferentially two complexes with 1:1 and 1:2 (quercetin: Al3+) stoichiometries where the first cation binds to the site of the pyrone ring but the second one is bound to the cathecol group of the molecule. However, the multichelation character of the quercetin ligand allows larger aggregates to be formed, thereby the species Al2Q3 is also detected in methanol. The lifetime of the 1:1 complex is about 2.7 ns, while for 1:2 and 3:2 complexes the lifetimes measured are 3.5 and 1.8 ns, respectively.     

A clean, well-defined solid system for photosensitized 1O2 production measurements

Generation of singlet molecular oxygen ((1)O(2)) by photosensitization with methylene blue (MB) supported in Nafion-Na films has been quantified by integration of the (1)O(2) emission decay at 1270 nm. The quantum yield of (1)O(2) production (Phi(Delta)) in the air-equilibrated solid phase is 0.24 +/- 0.03. Information on the (1)O(2) generation environment has been gained from complementary techniques such as UV-Vis absorption and emission spectroscopy, as well as MB fluorescence and triplet-triplet absorption decay. Results are compared with the (1)O(2) generation by MB in methanol solution (Phi(Delta) = 0.51) and in methanol-swollen Nafion films (Phi(Delta) = 0.49 +/- 0.06). Differences and similarities are discussed in terms of the factors that influence Phi(Delta) in solution and in the solid media. The optical and mechanical features of Nafion, ease of dye loading, compatibility with most solvents, homogeneity, reproducibility and stability of the photosensitizing material makes it a convenient reference for (1)O(2) generation quantum yield measurements in transparent (micro)heterogeneous and homogeneous media.     

PHOTOCHEMICAL CHARACTERIZATION OF COVALENTLY-LINKED PORPHYRIN-QUINONE COMPLEXES*

Abstract— The fluorescence properties of a covalently-linked porphyrin-quinone complex and its zinc derivative were studied in a variety of organic solvents. The kinetics of fluorescence decay for both the quinone and hydroquinone oxidation states were measured in acetonitrile, dichloromethane, dimethyl-formamide, and pentane. The fluorescence yield and kinetics of decay at room temperature were little affected in the porphyrin or zinc porphyrin complexes when the attached quinone was reduced. However, for these complexes the fluorescence yield and lifetimes were both substantially decreased in acetonitrile and dichloromethane when the quinone was in its oxidized state. These latter decay kinetics were not explainable by a process having a single exponential decay. On the other hand, little fluorescence quenching or lifetime shortening was observed in dimethylformamide or pentane, indicating unique solvent dependencies for the quenching process. Evidence was obtained for photoproduced charge separation from EPR measurements on the covalently-linked zinc porphyrin-quinone complex. The EPR data showed equivalent concentrations of a Zn porphyrin cation radical and a benzoquinone anion radical in acetonitrile or dichloromethane at both room temperature and 77 K. The charge separated state rapidly decayed at room temperature (in sub-millisecond times) but was quite stable at 77 K. It is concluded that light-induced charge separation in acetonitrile and dichloromethane at room temperature may occur from the excited singlet state with a high quantum efficiency. A photoproduced charge separated state also occurred when the covalently-linked complexes were incorporated into egg yolk phosphatidylcholine liposomes. The quantum yield for radical formation in this latter system was 0.1 and the lifetimes of the radical species formed were many minutes.     

Photoexcitation processes of CH3OH: Rydberg states and photofragment fluorescence

Photoabsorption and fluorescence cross sections of methanol vapor were mearured using synchrotron radiation. Weak structures observed in the 110–140 nm region are classified into three Rydberg series. Quasidiatomic repulsive potential curves for the states dissociating into CH₃ + OH(A²Σ⁺) are obtained from the measured fluorescence cross section. The photodissociation processes are discussed in accord with the fluorescence observed. The fluorescence quantum yield (< 0.8%) for photodissociation of CH₃OH is one order of magnitude smaller than that of H₂O, indicating a correlation that the fluorescence quantum yield decreases with increasing number of molecular orbitals.     

