[Au(PH3)]+修饰的芳香基炔基配合物发光机制的从头计算研究

用从头计算法研究H3PAuC≡CPh(a), H3PAu(C≡C-1,4-C6H4)Ph(b)和H3PAu(C≡C-1,4-C6H4)C≡CPh(c) 3种Au(Ⅰ)配合物的磷光发光性质, 使用MP2和CIS方法分别优化配合物的基态和激发态的几何结构. 计算结果表明, 激发态的电子跃迁减弱了Au与配体的成键作用. 由计算得出3种Au(Ⅰ)配合物的最低能量磷光发射光谱分别为530, 610和615 nm, 皆由A3A′→1A′产生, 属于Au(6p)→C(2p)的电荷转移(MLCT)修饰下的pπ*(C≡C, )→pπ(C≡C, )跃迁本质, 并伴有Au(6p)→Au(5d)的金属中心电荷转移(MCCT)性质. 随着分子增长, 其激发态轨道中Au的p轨道成分减少, 相应的最低能量磷光发射的波长红移.     

一类新型苯基吡唑铱(Ⅲ)配合物的电子结构及光谱性质

为了探索新型苯基吡唑铱(Ⅲ)配合物的电子结构与光谱性质之间的关系,采用密度泛函理论(DFT)优化了铱金属配合物(ppz)2Ir(BTZ)(1)和(ppz)2Ir(4-TfmBTZ)(2)的基态与激发态的几何结构.通过含时密度泛函理论(TD-DFT)方法计算了配合物的吸收和发射谱,指认了它们的跃迁性质.和Ir(ppz)3相比,通过引入新的辅助配体并对其修饰实现了发光颜色的调节.配合物1和2的最低能磷光发射可指认为3MLCT/3LLCT/3ILCT[π*(R-BTZ)→d(Ir)+π(ppz)+π(R-BTZ)]的电荷混合跃迁.此外,它们的磷光发射和吸收有相似的跃迁性质.MLCT主要发生在Ir(R-BTZ)片段而不是Ir(ppz)2片段.第二配体在此配合物的发光过程中起了主要作用.     

双核Au(Ⅰ)配合物[Y+]2[Au(i-mnt)]2(Y+=[n-Bu4N]+,K+,[Ph4As]+)发光机制的从头计算研究

用从头算方法研究[Au(i-mnt)]22-(i-mnt=i-marononitriledithiolate)的电子吸收和磷光发射性质,利用MP2和CIS方法分别优化了[Au(i-mnt)]22-基态和激发态几何结构.计算的基态Au(Ⅰ)—Au(Ⅰ)键长为0.2825nm,表明Au(Ⅰ)之间存在弱吸引作用.采用SCRF方法中IPCM模型模拟配合物在乙氰溶液中的行为,计算得到的最大吸收波长为315.5nm,指认X1Ag→A1Au来源于i-mnt配体内电荷转移跃迁.在436.2nm处得到具有B3Au→1Ag跃迁的磷光发射,指认为i-mnt配体内电荷转移和金属到配体电荷转移跃迁,与500nm乙氰溶液的发射相对应,为金属修饰的有机配体发光机制.     

[Os（PH3）2（CN）2（N^N）]配合物的溶剂化显色效应

采用HF/DFT的混合泛函PBE0和UPBE0优化了配合物[Os(PH3)2(CN)2(N^N)](其中N^N=2,2′-吡啶)的基态和激发态结构.在基态和激发态结构的基础上,利用含时密度泛函理论(TD-DFT)方法,结合极化连续介质(PCM)模型分别计算了它在二氯甲烷(1)、甲醇(2)、气态(3)和乙腈(4)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.在极性较大的溶剂(2和4)中Os—P(1)和Os—C(1)键较长,Os—N(3)键较短,溶剂的极性会影响配合物的电子云分布.配合物在1-4溶剂中的最低能吸收和发射均来自分子轨道68→71的激发,该激发被指认为[d(Os)+π(CN)+π(N^N)→π*(N^N)]的跃迁具有混合的MLCT/LLCT特征.配合物在1-4溶剂中的最低能吸收和发射分别在471,410,488和445nm以及598,536,634和545nm,表明随着溶剂极性的逐渐增大(3<1<4<2),最低能吸收和发射发生明显的蓝移.这显示出通过改变溶剂极性可以调节配合物的发光颜色.     

