REPS4(RE=Y, La～Lu)系列化合物的合成和结构化学研究

采用高温固相反应合成了稀土硫代磷酸盐ＲＥＰＳ４（ＲＥ＝Ｙ，Ｌａ～Ｌｕ），并通过Ｘ射线粉末衍射测定了晶胞参数以及ＨｏＰＳ４，ＥｒＰＳ４和ＴｍＰＳ４的晶体结构。其中ＲＥＰＳ４（ＲＥ＝Ｙ，Ｌａ～Ｙｂ）系列化合物的结构均属四方晶系，其空间群为Ｉ４１／ａｃｄ，ａ≈１１ｎｍ，ｃ≈１９ｎｍ，Ｚ＝１６。四方结构中的三价稀土离子为反四方棱柱八配位。该结构具有较大的孔洞空间，孔洞直径分别为０６２５ｎｍ（沿ｃ轴方向）和０３５ｎｍ（沿ａ、ｂ轴方向）。ＬｕＰＳ４晶体为单斜晶系，很可能是层状（２Ｄ）结构。研究了镧系收缩效应对四方结构稳定性的影响，发现对ＲＥＡＸ４系列化合物来说，四方结构能稳定存在的前提是２４ｄＡＸ／ｒ１９。     

QUANTUM CHEMICAL STUDY ON THE MECHANISM OF PRODUCING OXYGENATES IN FISCHER－TROPSCH SYNTHESIS ON M／SiO＿2 （M＝Ni， Ru， Rh， Pd） CATALYSTS

ＱＵＡＮＴＵＭ　ＣＨＥＭＩＣＡＬ　ＳＴＵＤＹ　ＯＮ　ＴＨＥ　ＭＥＣＨＡＮＩＳＭ　ＯＦ　ＰＲＯＤＵＣＩＮＧ　ＯＸＹＧＥＮＡＴＥＳ　ＩＮ　ＦＩＳＣＨＥＲ－ＴＲＯＰＳＣＨ　ＳＹＮＴＨＥＳＩＳ　ＯＮ　Ｍ／ＳｉＯ＿２　（Ｍ＝Ｎｉ，　Ｒｕ，　Ｒｈ，　Ｐｄ）　ＣＡ...     

新型双核铜配合物的合成,表征及其对苯乙烯环氧化的催化作用

设计合成了５种新型双核铜配合物，用ＥＡ，ＩＲ，ＵＶ－Ｖｉｓ，ＸＰＳ，ＥＰＲ等进行了结构表征，并研究了这些Ｃｕ２配合物模拟双核铜单加氧酶多巴胺β－羟化酶催化苯乙烯环氧化反应的特征。结果表明，这些配合物具有两种类型的结构：脱质子型Ｃｕ２ＬＯＨ和非脱质子型「（Ｃｕ２Ｈ２ＬＸ）Ｙ」Ｙ（Ｘ＝Ｙ＝Ｃｌ＾１－，Ｂｒ＾－；Ｘ＝ＯＨ，Ｙ＝Ｏ２ＣｌＯ＾－２），两类配合物可相互转化。非脱质子型配合物催化ＰｈＩＯ对苯乙烯     

三羰基环戊二烯基钼负离子与1,3—二卤丙烷的反应

三羰基环戊二烯基钼负离子与１，３－二卤丙烷在一缩二乙二醇二甲醚介质中反应，生成环卡宾配合物ＣｐＭｏＸ（ＣＯ２）ＣＯ（ＣＨ２）２ＣＨ２（Ｘ＝Ｂｒ．Ｉ）硅桥连双环戊二烯基三羰基钼负离子与１，３－二卤丙烷顺利地进行类似反应，生成相应的硅桥连双（环卡宾钼配合物）－Ｅ（Ｃ５Ｈ１ＭｏＸ（ＣＯ）２ＣＯ（ＣＨ２）２ＣＨ２）２（Ｅ＝Ｍｅ２Ｓｉ，Ｍｅ２ＳｉＳｉＭｅ２，Ｍｅ２ＳｉＯＳｉＭｅ２），化合物硅氧硅桥联二茂二钼     

