双核铜配合物[Cu2（pida）2（2,2′-bipy）2]的合成、表征及其结构

N-苯基亚氨基二乙酸,Cu2 离子和2,2′-联吡啶在溶液中组装得到标题配合物[Cu2(pida)2(2,2′-bipy)2](H2pida=N-苯基亚氨基二乙酸)。用元素分析、红外光谱、单晶衍射对配合物的组成和结构进行了表征,结果表明,该标题配合物为N-苯基亚氨基二乙酸根桥联的双核结构,配体pida中的N原子没有参与配位,中心铜离子为五配位畸变的四方锥构型。     

双核铜配合物[Cu2(pida)2(2,2''-bipy)2]的合成、表征及其结构

N-苯基亚氨基二乙酸,Cu2 离子和2,2'-联吡啶在溶液中组装得到标题配合物[Cu2(Pida)2(2,2'-bipy)2](H2pida=N-苯基亚氨基二乙酸).用元素分析、红外光谱、单晶衍射对配合物的组成和结构进行了表征,结果表明,该标题配合物为N-苯基亚氨基二乙酸根桥联的双核结构,配体pida中的N原子没有参与配位.中心铜离子为五配位畸变的四方锥构型.     

新型苯基吡唑铱(Ⅲ)配合物的合成及光物理性能研究

合成了4种新型铱配合物(ppz)₂Ir(LX)(ppz＝1-苯基吡唑,LX＝2-(2’-羟基苯基)苯并噻唑(BTZ),2-(3’-甲基-2’-羟基苯基)苯并噻唑(3-MeBTZ),2-(4’-甲基-2’-羟基苯基)苯并噻唑(4-MeBTZ),2-(4’-三氟甲基-2’-羟基苯基)苯并噻唑(4-TfmBTZ)),并对其分子结构和光物理性能进行了表征。结果表明,4种配合物的最大发光峰分布在583～615 nm,并都在400 nm左右出现一个弱发射带。400 nm的弱发射被认为是金属离子微扰的辅助配体BTZ的单重态激子的辐射跃迁,长波段的光发射被认为是Ir(BTZ)的3MLCT三重态激子的辐射跃迁。而Ir(ppz)₂的3MLCT的三重态激子在室温下被猝灭。最强激发带位于250～310 nm,表明这些配合物的发射主要源于ppz和BTZ配体的跃迁,而不是3MLCT跃迁。与Ir(ppz)₃相比,不仅实现了室温磷光,也通过第二配体的修饰实现了对发光颜色的调制。     

轻稀土与苯基乙酰甲基亚砜配合物的合成表征及光致发光

合成了五种轻稀土高氯酸盐与苯基乙酰甲基亚砜(L)的配合物RE(C1O₄)·L₅·2H₂O(RE=La,Pr,Nd,Sm,Eu),该系列配合物可溶于水,红外光谱及摩尔电导表明,配体通过亚砜基团上的氧原子与稀土离子配位,羰基氧不参与配位,３个高氯酸根离子有2个在内界与稀土离子配位,另1个在外界不参与配位。测定了配体的磷光光谱,并对配合物进行了热重和核磁共振氢谱等表征。铕(Ⅲ)配合物荧光光谱表明,Eu3+处于无反演对称中心格位上,且该配合物的发光机理属于M→M型发光。     

一种基于环金属铱配合物的高效绿色聚合物电致发光器件

以2-苯基吡啶为主配体,3-乙酰基樟脑为辅助配体合成了一种新型的具有大空间位阻的环金属铱配合物Ir[(PPy)2(acam)],对它的化学结构和光物理性质进行了表征.以环金属铱配合物Ir[(PPy)2(acac)]的发光效率(0.34)为参照物,配合物在2-甲基四氢呋喃溶液中的光致发光效率为0.54,表明在配合物中引入...     