Ph3PAuX和Ph3AsAuX(X=C1,Br)的最低三重激发态

分子水平上的激发态理论研究能够用来解释分子材料的多色发光机理.采用单组态相瓦作用方法,计算研究了四种二配位的An(Ⅰ)配合物Ph3PAuCl,Ph3PAuBr,Ph3AsAuCl和Ph3AsAuBr的分子结构限制的三重激发态(T1a)和分子结构松弛的三重激发态(T1b)的分子结构与光物理性质.由于θ(PAuX)/θ(AsAuX)从180°扭曲到120°左右,T1b态的能量在单线态组态相互作用(CIS)水平上降低了0.805-1.124 eV,在密度泛函理论(DFT)水平上降低了0.820-0.947 eV.自然键轨道电荷布居数分析表明,在T1a态中两个单电子主要分布在一个苯基上,而在T1b态中两个单电子分布在PAuX/AsAuX上.因此,在晶体中观察到的较高能磷光归属于T1a态的苯基之间的3π*→1π电子跃迁,而较低能磷光主要起源于T1b态的Au的3σ*→1σ电子跃迁.     

作为Be2+磷光探针的含9-冠-3的铱配合物

以4′-(2-苯并噻唑基)苯并-9-冠-3(BTZ9C3)为主配体,用2,2′-联吡啶(bpy)及3-三氟甲基-5-(2′-吡啶基)-1,2-二唑(Hfppz)辅助配体分别合成了离子型铱配合物[Ir(BTZ9C3)2(bpy)]PF6(1)和中性铱配合物[Ir(BTZ9C3)2(fppz)](2)。配合物的结构通过核磁、高分辨质谱进行了表征,并测定了配合物1的单晶结构。对它们光物理性能的研究表明,2种配合物掺杂在PMMA中的发光为黄绿光发射,配合物1的发光波长为535 nm,配合物2的发光波长为541 nm,发光量子效率分别为10.8%,45.0%,发光寿命分别为3.01和2.58μs,为典型的磷光发射。通过循环伏安法测得配合物1和2的HOMO能级分别为-5.60和-5.35 eV。2种配合物对Be2+都有发光增强的选择性识别效果,化学计量比为1∶2,最低检测限低至6.0μmol·L-1。抗干扰能力方面,离子型配合物1的抗干扰能力较好,而中性配合物2受Al3+的干扰较大。     

以2，2′-联嘧啶为副配体的铱配合物的合成、晶体结构和发光性质研究

利用环金属配体2-(4',6'-二氟苯基)吡啶(dfppy)和副配体2,2'-联嘧啶(bpm)合成了一个铱配合物[Ir(dfppy)z(bpm)]Cl,通过1H NMR,质谱,元素分析及红外光谱对其进行了表征,并且测定了其晶体结构.同时利用得到的中间配合物[Ir(dfppy):(bpm)] [Ir(dfppy)2(Cl)2]n晶体结构讨论了配合物形成过程.对配合物[Ir(dfppy)2(bpm)]Cl的紫外可见吸收光谱和发光光谱的研究表明,其常温发射位于609 nm处,初步推测该磷光发射可能来自金属到配体的电荷转移(MLCT)跃迁和配体自身,π→π*跃迁(LC)的混合.     

三联吡啶Pt(Ⅱ)配合物的基态和激发态的理论研究

为了探究取代基对三联吡啶Pt(Ⅱ)配合物发光性质的影响, 采用MP2和CIS方法分别对配合物[Pt(trpy)C≡CC6H4R]+[trpy=2,2',6',2″-Terpyridine; R=NO2(1), Cl(2), H(3), CH3(4)]的基态和激发态的几何构型进行了优化, 通过TDDFT/B3LYP方法得到了这些化合物在二氯甲烷溶液中的磷光发射光谱以及它们的跃迁性质. 研究结果表明, 由于NO2的强吸引作用以及在C≡CC6H4NO2部分可能存在的电子共振结构, 化合物1的最低发射可以指认为Pt—C≡C→trpy(3MLCT/3LLCT) 的跃迁, 并且还有很大的一部分来自于π→π*(C6H4NO2) 跃迁的贡献, 而化合物3和化合物4由于含有给电子基团, 因此其最低发射仅仅是来自于3MLCT/3LLCT的跃迁. 但是并不是所有的取代基为吸电子基团时都能有类似的π→π*跃迁性质. 对于化合物2, Cl是仅次于NO2的吸电子取代基, 但是由于缺少电子共振的贡献, 它的跃迁性质却与化合物3和4相同. 另外, 激发态几何相对于基态几何没有发生太大的变化, 这与实验上所观察到的较小斯托克斯频移现象一致.     