CH_2=CH(XM)(X=S,Se,Te;M=H,Li,Na,K,Rb,Cs,-)的从头算研究

应用相对论有效势在ＭＰ２水平上对ＣＨ２ＣＨ（ＸＭ）（Ｘ＝Ｓ，Ｓｅ，Ｔｅ；Ｍ＝Ｈ，Ｌｉ，Ｎａ，Ｋ，Ｒｂ，Ｃｓ，－）进行了从头计算研究．结果表明，所研究的化合物都有平面式和非平面桥式两种构型．分析了碱金属离子对两可亲核底物ＣＨ２ＣＨＸ－（Ｘ＝Ｓ，Ｓｅ，Ｔｅ）离域化的影响，并用自然布局分析方法（ＮＰＡ）研究了电荷分布的变化，得出了有价值的结论．     

A DV－X_∝ QUANTUM CHEMICAL STUDY OF THE LEWIS ACIDITY SCALE OF BORON TRIHALIDES BX_з（X＝F，C1，Br，I）

ＡＤＶ－Ｘ＿∝ＱＵＡＮＴＵＭＣＨＥＭＩＣＡＬＳＴＵＤＹＯＦＴＨＥＬＥＷＩＳＡＣＩＤＩＴＹＳＣＡＬＥＯＦＢＯＲＯＮＴＲＩＨＡＬＩＤＥＳＢＸ＿з（Ｘ＝Ｆ，Ｃ１，Ｂｒ，Ｉ）￥ＺｈｅｎｇＴｉｎｇＣＡＩａｎｄＣｉＲａｎＬＩ（ＤｅｐａｒｔｍｅｎｔｏｆＣｈｅｍｉｓ...     

金属性Zintl相化合物RE_3Cu_3Sb_4(RE=Nd,Sm,Tb,Dy,Ho)的合成、结构及成键特性

用电弧熔炼方法合成了化合物ＲＥ３Ｃｕ３Ｓｂ４（ＲＥ＝ Ｎｄ,Ｓｍ ,Ｔｂ,Ｄｙ,Ｈｏ）, 采用粉末Ｘ射线衍射方法测定了其晶体结构。化合物属立方晶系,Ｙ３Ａｕ３Ｓｂ４ 类型, 空间群Ｉ４３ｄ（Ｎｏ．２２０）,皮尔森玛ｃＩ４０。晶胞参数：Ｎｄ３Ｃｕ３Ｓｂ４ ：ａ＝０．９６７４９（１） ｎｍ, Ｖ＝０．９０５６１（３） ｎｍ３;Ｓｍ３Ｃｕ３Ｓｂ４：ａ＝ －０．９６１４５（１） ｎｍ ,Ｖ＝０．８８８７５（３） ｎｍ３ ;Ｔｂ３Ｃｕ３Ｓｂ４： ａ＝０．９５３６２（１） ｎｍ , Ｖ＝ ０．８６７２１（３）ｎｍ３;Ｄｙ３Ｃｕ３Ｓｂ４： ａ＝０．９５０８８（１） ｎｍ , Ｖ＝０．８５９７５（３） ｎｍ３;Ｈｏ３Ｃｕ３Ｓｂ４ ： ａ＝０．９４８８（２） ｎｍ , Ｖ＝０．８５４１（５） ｎｍ３。每个单胞中包含４ 个化合式量。此结构中,Ｃｕ 原子均处于Ｓｂ 原子所形成的配位四面体中心, 这些共价结合的配位四面体通过共顶最终联接形成三维ＣｕＳｂ 网络,稀土原子则散布在网络之间的空隙中。化合物电荷平衡结构式可表示为ＲＥ３＋３ Ｃｕ１＋３ Ｓｂ３－４ , 化合物具有导电性, 为金属性Ｚｉｎｔｌ 相。原子成键具有典型过渡性。原子的“配位数”遵从配位环境规律。化合物的     