Ni2+、联吡啶和N-苯基亚氨基二乙酸三元金属混配配合物的合成与表征

N-苯基亚氨基二乙酸、2 ,2′-联吡啶和 Ni Cl2 · 6 H2 O在溶剂中进行自组装形成了一种新的三元金属混配配合物。用元素分析、热重分析、红外和紫外光谱对配合物的组成和结构进行了表征 ,初步确定配体N -苯基亚氨基二乙酸中的 2个羧基为单齿形式与中心金属离子 Ni2 配位。     

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。     

新型蓝色有机电致磷光配合物二(2-二氟苯基-4-甲基吡啶)[2-(2′-吡啶基)咪唑]合铱的合成及光谱学性能

合成了三个以含氟苯基吡啶及吡啶基咪唑为配体的蓝色磷光电致发光铱配合物(P)2Ir(pym),其中主配体(P)分别为2-(2′,4′-二氟苯基)-4-甲基吡啶、2-(3′,4′-二氟苯基)-4-甲基吡啶、2-(3′,5′-二氟苯基)-4-甲基吡啶;辅助配体pymH为2-(2′-吡啶基)咪唑。通过元素分析、核磁、质谱、红外进行结构表征;用紫外可见吸收光谱、荧光光谱以及循环伏安进行其光谱学性能表征。以pymH取代辅助配体picH(2-吡啶甲酸)的方法,得到含吡啶基咪唑的铱配合物,在室温下二氯甲烷溶液中获得强的蓝光发射,其最大发光波长分别是461,480,490nm,其中(46fpmpy)Ir(pym)较经典蓝光磷光材料FIrpic蓝移5nm。     

稀土Tb3+,Eu3+对N-苯基邻氨基苯甲酸及邻菲咯啉间能量传递与蓝色发射的强化作用

合成了一种由稀土离子与N—苯基邻氨基苯甲酸(N—HPA)和邻菲咯啉(phen)形成的蓝色发光配合物。该配合物是典型的配体发光配合物，其发射峰位于444nm，激发波长为334nm和407nm。元素分析、红外光谱、紫外—可见光谱和差热—热重的分析结果表明：配合物中含有大量的N—HPA和相对较少的稀土离子和phen，其中稀土离子与N—PA中的羧酸根配位，而N—PA中的氨基通过氢键与phen的氯原子结合，形成了有利于配体之间的能量传递和电子转移的通道。稀土离子Tb^3 ，Eu^3 的共同存在促进了这一能量转移通道的形成，进而强化了配体的蓝色发射。     

一种橙光磷光铱(Ⅲ)配合物的合成、晶体结构及光电性质研究

采用二氯甲烷为溶剂,无水碳酸钾为缚酸剂,在25℃温和条件下,以2-苯基-4-甲基喹啉铱(III)氯桥二聚体[(4m2pq)2Ir(μ-Cl)2Ir(4m2pq)2]和乙酰丙酮(Hacac)进行配位,反应合成了新型铱(Ⅲ)配合物[(4m2pq)2Ir(acac)]。通过核磁共振氢谱(1H NMR)、碳谱(13C NMR)、X射线单晶衍射等确定分子结构,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:(4m2pq)2Ir(acac)的单晶结构属三斜晶系,空间群为P1;(4m2pq)2Ir(acac)在二氯甲烷溶液中呈橙光发射,发射峰为597 nm,磷光寿命0.33μs,量子效率达50.4%。以(4m2pq)2Ir(acac)为客体掺杂在CBP中,制备了结构为ITO/NPB(30 nm)/CBP:(4m2pq)2Ir(acac)(质量分数6%和8%,20 nm)/BCP(10 nm)/Alq3(20 nm)/LiF(1 nm)/Al(150 nm)的橙色磷光有机电致发光器件,器件的最大亮度达到39 667 cd/m2,发射峰位于597 nm,最大电流效率为14.2 cd/A,最大功率效率为8.1 lm/W。     

Theoretical Study of the Collision-Induced Double Transition CO(2) (nu(3) = 1) + N(2) (nu(1) = 1) <-- CO(2) (nu(3) = 0) + N(2) (nu(1) = 0) at 296 K

