TiP2^+,TiP4^+,Ti2P4^+二元团簇的理论研究

利用含有电子相关效应校正的密度泛函理论DFT中的B3LYP方法,选择LANL2DZ双ξ基组,并考虑极化函数,对TiP2^+,TiP4^+,Ti2P4^+二元团簇各种可能存在的几何构型及电子结构进行了密度泛函理论研究,得到了TimPn^+二元团族的最稳定构型,其中TiP2^+的最稳定构型为C2v对称性的三角形,TiP4^+的最稳定构型亦具有C2v对称性,Ti2P4^+的最稳定构型为具有D2d对称性的共边双四面体,所得构型很好地说明了激光光解的实验结果。     

Ti_3P_6~+团簇结构的理论研究

利用密度泛函理论中的B3LYP方法，选择LANL2DZ双Zeta基组，并考虑极化函数 ，对Ti_3P_6~+团簇可能存在的几何构型进行了理论计算研究，得到了Ti_3P_6~+具 有C_s对称性的最稳定构型，所得构型很好地说明了激光光解的实验结果。     

正、负和中性TiP10团簇结构与电子性质的密度泛函研究

采用密度泛函理论的B3LYP方法研究了正、负和中性TiP10团簇的几何构型和电子结构. 计算结果表明, 中性TiP10团簇的基态构型为金属夹心结构, 正、负离子团簇同样具有该基态稳定结构. 通过对基态稳定结构的分子轨道分析表明, δ键对形成夹心结构起到重要作用. 理论计算得到的中性TiP10团簇的垂直和绝热电离能分别为7.84和7.68 eV, 垂直和绝热电子亲和势分别为3.18和3.35 eV.     

钴硫团簇ConSn+-1(n=2,3)的结构和稳定性

用ab initio分子轨道方法(RHF,UHF)和密度泛函(DFT)方法研究了团簇Co2S+,Co3S2+的各种可能的几何构型和电子结构,并计算了相应的较稳定构型的振动光谱,发现Co2S+和Co3S2+团簇最稳定结构均具有C,对称性.对团簇的成键作用机理进行了理论分析.     

团簇Ti4 P的反应活性研究

为了得到团簇Ti4P参与化学反应时反应活性最好的结构模型,对团簇Ti4P分析时依据密度泛函理论,并在B3LYP和BP86杂化泛函和Lan12dz赝势基组分别进行分析研究.首先从能量角度分析团簇Ti4P的稳定性,得到构型1(4)即四重态构型中能量最低的戴帽三角锥构型稳定性最好,3(2)即二重态构型中能量最高的戴帽三角锥构...     

Pdn(n=2～13)团簇的密度泛函理论研究

采用密度泛函理论B3LYP方法计算并讨论钯原子团簇Pdn(n=2～13)结构模型.通过对钯原子团簇进行几何构型优化和振动频率计算,找出团簇总能量最低的同分异构体.由于Jahn-Teller效应的存在,团簇的最稳定结构采取对称性较低的几何构型.在钯原子数相同时,往往存在多个能量极为相近的稳定构型.单位原子平均静态极化率呈奇偶变化.     

(Mg3N2)n(n=1～4)团簇结构与性质的密度泛函研究

用密度泛函理论(DFT)的杂化密度泛函B3LYP方法在6-31G*基组水平上对(Mg3N2)n(n=1～4)团簇各种可能的构型进行几何结构优化,预测了各团簇的最稳定结构.并对最稳定结构的振动特性、成键特性、电荷特性和稳定性等进行了理论分析.结果表明:(Mg3N2)n=1～4团簇易形成笼状结构,其最稳定构型中N原子配位数以3、4较多见;团簇主要由Mg-N键组成,Mg-N键长为0.194～0.218nm,Mg-Mg 键长为0.262～0.298 nm;N原子的平均自然电荷为-2.06 e,Mg原子的平均自然电荷为 1.37 e;(Mg3N2)2团簇有相对较高的动力学稳定性.     

