[Au(PH_3)]~+芳香基发光材料的光谱性质研究

用二阶微扰(MP2)法和单激发组态相互作用(CIS)法分别优化了发光材料H3PAuPh和(H3PAu)2(1,4-C6H4)2的基态和激发态的几何结构,并用含时密度泛函(TD-DFT)法计算了各发光材料的吸收光谱与磷光发射光谱。计算结果表明,H3PAuPh和(H3PAu)2(1,4-C6H4)2的磷光发射光谱均具有在Au(6p)→C(2p)的金属向配体的电荷转移(MLCT)参与下的pπ*(Ph)→pπ(Ph)跃迁的本质,并伴有Au(6p)→Au(5d)的金属中心电荷转移(MCCT)的性质。(H3PAu)2(1,4-C6H4)2是由两个H3PAuPh连接而成的。因此(H3PAu)2(1,4-C6H4)2的分子轨道也是由H3PAuPh的分子轨道组合而成的。在磷光发射中,由于轨道组合中存在pπ*或pπ的相互作用,所以(H3PAu)2(1,4-C6H4)2的最低能量磷光发射光谱谱线的波长大于H3PAuPh的相应值。     

一种嘧啶铱（Ⅲ）配合物的结构及光电性质研究

合成了一种铱配合物（DFPPM=2-（2,4-二氟苯基）嘧啶,acac=乙酰丙酮）,利用 X 射线单晶衍射仪测定了该化合物的晶体结构。利用紫外-可见吸收光谱、发射光谱对其光物理性质进行研究。结果表明：（DFPPM）₂ Ir（acac）的单晶结构属于三斜晶系,P-1空间群,晶胞参数a=14.444 4（7）nm,b=18.047 9（10）nm,c=19.220 0（9）nm,α=113.115（5）°;,β=90.453（4）°;,γ=90.989（4）°;,V=4 607.0（4）nm³。（DFPPM）₂ Ir（acac）在二氯甲烷溶液中的发射峰为 496 nm。以（DFPPM）₂ Ir（acac）为客体材料,制备了结构为ITO/NPB（40 nm）/CBP：（DFPPM）₂Ir（acac）（质量分数10%,30 nm）/TPBi（15 nm）/Alq₃（50 nm）/Mg：Ag（150 nm,10：1）/Ag（10 nm）的器件,器件的发射峰位于494 nm,最大亮度达到21 400 cd/m²,最大电流效率为12.0 cd/A,最大功率效率为 5.4 lm/W。     

新型绿色磷光铱配合物的合成及其光物理性能研究

合成并表征了以2-苯基吡啶为第一配体,水杨酸及其衍生物为第二配体,以铱为内核的新型配合物(ppy)₂Ir(LX)(ppy=2-苯基吡啶,LX=水杨酸Sal、4甲基水杨酸MSal、4-三氟甲基水杨酸FSal)。对其分子结构、光物理性能及热稳定性进行了测试和分析。结果表明, 室温下在二氯甲烷溶液中(ppy)₂Ir(LX)(LX= Sal, MSal, FSal)的吸收峰分别在270, 370, 450及484 nm附近,其中前2个吸收峰应归属于第一配体2-苯基吡啶的1π—π*跃迁和水杨酸配体到2-苯基吡啶的电荷转移跃迁,在450及484 nm附近的吸收峰,应该归属于金属到配体的电荷转移(1MLCT和3MLCT)跃迁和配体3π—π*跃迁的混合;其PL发射峰最大波长分别为520,522,510 nm;(ppy)₂Ir(Sal)和(ppy)₂Ir(MSal)的发射主要来源于三重态3MLCT的辐射跃迁,而(ppy)₂Ir(FSal)的发射主要来源于水杨酸到2-苯基吡啶的电荷转移态的辐射跃迁,也有单重态1MLCT和三重态3MLCT的辐射跃迁的贡献。其量子效率分别为0.37,0.33,0.29,热分解温度为306～328 ℃。(ppy)₂Ir(LX)是一组热稳定性较好的高效有机磷光材料,可用于有机电致发光器件中。     