A procedure is presented for the calculation of the double vibrational collision-induced absorption CO(2) (nu(3) = 1) + N(2) (nu(1) = 1) <-- CO(2) (nu(3) = 0) + N(2) (nu(1) = 0) on the basis of quantum lineshapes computed using an isotropic potential and dipole-induced dipole functions. The linestrengths and energies of the vibration-rotation transitions are treated explicitly for N(2), utilizing the HITRAN database for CO(2). The theoretical absorption profile is compared to recent experimental results. By narrowing the width of the individual lines contributing to the overall absorption profile relative to their values determined for N(2)-N(2) collision-induced absorption, excellent agreement between theory and experiment is obtained. Copyright 2000 Academic Press.     

First Observation of the nu(17)-nu(4) Difference Bands of Diborane (10)B(2)H(6) and (11)B(2)H(6)

An analysis of the nu(17)-nu(4) difference bands near 800 cm(-1) of two isotopic species, (10)B(2)H(6) and (11)B(2)H(6), of diborane has been carried out using infrared spectra recorded with a resolution of ca. 0.003 cm(-1). In addition, the nu(17) band of (10)B(2)H(6) has been recorded and assigned. Since this band in (11)B(2)H(6) had already been studied (R. L. Sams, T. A. Blake, S. W. Sharpe, J.-M. Flaud, and W. J. Lafferty, J. Mol. Spectrosc. 191, 331-342 (1998)), it was possible to derive precise energy levels and Hamiltonian constants for the 4(1) vibrational states of both isotopic species. Copyright 2000 Academic Press.     

The 2(3)Delta(g) State of (7)Li(2)

Using pulsed perturbation-facilitated optical-optical double resonance (PFOODR) spectroscopy, the 2(3)Delta(g) state of (7)Li(2) (electronic configuration (varsigma(g)2s) (4ddelta(g)), effective principal quantum number n* = 4.101) has been observed and assigned. Molecular constants and a RKR potential energy curve were obtained. The major molecular constants are Copyright 2000 Academic Press.     

The Perturbation between the G(1)Pi(g) and 2(1)Delta(g) States of (7)Li(2)

We have observed the rotational levels in the v = 2, 3, 5, 6, 7, and 8 vibrational manifolds of the 2(1)Delta(g) state of (7)Li(2) via the A(1)Sigma(+)(u) intermediate levels by DeltaLambda = 2 transitions. This violation of the DeltaLambda = 0, +/-1 selection rule is due to the interaction with the G(1)Pi(g) state. Band-by-band deperturbations of the G(1)Pi(g) approximately 2(1)Delta(g) (v(Pi), v(Delta)) = (11, 2), (12, 3), (15, 5), (16, 6), (18, 7), and (19, 8) bands have been performed. Deperturbed molecular constants and rotational-electronic interaction parameters are reported here. Copyright 2000 Academic Press.     

Rovibrational Intensities of the (00(0)3) <-- (10(0)0) Dyad Absorption Bands of (12)C(16)O(2)

Absolute line intensities of (12)C(16)O(2) are experimentally measured for the first time for the (00(0)3)(I) <-- (10(0)0)(II) band at 5687.17 cm(-1) and the (00(0)3)(I) <-- (10(0)0)(I) band at 5584.39 cm(-1). The spectra were obtained using a Bomem DA8 Fourier transform spectrometer and a 25-m base-path White cell at NASA-Ames Research Center. The rotationless bandstrengths at a temperature of 296 K and the Herman-Wallis parameters are S(0)(vib) = 6.68(30) x 10(-25) cm(-1)/(molecule/cm(2)); A(1) = 1.4(9) x 10(-4), and A(2) = -1.1(5) x 10(-5) for the (00(0)3)(I) <-- (10(0)0)(II) band and S(0)(vib) = 6.07(22) x 10(-25) cm(-1)/(molecule/cm(2)); A(1) = 5.2(1.5) x 10(-4) and A(2) = -4.0(7) x 10(-5) for the (00(0)3)(I) <-- (10(0)0)(I) band.     