利用吡啶衍生物主配体共轭效应调控铱配合物发光颜色(英文)

利用2-苯基吡啶及其衍生物为主配体、四苯基膦酰亚胺为辅助配体合成了3个铱配合物Ir(ppy)2tpip(Hppy:2-苯基吡啶,Htpip:四苯基膦酰亚胺)、Ir(npy)2tpip(Hnpy:2-(1-萘基)吡啶)和Ir(pnpy)2tpip(Hpnpy:2-(9-菲基)吡啶)。它们的结构通过1H NMR和MALDI-TOF质谱进行了表征,其中配合物Ir(ppy)2tpip还进一步通过晶体结构分析验证。主配体从苯环到萘环和菲环的改变增加了配合物的π共轭,减小了能级差,导致了3种配合物的磷光发射光谱从516 nm红移到600和633 nm(从绿光到红光),发光量子效率也从0.36增加到0.51和0.53。从量化计算的结果可以看出,这种共轭效应增加了主配体的电子密度,提高了配合物的LUMO能级。配合物结构和发射性质之间的关系规律为设计不同发光颜色的铱配合物提供了思路。     

三缺位Keggin结构磷钨酸甲基苯基硅衍生物[(C4H9)4N]3[α-A-PW9O34(C6H5SiCH3)3]的合成和表征

通过三缺位Keggin结构杂多阴离子[α-A-PW9O34]9-和二氯甲基苯基硅烷在乙腈溶液中反应,合成了一例结构新颖的甲基苯基硅衍生物[(C4H9)4N]3[α-A-PW9O34(C6H5SiCH3)3](1),并对其进行元素分析,红外光谱,紫外光谱,热分析和X-射线单晶衍射等表征。该配合物属于三方晶系,空间群为R3m,晶胞参数:a=2.261 3(2)nm,b=2.261 3(2)nm,c=1.797 6(4)nm,V=7.960 2(18)nm3,Z=3。在配合物中,阴离子[α-A-PW9O34(C6H5SiCH3)3]3-呈C3v对称,3个甲基苯基硅基团连接在三缺位的阴离子[α-A-PW9O34]9-表面,整个阴离子显示"开放结构"。     

Au(Ⅰ)电荷转移配合物光谱性质的从头算研究

过渡金属电荷转移配合物的电荷分离是光能转化为电能的光物理过程, 与配合物的电子结构密切相关. 采用从头算方法探索了双核Au(Ⅰ)配合物, cis-[Au2(SHCH2PH2)2]2+(1), cis-[Au2(SHCH2S)2](2) 和cis-[Au2(PH2CH2S)2](3)的电荷转移性质. 采用MP2计算得到基态的Au(Ⅰ)—Au(Ⅰ)距离分别为0.2972, 0.2888和0.2903 nm, 表明Au(Ⅰ)之间存在弱吸引作用; 电子激发使得配合物2和3的金属间的距离缩短了约0.016 nm, 而配合物1仅增长了0.002 nm. CIS方法预测配合物1~3的3A激发态分别产生383, 463和422 nm最低能发射, 具有金属中心(Metal-centered, MC)跃迁和分子内电荷转移(Intramolecular Charge Transfer, ICT)的混合性质.     

