Synthesis and Structure of Dimolybdenum Carbonyl Thiolate Compound [Et4N]2[Mo2（CO）8（SC6H4—CH3—m）2]

1 INTRODUCTION In 1984, thiolate ligand was successfully introduced into molybdenum carbonyl compound by the reaction of Mo(CO)6 with [Et4N]SR( R = C6H5, But) in a moderate condition[1]. From then on, a series of dinuclear molybdenum(0) carbonyl thiolate compounds have been synthesized and characterized by using a variety of thiolate ligands in our research group. It was found that a planar Mo2S2 unit is in the compound [Et4N]2[Mo2(CO)8(SC6H4-CH_3-p)2][2] (2) and a "butterfly" t…     

混合价簇合物[Et_4N]_2[{(CO)_4M}_xM′S_4][x=1,2;M=Mo(0)或W(0);M′=Mo(Ⅵ)或W(Ⅵ)]的共振Raman光谱及IR光谱研究

研究了[{(CO)4_M}_xM′S_4]~(2-)[X=1,2;M=Mo(O),W(O);M′=Mo(Ⅵ),W(Ⅵ)]系列簇合物的共振Raman(RR)光谱及红外(IR)光谱.除了对:v_(c—o),v_(M(Ⅵ)—S(b))[S(b):桥基S],v_(M(Ⅵ)—S(t))[S(t):端基S],v_(M(o)—c),δ_(M(O)—C—O)进行归属外,着重讨论v_(M(O)—S(b)),v_(M(O)-M(Ⅵ))的归属.研究了IR谱中Δv[v_(M(Ⅵ)—S(b))(—v)_(M(O)—S(b))]与M(0)→M(Ⅵ)电荷迁移的关系.RR谱研究结果表明,在[(CO)_(4-)MS_2MoS_2]~(2-),[(CO)_4MoS_2MoS_2Mo(CO)_4]~(2-)中S(b)一M(0)电荷迁移与M(0)-MO(Ⅵ)电荷迁移之间有较明显的相互偶合;在[(CO)_4MS_2WS_2]~(2-)中S(b)→W(Ⅵ)与M(O)→W(Ⅵ)电荷迁移、S(t)→W(Ⅵ)与M(0)→W(Ⅵ)电荷迁移之间也分别存在明显的相互偶合,说明了它们存在强的电子离域.本系列簇合物中二核簇的电子离域程度比三核簇强.     

Synthesis, Structure and Secondorder Nonlinear Optical Activities of a New Tungsten（0） Compound with Pyridine-2-thiolato Ligand, [Et4N][W（pyS）（CO）4] （pys = C5H4NS^-）

The reaction of W(CO)6 with pyOSNa (C5-H4NOSNa) and Et4NCl in MeCN affords a new tungsten(0) complex [Et4N][W(pyS)(CO)4] 1 (Mr.= 536.29).The crystal and molecular structures have been determined by X-ray single-crystal diffraction.Complex 1 crystallizes in the orthorhombic system,space group P212121 with a = 8.2429(5),b = 9.1045(4),c =26.8851(14) (A),β = 90.00°,V= 2017.66(18) (A)3,Z = 4,Dc.= 1.765 g/cm3,μ = 58.51 cm-1,F(000) =1048,the final R = 0.0204 and wR = 0.0400 for 4432 observed reflections with I ＞ 2σ(I).X-ray structure analysis revealed that the molecule is acentric and has large first-order hyperpolarizability (7.2 × 10-30 esu),so it could be an IR second-order nonlinear optical candidate material.     

三核簇合物(Et4N)2[(CO)4MoS2MoS2Mo(CO)4]和(Et4N)2[(CO)4MoS2WS2Mo(CO)4]的合成及晶体结构

合成了含Mo(0)的三核化合物(Et₄N)₂[(CO)₄Mo(μ-S)₂Mo(μ-S)₂Mo(CO)₄](Ⅰ)和(Et₄N)₂[(CO)₄Mo(μ-S)₂W(μ-S)₂Mo(CO)₄](Ⅱ),测定了(Ⅰ)的晶体结构.Ⅰ属单斜晶系,空间群P2相似文献   

Synthesis,Structure,Characterization and Electrochemistry of a New Din

Reaction of Et4NCl, NaSCH2COOMe and W(CO)6 in MeCN affords a new dinuclear tungsten(0) complex [Et4N]2[W2(CO)8(SCH2COOMe)2] (1). The crystal and molecular structure has been determined by X-ray single crystal diffraction. 1 Crystallized in the triclinic, space group P with a=11.141(7), b=10.267(4), c=10.798(3)(); α=93.96(3), β=96.88(4), γ=114.97(5)°; V=1003()3, Z=1, Dc=1.76 g/cm3, μ=60.1 cm-1, R=0.042 and Rw=0.050 for 2967 independent reflections with I>3.0 σ(I). 1 contains a WS2W planar core with nonbonding W...W distance of 3.9611(5)(), and its IR, 13C NMR, and cyclic voltammetry were measured and discussed.     

过渡金属体系非线性光学性质计算的ECP基组研究

有效核势(ECP)方法是计算含有过渡金属体系的电子结构及物理性质的有效方法. 本文比较了一系列典型的ECP基组对计算含过渡金属体系非线性光学性质精度的影响. 分别在HF, MP2和DFT理论水平上对过渡金属元素使用不同的ECP基组, 计算了几个过渡金属有机化合物的静态一阶超极化率β₀. 研究结果表明: 使用有效核势计算含过渡金属体系时, 核电子的选取是提高计算精度的前提, ns和np电子应该和nd电子一同作为价电子处理; 对于重原子, 必须考虑自旋-轨道耦合相对论效应. 经过综合评估, 认为使用Stuttgart/Dresden赝势的ECP基组, MHF, 在计算含有过渡金属体系非线性光学性质方面是比较好的基组; Stuttgart RSC 1997和SBKJC VDZ相对而言是较好的基组; 基组Lanl2dz, Hay-Wadt MB (n＋1)和Hay-Wadt VDZ (n＋1)由于没有考虑自旋-轨道耦合, 计算精确度次之; 而基组CRENBL和CRENBS计算的偏差要大一些, 尤其是CRENBS基组由于价电子选择得太少而导致与实验值的偏差最大.     

三核簇合物(Et_4N)_2[(CO)_4MoS_2MoS_2Mo(CO)_4]和(Et_4N)_2[(CO)_4MoS_2WS_2Mo(CO)_4]的合成及晶体结构

合成了含Mo(O)的三核化合物(Et_4N)_2.[(CO)_4Mo(μ-S)_2Mo(μ-S)_2Mo(CO)_4](Ⅰ)和(Et_4N)_2[(CO)_4Mo(μ-S)_2W(μ-S)_2Mo(CO)_4](Ⅱ),测定了(Ⅰ)的晶体结构.Ⅰ属单斜晶系,空间群P2_1/c,a=22.790(5),b=8.701(1),c=17.764(5)(?).γ=94.09(2)°,Z=4,最终R=0.045.Ⅰ的阴离子中,三个Mo间键角175°,接近共线.整个阴离子可以看作是由2个以Mo(0)为中心的八面体和1个以Mo(Ⅵ)为中心的准四面体分别共用一条边(各由2个μ-S原子连线所成)组成的结构.Mo-Mo-Mo键距分别是2.998(1)和3.000(1),Mo(μ-S)_2Mo共平面.