稀土配合物（RE（DBM）3，RE=Nd、Sm、Gd）分子内能量弛豫过程的光声光谱研究

利用光声振幅谱和位相谱对稀土配合物(Nd(DBM)3、 Sm(DBM)3和Gd(DBM)3分子内弛豫过程进行了研究。Sm(DBM)3、 Gd(DBM)3和Nd(DBM)3的配体π-π*跃迁的光声振幅强度依次增强,而Gd、 Sm和Nd的配合物在配体吸收波段内位相依次减小,反映分子内的弛豫过程。对于Gd(DBM)3,配体最低三重态能量不能传递到中心离子4f激发态能级上而直接弛豫回基态;对于Sm(DBM)3和Nd(DBM)3,配体三重态能量有效地传递到中心离子上, Nd3+各能级间隔小且相互重叠,激发态能量几乎全部以无辐射跃迁回基态; Sm3+为荧光离子,激发态上的部分能量以荧光形式发射。由此并结合荧光光谱的结果建立了分子内能量弛豫模型。     

光致发光稀土大配合物

对当胶国际上溶液中发光的稀土大环配合物进行了综述，讨论了配体与金属间能量转移机理和大环配体对稀土离子的屏蔽效应。     

Eu3+,Tb3+掺杂荧光二氧化硅纳米粒子的合成及其结构、成分和荧光性质的调控

针对目前存在的稀土螯合物掺杂量低、发射吸收波长受到限制等问题,首先用设计好的敏化剂-配体-硅烷偶联剂来螯合稀土离子得到稀土螯合物,然后在反相微乳液中将上述稀土螯合物与正硅酸乙酯(TEOS)共同水解缩聚,合成了稀土掺杂的二氧化硅纳米粒子。通过这种方法,不仅实现了对FSNPs粒径、成分、发射波长的调控,还通过使用不同生色团和稀土离子,获得了对激发波长的调控能力。此外,进一步阐述了稀土掺杂FSNPs中的能量转移过程,提出了一种通过能级调节FSNPs荧光的新方法。     

Au(I)炔基配合物激发态性质的理论研究

用MP2方法和CIS方法分别优化了Au(I)炔基配合物及相应炔烃的基态和激发态的结构. 计算结果表明, 在基态, 分子有向中间收缩的趋势, Au(I)的修饰作用减弱了配体内部原子间的成键作用. 随着分子链长增长, Au(I)与配体间的相互作用减弱; 激发态的电子跃迁减弱了, Au(I)与配体间的相互作用, 并且这种影响随着分子链增长而更加明显. 计算得出Au(I)炔基配合物体系的荧光发射光谱并发现其独特的发光性质, 说明取代H原子的—AuPH3比—H更具有离子性.     

光致发光稀土大环配合物

对当前国际上溶液中发光的稀土大环配合物进行了综述,讨论了配体与金属间能量转移机理和大环配体对稀土离子的屏蔽效应.     

合成双分子膜多元体系的激发态能量转移

发现在４－（４－癸氧基联苯－４－氧基三甲基）溴化铵双分子膜体系内，从联苯给体通过结合在膜表面上的达旦黄传递到罗丹明Ｂ受体的三元激发态的能量转移效率较高．探讨了囊泡在此能量转移过程中的特殊功能作用和能量转移的机制．同时还观察到了在此体系内通过静电相互作用，组织在囊泡表面上的达旦黄、荧光黄、罗丹明Ｂ和四苯基卟啉间的多元能量转移，这种能量转移可改善光的输出，扩展光波的覆盖范围．     