1-trimethylsilylphosphirane as a ligand and as a stable masked reagent for phosphirane

1-Trimethylsilylphosphirane, C2H4PSiMe3, has been prepared on a multi gram scale from P(SiMe3)3 via CICH2CH2P(SiMe3)2. C2H4PSiMe3 is readily susceptible to protonolysis forming the thermally unstable parent phosphirane, C2H4PH, in good yields. Reaction of C2H4PSiMe3 with fac-M(CO)3(CH3CN)3 (M = Cr, Mo) or [Fe(eta5-C5H5)(eta6-C6H6)](PF6) give rise tofac-M(CO)3(C2H4PSiMe3)3 and [Fe(eta5-C5H5)(C2H4PSiMe3)3](PF6) respectively. Protonolysis of the free or coordinated 1-trimethylsilylphosphirane readily causes P-Si cleavage to give rise to the parent C2H4PH or the respective complexes,fac-M(CO)3(C2H4PH)3 andfac-[Fe(eta5-C5H5)(C2H4PH)3](PF6) in situ. All new complexes are characterised by analytical and spectroscopic methods and the X-ray crystal structures of fac-Cr(CO)3(C2H4PSiMe3)3 and fac-Mo(CO)3(C2H4PH)3 have also been determined.     

烯丙基自由基(·C3H5)与氧气(O2)反应机理的理论计算

用量子化学计算方法对CH3CH=·CH与O2气的反应机理进行了理论研究, 在B3LYP/6-311G(d,p) 水平下优化稳定分子结构和寻找过渡态, 并在此构型的基础上, 采用CCSD(T)/6-311G(d,p)方法得到各驻点的高级单点能量. 找到主要路径R(CH3CH=·CH+O2)→m1(trans-CH3CH=CHOO)→m2(形成COO三元环)→m3(C—C键断裂,同时生成CH3CH—O—CHO)→P2(C—O键断裂生成CH3CHO+CHO); 并与C2H3等共轭体系进行了对比.     

From diphosphane to diphosphodiide gold(III) derivatives of 1,2-diphosphinobenzene

Treatment of 1,2-diphosphinobenzene with [Au(C6F5)3(tht)] leads to the diphosphane derivative [{Au(C6F5)3}(1,2-PH2C6H4PH2)] (1), which further reacts with other pentafluorophenylgold(III) reagents in the presence of acetylacetonate as deprotonating agent to afford phosphane-phosphide complexes. The noncyclic PPN[{Au(C6F5)3}2(1,2-PHC6H4PH2)] (2; PPN = bis(triphenylphosphine)iminium) has been shown to be a useful starting material for the synthesis of higher nuclearity cyclic or noncyclic diphosphide or even diphosphodiide derivatives through similar reactions. The crystal structures of the trinuclear anionic NBu4[{Au(C6F5)3}(1,2-PHC6H4PH){Au(C6F5)2Cl}{mu-Au(C6F5)2}] (3) and the hexanuclear [{Au(C6F5)3}(1,2-PC6H4P){Au(C6F5)3}{mu-M(dppe)M}2] (M = Au (12), Ag (13)) have been established by X-ray diffraction methods, the last complexes having a bicyclic ring containing three intramolecular interactions between the M(I) centres.     

Triple-decker-sandwich versus rice-ball structures for tris(benzene)dimetal derivatives of the first-row transition metals

Compounds of the type M(2)Bz(3) (Bz = benzene, C(6)H(6)) have been of interest since the related triple-decker mesitylenechromium sandwich (1,3,5-Me(3)C(6)H(3))(3)Cr(2) has been synthesized and characterized structurally by X-ray crystallography. Theoretical studies predict the lowest-energy M(2)Bz(3) structures of the early transition metals Ti, V, and Cr to be the triple-decker sandwiches trans-Bz(2)M(2)(η(6),η(6)-μ-C(6)H(6)) having quintet, triplet, and singlet spin states, respectively. In these structures, the central benzene ring functions as a hexahapto ligand to each metal atom. The singlet rice-ball cis-Bz(2)M(2)(μ-C(6)H(6)) structures with a 2.64-? Mn═Mn double bond or a 2.81-? Fe-Fe single bond are preferred for the central transition metals Mn and Fe. Singlet triple-decker-sandwich structures trans-Bz(2)M(2)(μ-C(6)H(6)) return as the lowest-energy structures for the late transition metals Co and Ni but with the central benzene ring only partially bonded to each metal atom. Thus, the lowest-energy cobalt derivative has a trans-Bz(2)Co(2)(η(3),η(3)-μ-C(6)H(6)) structure in which the central benzene ring acts as a trihapto ligand to each metal atom. Similarly, the lowest-energy nickel derivative has a trans-Bz(2)Ni(2)(η(2),η(2)-μ-C(6)H(6)) structure in which the central benzene ring acts as a dihapto ligand to each metal atom, leaving an uncomplexed C═C double bond. The metal-metal bond orders in the singlet "rice-ball" structures cis-Bz(2)M(2)(μ-C(6)H(6)) (M = Mn, Fe) and the hapticities of the central benzene rings in the singlet late-transition-metal triple-decker-sandwich structures trans-Bz(2)M(2)(μ-C(6)H(6)) (M = Co, Ni) are governed by the desirability for the metal atoms to attain the favored 18-electron configuration.     

