手性配体2,5-二(4,5-蒎烯-2-吡啶)吡嗪及其铼配合物的合成与表征

本文报道了手性配体2,5-二(4,5-蒎烯-2-吡啶)吡嗪(L)及其铼配合物[Re(CO)3Cl(L)].DMF的合成与表征。X射线单晶衍射分析表明配体L晶体为单斜P21空间群,而配合物[Re(CO)3Cl(L)].DMF晶体为正交P212121空间群。配合物[Re(CO)3Cl(L)].DMF中铼原子与配体中的2个氮原子、3个羰基中的碳原子以及1个氯原子配位。CD谱和VCD谱测试表明,配体和配合物都表现出光学活性。受光激发时,配体和配合物分别在420和650 nm处发光。配体和配合物都具有二阶非线性光学性质,其二阶非线性光学效应分别为尿素的0.4和0.3倍。     

螺芴对含三齿磷配体的铱配合物光电性能的影响（英文）

合成了一种含4,5-二氮-9,9-螺二芴(sb)配体的三齿磷铱配合物Ir(tpit)(sb)Cl(tpitH_2=亚磷酸三苯基酯),通过核磁共振氢谱和磷谱及高分辨质谱对其结构进行了确定。X射线单晶衍射分析表明,sb配体的存在扭曲了分子结构,有助于降低分子聚集及发光淬灭。与存在分子内π-π堆积的模型配合物Ir(tpit)(bpy)Cl(bpy=2,2′-联吡啶)对比进行了光电性能的研究。结果表明在聚甲基丙烯酸甲酯(质量分数1%)中配合物Ir(tpit)(sb)Cl的发光波长为512 nm,相对配合物Ir(tpit)(bpy)Cl的波长(520 nm)有了8 nm蓝移。配合物Ir(tpit)(sb)Cl的发光量子效率为30%,与配合物Ir(tpit)(bpy)Cl的94%相比有明显降低,说明了分子内π-π堆积作用在降低柔性基团非辐射跃迁率方面的重要作用。基于配合物Ir(tpit)(sb)Cl的有机电致发光器件,最大电流效率和外量子效率分别为14 cd·A~(-1)和4.5%。而由于分子内π-π堆积作用,基于配合物Ir(tpit)(bpy)Cl器件的最大电流效率和外量子效率分别高达60 cd·A~(-1)和18.2%。     

螺芴对含三齿磷配体的铱配合物光电性能的影响

合成了一种含4,5-二氮-9,9-螺二芴(sb)配体的三齿磷铱配合物Ir(tpit)(sb)Cl(tpitH2=亚磷酸三苯基酯),通过核磁共振氢谱和磷谱及高分辨质谱对其结构进行了确定。X射线单晶衍射分析表明,sb配体的存在扭曲了分子结构,有助于降低分子聚集及发光淬灭。与存在分子内π-π堆积的模型配合物Ir(tpit)(bpy)Cl(bpy=2,2′-联吡啶)对比进行了光电性能的研究。结果表明在聚甲基丙烯酸甲酯(质量分数1%)中配合物Ir(tpit)(sb)Cl的发光波长为512 nm,相对配合物Ir(tpit)(bpy)Cl的波长(520 nm)有了8 nm蓝移。配合物Ir(tpit)(sb)Cl的发光量子效率为30%,与配合物Ir(tpit)(bpy)Cl的94%相比有明显降低,说明了分子内π-π堆积作用在降低柔性基团非辐射跃迁率方面的重要作用。基于配合物Ir(tpit)(sb)Cl的有机电致发光器件,最大电流效率和外量子效率分别为14 cd·A-1和4.5%。而由于分子内π-π堆积作用,基于配合物Ir(tpit)(bpy)Cl器件的最大电流效率和外量子效率分别高达60 cd·A-1和18.2%。     

