锌族和钛族卤化物振动光谱的理论计算

采用ab initio RHF,MP2和B3LYP方法以及LanL2DZ和SDD基组计算了四面体锌族卤素阴离子化合物(MX₄^2-,M=Zn(Ⅱ),Cd(Ⅱ),Hg(Ⅱ);X=F^-,Cl^-,Br^-,I^-)和钛族卤化物(MX₄,M=Ti(Ⅳ),Zr(Ⅳ),Hf(Ⅳ);X=F^-,Cl^-,Br^-,I^-)的几何构型和振动频率。计算结果表明,LanL2DZ基组是合适的基组,能得到合理的电荷分布,几何参数以及振动频率。在锌族卤化物的计算中发现,角弯曲振动频率与实测值相当一致,键伸缩振动频率略为偏低,这主要是由于计算的键长略为偏长所致。MP2方法计算的振动频率更接近于实测值。在钛族卤化物的计算中,三种计算方法都相当地再现了实测值,而以B3LYP方法更为满意。     

抗癌性钌配合物[HL][trans-RuⅢCl4L2](L=4H-1，2，4-triazole)水解机理的理论研究

采用密度泛函理论(DFT)方法,并结合导体极化连续模型(CPCM)研究了具有抗肿瘤活性的"Keppler型"钌配合物[Htrz][trans-RuⅢCl4(4H-1,2,4-triazole)2](1)的水解反应过程。首先,在B1B95/(LanL2DZ+6-31G(d))理论水平上对水解反应中各平衡构型在气相条件下的有关结构进行全几何优化及振动频率分析。然后,在更高的基组水平LanL2DZ(f)+6-311++G(3df,2dp)上对优化的结构进行单点能计算,并考虑溶剂效应。计算得到水解反应过程中相应的结构特征和详细的反应势能面。对于第一步水解,水溶液中配合物1的活化能垒为116.6 kJ.mol-1,比已经报道的配合物[ImH][trans-RuⅢCl4(Im)2](ICR)的活化能垒高得多,进一步证实了降低含氮杂环中N原子碱性,可增强配合物在水溶液中的稳定性的水解规律。对于第二步水解,如同已经研究的多数"Keppler型"抗肿瘤钌配合物一样,反应在热力学上优先生成顺式双水解产物。     

平面型四核铜簇合物Cu_4(CH_2XMe_n)_4桥键性质的密度泛函研究

采用密度泛函B3LYP方法,用LanL2DZ和6 31G*基组分别优化了平面型四核铜簇合物Cu4(CH2SiMe3)4和Cu4(CH2XMe2)4(X=P,As)的几何构型,并对B3LYP/LanL2DZ方法优化的结构进行了红外振动频率计算和自然键轨道分析.结果表明,簇合物均呈笼状结构,Cu-C-Cu三中心桥键之间电子的离域增强了Cu簇合物的稳定性,配位C原子的C-H平伏键与C-Cu配位键之间存在σ超共轭效应.     

平面型四核铜簇合物Cu4(CH2XMen)4桥键性质的密度泛函研究

采用密度泛函B3LYP方法，用LanL2DZ和6—31G^＊基组分别优化了平面型四核铜簇合物Cu4（CH2SiMe3）4和Cu4（CH2XMe2）4（X=P，As）的几何构型，并对B3LYP／LanL2DZ方法优化的结构进行了红外振动频率计算和自然键轨道分析．结果表明，簇合物均呈笼状结构，Cu—C—Cu三中心桥键之间电子的离域增强了Cu簇合物的稳定性，配位C原子的C—H平伏键与C—Cu配位键之间存在σ-超共轭效应．     

过渡金属(Ni、Pd、Pt)配合物二阶超极化率的量子化学研究

对ⅧA族过渡金属有机配合物(trans-[Ni(C≡CPh)2(PEt3)2]、trans-[Pd(C≡CPh)2(PEt3)2]、trans-[Pt(C≡CPh)2(PEt3)2])的二阶超极化率进行了量子化学计算研究.分别使用Lanl2dz基组、CEP-31G和CEP-31+G基组,在MP2、HF、B3LYP水平上计算分子的二阶超极化率,各金属配合物的二阶超极化率(γ)的变化趋势为:trans-[Ni(C≡CPh)2(PEt3)2]相似文献   

