镱(Ⅲ)卟啉配合物的合成、结构表征和近红外光谱研究

合成了5个meso-位和β-位具有不同取代基的Yb(Ⅲ)卟啉配合物(2a~2e), 并对其结构进行了表征; 研究了配合物的可见光谱和近红外光谱性质, 测得了相关的量子产率和荧光寿命. 研究结果表明, 此类中性单核Yb(Ⅲ)卟啉配合物由于Yb³⁺的存在, 导致卟啉配体发生π→π*跃迁, 并将吸收的可见光能量传递给Yb³⁺的激发态, 使得配合物在近红外光区有很强的发光, 且meso-位为供电子基团的Yb(Ⅲ)卟啉配合物的发光效率比含吸电子基团的Yb(Ⅲ)卟啉配合物高, 而β-位溴化的Yb(Ⅲ)卟啉配合物的发光效率较差.     

一类[Os(II)(CO)3(tfa)(L)](L=O^O,O^N,N^N)配合物的结构和光谱特征

采用密度泛函理论以及B3LYP方法和单激发组态相互作用(CIS)方法分别优化了一系列[Os(II)(CO)3(tfa)(L)](tfa为三氟乙酸; L=O^O(1), O^N(2), N^N(3), 其中O^O为六氟乙酰丙酮, O^N为羟基喹啉, N^N为3-(三氟甲基)-5-(2-吡啶基)吡唑)配合物的基态和激发态结构. 利用含时密度泛函理论(TD-DFT)结合极化连续溶剂化模型(PCM)计算了配合物在CH2Cl2溶液中的吸收和发射光谱. 研究结果表明, 优化得到的几何结构参数和相应的实验值符合得非常好, 激发态几何构型相对基态变化较小, 这与实验上观察到的较小的斯托克斯频移现象一致. 配合物1-3的最低能吸收分别在342、431和329 nm, 其磷光发射分别在521、638 和488 nm. 配合物1-3的最高占据分子轨道和最低空轨道主要表现为L配体的π和π*轨道特征, 所以它们的最低能吸收归属于π-π*电荷跃迁, 并混有少量的金属到配体的电荷跃迁(MLCT)和配体之间电荷跃迁(LLCT)微扰, 且其高能吸收也表现为配体内部(IL)和配体间(LL)的电荷跃迁. 此外, 它们的磷光发射和吸收有相似的跃迁特征.     

樟脑型β-二酮环金属铂配合物的电子光谱和二阶非线性光学性质的DFT研究

对标题化合物分子的理论研究表明,樟脑型β-二酮环金属铂配合物分子由基态到第一,第二激发态的π→π^*跃迁伴随MLCT电荷转移。β-二酮羰基环上引入供电基-CH₃,-C₆H₅与吸电基-CF₃,-C₃F₇的最大吸收波长分别位于374～410 nm范围,位于近紫外区。β-二酮羰基环上和配体苯环上引入供电子基团,樟脑型β-二酮环金属铂配合物分子显示更良好的非线性光学性质。     

折叠型双银配合物电子结构与相关性质

在密度泛函B3LYP/LanL2DZ的水平上,对具有π-π弱相互作用调控的折叠型银配合物Ag₂(MPTQ)₂²⁺进行计算研究。探讨该配合物的电子结构、成键特征、π-π弱相互作用机理、电荷布居及其相关性质。计算结果表明,Ag…Ag之间存在弱的直接相互作用,HOMO主要布居在配体中芳香环的σ-p轨道、S的σ-p轨道及与S相连的C12的S轨道上,LUMO主要布居在配体中芳香环的π^*-p轨道上,基态电子光谱主要是配体中的n→π^*跃迁产生的电荷转移光谱。论文还讨论了分子间π-π弱相互作用的本质及活性部位等。计算结果能较好地解释实验现象与规律。     

外围取代基团对卟啉铂(Ⅱ)配合物发光性能的影响

设计合成了具有不同外围取代基的卟啉铂(Ⅱ)配合物PtTEMP, PtTBMP, PtOMPP和PtDMPP, 并对其结构和光电性能进行了表征. 晶体结构分析结果表明, 这些卟啉铂(Ⅱ)配合物具有较理想的平面配位构型, β-位叔丁基的引入有效抑制了分子间的π-π相互作用. 外围取代基几乎不影响配合物的吸收和发光性质, 最大发射峰位于646~656 nm之间, 为配体中心的 ³π^*-π磷光发射. 空间位阻效应更强的叔丁基取代配合物(PtTBMP)的溶液态荧光量子效率和外量子效率最高, 分别为0.58和6.3%. 3个甲氧基取代的PtDMPP的发光效率优于2个甲氧基取代的PtOMPP, 二者的溶液态荧光量子效率分别为0.36和0.29, 外量子效率分别为2.4%和1.7%.     