8-羟基喹啉衍生物铜（Ⅱ）配合物的合成及发光性能

设计合成了（E）-3-[2-（8-羟基喹啉基）-乙烯基]-N-对甲苯基咔唑8和（E）-3-[2-（8-羟基喹啉基）-乙烯基]-N．对甲氧苯基咔唑9及它们相应金属铜配合物10和11四个新的化合物,用UV—Vis,FT—IR,ESI—MS,FAB—MS,^1H NMR,^13C NMR和元素分析确认了化合物的结构．热重分析实验表明金属铜配合物10和11有很好的热稳定性,并把这两个金属铜配合物做成有机单层发光器件,都能发出稳定的蓝绿光．这两个发光器件的最大亮度分别是345cd／m^2,325cd／m^2,最大电流效率分别为0．68cd·A^-1,1．53cd·A^-1．     

一种含咔唑基哒嗪的新型金属铱电致磷光材料的合成与性能研究

合成了一种新型的以咔唑基哒嗪为配体的环金属化铱配合物Ir(pcpd)2(acac)(其中pcpd=3-(9-苯基-3-咔唑基)-6-甲基哒嗪,acac为乙酰丙酮),并以其作为发光体,制备了有机电致发光器件.其中结构为ITO/HIL001/HTL001/CBP:Ir(pcpd)2acac(12.3%)/TPBi/AlQ/LiF/Al的器件最大发光亮度19656cd/m2,最大效率14cd/A,发光峰值580nm.器件表征结果显示该配合物具有强磷光发光特性.     

含咔唑基团的新颖Re(Ⅰ)配合物的合成、表征和光电性质的研究

合成了一种含咔唑基团的新颖配合物Re(CO)_3CLL[L=1-乙基-2-(N-乙基－咔唑 并-4-)咪唑并[4.5-f]1,10-邻菲咯啉],通过元素分析、红外光谱、紫外光谱、~1H NMR、荧光光谱和循环伏安学对其进行了表征，制备了基于真空沉积膜的双层电致 发光器件：ITO/TPD (30 nm)/Re(Co)_3CLL (10 nm)/Mg_(0.9)Ag_(0.1) (110 nm) /Ag(60 nm)该器件启动电压为5V，在电压为9V时达到最大亮度113cd/m~2，发出桔 红色的光。     

含咔唑基团的新颖Re(Ⅰ)配合物的合成、表征和光电性质的研究

合成了一种含咔唑基团的新颖配合物Re(CO)_3CLL[L=1-乙基-2-(N-乙基－咔唑 并-4-)咪唑并[4.5-f]1,10-邻菲咯啉],通过元素分析、红外光谱、紫外光谱、~1H NMR、荧光光谱和循环伏安学对其进行了表征，制备了基于真空沉积膜的双层电致 发光器件：ITO/TPD (30 nm)/Re(Co)_3CLL (10 nm)/Mg_(0.9)Ag_(0.1) (110 nm) /Ag(60 nm)该器件启动电压为5V，在电压为9V时达到最大亮度113cd/m~2，发出桔 红色的光。     

磷光配合物(L)Re(CO)3Cl(L=α,α-diamine)的电化学性质和电子能级

通过循环伏安法对磷光发光材料(L)Re(CO)3Cl(L=α,α-diamine)系列配合物的电化学性质进行了研究.结合电子吸收、荧光光谱和量子化学计算确定了其能级结构,考察了二胺配体的取代基修饰对能级结构影响的规律.(L)Re(CO)3Cl系列配合物表现为单一的氧化(正电位方向)和多步还原(负电位方向)过程,分别反映了Re—Cl的杂化轨道组成的HOMO能级和二胺配体的π*轨道组成的LUMO能级的结构.与光谱数据比较发现,(L)Re(CO)3Cl配合物电化学数据主要反映的是三重态电子能级结构.     