芳环上硝基取代基对苯甲酸功能化聚苯乙烯-Eu（Ⅲ）配合物光致发光性能的双重影响

将硝基苯甲酸配基(NBA)键合在聚苯乙烯侧链,制得了硝基苯甲酸功能化的聚苯乙烯(PS-NBA),在此基础上使大分子配体PS-NBA与Eu(III)离子配位,制备了二元高分子-稀土配合物PS-(NBA)3-Eu(III),也以邻菲罗啉(Phen)为小分子配体,制备了三元高分子-稀土配合物PS-(NBA)3-Eu(III)-Phen1,重点研究了芳环上硝基取代基对高分子-稀土配合物光致发光性能的影响.研究结果表明,芳环上的硝基取代基对以Eu(III)为中心离子的苯甲酸功能化聚苯乙烯-稀土配合物的发光性能具有双重影响.硝基取代基通过配基内的电荷转移(ILCT),耗损配基激发单线态的能量,有效降低苯甲酸配基的三线态能量,使配基NBA最低三线态能级与Eu(III)离子共振能级之间的匹配程度显著增强,对Eu(III)离子的荧光发射发生强敏化作用,使配合物PS-(NBA)3-Eu(III)以及PS-(NBA)3-Eu(III)-Phen1产生了高强度的荧光发射,显现出硝基取代基对配合物发光性能的正性影响.另一方面,即使在稀溶液中,随着高分子-稀土配合物浓度从4.0×10-6mol·L-1增大至4.0×10-4mol·L-1,配合物的荧光发射也会逐渐变弱,这是由激发态的配合物向硝基发生荧光共振能量转移(FRET)的淬灭作用所导致的,表现出硝基取代基对配合物发光性能的负性影响.     

稀土有机螯合物发光研究进展

总结了稀土有机螯合物结构与发光性能的关系：配体最低三重态能级与稀土离子激发态能级的匹配是中心稀土离子能否发光的主要因素;螯合物结构的平面性和刚性是中心离子发光效率高低的重要因素;适宜的第二配体的加入一般导致螯合物分子刚性和稳定性增高,因而有利于能量的传递,致使中心离子发光效率增高,但也不能忽视第二配体加入所引起光能的吸收和能量传递过程的竞争;配体的耐热,耐辐射性是配合物能否作为材料的必要因素,自行设计,合成了5类25种新的有机配体及其相应的二元,三元稀土螯合物,研究了这些螯合物的配位性质,发光性能,发光与结构关系及发光机制。提出并发展了稀土离子发光和电子振动光谱作为配合物和生物分子结构探针的两种新的方法。将稀土－β－二酮的发光螯合物与树脂制成荧光塑料;利用铕和铽螯合物的发光和免疫反应,检测了体液中生物活性物质的含量,证实以稀土离子替代放射性同位素作为标记物,有希望替代放射免疫分析方法,成为常规的临床检验方法,利用Tb^3 荧光检测了植物中生长激素的含量。     

烟酸稀土分子杂化发光材料的制备与性能研究

利用烯-巯加成的方法,合成了一种带有三联吡啶基团的有机硅氧烷,该中间体用核磁共振、红外、质谱等手段进行了表征确认.以该中间体作为第二配体,加入稀土(Eu3+、Tb3+)烟酸配合物,在正硅酸乙酯的存在下用溶胶-凝胶法原位制备了稀土(Eu3+、Tb3+)烟酸配合物与二氧化硅基质以共价键相连的烟酸稀土分子杂化发光材料.通过红外光谱、紫外-可见光漫反射光谱、荧光光谱和寿命测试表征了制备的杂化发光材料.荧光光谱数据表明在杂化材料中,由于三联吡啶配体通过有效的分子内传能过程将其激发态的能量传递给稀土离子的发射能级,从而极大地提高了稀土离子的特征发射.掺铕离子的最强发射为617nm,是纯红光发射;而掺铽离子的最强发射为543nm,是典型的绿光发射.掺铕和铽的分子杂化材的荧光寿命分别为0.66ms,0.68ms,同时荧光衰减均为一级指数衰减,说明稀土离子在杂化材料中分散得很均匀.     

金属离子响应型荧光传感分子的设计原理及研究进展

荧光传感凭借其高灵敏度、可实现远程监测和实时性等优越性而广受关注,在离子识别中常被用于离子识别信号的输出.随着主客体化学的迅速发展,许多具有良好性能的离子响应型荧光探针相继被报道,从分子内电荷转移(ICT)、光诱导的电子转移(PET)、荧光共振能量转移(FRET)、激发态分子内质子转移(ESIPT)、激基缔合物的生成/消失、螯合作用导致的荧光增强(CHEF)等不同机理对荧光传感型离子识别受体的设计思路进行了理论阐释,归纳总结了近5年来相关文献报道,阐述了其研究现状和研究进展,并展望了该领域的研究方向.     