杯[4]芳烃对单糖及嘧啶衍生物的分子识别和分子开关

用AM1和INDO/SCI方法对八羟基杯[4]芳烃与单糖及嘧啶衍生物形成的超分子体系进行理论研究,结果表明,主体通过CH-π相互作用对单糖类进行分子识别,尤其对赤藓糖识别效果更好;主体与嘧啶没有明显的π-π堆砌作用,但能识别含吸电子基团的嘧啶衍生物,据此可设计酸碱调控的分子开关.讨论了配合物的UV谱带与主体相比发生红移的原因.     

外围取代基团对卟啉铂(Ⅱ)配合物发光性能的影响

设计合成了具有不同外围取代基的卟啉铂(Ⅱ)配合物PtTEMP,PtTBMP,PtOMPP和PtDMPP,并对其结构和光电性能进行了表征.晶体结构分析结果表明,这些卟啉铂(Ⅱ)配合物具有较理想的平面配位构型,β-位叔丁基的引入有效抑制了分子间的π-π相互作用.外围取代基几乎不影响配合物的吸收和发光性质,最大发射峰位于646~656 nm之间,为配体中心的3π*-π磷光发射.空间位阻效应更强的叔丁基取代配合物(PtTBMP)的溶液态荧光量子效率和外量子效率最高,分别为0.58和6.3%.3个甲氧基取代的PtDMPP的发光效率优于2个甲氧基取代的PtOMPP,二者的溶液态荧光量子效率分别为0.36和0.29,外量子效率分别为2.4%和1.7%.     

BPh-2(mqp)的电子结构和光谱性质的含时密度泛函理论研究

采用abinitioHF和DFTB3LYP方法,对配合物BPh₂(mqp)基态结构进行优化,分析了前线分子轨道特征和能级分布.用abinitioCIS方法优化体系激发态结构.用含时密度泛函理论(TD-DFT)对BPh₂(mqp)的电子光谱进行了研究.结果发现,该物质是配体发光配合物,其发光源于mqp配体内π^*→π的电子跃迁.这表明在mqp配体上进行修饰,可有效地影响配合物前线分子轨道分布,达到调整发光波段的目的.     

四配位铂磷光发射体结构与光物理性质关系的理论研究

定量理解光物理过程对于开发新型高效发射极至关重要. 优化提升二价铂配合物磷光量子效率是提升基于金属铂有机发光二极管发光效率的关键. 本文借助密度泛函理论计算, 探讨了一类平面四齿配位二价铂配合物磷光辐射的微观机制, 包括自旋轨道耦合积分、 辐射寿命、 速率常数、 跃迁偶极矩和隙间蹿跃通道. 综合研究发现, 沿着N→Pt方向推电子, 可有效屏蔽非辐射跃迁过程, 从而提升磷光发射效率. 本文将为高效发射器的分子工程学设计提供必要的指导.     

交联PPE固态π-π堆积效应的研究

本文合成了数种乙烯基封端及结构规整无侧基的PPE齐聚物, 通过端乙烯基的交联反应, 制备了柔性端基交联的三维PPE交联网络. 通过FTIR, PL, WXRD分析, 研究了乙烯基交联程度和热处理条件等对交联PPE π-π堆积效应的影响, 成功地制备了固态无π-π堆积和单色性好的紫/蓝光发光材料.     