磷光吡嗪铱(Ⅲ)配合物的合成及发光性质

合成了4种吡嗪铱配合物,用质谱和1H NMR对配合物结构进行了表征,通过紫外-可见吸收光谱和光致发光光谱对其光物理性质进行了研究。结果表明:4种铱配合物都出现了金属-配体电荷转移(MLCT)吸收峰。铱配合物1[(DFMPPZ)_2Ir(pic)]、2[(DFMPPZ)_2Ir Cl(PPh_3)]、3[(DFMPPZ)_2Ir(CN)(PPh_3)]和4[(DPPF)_2Ir(acac)]的发射波长分别为528,536,535,561 nm,都是潜在的黄、绿色磷光材料。以铱配合物4为客体材料,制备了结构为ITO/Mo O_3(1 nm)/CBP(35 nm)/CBP∶Ir(15 nm)/TPBi(50 nm)/Li F(1nm)/Al(100 nm)的一系列不同掺杂浓度的器件,器件的发射波长为567 nm,最大亮度达到32 110 cd·m-2,最大电流效率为32.4 cd·A-1,最大功率效率为28.2 lm·W-1。     

铜苯配合物结构与性质的理论研究

采用密度泛函理论的B3LYP、BP86、BPW91、B3PW91四种方法,在6-311+G(d,p)基组水平上计算研究了Cu_n(n=1-6)团簇与Cu_nC_6H_6(n=1-6)配合物的各个异构体结构和频率,比较各异构体间的能量关系,得到最稳定的几何构型.通过分析铜苯配合物的结合能和前线轨道等性质,从而了解该类配合物的作用机理.     

Au原子高Rydberg态场致电离的实验研究

利用电热法将含金物质加热,产生Au原子束,再以两束UV脉冲激光垂直照射,将处于基态的Au原子共振激发至高Rydberg态。滞后于激光脉冲200ns的高压脉冲电场(6500V/cm)加到反应区,使处于Rydberg态的Au原子电离。激光波长在一定范围内扫描,共测出了Au原子的n²D_3/2(n=18—38)和n²S_1/2(n=21—34;36—38)两通道的38条能级的位置。用参数拟合得到²D_3/2和²S_1/2两系列的极限分别为:E_D=74409.8(3)cm^-1,E_S=74410.0(2)cm^-1,计算了每条能级的量子亏损。我们的实验还证明了场电离是一种十分有效的电离手段,比用通常的激光光电离效率要高得多。这在共振电离谱学(RIS)的研究中是一种很有效的方法。 关键词：     

新型蓝色磷光嘧啶铱(Ⅲ)配合物的合成及发光性质

设计并合成了以2-(2,4-二氟苯基)嘧啶(DFPPM)为主配体的两种新型二嗪铱配合物 (Ph:苯基)和,用核磁共振(NMR)和质谱等方法对其进行了表征,并用紫外-可见吸收光谱和光致发光光谱对其光学性质进行了研究。光致发光光谱结果显示:配合物 的发射峰波长为472 nm和489 nm;而配合物 的发射峰波长为447 nm和472 nm,1931CIE色度坐标为(0.14,0.15),是一种深蓝色磷光材料。以 为客体材料、PVK为主体材料制备了电致发光器件,研究了其电致发光光谱。结果表明,电致发光光谱与光致发光光谱相比有较大程度的红移。     

含铱配合物的聚对苯类电磷光聚合物

通过Suzuki聚合法合成了以聚对苯为主链的含铱配合物的电磷光共轭聚合物。部分苯环单元被β-二酮结尾的烷氧基链取代,进而与2-苯基吡啶配位形成悬垂的铱配合物侧链。宽带隙的聚对苯主链使主体与客体的能级匹配,从而有利于能量的转移。铱配合物通过长β-二酮结尾的烷氧基链悬挂在聚对苯的侧链上提高了聚合物的溶解性,有利于器件的制作。另外,由于连在氧原子上的β-二酮具有较大的旋转自由度,增大了β-二酮的反应活性有利于配位反应的进行。聚合物的EL光谱只显示客体铱配合物的发射,主体的发射已被完全猝灭。这表明聚合物主体和铱配合物客体之间发生了有效的能量转移。PPPIrPPy2聚合物发光器件的EL光谱发光波长为525nm,最大外量子效率为2.6%。     

新型蓝绿色磷光配合物二(1-苯基吡唑)铱(吡啶三唑)的发光性能

利用1-苯基吡唑、吡啶三唑与水合三氯化铱反应合成了一种新型铱配合物Ir(2N)₂(PZ),研究了配合物的吸收光谱、光致发光光谱以及光致发光效率。利用该材料作为磷光客体,掺杂到高分子主体材料中制作了电致发光器件,研究了其电致发光光谱。结果表明,该配合物在228,250,328nm处存在自旋允许的¹π-π^*跃迁;荧光光谱结果显示在470nm处有较强的磷光发射;电致发光光谱与光致发光光谱相比却发生较大程度的红移。     