抗癌性钌配合物[HL][trans-RuIIICl4L2](L=2-NH2-5-Me-STz)的水解机理

用量子化学密度泛函理论(DFT), 并结合导体极化连续模型(CPCM)研究了具有潜在抗肿瘤活性的“Keppler型”钌配合物trans-[RuIIICl4(2-NH2-5-Me-STz)2](1)的水解反应过程. 首先, 在UB3LYP/(LanL2DZ+6-31G(d))理论水平上对水解反应中各平衡构型在气相条件下的有关结构进行全几何优化及振动频率分析; 然后, 在更高的基组水平LanL2DZ(f)+6-311++G(3df,2dp)上对优化的结构进行单点能计算, 并考虑溶剂效应. 计算得到水解反应过程中相应的结构特征和详细的反应势能面. 对于第一步水解, 液相中配合物1的活化能垒为92.9 kJ·mol-1, 与已经报道的配合物trans-[RuIIICl4(2-NH2-Tz)2](2)的活化能垒(96.3 kJ·mol-1)相接近, 并与实验结果相符. 对于第二步水解, 反应在热力学上优先生成顺式双水解产物, 恰如顺铂的水解反应机理一样, 存在着所谓“顺式效应”, 即生成的顺式水解产物有利于其与生物分子靶标的键合, 因此, 顺式双水解产物在生物反应中有望成为重要的前体药物. 本文研究结果有助于深入理解抗癌性Ru(III)配合物与相关生物靶标的作用机理.     

三种席夫碱-Ni(Ⅱ)配合物的电子结构和吸收光谱的理论计算

采用B3LYP/6-31+G(d)-LANL2DZ方法优化了三种Ni(Ⅱ)的席夫碱配合物基态的几何构型,并在相同水平下进行了频率分析以确认稳定点的性质;利用含时密度泛函理论和极化连续介质模型(PCM),按TDB3LYP/6-31+G(d)-LANL2DZ水平计算了目标配合物在N,N-二甲基甲酰胺溶剂中的电子结构和吸收光谱.计算结果表明,配体中间位甲氧基的存在使配合物A具有较大的HOMO-LUMO能级差;且三种Ni(Ⅱ)配合物的S0→S1态的跃迁能按照A→B→C的顺序依次降低.     

Kr和Kr2的实验和理论研究

利用超声分子束技术、同步辐射和反射式飞行时间质谱仪得到了Kr和Kr2的光电离质谱和光电离效率谱, 确定了Kr和Kr2的电离能. 利用Gaussian-03程序中的MP2(Full)/6-31G*, QCISD/cc-pVTZ以及B3LYP/6-31G方法优化了Kr2的结构, 计算了它们的振动频率和电离能, 计算结果显示: 当采用相同的理论水平和基组时, 随着Kr同位素质荷比(m/z)的增大, 它们结构和电离能保持不变, 而振动频率逐渐变小. 与此同时, 用G2方法计算了Kr (84)和Kr2 (168)的电离能, 它们的电离能的理论值与实验结果符合得比较好.     

抗癌性钌配合物[HL][trans-Ru~ⅢCl_4L_2](L=2-NH_2-5-Me-STz)的水解机理

用量子化学密度泛函理论(DFT),并结合导体极化连续模型(CPCM)研究了具有潜在抗肿瘤活性的"Keppier型"钌配合物trans-[Ru~ⅢCl_4(2-NH_2-5-Me-STz)2](1)的水解反应过程.首先,在UB3LYP/(LanL2DZ+6-31G(d))理论水平上对水解反应中各平衡构型在气相条件下的有关结构进行全几何优化及振动频率分析;然后,在更高的基组水平LanL2DZ(f)+6-311HG(3df,2dp)上对优化的结构进行单点能计算,并考虑溶剂效应.计算得到水解反应过程中相应的结构特征和详细的反应势能面.对于第一步水解,液相中配合物1的活化能垒为92.9 kJ·mol~(-1),与已经报道的配合物trans.[Ru~ⅢCl_4(2-NH_2-Tz)_2](2)的活化能垒(96.3 kJ·mol~(-1))相接近,并与实验结果相符.对于第二步水解,反应在热力学上优先生成顺式双水解产物,恰如顺铂的水解反应机理一样,存在着所谓"顺式效应".即生成的顺式水解产物有利于其与生物分子靶标的键合,因此,顺式双水解产物在生物反应中有望成为重要的前体药物.本文研究结果有助于深入理解抗癌性Ru(Ⅲ)配合物与相关生物靶标的作用机理.     

M(bpy)2+3(M=Fe,Ru,Os)电子结构与相关性质

报导了对配合物(M=Fe,Ru,Os)的量子化学密度泛函(DFT)法研究的结果.在B3LYP/LanL2DZ方法与基组的水平上进行计算,探讨的电子结构特征及相关性质,特别是中心原子对配合物的配位键长、光谱性质、电荷布居及化学稳定性等的影响规律,为该类配合物的合成,为分析光、电、催化作用机理提供理论参考.     