侧链含金属铱配合物的电磷光白光聚合物

设计了一系列新型芴-咔唑电磷光共轭聚合物.通过共价键将双(2-(9,9-二乙基-9H-芴-2-基)吡啶-N,C2’)合铱(III)(Ir Fpy)接枝到3,6-二溴咔唑的N-烷基侧链,采用Suzuki缩聚反应合成了铱配合物(Ir Fpy)含量分别为0.25 mol%,0.5 mol%和1 mol%的聚合物PF-Ir Fpy.当引入的配合物Ir Fpy含量为1 mol%时,得到的共轭聚合物发射色坐标为(0.44,0.56)的黄光.随着接枝的铱配合物Ir Fpy在共轭聚合物中含量降低,作为主体的聚(9,9-二辛基芴)蓝光发射不能被完全淬灭,得到共聚物同时发射主体蓝光及客体铱配合物黄光的单分子白光共轭聚合物.共聚物发光器件结构为ITO/PEDOT:PSS(50 nm)/polymer+PBD(30 wt%)(80nm)/Ba(4 nm)/Al(150 nm)[氧化铟锡/苯磺酸掺杂聚乙烯基二氧噻吩/聚合物+(2,4-二苯-5-4-叔丁基苯-1,3,4-噁二唑)(w=30%)/钡/铝],基于共聚物PF-Ir Fpy025的器件流明效率为3.97 cd/A,色坐标为(0.34,0.34),非常接近于标准白光发射的色坐标(0.33,0.33).为了研究采用共聚物PF-Ir Fpy025和PF-Ir Fpy05制备的白光器件的光谱稳定性,测试了外加电压在8~13 V范围内的EL光谱,当外加电压从8 V升高到13 V时,两个EL器件都表现出了良好的EL光谱稳定性.研究结果表明,在共轭聚合物侧链上引入螯合金属铱配合物单元是实现高效、稳定的白光电致磷光器件的有效方法之一.     

9,9-二-(3-(9-苯咔唑基))-2,7-芘基芴的光电性质

芴类化合物作为有机电致发光材料近年来引起了人们的广泛关注, 其具有高亮度和高工作效率等性能. 本论文采用量子化学方法研究了一种新型的芴类发光材料, 9,9-二-(3-(9-苯咔唑基))-2,7-芘基芴的光电性质. 具体研究内容包括基态和激发态几何结构、前线分子轨道、能隙、电离能、电子亲和势、重组能以及吸收光谱和发射光谱等. 理论计算结果表明, 9,9-二-(3-(9-苯咔唑基))-2,7-芘基芴发射光谱为450.6 nm, 其在电致发光器件应用上是一种具有开发前景和实用价值的蓝光发光材料.     

High luminance phosphorescent organic light emitting diodes based on Re(I) complex

A novel Re(I) complex with the acenaphtho[1,2-b]pyrazino[2,3-f][1,10]phenanthroline (APPT) ligand Re(APPT)(CO)₃Br (abbreviated as Re-APPT) was used to fabricate organic light emitting diodes (OLEDs). From the electroluminescence (EL) spectra of the device at different bias voltages, it could be found that the EL maxima shifted approximately 30 nm. For OLEDs with 5% Re-APPT doped emissive layer, turn-on voltage of 6 V, maximum luminance of 7631 cd/m² and a current efficiency up to 2.36 cd/A were obtained. We suppose that a direct charge trapping took the dominant position in the EL process. Trapping contributed mostly to this relatively higher luminance.     

pH-Dependent spectroscopic and luminescent properties, and metal-ion recognition studies of Re(I) complexes containing 2-(2'-pyridyl)benzimidazole and 2-(2'-pyridyl)benzimidazolate

A series of Re(I) complexes, [Re(CO)(3)Cl(HPB)] (1), [Re(CO)(3)(PB)H(2)O] (2), [Re(CO)(3)(NO(3))(PB-AuPPh(3))] (3), and [Re(CO)(3)(NO(3))(PB)Au(dppm-H)Au](2) (4) [HPB = 2-(2'-pyridyl)benzimidazole; dppm = 2,2'-bis(diphenylphosphinomethane)], have been synthesized and characterized by X-ray diffraction. Complex 1, which exhibits interesting pH-dependent spectroscopic and luminescent properties, was prepared by reacting Re(CO)(5)Cl with an equimolar amount of 2-(2'-pyridyl)benzimidazole. The imidazole unit in complex 1 can be deprotonated to form the imidazolate unit to give complex 2. Addition of 1 equiv of AuPPh(3)(NO(3)) to complex 2 led to the formation of a heteronuclear complex 3. Addition of a half an equivalent of dppm(Au(NO(3)))(2) to complex 2 yielded 4. In both 3 and 4, the imidazolate unit acts as a multinuclear bridging ligand. Complex 4 is a rare and remarkable example of a Re(2)Au(4) aggregate in combination with μ(3)-bridging 2-(2'-pyridyl)benzimidazolate. Finally, complex 2 has been used to examine the Hg(2+)-recognition event among group 12 metal ions. Its reversibility and selectivity toward Hg(2+) are also examined.     