铱金属配合物磷光材料掺杂聚合物体系的电致发光特性

通过对一种新型贵金属铱的配合物磷光材料(pbi)₂Ir(acac)与咔唑共聚物进行物理掺杂, 制备了结构为indium-tin oxide(ITO)/poly(N-vinylcarbazole)(PVK): (pbi)₂Ir(acac)(x)/2,9-dimethyl-4,7-diphenyl-1,10-phenan throline(BCP)(20nm)/8-Hydroxyquinoline aluminum(Alq₃)(10nm)/Mg:Ag的聚合物电致磷光器件,研究了磷光聚合物掺杂体系在低掺杂浓度时(0.1%和0.5%(质量百分数,全文同))的光致发光(PL)和电致发光(EL)特性. 结果表明, 该掺杂体系的PL光谱和EL光谱中均同时存在主体材料PVK与磷光客体(pbi)₂Ir(acac)的发光光谱, 但主客体的发射强度不同,推测该掺杂体系在电致发光条件下, 同时存在主体材料到客体的不完全的能量传递和载流子直接俘获过程. 磷光掺杂浓度为0.1%的器件在19V电压下实现了白光发射, 色坐标为(0.32, 0.38), 掺杂浓度为0.5%的器件在20.6V电压下的最大发光亮度为11827 cd·m^-2, 而在13.4V电压下的最大流明效率为4.13 cd·A^-1. 关键词： 有机电致发光器件 铱配合物磷光 聚合物掺杂     

Theoretical study of the phosphorescence of 8-azasteroids

We have used quantum chemical methods for a theoretical study of the luminescent characteristics (including estimating the rate constants for intramolecular T₁ → S₀ electronic transitions) of the molecules of four immunoactive compounds of the 8-azasteroid class. We have established that the T₁ state is localized on the enaminodicarbonyl moiety that is common to all the molecules. We have shown that for the studied compounds, the phosphorescence spectra and the physical mechanisms for deactivation of the lower triplet state T₁ are similar. For all the compounds, the results of the theoretical study are consistent with the corresponding conclusions of experimental studies of 8-azasteroids. __________ Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 73, No. 6, pp. 751–755, November–December, 2006.     

有机电致发光器件的磷光发光研究

研制了一种以铕钇络合物（Eu0.1Cd0.9)(TTA)3(TPPO)2为发光材料的新型有机电致发光器件,观察到了三重态的磷光发光现象,分析表明此电致磷发光是Gd^3 对络合物配体电子自旋轨道强烈扰动引起的三重态发光。同时用积分球方法测定了该器件在不同温度下的光致发光和电致发光效率,结果表明此磷发光效地提高了器件的电致发光效率。     

分子高激发振动态的理论研究

简要综述了分子高激发振动态的理论研究方法和研究进展.介绍了李代数方法在高激发振动态能级的归属和分类、分子高激发振动态动力学以及分子内振动能量弛豫和分子解离等方面的应用.随后,作者对分子高激发振动态研究领域今后的发展方向作了展望.     

理论研究强激光场中2pz态氢原子的电离

运用强场近似速度规范理论研究了激发态氢原子的电离情况,当 a.u. 时（ω是激光场的频率,γ是Keldysh绝热参数）,在线性极化激光场中推导了2pz态氢原子电离率的简单表达式,从公式中可以看出在低频极限的情况下,电离率和激光场频率ω成正比,这一公式对激发态氢原子电离机制的研究提供了重要的理论参考。     

Theoretical study of electronic structure and excited states properties of two dyes for dye-sensitized solar cells

Two conjugated organic dyes comprising the benzo[b]furan moieties as the electron donor and cyanoacetic acid moieties as the electron acceptor/anchoring groups have been investigated using a quantum chemical method. The molecular equilibrium geometries and ground state character were studied using density functional theory. Absorption spectra were obtained using time-dependent density functional theory and semiempirical ZINDO. The nature of absorption spectra was further studied using 2D and 3D real-space analysis; here, 2D real-space analysis showed electron–hole coherence, and 3D real-space analysis showed intramolecular charge transfer during photo-excitation. As important parameters, excited state oxidation potential and driving force energy were obtained to reveal the relationship between molecular structure and performance of two compounds.     