SYNTHESIS AND CHARACTERIZATION OF HETEROBIMETALLIC COMPLEXES： （Cp_2LnOCH_2C_6H_5）Cr（CO）_3（Ln＝Gd，Dy，Yb，Y）

ＳＹＮＴＨＥＳＩＳ ＡＮＤ ＣＨＡＲＡＣＴＥＲＩＺＡＴＩＯＮ ＯＦ ＨＥＴＥＲＯＢＩＭＥＴＡＬＬＩＣ ＣＯＭＰＬＥＸＥＳ：（Ｃｐ_２ＬｎＯＣＨ_２Ｃ_６Ｈ_５）Ｃｒ（ＣＯ）_３（Ｌｎ＝Ｇｄ，Ｄｙ，Ｙｂ，Ｙ）￥ＣｈａｎｇＴａｏＱｉＡＮ；ＪｉａｎＨｕａＧＵＯ?..     

XO（X=F,Cl,Br,I）自由基的PES和DFT理论研究

ＸＯ（Ｘ＝Ｆ，Ｃｌ，Ｂｒ，Ｉ）自由基的ＰＥＳ和ＤＦＴ理论研究洪功义王殿勋＊（北京分子动态与稳态结构国家重点实验室，中国科学院化学研究所，北京１０００８０）南极臭氧空洞的发现引起全球人的震动，继而人们在北半球欧洲和北美上空也发现臭氧空洞。今天人们逐渐认...     

标题固相合成V—Cu—S簇合物;VS4（CuPPh3）5X2（X=Br,I）的晶体结构

标题两个化合物是在反应体系（ＮＨ４）３ＶＳ４／ＣｕＸ／ＰＰｈ３／ＮＥｔ４Ｘ中采用低温固相反应方法得到的，单晶Ｘ射线结构分析表明：ＶＳ４（ＣｕＰＰｈ３）５Ｂｒ２（Ｉ）和ＶＳ４－（ＣｕＰＰｈ３）５Ｉ２是同构的，其中晶体属于单斜晶系，空间群Ｐ２１ｃ，Ｍｒ＝１９６８．２，ａ＝２０．２１５（７），ｂ＝１５．６９１（４），ｃ＝２７．３４５（９）Ａ，β＝９５．２９（３）°，Ｖ＝８６３７．０Ａ＾３，Ｚ＝４，Ｄｃ＝     

Use of oxidation-state differences and molecular orbitals to interpret bonding in the series ONXYZ (X, Y, Z=H, F, Cl), HNNX3, HNNX2Y, and HNNXY2 (X, Y=H, F) and OCX3-, OCX2Y-, and OCXY2- (X, Y=H, F)

Bonding in the series ONXYZ (X, Y, Z=H, F, Cl), HNNX3, HNNX2Y, HNNXY2 (X, Y=H, F), and OCX3-, OCX2Y-, OCXY2- (X, Y=H, F) shows evidence of a significant ionic contribution modifying the underlying covalent bonding. Increased ionic character can be correlated with oxidation-state differences between the bound atoms and is expressed in terms of shorter bond lengths. All members of the series, with the exception of ONH3, HNNH3, and OCH3-, possess a multiple O-N, N-N, or C-O bond modified by the ionic character of that bond. The O-N, N-N, and O-C single bonds in ONH3, HNNH3, and OCH3-, respectively, show some variation in length relative to "typical" single bonds of these types due to differences in ionic character. The two highest-occupied molecular orbitals in the ONXYZ or OCXYZ- (X, Y, Z=H, F) series which are piNO or piCO (when X=Y=Z=H) exhibit a distinct shift in their nodal plane as hydrogen is replaced by fluorine. The nodal plane moves from a location between the oxygen and the nitrogen or carbon to between the nitrogen or carbon and the fluorines impacting on the nature and length of the bonds joining these atoms. The pattern of N-F and C-F bond lengths in the series, ONH3-ONF3 and OCH3--OCF3-, respectively, lends support to the idea of resonance structures of the form ONXY+ F- or OCXY F- (where X, Y=H, F).     