Reactions of the Dirhenium(II) Complexes Re(2)X(4)(&mgr;-dppm)(2) (X = Cl, Br; dppm = Ph(2)PCH(2)PPh(2)) with Isocyanides. 11.(1) A Triply Bonded Dirhenium Complex Containing a Labile Acetonitrile Ligand. Synthesis, Structural Characterization, and Reactivity of [(XylNC)(CH(3)CN)ClRe(&mgr;-dppm)(2)ReCl(2)(CO)]O(3)SCF(3)

The reaction of the open bioctahedral form of Re(2)Cl(4)(&mgr;-dppm)(2)(CO)(CNXyl) (1), where XylNC = 2,6-dimethylphenyl isocyanide, with TlO(3)SCF(3) in the presence of acetonitrile proceeds with retention of stereochemistry at the dirhenium unit to afford the complex [Re(2)Cl(3)(&mgr;-dppm)(2)(CO)(CNXyl)(NCCH(3))]O(3)SCF(3) (3). The single-crystal X-ray structure determination of 3 shows that a Re&tbd1;Re bond is retained (the Re-Re distance is 2.378(3) ?) and that it is the chloride ligand trans to the XylNC ligand of 1 which is labilized. Complex 1 reacts with TlO(3)SCF(3) in a noncoordinating solvent to produce the unsymmetrical complex [Re(2)Cl(3)(&mgr;-dppm)(2)(CO)(CNXyl)]O(3)SCF(3) (2), through loss of this same chloride ligand of 1 and CO transfer from the adjacent Re center. The acetonitrile ligand of 3 is very labile and is readily displaced by XylNC and t-BuNC, with retention of stereochemistry, to produce complexes of stoichiometry [Re(2)Cl(3)(&mgr;-dppm)(2)(CO)(CNXyl)(CNR)]O(3)SCF(3) (R = Xyl, 4a; R = t-Bu, 4b). In a noncoordinating solvent, the nitrile ligand of 3 is lost and 2 is formed following CO transfer; this conversion is reversed upon the reaction of 2 with acetonitrile. When 3 is treated with CO, the acetonitrile ligand is again displaced, but in this instance the reaction is accompanied by a structure change to produce an edge-sharing bioctahedral complex of the type [Re(2)(&mgr;-CO)(&mgr;-Cl)(&mgr;-dppm)(2)Cl(2)(CO)(CNXyl)]O(3)SCF(3) (5).     

Metal-induced tautomerization of p- to o-quinone compounds: experimental evidence from CuI and ReI complexes of azophenine and DFT studies

Azophenine (7,8-diphenyl-2,5-bis(phenylamino)-p-quinonediimine, L(p)) reacts with [Cu(PPh3)4](BF4) or [Re(CO)(5)Cl] to yield the (Ph3P)(2)Cu(+) or [(OC)(3)ClRe] complex of the tautomeric form 7,8-diphenyl-4,5-bis(phenylamino)-o-quinonediimine, L(o), as evident from structure determinations and from very intense metal-to-ligand charge transfer (MLCT) transitions in the visible region. Time-dependent DFT (TD-DFT) calculations on model complexes [(N intersection N)Re(CO)(3)Cl] confirm the spectroscopic results, showing considerably higher oscillator strengths of the MLCT transition for the o-quinonediimine complexes in comparison to compounds with N intersection N=1,4-dialkyl-1,4-diazabutadiene. The complexes are additionally stabilized through hydrogen bonding between two now ortho-positioned NHPh substituents and one fluoride of the BF(4) (-) anion (Cu complex) or the chloride ligand (Re complex). DFT Calculations on the model ligands p-quinonediimine or 2,5-diamino-p-quinonediimine and their ortho-quinonoid forms with and without Li(+) or Cu(+) are presented to discuss the relevance for metal-dependent quinoproteins.     