Organic triplet emissions of arylacetylide moieties harnessed through coordination to [Au(PCy(3))]+. Effect of molecular structure upon photoluminescent properties

A family of mono- and binuclear Cy(3)P-supported gold(I) complexes containing various pi-conjugated linear arylacetylide ligands, including the two homologous series (Cy(3)P)Au(Ctbd1;CC(6)H(4))(n)()(-)(1)(Ctbd1;CPh) and (Cy(3)P)Au(Ctbd1;CC(6)H(4))(n)()Ctbd1;CAu(PCy(3)) (n = 1-4), have been prepared. X-ray crystal analyses revealed no intermolecular aurophilic interactions in their crystal lattice. The lowest-energy singlet transitions are predominately intraligand in nature and exhibit both phenyl and acetylenic (1)(pipi) character. Strong photoluminescence is detected in solid and solution states under ambient conditions, with lifetimes in the microsecond regime. For complexes with a single arylacetylide group, only phosphorescence from the arylacetylide (3)(pipi) state is observed. Vibrational spacings in the solid-state emission spectra can be attributed to a combination of phenyl ring deformation and symmetric phenyl ring and Ctbd1;C stretches. Additional delayed-fluorescence emission is recorded for complexes with multiple p-arylacetylide units, and this is attributed to a triplet-triplet annihilation process. The phosphorescence energy of these complexes are readily modified by altering the length of the conjugated arylacetylide system, while the intensity of phosphorescence relative to fluorescence decreases when the p-arylacetylide chain is elongated. Information regarding the nature and relative energies of arylacetylide singlet and triplet excited states has been derived from the two homologous series and extrapolated to polymeric arylacetylide species. The (3)(pipi) excited-state reduction potentials E degrees [Au(+)/Au] (Au = 1a, 2, and 4) are estimated to be -1.80, -1.28, and -1.17 V versus SSCE, respectively.     

吡啶与HCl和CHCl3形成分子间红移氢键和蓝移氢键的理论研究

采用量子化学从头算的MP2方法, 分别在6-31G(d,p), 6-311+G(d,p)和AUG-cc-pVDZ基组下, 研究了复合物C5H5N…HCl(1), C5H5N…HCCl3(2)和C5H5N…HCCl3(3)的分子间氢键. 计算结果表明, 在复合物1中, HCl中Cl—H键伸长, 形成Cl—H…N红移氢键; 在复合物2中, HCCl3中C—H键伸长, 形成C—H…N 红移氢键; 在复合物3中, HCCl3中C—H键收缩, 形成C—H…π蓝移氢键. 自然键轨道(NBO)分析表明, 影响氢键红移和氢键蓝移主要有3个因素: n(Y)→σ*(X—H)超共轭作用、X—H键轨道再杂化和质子供体电子密度重排. 其中, 超共轭作用属于键伸长效应, 电子密度重排和轨道再杂化属于键收缩效应. 在复合物1和2中, 由于键伸长效应处于优势地位导致形成红移氢键; 在复合物3中, 由于键收缩效应处于优势地位导致形成蓝移氢键.     

Synthesis and Crystal Structure of 2,3-Diethoxycarbonyl-4-phenyl-5-morpholinyl Thiophene

1INTRoDUCTIONa-Thiocarbonylthioformamidesweresynthesizedin198o[l~2i,however,thereisnoreportofthesecompoundsconcerningtheirpropertiesandreactionactivitiest33.Accordingtotheirstructure,theyseemtohavereactionwithdienophi1es,likesubsti-tutedolefinicandacetylenicdienophilestoleadcorrespondingDiels-Alderproduct.xylene(15ml),diethylbutynedioicester(O.2g,1.2mmol)wasadded,themix-turewasrefluxedfor20h,thencooledtoroomtemperatureandconcentrated.Theresiduewaspurifiedbysilicagelcolumnusingacetone/petr…