Solvent Effects on Spectral Property and Dipole Moment of the Lowest Excited State of Coumarin 343 Dye

Steady-state absorption and fluorescence spectra, and time-resolved fluorescence spectra of coumarin 343 (C343) were measured in different solvents. The effect of the solvent on the spectral properties and dipole moment of the lowest excited state of C343 were investigated. It was found that the absorption and fluorescence spectra red-shifted slightly and strongly with increasing solvent polarity, respectively, because the charge distribution of the excited state leaded to the increasing difference between the absorption and fluorescence spectra with increasing solvent polarity. The dipole moment of the lowest excited state of C343was determined from solvatochromic measurements and the quantum chemical calculation, and the results obtained from these two methods were fully consistent. Investigations of the time-resolved fluorescence of C343 in different solvents indicated that the fluorescence lifetimes increased nearly linearly with increasing solvent polarity from 3.09 ns in toluene to 4.45 ns in water. This can be ascribed to the intermolecular hydrogen bonding interactions between C343 and hydrogen donating solvents.     

Temperature‐Dependent Behavior of the Dual Fluorescence of 2‐(3‐Fluorophenyl)‐2,3‐dihydro‐1H‐benzo[f]isoindole‐1,3‐dione

The fluorescence behavior of 2‐(3‐fluorophenyl)‐2,3‐dihydro‐1H‐benzo[f]isoindole‐1,3‐dione ( 1 ) was studied in solvents of different polarity and viscosity. Dual luminescence is observed and the short‐wavelength emission is found to increase considerably with the solvent polarity. The ratio of the fluorescence quantum yield of the two states emitting, the one (SW*) at short wavelength and the other (LW*) at long wavelength, shows a bell‐shaped dependence on the reciprocal of the temperature in diethyl ether, butyronitrile, and propane‐1,2,3‐triol triacetate (glycerol triacetate; GTA). This has been interpreted as the result of a reversible interconversion between the two states. The enthalpy difference between the SW* and LW* excited states, as deduced from the slope of the ln (Φ/Φ) vs. 1/T curves in the high temperature range, is found to be solvent polarity and solvent viscosity independent as the same value (−7.3 kJ/mol) is obtained in the three above‐mentioned solvents. The independence from polarity is the consequence of a similar difference in dipole moment between the ground‐state and the SW* and LW* excited states (4.5 and 4.9 D, respectively, derived from solvatochromy). The activation energy of the SW*→LW* step deduced from the low temperature measurements in the nonviscous solvents, increases with solvent polarity (11.6 and 17.5 kJ/mol for diethyl ether and butyronitrile, respectively); they are greater than the viscous‐flow activation energy of the solvents indicating that the resolvation of the excited dipole controls the kinetics. In the nonviscous solvents, the LW* state originates from the SW* state, while in the viscous GTA solution, both states are formed simultaneously within the 1‐ps laser pulse.     

Excited state dipole moments and polarizabilities of centrosymmetric and dimeric molecules. II. Polyenes, polyynes and cumulenes

Electro-optical absorption spectra are measured for a series of polyenes, polyynes and cumulenes with centrosymmetric π-chromophores in cyclohexane solution at 298 K. For all molecules the long-axis component of the polarizability tensor is considerably larger in the first dipole-allowed singlet state compared to the ground state. The transition moments are found to be parallel to the long molecular axis. All polyenes and one cumulene show a linear Stark component indicating a long-axis excited state dipole moment. Both the dipole moments and the polarizabilities are corrected within the extended Onsager model for solvent cavity and reaction field effects. It is suggested that symmetry lowering solvent perturbations are the reason for the apparent excited state dipole moments.     