Cyclometalated platinum(II) complexes with sterically bulky camphor-derived groups as β-diketonate ancillary ligand: a new route to efficiently reducing π-π interactions and Pt-Pt interactions

A new series of mono-cyclometalated square planar platinum(II) complexes have been synthesized and the single-crystal X-ray structures of complex 1 and 2 have been determined. The complexes have the general formula ppyPt(O∧O), where ppy is 2-phenylpyridyl, and O∧O is β-diketonate ancillary ligands with the acyl substituent group in position 3 of (D)-(+)-camphor. Although, like the many Pt(II) complexes with square-planar geometry, these complexes have plane stacking modes in crystal structure, the sterically bulky camphor-derived groups compel extensive slipping of the molecular stacking planes, resulting in the negligible overlapping of the aromatic ring fragments between molecules and the considerable Pt-Pt distance. The resolved spectra and a little shifted emission in solid state of complexes show that there is significant reduction of π-π interactions and Pt-Pt interactions, and suggest these complexes may be good candidates for doped phosphorescent organic light emitting diodes (PhOLEDs) and even for nondoped PhOLEDs.     

Synthesis and characterization of amidate bridged dimeric and oligomeric platinum complexes having short platinum-platinum interactions

A number of pivalamidate bridged dinuclear [PtII2(RNH2)4(NHCOtBu)2]2+, [PtIII2LL (RNH2)4(NHCOtBu)2]n+ (2RNH2 = 2NH3, 1,2-ethylenediamine, 1,2-diaminocyclohexane; L, L' = NO3-, H2O, or ketonate), trinuclear [{PtII(dap)(NHCOtBu)2}2PdIII]3+ (dap = 1,2-diaminopropane), tetranuclear [{PtII2(NH3)2(DACH)(NHCOtBu)2}2]4+ (DACH = 1,2-diaminocyclohexane), pentanuclear [{Pt2(C5H7O)(NH3)2Cl2(NHCOtBu)2}2PtCl4], and hexanuclear [Pt2(NH3)2(en)(NHCOtBu)2Pt(NO2)4]2 platinum complexes containing Pt(II)-Pt(II), Pt(II)-Pt(III), Pt(II)-Pd(III), and Pt(III)-Pt(III) interactions have been prepared and structurally characterized. The Pt-Pt interactions are characteristic of covalent, dative, or orbital symmetric Pt-Pt bonds. The dimeric Pt(III) complexes are able to activate C-H bonds of ketones to afford ketonate platinum(III) complexes. The Pt-Pt bonds are either doubly amidate-bridged or ligand unsupported. Their distances are 2.99-3.22 A for Pt(II)-Pt(II), 2.59-2.72 A for Pt(III)-Pt(III), 2.98 A for Pt(II)-Pt(III), and 2.66 A for Pt(II)-Pd(III) bonds depending on the oxidation states of the two metals and the ancillary ligands.     

A trinuclear Pt(II) compound with short Pt-Pt-Pt contacts. An analysis of the influence of pi-pi stacking interactions on the strength and length of the Pt-Pt bond

In this work we report the first example of a trinuclear Pt(II) complex with Pt-Pt-Pt bonds that are not facilitated by direct intervention of bridging ligands but are partially held by the attractive pi-pi stacking interaction between the phenyl units of the 4,4'-dimethyl-2,2'-bipyridyl ligands. The effect of the pi-pi stacking interactions on the strength and length of the Pt-Pt bond has been discussed using reduced models of the interacting moieties in which the aromatic rings have been removed. The nature of the Pt-Pt bonds has been studied through energy decomposition and atoms-in-molecules analyses. The results indicate that the relatively strong (about 40 kcal mol(-1)) Pt-Pt metallic bond has similar covalent and ionic contributions.     

Noncovalent interactions between cytosine and SWCNT: curvature dependence of complexes via pi...pi stacking and cooperative CH...pi/NH...pi

Fragments of C24H12, adapted from a variety of armchair [(n,n), (n = 5, 7, and 8)] and zigzag [(m,0) (m = 8, 10, and 12)] single-walled carbon nanotube (SWCNT), are used to model corresponding SWCNTs with different diameters and electronic structures. The parallel binding mainly through pi...pi stacking interaction, as well as the perpendicular binding via cooperative NH...pi and CH...pi between cytosine and the fragments of SWCNT have been extensively investigated with a GGA type of DFT, PW91LYP/6-311++G(d,p). The eclipsed tangential (ET) conformation with respect to the six-membered ring of cytosine and the central ring of SWCNT fragments is less stable than the slipped tangential (ST) conformation for the given fragment; perpendicular conformations with NH2 and CH ends have higher negative binding energy than those with NH and CH ends. At PW91LYP/6-311++G(d,p) level, two tangential complexes are less bound than perpendicular complexes. However, as electron correlation is treated with MP2/6-311G(d,p) for PW91LYP/6-311++G(d,p) optimized complexes, it turns out there is an opposite trend that two tangential complexes become more stable than three perpendicular complexes. This result implies that electron correlation, a primary source to dispersion energy, has more significant contributions to the pi...pi stacking complexes than to the complexes via cooperative NH...pi and CH...pi interactions. In addition, it was found for the first time that binding energies for two tangential complexes become more negative with increasing nanotube diameter, while those for three perpendicular complexes have a weaker dependence on the curvature; i.e., binding energies are slightly less and less negative. The performance of a novel hybrid DFT, MPWB1K, was also discussed.     