Theoretical studies on vibrational spectra of some halides of Group IIB elements

The vibrational spectra of Group IIB elements halides MX2 and their dimers M2X4 (M=Zn(II), Cd(II) and Hg(II); X=F, Cl, Br and I) have been systematically investigated by ab initio RHF and B3LYP methods with LanL2MB, LanL2DZ and SDD basis sets. The optimized geometries, calculated vibrational frequencies are evaluated via comparison with the experimental data. The vibrational frequencies, calculated by these methods with different basis sets, are compared to each other too. The best results can be obtained by RHF/SDD method, with this method, the deviations for MX2 and Hg2X4 are <7%. Some vibrational frequencies of M2X4 that have not been experimentally reported are also predicted.     

Theoretical studies on vibrational spectra of some halides of group IVB elements

The vibrational spectra of group IVB elements halides MX4 (M=Ti(IV), Zr(IV), Hf(II); X=F, Cl, Br and I), have been investigated by ab initio RHF, MP2 and density functional theory B3LYP method with LanL2DZ basis sets. The optimized geometries, calculated vibrational frequencies and Far-IR intensities of MX4 are evaluated via comparison with experimental data. The vibrational frequencies, calculated by these methods, are compared to each other. The results indicate that B3LYP method is more reliable than RHF and MP2 methods for the frequencies calculations for these compounds. With this method, some vibrational frequencies of M2X6(2+)(M=Ti(IV), Zr(IV) and Hf(II); X=F, Cl, Br and I) are also predicted.     

Ab initio and DFT studies on vibrational spectra of some halides of group IIIB elements

The vibrational spectra of some group IIIB elements halides MX(3) and their dimmers, M(2)X(6) (M=Sc(III), Y(III), La(III); X=F, Cl, Br, I), have been systematically investigated by ab initio restricted Hartree-Fock (RHF) and density functional B3LYP methods with LanL2DZ and SDD basis sets. The optimized geometries and calculated vibrational frequencies are evaluated via comparison with experimental values. The vibrational frequencies, calculated by two methods with different basis sets, are compared to each other. The effect of the methods and the basis sets used on the calculated vibrational frequencies are discussed. Some vibrational frequencies of these complexes are also predicted.     

Ab initio and density functional theory studies on vibrational spectra of palladium (II) and platinum (II) complexes of methionine and histidine: effect of theoretical methods and basis sets

The vibrational spectra of methionine and histidine-containing palladium (II) and platinum (II) complexes, cis-M(Met)X2 and cis-M(His)X2 (M = Pd and Pt; X = F, Cl, Br and I; Met = methionine, His = histidine), have been systematically investigated by ab initio Restricted Hartree-Fock (RHF) and density functional B3LYP methods with LanL2DZ and SDD basis sets. The geometries of cis-Pd(Met)Cl2, cis-Pt(Met)Cl2, cis-Pd(His)Cl2 and cis-Pt(His)I2 optimized and vibrational frequencies and IR intensities of cis-M(Met)Cl2 and cis-M(His)Cl2 (M = Pd and Pt) calculated are evaluated via comparison with the experimental values. The vibrational frequencies calculated show that the methods, rather than basis sets, affect the accuracy of the calculation. The best results that can reproduce the experimental ones are obtained at B3LYP level without any scale factor used. The vibrational frequencies of cis-M(Met)X2 and cis-M(His)X2 (M = Pd and Pt; X = F, Br and I) that have not yet been experimentally reported are predicted.     

Comparison between optimized geometries and vibrational frequencies calculated by the DFT methods for the Anderson-type heteropolyanion: hexamolybdoaluminate(III), [AlIII(OH)6Mo6O18]3-

Optimized geometries and vibrational frequencies were calculated for the hexamolybdoaluminate(III), [AlIII(OH)6Mo6O18]3-, Anderson-type heteropolyanion with the HF, B3LYP, B3PW91, B3P86 and B1LYP methods of theory using the LanL2DZ, SDD and combination of LanL2DZ with 6-31G (d, p) basis sets. The agreement between the optimized and experimental geometries was in the decreasing order: HF, B3P86, B3PW91, B1LYP and B3LYP. The calculated frequencies by the B3LYP have the smallest mean root mean square (RMS) error. The effect of the basis set on the calculated bond lengths and frequencies by the density functional calculations (DFT) methods was minor. The agreement between the previously reported IR and Raman spectra and the calculated values is, in general, good.     