Studies on odd-parity states of the Sm atom

Two-step excitation and ionization processes are used to detect Sm atoms in many excited states populated with tunable lasers. The wavelength of the first laser is tuned to the resonances from the Sm 4f^6 6s^2 ^7FJ （J=0 6） states to many odd-parity states with different electronic configurations, where the atoms are detected by photoionization process using an ultraviolet laser with a wavelength of 355 nm. Precise measurements on the energy level and intensity for many Sm 4f^6 6s6p and 4f^5 5d6s^2 states have been carried out. In a theoretical analysis on the spectral data, such as peak position, relative intensity, many transitions can be identified as the resonances from the Sm 4f^6 6s^2 7FJ （J=0-6） states to the atomic states with 4f^6 6s6p and 4f^5 5d6s^2 electronic configurations. This work also reports many spectral data on the odd-parity states that cannot be found in the literature.     

New feature of the phosphorescence of copper complexes ofmeso-tetraarylporphyrins

Introduction of methyl groups in orthopositions of phenyl rings of a Cu-meso-tetraphenylporphin (Cu-TPhP) molecule is shown to lead to a substantial decrease in the diffusivity of the spectrum of low-temperature (77 K) phosphorescence. It is found that the long-lived (580 μsec) and short-lived (0.7 μsec) components of Cu-TPhP phosphorescence differ in emission and absorption (phosphorescence-excitation) spectra and belong to two forms of molecules. The phosphorescence spectrum of the predominant form with small τ_p is diffuse, while its absorption spectrum is shifted slightly in a bathochromic manner. The phosphorescence spectrum with large τ_p is structural and is similar to the spectrum of Cu-meso-tetrakis-(ortho-tolyl)porphin. The difference is attributed to the nonplanarity (saddle distortion) of a Cu-TPhP molecule in the lower triplet state in the case of the form with small τ_p. Institute of Molecular and Atomic Physics, National Academy of Sciences of Belarus, 70 F. Skorina Ave., Minsk, 220072, Belarus; e-mail: llum@imaph.bas-net.by. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 66, No. 6, pp. 743–747, November–December, 1999.     

Molecule opacity study on low-lying states of CS

CS molecule, which plays a key role in atmospheric and astrophysical circumstances, has drawn great attention for long time. Owing to its large state density, the detailed information of the electronic structure of CS is still lacking. In this work, the high-level MRCI+Q method is used to compute the potential energy curves, dipole moments and transition dipole moments of singlet and triplet states correlated with the lowest dissociation limit of CS, based on which high accurate vibration—rotation levels and spectroscopic constants of bound states are evaluated. The opacity of CS relevant to atmospheric circumstance is computed at a pressure of 100 atms for different temperatures. With the increase of temperature, band systems from different transitions mingle with each other, and band boundaries become blurred, which are originated from the increased population on vibrational excited states and electronic excited states at high temperature.     

Energies and Auger widths of the triply excited states of He-

Some triply excited states of He^- ion are studied using the saddle-point complex-rotation method. The energies and Auger widths of these resonances are calculated with the relativistic corrections and mass polarization taken into account. The total Auger width is obtained by coupling the important open channels and summing over the other channels. These results are in good agreement with other theoretical and experimental data in the literature.     

Theoretical study on the isomerization mechanisms of phenylazopyridine on S0 and S1 states

In this work, some important structures tied closely to the isomerization of 2‐(phenylazo)pyridine (2‐PAPy) and 4‐(phenylazo)pyridine (4‐PAPy) on the S₀ and S₁ states were characterized in detail by using the complete active space SCF (CASSCF) theory. The isomerization mechanism was discussed on the basis of the mapped potential energy surfaces (PESs) and conical intersections (CIs). A comparison of PAPy with azobenzene was carried out to stress the effect of molecular structure on the photoisomerization details. The results indicate that the thermal isomerization for both 2‐PAPy and 4‐PAPy are mainly attributed to the inversion of CNN angle on the side of the pyridine ring. In view of the energy, an optimized CI_rot with a twisting structure supports the rotation mechanism in the photoisomerization of PAPy on the S₁ state. However, it was found that another conical intersection (CI_inv) with a planar structure is higher in energy than the corresponding trans‐FC structure, via which only the PAPy excited on S₂ state or vibrationally hot S₁ state can relax their excitation energy. Minimum energy paths (MEPs) showed that the relaxation process of cis‐PAPy being excited on the S₁ state is characterized by a smoothly falling curve, which is very similar to that of azobenzene. Furthermore, a S₁ minimum and a transition state (TS₁) were found to exist on the MEP starting from the trans‐FC point to the CI_rot for 4‐PAPy, but these two typical structures were not found on the MEP of 2‐PAPy. Compared with azobenzene, 4‐PAPy exhibits a very similar photoisomerization PES, but a subtly different one can be predicted in the case of 2‐PAPy. The present results are expected to provide useful information for the design of photoresponsive materials based on the PAPy units. Copyright © 2009 John Wiley & Sons, Ltd.