Synthesis, structural characterization, and photophysical properties of palladium and platinum(II) complexes containing 7,8-benzoquinolinate and various phosphine ligands

A series of mononuclear cyclometalated benzo[h]quinolinate platinum and palladium(II) complexes with phosphine ligands, namely, [M(bzq)ClL] (L=PPh2H, Pt 1, Pd 2; PPh2CCPh, Pt 3, Pd 4), [Pt(bzq)(PPh2H)(PPh2CCPh)]ClO4 5, [Pt(bzq)(PPh2C(Ph)=C(H)PPh2)]ClO4 6, and [Pt(bzq)(CCPh)(PPh2CCPh)] (7a, 7b), were synthesized. The X-ray crystal structures of 1, 6.CH3COCH3.1/2CH3(CH2)4CH3, and 7b.CH3COCH3 have been determined. In 1, the metalated carbon atom and the P atom are mutually cis, whereas in 7b they are trans located. For complex 6, C and N are crystallographically indistinguishable. Reaction of [Pt(bzq)(mu-Cl)]2 with PPh2H and excess of NEt3 leads to the phosphide-bridge platinum dimer [Pt(bzq)(mu-PPh2)]2 8 (X-ray). Moderate pi-pi intermolecular interactions and no evident Pt-Pt interactions are found in 1, 7b, and in 8. All of the complexes exhibit absorption bands at high energy due to the intraligand transitions (1IL pi --> pi) and absorptions at lower energy which are attributed to MLCT (5d) pi --> pi (CLambdaN) transition. Platinum complexes show strong luminescence in both solid state and frozen solutions. The influence of the coligands on the photophysics of the platinum complexes has been examined by absorption and emission spectroscopy.     

Novel [2]catenane structures introducing communication between transition metal centers via pi...pi interactions

[2]Catenane systems containing copper(II) and nickel(II) as metal centers have been self-assembled using tetraazamacrocyclic complexes and benzo-24-crown-8 as building blocks. A variety of methods, including X-ray crystallography, ESI mass spectrometry, (13)C and (1)H NMR, and electrochemistry, were applied to characterize these new face-to-face bismacrocyclic systems. Weak pi...pi interactions introduced by interlocking transition metal complexes with benzocrown moieties were shown to increase the communication (cooperativity) of metal centers. Introduction of the benzocrown increases the stability of the mixed valence state of the macrocyclic complex, which is reflected in high values of conproportionation constants. Moreover, this effect was found to be stronger than that obtained by shortening the length of the spacer between the two tetraazamacrocyclic subunits in the parent bismacrocycles. The extent of communication is larger for the nickel catenane than for the copper one.     

Metal(II) Complexes Based on Imidazo[4, 5‐f]‐1, 10‐phenanthroline and Bridging Dicarboxylato Ligands: Synthesis,Characterization and Photoluminescence