Structures and electron attachment properties of halomethanes (CX(n)Y(m), X=H, F; Y=Cl, Br, I; n=0,4; m=4-n)

Theoretical studies of structures of neutral molecules and their anions as well as dissociative electron attachment properties are presented for the halomethanes of general formula CX(n) Y(m); X=H, F; Y=Cl, Br, I; n=0,4; m=4-n. The dissociative electron attachment seems to be the primary process resulting in toxicity of these species. The halomethane anions containing hydrogens are formed as radical-anion adducts. When H is replaced by F, these species become true sigma* radicals. The electron affinities are computed using a variety of computational techniques including the four-order M?ller-Plesset (MP4) technique that included 250 basis functions. It is challenging to compare the computed results with experiment due to dearth of experimental data and uncertainties in the existing experimental data. Thus in certain cases larger differences are found between the computed and experimental values.     

Interactions of (MY)6 (M = Zn,Cd; Y = O,S, Se) quantum dots with N-bases

Structural Chemistry - (MY)6 clusters, with M = Zn and Cd and Y = O, S, Se, form double-layer drum-like structures containing M–Y covalent bonds. The positive regions near the M atoms attract...     

The preparation of WMeCl3Y (Y = S OR Se) and some coordination compounds of WMeCl3Y (Y = O,S OR Se)

The reaction of WCl₄Y (Y = S or Se) with Me₂Mg leads to the formation of WMeCl₃Y. The compounds WMeCl₃Y (Y = O, S or Se) are very reactive and attempts to isolate them in pure form failed. However, a range of complexes which they form with some nitrogen and oxygen donors have been isolated and characterised.     

A comparative computational study of FKrCCH...Y, FCCKrH...Y, and FCCH...Y complexes (Y = BF, CO, N2, OH2, OH(CH3), O(CH3)2)

The structural and spectroscopic changes in complexes of FCCKrH...Y and FKrCCH...Y (Y = BF, CO, N(2), OH(2), OH(CH(3)), O(CH(3))(2)) were computed at the MP2∕6-31++G(d,p) level of theory and compared with the corresponding properties for FCCH...Y. The computed bond length changes and frequency shifts on complexation were rationalized by comparing with a perturbation model, which gives quantitative agreement with the standard ab initio results. A recently proposed model also gives a reasonable qualitative account of the observed trends in these complexes.     

New layered germanide halides RE2GeX2 (RE = Y, Gd; X = Br, I)

The title compounds were synthesized from RE, REX3, and Ge under an Ar atmosphere at 1200-1370 K. Y2GeI2 and Gd2GeI2 crystallize in space group Rm with lattice constants a = 4.2135(3) and 4.2527(1) A and c = 31.480(2) and 31.657(1) A, respectively. Gd2GeBr2 crystallizes in two modifications, the 1T-type (space group Pm1; a = 4.1668(2) A, c = 9.8173(6) A) and the 3R-type (space group Rm; a = 4.1442(9) A, c = 29.487(7) A). The structural motifs of RE2GeX2 compounds are Ge-centered slightly distorted RE6 octahedra connected via their common edges and extending in the a and b directions. The resulting close-packed double layers are separated by halogen atoms. The electrical resistivity measurements revealed semiconductor behavior for Y2GeI2 and Gd2GeI2 and a metal-semiconductor transition for 1T-Gd2GeBr2. Magnetic susceptibility and heat capacity measurements show long-range magnetic ordering for Gd2GeI2 and 1T-Gd2GeBr2 at approximately 15 and approximately 13 K, respectively.     

C_4H_4Y(Y=O,S,Se)与BX_3(X=H,F,Cl)作用的计算化学研究

采用量子化学的密度泛函B3LYP和二阶微扰MP2(full)方法对C4H4Y(Y=O,S,Se)与BX3(X=H,F,Cl)形成的电子授受型复合物进行了研究,所得18个复合物的构型包括BX3位于C=C双键上方的π-p作用型和B与O,S,Se直接作用的n-p作用型.体系C4H4Y-BH3以n-p作用型较为稳定,体系C4H4Y-BF3,C4H4Y-BCl3的π-p和n-p作用型复合物稳定性相当.对各复合物的几何构型、振动频率和自然键轨道分析表明,复合物的形成过程中均存在几何构型的改变、电荷的转移和振动频率的变化,它们的变化规律与复合物稳定性的变化规律基本一致,即按H,F,Cl的顺序依次降低.     