The v(1)+v(3) Bands of the (16)O(17)O(16)O and (16)O(16)O(17)O Isotopomers of Ozone

Using 0.002 cm(-1) resolution Fourier transform absorption spectra of an (17)O enriched ozone sample, an extensive analysis of the v(1)+v(3) bands of the (16)O(17)O(16)O and (16)O(16)O(17)O isotopomers of ozone has been performed for the first time. The experimental rotational levels of the (101) vibrational states were satisfactorily reproduced using a Hamiltonian matrix that takes into account the observed rovibrational resonances. More precisely, for (16)O(17)O(16)O, as for the other C(2v)-type ozone isotopomers, it was necessary to account for the Coriolis type resonances linking the (101) rotational levels with the levels of the (200) and (002) vibrational states and the Darling-Dennison interaction coupling the levels of (200) with those of (002). For the C(s)-type isotopomer, namely (16)O(16)O(17)O, as for (16)O(16)O(18)O and (16)O(18)O(18)O, it proved necessary to also account for an additional DeltaK(a)&equals+/-2 resonance involving the rotational levels from (101) and (002) (J.-M. Flaud and R. Bacis, Spectrochimica Acta Part A 54, 3-16 (1998)). Using a Hamiltonian matrix which takes these resonances explicitly into account, precise vibrational energies and rotational and coupling constants were deduced, leading to the following band centers: v(0)(v(1)+v(3))=2078.3496 cm(-1) for (16)O(17)O(16)O and v(0)(v(1)+v(3))=2098.8631 cm(-1) for (16)O(16)O(17)O. Copyright 2001 Academic Press.     

CO2同位素分子16O12C16O, 16O12C17O, 16O13C17O配分函数研究

本文主要研究了CO2的三种同位素分子16O12C16O , 16O12C17O ,16O13C17O 70 K~6000 K的总内配分函数 (TIPS)。在总内配分函数的计算中, 转动配分函数的计算采用了McDowell的解析式法, 振动配分函数则采用了简谐振动近似(HOA)获得。最后通过将两配分函数乘积近似计算得出TIPS, 并将其70~3000 K的数据和HITRAN04数据进行了比较, 发现所得结果和数据库符合的较好, 且其误差可以近似看成一条直线。并通过对误差的拟合修订了高温区(3000~6000 K)的计算数据, 给出了在高温下的较为准确的TIPS值。     

Torsional Splitting in the nu(5) Fundamental Infrared Band of CH(3)CD(3) and (13)CH(3)CD(3)

The nu(5) fundamental (C-C stretching) of CH(3)CD(3) shows a resolved torsional structure, caused by perturbations due mainly to the linear dependence of the torsional potential barrier on the normal coordinate Q(5). We were able to analyze this structure and to assign vibration-rotation transition wavenumbers for all five torsional components, classified according to the symmetry species of the G(18)((3)) extended molecular group. The torsional splitting pattern is qualitatively similar to that of a nondegenerate vibrational state with an even number of excited torsional quanta v(6). Explorative calculations show that the main perturber system should consist of the torsional components of the vibrational ground state correlating with v(6)=4 in the high barrier limit. The strength of the perturbation on the E(r0) torsional components of nu(5) increases rapidly with r, the E(40) component being the most affected. The observed transition wavenumbers can be reasonably fitted by a simplified model containing independent effective vibration-rotation parameters for the five different torsional components of nu(5), for both CH(3)CD(3) and (13)CH(3)CD(3). The trend of the determined values of the effective vibrational wavenumbers and rotational parameters over the torsional components supports the proposed vibration-torsion interaction mechanism, responsible for the observed torsional splittings. A strong anomaly observed in the rotational intensity distribution of nu(5) is discussed. Copyright 2001 Academic Press.