Eight metal(II) complexes based on imidazo[4, 5‐f]‐1, 10‐phenanthroline (HIMP) and bridging dicarboxylato ligands such as 4, 4′‐biphenyldicarboxylic acid (H₂BPDC), 1, 4‐benzenedicarboxylic acid (H₂BDC), thiophene‐2, 5‐dicarboxylic acid (H₂TDC), and 2, 6‐naphthalenedicarboxylic acid (H₂NDC) were hydrothermally synthesized and structurally characterized by single‐crystal X‐ray diffraction. Complexes 1 , 3 , 6 , and 7 are molecular dinuclear metal complexes. Complexes 2 , 4 , and 5 exhibit chain‐like structures. Compound 8 shows a novel 3D architecture, in which Zn^II dimers are connected by four NDC^2– anions. In the metal(II) complexes, HIMP exhibits a similar chelating coordination mode. Different π ··· π stacking interactions are observed in the complexes. The emission of HIMP is completely quenched in complexes 1 – 4 due to the strong π ··· π stacking interactions in the structures. Complexes 5 – 8 exhibit different photoluminescence properties. Firstly, we quantitatively investigated the effect of the strong HIMP–HIMP stacking interactions on the emission quenching of HIMP in the metal complexes. It was found that a higher extent of π ··· π stacking interactions in the complexes resulted in a higher extent of the emission quenching of HIMP. The introduction of aromatic conjugated carboxylate groups into metal(II)‐HIMP complexes changed the extent of the strong π ··· π stacking interactions in the structures and thus the photoluminescence properties of the complexes.     

Coordination complexes exhibiting anion...pi interactions: synthesis, structure, and theoretical studies

The polydentate ligand 2,4,6-tris(dipyridin-2-ylamino)-1,3,5-triazine (dpyatriz) in combination with the Cu(ClO 4) 2/CuX 2 salt mixtures (X (-) = Cl (-), Br (-), or N 3 (-)) leads to the formation of molecular coordination aggregates with formulas [Cu 3Cl 3(dpyatriz) 2](ClO 4) 3 ( 2), [Cu 3Br 3(dpyatriz) 2](ClO 4) 3 ( 3), and [Cu 4(N 3) 4(dpyatriz) 2(DMF) 4(ClO 4) 2](ClO 4) 2 ( 4). These complexes consist of two dpyatriz ligands bridged via coordination to Cu (II) and disposed either face-to-face in an eclipsed manner ( 2 and 3) or parallel and mutually shifted in one direction. The copper ions complete their coordination positions with Cl (-) ( 2), Br (-) ( 3), or N 3 (-), ClO 4 (-), and N, N-dimethylformamide (DMF) ( 4) ligands. All complexes crystallize together with noncoordinate ClO 4 (-) groups that display anion...pi interactions with the triazine rings. These interactions have been studied by means of high level ab initio calculations and the MIPp partition scheme. These calculations have proven the ClO 4 (-)...[C 3N 3] interactions to be favorable and have revealed a synergistic effect from the combined occurrence of pi-pi stacking of triazine rings and the interaction of these moieties with perchlorate ions, as observed in the experimental systems.     

Strong magnetic interactions through weak bonding interactions in organometallic radicals: combined experimental and theoretical study

The magnetic properties of a series of three neutral radical organometallic complexes of general formula [CpNi(dithiolene)]. have been investigated by a combination of X-ray crystal structure analysis and magnetic susceptibility measurements, while the assignment of the exchange coupling constants to the possible exchange pathways has been accomplished with the help of calculations based on density functional theory (DFT). The syntheses and X-ray structures of [CpNi(adt)] (adt=acrylonitrile-2,3-dithiolate) and [CpNi(tfd)] (tfd=1,2-bis(trifluoromethyl)ethene-1,2-dithiolate) complexes are described, while [CpNi(mnt)] (mnt=maleonitriledithiolate) was reported earlier. In the three complexes, we observed strong antiferromagnetic coupling that could not be explained solely by short SS intermolecular contacts. Our calculations indicated that spin density in these complexes is strongly delocalized on the NiS2 moiety, with up to 20% on the Cp ring. As a consequence, CpCp and Cpdithiolene overlap interactions have been identified as responsible for antiferromagnetic couplings. The [CpNi(adt)] complex thus has a value J=-369.5 cm(-1) for an exchange interaction through a pi stacking due to the CpCp overlap.     

Azobenzene palladium(II) complexes with β-diketones

A procedure has been developed for the synthesis of cyclometalated azobenzene palladium(II) complexes [Pd(O^O)Azb], where Azb^– is deprotonated azobenzene and (O^O)^– is deprotonated β-diketone (acetylacetone, thenoyltrifluoroacetone, benzoylacetone, or dibenzoylmethane). Electronic absorption spectra and electrochemical behavior of the synthesized complexes have been studied. It has been found that the lowest unoccupied molecular orbital of the complexes is contributed most by the π* orbital of azobenzene, and the highest occupied molecular orbital, by the palladium d orbital.