Pt_nNi_m（n＋m=7,n,m≠0）团簇结构稳定性与磁学性质

采用密度泛函理论（DFT）中的杂化密度泛函B3LYP方法在LANL2DZ基组水平上对PtnNim团簇的各种可能构型进行了几何结构全优化,得出了它们的基态构型,并对其稳定性和磁学性质进行了计算研究.研究结果表明：PtnNim团簇的基态结构都为立体结构,对称性较低,多重度较高,Pt5Ni2团簇的稳定性最好;从磁性上看,Pt...     

M6^0，±（M=Os，Ir，Pt）团簇结构与性质的密度泛函理论研究

采用密度泛函理论（DFT）中的杂化密度泛函（B3LYP）方法,在LANL2DZ基组水平上对M6^0,±（M=Os,Ir,Pt）团簇的各种可能构型进行了几何结构优化,得出各团簇的最稳定构型,并对其能量、振动频率、热力学性质、核独立化学位移（NICS）和极化率进行了理论研究．结果表明,M6^0,±（M=Os,Ir）团簇的基态都是三棱柱结构,％团簇的基态是平面三角形结构;M6^0,±（M=Os,Ir,Pt）团簇生成焓都为负值,热力学上是稳定的;NICS值都为负值,表明M6^0,±（M=Os,Ir,Pt）团簇都具有芳香性,其中Os6^-团簇的芳香性最强;从光谱分析来看,Os6的IR和Raman谱的较强吸收峰的个数最多,Ir6的IR和Raman谱的最强吸收峰都只有一个,IR最强吸收峰在137．0和143．5cm^-1之间,Raman谱最强的吸收峰位于169．5cm^-1处;Pt6的IR和Raman谱的最强吸收峰分别位于50．2和194．7cm^-1处．     

硅硫团簇[(SiS2)nS]+(n=1～4)的结构及振动光谱的量子化学研究

用密度泛函(DFT)方法(B3LYP/6-31G*)研究了硅硫团簇[(SiS~2)~nS]^+(n=1～4)的可能几何构型,得到各稳定构型的电子结构,并计算了相应的振动频率,预测了稳定构型的振动光谱。由其稳定构型的比较可在理论上预测团簇的生长规律,并可初步预测团簇的形成机理。     

原子团簇离子TinP+m的几何结构与电子性质研究

用量子化学ｂｐｉｎｉｔｉｏ方法研究激光等离子体反应生成的ＴｉｎＰｍ＾＋簇离子,优化了其可能的几何构型,ＴｉＰ＾＋ｍ簇离子中,钛连接两个磷原子形成平面体系,ＴｉＰ＾＋４和ＴｉＰ＾＋６是较稳定构型。     

SinP+m(n+m=5)结构和稳定性的理论研究

在实验的基础上 ,利用量子化学方法对 Sin P+ m( n+m=5 )的各种可能构型进行几何构型优化 ,预测各团簇的稳定结构 ,从中得出各个团簇稳定构型之间的基本关系 ,当 n>m时 ,团簇的稳定构型与 Si+ n 相似 ,而当 n相似文献   

Defect models of the three trigonal Ti3+ centers in LiF:Ti3+ and LiF:Ti3+:Mg2+ crystals

The EPR g factors of the trigonal Ti3+ center A in LiF:Ti3+ and two additional trigonal Ti3+ centers B and C in LiF:Ti3+:Mg2+ crystals are calculated from the third-order perturbation formulas based on the cluster approach. From the calculations and by considering the Ti3+ displacement along 111 axis obtained by ENDOR experiment, the defect models for the three Ti3+ centers are suggested. For center A, there are two possible models: (i) [Ti3+F3-O3(2-)] cluster and (ii) [Ti3+F6-] cluster with the Ti3+ off-center caused by a neighboring Li+ vacancy (VLi+) at <111> axis. The latter seems the more likely. The defect models of centers B and C are the [Ti3+F3-O(3)2-] clusters associated with a neighboring: Mg2+ ion at the Li+ site along 111 axis in the vicinity of three F- ions and three O2- ions, respectively. The reasonableness of these models is discussed.     