高温高压法提取金属富勒烯Lnm@C2nLn=Y, Gd, Tb)

笼内金属富勒烯以其独特的结构性质和潜在的应用价值而引起了人们极大的注意 [1～ 3] ,但因制备技术复杂、产率低以及将其从伴生的空心富勒烯中分离出来比较困难而使其研究受到很大的限制 .笼内金属富勒烯的分离提取始终是金属富勒烯研究的一个重要分支 .通常的方法是将放电得到的烟炱采用甲苯索氏提取的方法粗提 ,然后用高压液相色谱法分离得到纯品 ,笼内金属富勒烯的产率仅为烟炱的 0 .1 % [4～ 6] .我们改进了常规的提取方法 ,建立了一种新的提取方法—高温高压提取法 .具体的做法是采用甲苯索氏提取法从烟炱中提取出空心富勒烯和少量金…     

Theoretical examination of substituent effects on the stabilization of a Sn?Y (Y = Sb and Bi) multiple bond

The potential energy surface for the unimolecular rearrangement XSn?Y → TS → Sn?YX (Y = Sb, Bi) was investigated using the B3LYP and QCISD methods. To explore electronic effects on the relative stability of XSn?Y and Sn?YX, the first‐row substituents (X = H, Li, BeH, BH₂, CH₃, NH₂, OH, F) have been used. Our theoretical findings suggest that the doubly bonded Sn?YX species are always both kinetically and thermodynamically more stable than their corresponding triply bonded isomers, XSn?Y, regardless of the electronegativity of the substituent X. Nevertheless, our model calculations indicate that an aryl group can, if sufficiently bulky, stabilize triply bonded XSn?Y molecules with respect to both isomerization and polymerization. That is to say, it is not electronic but steric effects that play a dominant role in stabilizing both Sn?Sb and Sn?Bi triple bonds. © 2004 Wiley Periodicals, Inc. Int J Quantum Chem, 2005     

The CsLnMSe3 semiconductors (Ln = rare-earth element,Y; M = Zn,Cd, Hg)

CsLnCdSe(3) (Ln = Ce, Pr, Sm, Gd, Tb, Dy, Y) and CsLnHgSe(3) (Ln = La, Ce, Pr, Nd, Sm, Gd, Y) have been synthesized at 1123 K. These isostructural materials crystallize in the layered KZrCuS(3) structure type in the orthorhombic space group Cmcm and are group X extensions of the previously characterized Zn compounds. The structure is composed of two-dimensional [LnMSe(3)] layers that stack perpendicular to [010] and are separated by layers of face- and edge-sharing CsSe(8) bicapped trigonal prisms. Because there are no Se-Se bonds in the structure of CsLnMSe(3) (M = Zn, Cd, Hg), the formal oxidation states of Cs/Ln/M/Se are 1+/3+/2+/2-. CsSmHgSe(3) does not adhere to the Curie-Weiss law, whereas CsCeHgSe(3) and CsGdHgSe(3) are Curie-Weiss paramagnets with micro (eff) values of 2.77 and 7.90 micro (B), corresponding well with the theoretical values of 2.54 and 7.94 micro (B) for Ce(3+) and Gd(3+), respectively. Single-crystal optical absorption measurements were performed with polarized light perpendicular to the (010) and (001) crystal faces of these materials. The band gaps of the (010) crystal faces range from 1.94 eV (CsCeHgSe(3)) to 2.58 eV (CsYCdSe(3)) whereas those of the (001) crystal faces span the range 2.37 eV (CsSmHgSe(3)) to 2.54 eV (CsYCdSe(3) and CsYHgSe(3)). The largest band gap variation between crystal faces is 0.06 eV for CsYCdSe(3). Theoretical calculations for CsYMSe(3) indicate that these materials are direct band gap semiconductors whose colors and optical band gaps are dependent upon the orbitals of Y, M, and Se.