Comparison of photophysical properties of the hemicyanine dyes in ionic and nonionic solvents

The fluorescence properties of 4-[4-(dimethylamino)styryl]-1-n-alkylpyridinium bromide (hemicyanine) dissolved in solvents of different polarities and viscosities (methanol, ethylene glycol, tetra-ethylene glycol, glycerol, benzyl alcohol, pyridine, and two ionic liquids, 1-butyl-3-methylimidazolium tetrafluoroborate, [BMIM]BF4, and 1-butyl-3-methylimidazolium hexafluorophosphate, [BMIM]PF6) were investigated. Significant increase in the fluorescence quantum yield and the fluorescence decay lifetime was observed with the increase in the viscosity of the solvent medium. It is because the intramolecular rotational motion of the molecule becomes more difficult in viscous liquid, which leads to a decrease in the nonradiative decay processes. The fluorescence quantum yields for all of the solutions followed a semiempirical law that depends only on the solvent viscosity. The correlation function C(t) was obtained for each solution by joining fluorescence decay curves measured at different wavelengths. From the fitted results of C(t), we observed the distinctive feature unique to the ionic liquids, in which the correlation functions for ionic liquid solutions are fitted to be biphasic, while they are monophasic for other solvents. The fluorescence maximum of hemicyanine dissolved in these ionic liquids red-shifted following the increase in the excitation wavelength.     

Theoretical Insights into the Substituent Effects on the Fluorescence of Boron Complexes of 2-(Benzothiazol-2-yl)phenols: a Quantum Mechanics Study

The performance of organic fluorescent materials can be improved by chemical substitutions with auxochrome groups such as amino to increase solubility, alter emitting color, or modify film quality. The complex 6,6-difluoro-6-bora-5-oxa-11-thia-6 a-aza-benzo[a]fluorine(BOBTP) and its derivatives, which possess excellent luminescent property at room temperature, were theoretically simulated by density functional theory. The geometries of the ground state and the first excited state of BOBTPs complexes were investigated and their bond parameters were obtained. Further, these bond parameters are compared with each other, and the computational wavelengths of maximum absorption and emission of studied complexes match up with the experimental values. It was found that amino substituent bonding to appropriate positions of BOBTP can reduce the reorganization energy significantly, which is ascribed to electron-donating effect of the amino group. The reorganization energy also plays an important role in the fluorescence quantum yield of all the BOBTPs. In particular, the radiative decay of complexes 3 and 4 is dominant due to the smaller reorganization energies, so their fluorescence quantum yield is almost 1, on the contrary the non-radiative decay and intersystem crossing rate of both the 1 and 2 can not be ignored for the larger reorganization energies, and the corresponding fluorescence quantum yields were calculated when the radiative decay rate(kr) and nonradiative decay rate(k(nr)) were taken into account.     

Chasing BODIPY: Enhancement of Luminescence in Homoleptic Bis(dipyrrinato) ZnII Complexes Utilizing Symmetric and Unsymmetrical Dipyrrins

Dipyrromethene metal complexes are fascinating molecules that have applications as light-harvesting systems, luminophores, and laser dyes. Recently, it has been shown that structurally rigid bis(dipyrrinato) zinc(II) complexes exhibit high fluorescence with comparable quantum yields to those of boron dipyrromethenes or BODIPYs. Herein, eight new bis(dipyrrinato) Zn^II complexes, obtained from symmetric and unsymmetrical functionalization of the dipyrromethene structure through a Knoevenagel reaction, are reported. It was possible not only to vary the maximum visible absorption from 490 to 630 nm, but also to enhance the emission quantum yield up to 66 %, which is extraordinarily high for homoleptic bis(dipyrrinato) zinc complexes. These results pave the way for designing highly luminescent bis(dipyrrinato) zinc complexes.     

吩噻嗪-Corrole 镓(III)配合物的合成、荧光及其光断裂DNA性质

合成了吩噻嗪(PTZ)-corrole二元体1-3及其镓(III)配合物4-6.采用稳态吸收与稳态发射及时间分辨的瞬态光谱技术研究了这几种化合物的光物理特性.结合荧光量子产率和荧光寿命计算得到它们的辐射和无辐射速率常数.稳态吸收光谱表明:几种二元体中,corrole镓(III)单元表现出更强的Soret带和Q带.化合物1-3的荧光量子产率分别是0.156、0.134和0.139,辐射速率常数分别为4.02′107、3.47′107和2.89′107s-1.化合物4-6的荧光量子产率分别是0.502、0.443和0.494,辐射速率常数分别为20.90′107、16.78′107和21.11′107s-1.可见,化合物4-6的荧光量子产率和辐射速率常数均高于化合物1-3.然而,化合物4-6的荧光寿命分别是2.40、2.64和2.34ns,低于自由corrole1-3.琼脂糖凝胶电泳实验表明:在光照的条件下,这些吩噻嗪-corrole镓(III)二元体化合物能够把超螺旋DNA(formI)切割成缺刻型DNA(formII).