Effect of nitro groups on the photo physical properties of benzimidazolone: a solvatochromic study

Electronic absorption and fluorescence spectra of mono, di, and tri-nitro benzimidazolones are measured at room temperature (298 K) in nine solvents with different polarities and the observed shifts are compared with benzimidazolone. Ground and excited state electric dipole moments are determined using the solvatochromic method based on the bulk solvent properties, F(1)(ε, n) and F(2)(ε, n). A reasonable agreement is observed between the experimental and ab initio dipole moments. Change in dipole moment is also determined using the solvatochromic method based on the microscopic solvent polarity parameter, (E(T)(N)), which considers the polarization changes due to hydrogen bonding in different solvents. It has been observed that the correlation of the solvatochromic Stokes shifts with the parameter (E(T)(N)), is superior to that derived using bulk solvent polarity functions for all the benzimidazolones reported in the present study. Calculated difference between excited state and ground state dipole moments seems to be a good measure of the effect of nitro group when correlated with (E(T)(N)).     

The styrylpyridine dye for the silane sol-gel transition studies by time-dependent fluorescence

A trans-4-(p-N,N-dimethylaminostyryl)-N-vinylbenzylpyridinium chloride (vbDMASP) fluorescence probe was optimized in ground and excited state as a function of change in the microenvironment polarity, using the Amsol HyperChem program package. In the calculations, protic and aprotic solvents were used. On this basis a change in the molecule geometry after excitation, depending on the surrounding solvent, was determined. Absorption and steady-state fluorescence spectra of vbDMASP in the solvent of different polarity and in the model water-glycerol solutions were also recorded. On the basis of Stokes' shift change with the Onsager polarity scale a change in the dipole moment of the probe during transition from ground to excited state, in protic and aprotic solvents was determined. Since during the sol-gel transition of tetraethylorthosilane in the acidic environment both polarity and viscosity of the microenvironment change the vbDMASP probe was applied and fluorescence time-resolved measurements were done. On this basis the correlations between the results of time-resolved measurements for the multichromophoric probe applied in the gelation process and molecular optimization data are discussed.     

Highly Luminescent and Thermally Stable Lanthanide Coordination Polymers Designed from 4-(Dipyridin-2-yl)aminobenzoate: Efficient Energy Transfer from Tb(3+) to Eu(3+) in a Mixed Lanthanide Coordination Compound

Herein, a new aromatic carboxylate ligand, namely, 4-(dipyridin-2-yl)aminobenzoic acid (HL), has been designed and employed for the construction of a series of lanthanide complexes (Eu(3+) = 1, Tb(3+) = 2, and Gd(3+) = 3). Complexes of 1 and 2 were structurally authenticated by single-crystal X-ray diffraction and were found to exist as infinite 1D coordination polymers with the general formulas {[Eu(L)(3)(H(2)O)(2)]}(n) (1) and {[Tb(L)(3)(H(2)O)].(H(2)O)}(n) (2). Both compounds crystallize in monoclinic space group C2/c. The photophysical properties demonstrated that the developed 4-(dipyridin-2-yl)aminobenzoate ligand is well suited for the sensitization of Tb(3+) emission (Φ(overall) = 64%) thanks to the favorable position of the triplet state ((3)ππ*) of the ligand [the energy difference between the triplet state of the ligand and the excited state of Tb(3+) (ΔE) = (3)ππ* - (5)D(4) = 3197 cm(-1)], as investigated in the Gd(3+) complex. On the other hand, the corresponding Eu(3+) complex shows weak luminescence efficiency (Φ(overall) = 7%) due to poor matching of the triplet state of the ligand with that of the emissive excited states of the metal ion (ΔE = (3)ππ* - (5)D(0) = 6447 cm(-1)). Furthermore, in the present work, a mixed lanthanide system featuring Eu(3+) and Tb(3+) ions with the general formula {[Eu(0.5)Tb(0.5)(L)(3)(H(2)O)(2)]}(n) (4) was also synthesized, and the luminescent properties were evaluated and compared with those of the analogous single-lanthanide-ion systems (1 and 2). The lifetime measurements for 4 strongly support the premise that efficient energy transfer occurs between Tb(3+) and Eu(3+) in a mixed lanthanide system (η = 86%).     