Theoretical studies on vibrational spectra of mixed cyanide-halide complexes of platinum(IV) and palladium(IV)

The vibrational spectra of mixed cyanide-halide complexes, M(CN)4X 2 2- and M(CN)5X2- (M=Pt and Pd; X=F, Cl, Br and I), have been systematically investigated by ab initio RHF, B3LYP and MP2 methods with LanL2DZ and SDD basis sets. The calculated vibrational frequencies of platinum complexes are evaluated via comparison with the experimental values. In the infrared frequency region, the C--N stretching vibrational frequencies calculated at B3LYP level with two basis sets are in good agreement with the observed values with deviations, -16-4 cm(-1) for Pt(CN)4X 2 2- and -18 to -2 cm(-1) for Pt(CN)5X2-. However, in far-infrared region, the results obtained at RHF level are better than those calculated at B3LYP and MP2 levels. For RHF/SDD method, the deviations for Ptz.sbnd;X and Ptz.sbnd;C stretching vibrational frequencies are -14-1 and -12 to -2 cm(-1) in the complex Pt(CN)4X2 2-, -19 to -11 and -15-14 cm(-1) in the Pt(CN)5X2- complex, respectively. The vibrational frequencies of palladium(IV) and some platinum(IV) complexes that have not been experimentally reported are predicted.     

Theoretical studies on vibrational spectra of some mixed carbonyl-halide complexes of Osmium(II)

The vibrational spectra of Os(CO)(6)(2+) and some of its mixed carbonyl-halide complexes, cis-Os(CO)(2)X(4)(2-), fac-Os(CO)(3)X(3)(-) and Os(CO)(5)X(+) (X=F, Cl, Br and I), have been systematically investigated by ab initio RHF and density functional B3LYP methods with LanL2DZ and SDD basis sets. The calculated vibrational frequencies of complexes Os(CO)(6)(2+), cis-Os(CO)(2)X(4)(2-) and fac-Os(CO)(3)X(3)(-) are evaluated via comparison with the experimental values. In infrared frequency region, the C-O stretching vibrational frequencies calculated at B3LYP level with two basis sets are in good agreement with the observed values with deviations less than 5%. In the far-infrared region, the B3LYP/SDD method achieved the best results with deviations less than 9% for Os-X stretching and less than 8% for Os-C stretching vibrational frequencies. The vibrational frequencies for Os(CO)(5)X(+) that have not been experimentally reported were predicted.     

Ab initio and DFT studies on vibrational spectra of some mixed carbonyl-halide complexes of ruthenium(II)

The vibrational spectra of Ru(CO)6(2+) and some of its mixed carbonyl-halide complexes, cis-Ru(CO)2X4(2-), fac-Ru(CO)3X3- and Ru(CO)5X+ (X = F, Cl, Br and I), have been systematically investigated by ab initio RHF and density functional B3LYP methods with LanL2DZ and SDD basis sets. The calculated vibrational frequencies of complexes Ru(CO)6(2+), cis-Ru(CO)2X4(2-) and fac-Ru(CO)3X3- are evaluated via comparison with the experimental values. In the infrared frequency region, the C-O stretching vibrational frequencies calculated at B3LYP level with two basis sets are in good agreement with the observed values with deviations less than 5%. In the far-infrared region, the B3LYP/SDD method achieved the best results with deviations less than 8% for Ru-X stretching and less than 2% for Ru-C stretching vibrational frequencies. The vibrational frequencies for Ru(CO)5X+ that have not been experimentally reported were predicted.     

Vibrational assignments of 2-iodopyridine

A review of the vibrational assignments for 2-iodopyridine has been proposed based on the FT-Raman (3500-50cm(-1)) and IR (4000-400cm(-1)) spectral measurements. Equilibrium geometries and vibrational frequencies have been computed from a variety of electronic structure methods: the ab initio (RHF), six DFT (BLYP, BP86, B3LYP, B3P86, B3PW91 and SVWN) and MP2 methods using 3-21G*, LANL2DZ and DGDZVP basis sets. A normal coordinate analysis has been carried out: the normal modes and their couplings are characterized in terms of potential energy distributions (PEDs). The comparison of assignments for pyridine and halopyridines shows that several of the normal modes arise from coupled vibrations in 2-iodopyridine. The BP86 and B3LYP methods with LANL2DZ basis set have performed reasonably well in reproducing the observed spectra, demonstrating that the LANL2DZ basis set (with effective core potential representations of electrons near the nuclei for post-third row atoms) is suitable for 2-iodopyridine.