Synthesis, characterization and spectroscopic properties of 1,2-diiminetricarbonylrhenium(I)chloride complexes with o-benzoquinone diimines as ligands

The novel organometallic complexes Re(BQDI---R)(CO)₃Cl with BQDI---R=4,5-substituted o-benzoquinone diimines (R=H, Me, OMe, Cl) have been prepared and characterized by elemental analysis, IR, MS and ¹H-NMR spectroscopic methods. Their electronic spectra display a long-wavelength absorption band which can be ascribed to a metal-to-ligand charge transfer (MLCT) transition from Re(I) to the low-lying π*-orbitals of the o-benzoquinone diimine ligand, even though a significant degree of metal–ligand orbital mixing is occurring. The energy of this absorption band correlates very well with the nature of the substituents R in the 4,5-position of BQDI---R. In solvent series of decreasing polarity, the MLCT absorption maximum is shifted to longer wavelengths (negative solvatochromism). None of the Re(BQDI---R)(CO)₃Cl complexes studied is photoluminescent at 298 or 77 K.     

The effect of reduction on rhenium(I) complexes with binaphthyridine and biquinoline ligands: a spectroscopic and computational study

A number of rhenium complexes with binaphthyridine and biquinoline ligands have been synthesized and studied. These are [Re(L)(CO)3Cl] where L = 3,3'-dimethylene-2,2'-bi-1,8-naphthyridine (dbn), 2,2'-bi-1,8-naphthyridine (bn), 3,3'-dimethylene-2,2'-biquinoline (dbq), and 3,3'-dimethyl-2,2'-biquinoline (diq). This series represents ligands in which the electronic properties and steric preferences are tuned. These complexes are modeled using density functional theory (DFT). An analysis of the resonance Raman spectra for these complexes, in concert with the vibrational assignments, reveals that the accepting molecular orbital (MO) in the metal-to-ligand charge transfer (MLCT) transition is the LUMO and causes bonding changes at the inter-ring section of the ligand. The electronic absorption spectroelectrochemistry for the reduced complexes of [Re(dbn)(CO)3Cl], [Re(dbq)(CO)3Cl], and [Re(diq)(CO)3Cl] suggest that the singly occupied MO is delocalized over the entire ligand structure despite the nonplanar nature of the diq ligand in [Re(diq)(CO)3Cl]. The IR spectroelectrochemistry for [Re(dbn)(CO)3Cl], [Re(dbq)(CO)3Cl], and [Re(bn)(CO)3Cl] reveal that reduction lowers the CO ligand vibrational frequencies to a similar extent in all three complexes. The substitution of naphthyridine for quinoline has little effect on the nature of the singly occupied MO. These data are supported by DFT calculations on the reduced complexes, which reveal that the ligands are flattened out by reduction: This may explain the similarity in the properties of the reduced complexes.     

Synthesis and characterisation of luminescent rhenium tricarbonyl complexes with axially coordinated 1,2,3-triazole ligands