Theoretical Study on the Electronic Structures of Small TinNm （n ＋ m = 5, 6） Clusters

45 isomers of TinNm （n ＋ m = 5, 6） clusters, including linear, some planar and some stero configurations, have been predicted by density functional theory method. For five-atom clusters Ti3N2 and Ti2N3, the most stable structures are trigonal bipyramid in D3h symmetry, and for TiaN cluster, the isomer with one nitrogen atom occupying the center of quasi-tetrahedron is the most stable. In the isomers of Ti4N2 and Ti3N3, the planar networks are more stable, but for Ti2N4, the six-membered ring configuration is the most favorable. Most linear structures can form weak-strong bonds alternately with higher energy. As regards to planar structures, the more Ti-N bonds are formed, the more stable they will be; for stero closed polyhedral isomers, their energies are lower.     

Theoretical studies on the structure and aromaticity of Ti2P6+

Cationic cluster Ti2P6+ has been studied within density functional theory. The structure of this cluster is predicted to be a slightly distorted tetragonal prism. The dissociation energy of this cationic cluster is higher than that of the known sandwich compound, [(P5)2Ti]2-, because of the different bonding in these two compounds. In Ti2P6+, the hybridization of P atoms of the ring is sp3. The bonding between the metal atoms and the P ring is mainly sigma-pi. While in [(P5)2Ti]2-, the P atoms take sp2 hybridization, the bonding between the metal atom and the rings is the typical pi-pi interaction. The electronic delocalization is another stabilizing factor for Ti2P6+. The nuclear independent chemical shift indicates that Ti2P6+ is a three-dimensional aromatic molecule. The predicted infrared and NMR help to identify the Ti2P6+ conformations in experiment.     

六氢吡啶团簇的研究

The 6H-pyridine clusters have been studied by the TOF mass spectrometry, the VUV from synchrotron radiation and the molecular beam technique. Three-type clusters are observed in the VUV photoionization mass spectroscopy: Pn+(n=2-5,P stands for 6H-pyridine molecule), PnH+ (n=2-4) and Pn (H2O)m+(n=4,5, m=1;n=6, m=1,2). The PnH+ clusters may have the chain structures, the Pn+ and Pn(H2O)m+ clusters may have the cyclic structures, all of these are formed by the hydrogen-bond.     

Gas phase synthesis and reactivity of Agn+ and Ag(n-1)H+ cluster cations

Multi-stage mass spectrometry (MSn) on [(M + Ag - H)x + Ag]+ precursor ions (where M = an amino acid such as glycine or N,N-dimethylglycine) results in the formation of stable silver (Ag3+, Ag5+ and Ag7+) and silver hydride (Ag2H+, Ag4H+ and Ag6H+) cluster cations in the gas phase. Deuterium labelling studies reveal that the source of the hydride can be either from the alpha carbon or from one of the heteroatoms. When M = glycine, the silver cyanide clusters Ag4CN+ and Ag5(H,C,N)+ are also observed. Collision induced dissociation (CID) and DFT calculations were carried out on each of these clusters to shed some light on their possible structures. CID of the Agn+ and Ag(n-1)H+ clusters generally results in the formation of the same Ag(n-2)+ product ions via the loss of Ag2 and AgH respectively. DFT calculations also reveal that the Agn+ and Ag(n-1)H+ clusters have similar structural features and that the Ag(n-1)H+ clusters are only slightly less stable than their all silver counterparts. In addition, Agn+ and Ag(n-1)H+ clusters react with 2-propanol and 2-butylamine via similar pathways, with multiple ligand addition occurring and a coupled deamination-dehydration reaction occurring upon condensation of a third (for Ag2H+) or a fourth (for all other silver clusters) 2-butylamine molecule onto the clusters. Taken together, these results suggest that the Agn+ and Ag(n-1)H+ clusters are structurally related via the replacement of a silver atom with a hydrogen atom. This replacement does not dramatically alter the cluster stability or its unimolecular or bimolecular chemistry with the 2-propanol and 2-butylamine reagents.