Solvent effect on absorption and fluorescence spectra of coumarin laser dyes: evaluation of ground and excited state dipole moments

The effect of solvents on absorption and fluorescence spectra and dipole moments of coumarin 307 (C307) and coumarin 522B (C522B) have been studied extensively in various solvents, viz., general solvents, alcohols and binary mixtures (acetonitrile-benzene) at 298K. The bathchromic shift observed in absorption and fluorescence spectra of C307 and C522B with increasing solvent polarity indicates that transition involved are pi-->pi*. Solvatochromic correlations were used to obtain the ground and excited state dipole moments. The excited state dipole moments are observed to be greater than their ground state counterparts in all the solvents studied. Further, the experimentally obtained Deltamu were compared with those using normalized polarity terms E(T)(N) from Reichardt equation.     

Solvatochromic behavior on the absorption and fluorescence spectra of Rose Bengal dye in various solvents

The absorption and fluorescence spectra of Rose Bengal dye were studied in various solvents. It was found that solvent effects on the absorption wavelength are consistent with the solvatochromic model of Kamlet, Abboud and Taft. The solvent polarizability value pi* was found to have a linear relationship with the absorption wavelength of the dye in various solvents. Additionally, the normalized transition energy value (E(T)(N)) showed some scattering when plotted versus Deltanu(af). Density functional calculations were used to assign the absorption in the region 540-570 nm to a pi-pi* transition between the HOMO and LUMO of the anion. Experimental ground state and excited state dipole moments were calculated by using the solvatochromatic shifts of absorption and fluorescence spectra as a function of the dielectric constant (epsilon) and refractive index (n). The dipole moment for Rose Bengal was found to be 1.72 Debye in the ground state, whereas this value was 2.33 Debye in the excited state.     

Ce3+,Tb3+,Eu3+共掺杂Sr2MgSi2O7体系的白色发光和能量传递机理

通过正交试验,采用高温固相法制备了Sr2-x-y-zMgSi2O7∶xCe3+,yTb3+,zEu3+系列样品.使用X射线衍射仪和荧光光谱仪表征了样品的物相和发光性质,并讨论了Ce3+-Tb3+-Eu3+共掺杂Sr2MgSi2O7体系中的能量传递过程.实验结果表明,在327 nm波长激发下,所合成荧光粉的发射峰主要位于387 nm(蓝紫)、542nm(绿)和611 nm(红)处;分别以387,542和611 nm为监控波长,所得激发光谱显示荧光粉在327 nm处有最好的激发.在327 nm光激发下,系列样品发光进入白光区.最优化的荧光粉为Sr1.91MgSi2O7∶0.01Ce3+,0.05Tb3+,0.03Eu3+,其色坐标为(0.337,0.313),是一种潜在的发光二极管(LED)用白色荧光粉.     

吩噻嗪给体受体衍生物激发态的电荷转移

A series of N-bonded donor-acceptor derivatives of phenothiazine containing phenyl （PHPZ）, anisyl （ANPZ）, pyridyl （PYPZ）, naphthyl （NAPZ）, acetylphenyl （APPZ）, and cyanophenyl （CPPZ） as an electron acceptor have been synthesized. Their photophysical properties were investigated in solvents of different polarities by absorption and emission techniques. These studies clearly revealed the existence of an intramolecular charge transfer （ICT） excited state in the latter four compounds. The solvent dependent Stokes shift values were analyzed by the modified Lippert-Mataga equation to obtain the excited state dipole moment values. The large excited state dipole moment suggests that the full （or nearly full） electron transfer take place in the A-D systems. In the system of A-D phenothiazine derivatives, the transition dipole moments Mflu were determined mainly by direct interactions between the solvent-equilibrated fluorescence ^1CT state and ground state because of their lack of significant change with increase of the solvent polarity. The electron structure and molecular conformation of phenothiazine derivatives will be significantly changed with the increase of the electron affinity of the N-10 substituent.