A series of 1-alkyl-4-aryl-1,2,3-triazoles (1-methyl-4-phenyl-1,2,3-triazole (1a); 1-propyl-4-phenyl-1,2,3-triazole (1b); 1-benzyl-4-phenyl-1,2,3-triazole (1c); 1-propyl-4-p-tolyl-1,2,3-triazole (1d)) have been prepared through a one-pot procedure involving in situ generation of the alkyl azide from a halide precursor followed by copper catalysed alkyne/azide cycloaddition (CuAAC) with the appropriate aryl alkyne. Cationic Re(I) complexes [Re(bpy)(CO)(3)(1a-d)]PF(6) (2a-d) were then prepared by stirring [Re(bpy)(CO)(3)Cl] with AgPF(6) in dichloromethane in the presence of ligands 1a-d. X-ray crystal structures were obtained for 2a and 2b. In the solid state, 2a adopts a highly distorted geometry, which is not seen for 2b, in which the plane of the triazole ligand tilts by 13° with respect to the Re-N bond as a result of a π-stacking interaction between the Ph substituent and one of the rings of the bpy ligand. This π-stacking interaction also results in severe twisting of the bpy ligand. Infrared spectra of 2a-d exhibit ν(CO) bands at ～2035 and ～1926 cm(-1) suggesting that these ligands are marginally better donors than pyridine (ν(CO) = 2037, 1932 cm(-1)). The complexes are luminescent in aerated dichloromethane at room temperature with emission maxima at 542 to 552 nm comparable to that of the pyridine analogue (549 nm) and blue shifted relative to the parent chloride complex. Long luminescent lifetimes are observed for the triazole complexes (475 to 513 ns) in aerated dichloromethane solutions at room temperature.     

Synthesis,crystal structure,and photoelectric properties of Re(CO)(3)ClL (L = 2-(1-ethylbenzimidazol-2-yl)pyridine)

A novel Re(I) complex, Re(CO)(3)ClL (L = 2-(1-ethylbenzimidazol-2-yl)pyridine), has been synthesized and structurally characterized by single-crystal X-ray diffraction analysis. Crystal data for C(17)H(13)ClN(3)O(3)Re: space group, orthorhombic, Pbca; a = 12.713(6) A; b = 15.103(7) A; c = 18.253(8) A; Z = 8. Stable vacuum vapor deposition of the Re complex has been verified by UV-vis and infrared spectroscopy. A two-layer electroluminescent device with configuration of ITO/TPD/Re(CO)(3)ClL/Mg(0.9)Ag(0.1)/Ag has been fabricated, which gave a turn-on voltage of as low as 3 V and a maximum luminance of 113 cd/m(2) at a bias voltage of 10.5 V, and confirmed that the Re complex can function as a bright orange-red emitter and an electron transport material in an electroluminescent device.     

Rhenium-to-benzoylpyridine and rhenium-to-bipyridine MLCT excited states of fac-[Re(Cl)(4-benzoylpyridine)(2)(CO)(3)] and fac-[Re(4-benzoylpyridine)(CO)(3)(bpy)](+): a time-resolved spectroscopic and spectroelectrochemical study

The lowest allowed electronic transition of fac-[Re(Cl)(CO)(3)(bopy)(2)] (bopy = 4-benzoylpyridine) has a Re --> bopy MLCT character, as revealed by UV-vis and stationary resonance Raman spectroscopy. Accordingly, the lowest-lying, long-lived, excited state is Re --> bopy (3)MLCT. Electronic depopulation of the Re(CO)(3) unit and population of a bopy pi orbital upon excitation are evident by the upward shift of nu(CO) vibrations and a downward shift of the ketone nu(C=O) vibration, respectively, seen in picosecond time-resolved IR spectra. Moreover, reduction of a single bopy ligand in the (3)MLCT excited state is indicated by time-resolved visible and resonance Raman (TR(3)) spectra that show features typical of bopy(*)(-). In contrast, the lowest allowed electronic transition and lowest-lying excited state of a new complex fac-[Re(bopy)(CO)(3)(bpy)](+) (bpy = 2,2'-bipyridine) have been identified as Re --> bpy MLCT with no involvement of the bopy ligand, despite the fact that the first reduction of this complex is bopy-localized, as was proven spectroelectrochemically. This is a rare case in which the localizations of the lowest MLCT excitation and the first reduction are different. (3)MLCT excited states of both fac-[Re(Cl)(CO)(3)(bopy)(2)] and fac-[Re(bopy)(CO)(3)(bpy)](+) are initially formed vibrationally hot. Their relaxation is manifested by picosecond dynamic shifts of nu(C(triple bond)O) IR bands. The X-ray structure of fac-[Re(bopy)(CO)(3)(bpy)]PF(6).CH(3)CN has been determined.