系列异金属类立方烷原子簇化合物的振动光谱

通过振动光谱和X 射线结构分析数据的结合 ,归属了系列具有 [M3 YS3 M′](M =Mo ,W ;Y =O ,S ;M′=Cu ,Sn ,Sb ,Pb ,Bi)簇芯的异金属四核类立方烷原子簇化合物的主要振动谱峰。讨论了五种结构类型的光谱特征和成键状态。M′的加入使νM— (μ3—Y) 和νM S 频率下降。当M′为过渡金属 ,例如Cu时 ,Cu与[M3 YS3 ]结合紧密造成了与Cu—S共价键相当的νCu—S振动频率。而当M′为主族金属时 ,νM′—S远小于相应共价键的振动频率值。文中还对νM—M 振动进行若干论述。     

含MoFe3S4单元的μ2—OR或μ2—SR桥联双类立方烷簇合物的红？…

对下列含ＭｏＦｅ３Ｓ４单元的μ２－ＯＲ或μ２－ＳＲ桥联双类立方烷簇合物的红外光谱进行了研究：（Ｅｔ４Ｎ）３「Ｍｏ２Ｆｅ６Ｓ８Ｃｌ６（ＯＭｅ）３」（１）,（Ｅｔ４Ｎ）３「Ｍｏ２Ｆｅ６Ｓ８（ＳＰｈ）６（ＯＭｅ）３」（２）,（Ｂｕ４Ｎ）３「Ｍｏ２Ｆｅ６Ｓ８（ＳＰｈ）６（ＯＭｅ）３」（３）（Ｅｔ４Ｎ）３「Ｍｏ２Ｆｅ６Ｓ８（ＳＢｕ＾ｔ）６（ＯＭｅ０３」（４）ｍ,（Ｅｔ４Ｎ）３「Ｍｏ２Ｆｅ６Ｓ８（ＳＰｈ）９」     

[Mo3S7]分立簇和聚合簇合物的振动光谱和电子光谱

本文报道了分立簇 [Mo3 S7(dtp) 3 I]1及它的四聚物 { [Mo3 S7(dtp) 3 ]4 I}·{ (HgI3 ) 4·K} 2 (dtp =S2 P(OC2 H5) -2 )的IR ,Raman和UV Vis光谱 ,并讨论分立的 [Mo3 S7(dtp) 3 I]在四聚后这些光谱的变化。     

高压合成立方氮化硼的振动光谱

 本文利用FT-IR和Raman光谱对用不同触媒高压合成的不同颜色立方氮化硼晶格振动的声子吸收和散射进行了研究。获得了较完整的晶格振动信息，并在1 000~1 300 cm^-1范围内，观测到了3个新的振动谱带，其中一个位于1 089 cm^-1， 归属为体TO声子和表面TO声子组合带，另两条513、801 cm^-1推测为杂质诱发吸收带。     

立方氮化硼的振动光谱及反射光谱的研究

 将黑色、黄色、棕色三种小于50 μm立方氮化硼粉末为样品，研究了其红外光谱、拉曼光谱、反射光谱，结果表明：（1）样品的红外光谱中，1 818 cm^-1和1 548 cm^-1属于cBN的晶格本征振动，而立方氮化硼的晶格本征振动外的晶体缺陷吸收则发生在~800 cm^-1，1 580 cm^-1~1 740 cm^-1和大于2 400 cm^-1处。（2）拉曼光谱测试表明，在1 052 cm^-1和1 304 cm^-1附近出现的散射与cBN不具有反演中心及cBN具有立方结构这样的事实相一致，并且这种散射伴随着布里渊区中心声子的横向和纵向发射。144 cm^-1附近出现的散射，被认为是由于局部振荡模式的出现，在反斯托克斯区造成的信号，这与晶格中杂质缺陷有关。（3）依据得到的反射光谱，计算了cBN单晶禁带宽度，发现这三种cBN都具有大于金刚石的禁带宽度值，分别为：E_g(黑)=6.21 eV，E_g(黄)=5.73 eV，E_g(棕)=5.71 eV。     

[Mo3S7]分子簇和聚合簇合物的振动光谱和电子光谱

本文报道了分立簇「Ｍｏ３Ｓ７（ｄｔｐ）３Ｉ」１及它的四聚物｛「Ｍｏ３ＳＵ（ｄｔｐ）３」４Ｉ｝．｛（ＨｇＩ３）４．Ｋ｝２（ｄｔｐ＝Ｓ２Ｐ（ＯＣ２Ｈ５）＾－２的ＩＲ,Ｒａｍａｎ和ＵＶ－Ｖｉｓ光谱,并讨论分立的「Ｍｏ３Ｓ７（ｄｔｐ）３Ｉ」在四聚后这些光谱的变化。     

含MoFe3S4单元的μ2-OR或μ2-SR桥联双类立方烷簇合物的红外光谱研究

对下列含ＭｏＦｅ３Ｓ４ 单元的μ２－ＯＲ或μ２ －ＳＲ桥联双类立方烷簇合物的红外光谱进行了研究：（Ｅｔ４ Ｎ）３［Ｍｏ２Ｆｅ６ Ｓ８Ｃｌ６ （ＯＭｅ）３ ］（１）,（Ｅｔ４ Ｎ）３ ［Ｍｏ２ Ｆｅ６ Ｓ８ （ＳＰｈ）６ （ＯＭｅ）３ ］（２）,（Ｂｕ４Ｎ）３ ［Ｍｏ２Ｆｅ６Ｓ８ （ＳＰｈ）６ （ＯＭｅ）３ ］（３）,（Ｅｔ４Ｎ）３ ［Ｍｏ２Ｆｅ６Ｓ８ （ＳＢｕｔ）６（ＯＭｅ）３］（４）,（Ｅｔ４Ｎ）３ ［Ｍｏ２Ｆｅ６Ｓ８ （ＳＰｈ）９ ］（５）。通过这系列簇合物特征振动频率和结构参数及与线型Ｍｏ－Ｆｅ－Ｓ簇合物红外光谱的比较,对其νＭ ｏ－μ２Ｏ（Ｒ） ,νＭ ｏ－μ２Ｓ（Ｒ）,νＭ ｏ－Ｓ,νＦｅ－Ｓ,νＦｅ－ＳＲ,νＦｅ－Ｃｌ 进行了归属。对其中两条途径的亲电诱导效应及Δν（即νＭ ｏ－Ｓ－νＦｅ－Ｓ）与Ｆｅ→Ｍｏ 电荷迁移的关系进行了探讨。最后,讨论了桥联双类立方烷与线型Ｍｏ－Ｆｅ－Ｓ簇合物红外光谱的共性和差异。     

二元羧酸取代的三核钼原子簇化合物的红外光谱与结构

本文考察了新合成的两个二元羧酸取代的三核钼衍生物Ｍｏ３Ｓ４（ＤＴＰ）３（ｐｈｔｈａｌａｔｅ）（Ｐｙ）（Ａ）（ＤＴＰ＝ｄｉｅｔｈｙｌ ｄｉｔｈｉｏｐｈｏｓｐｈａｔｅ,「Ｓ２Ｐ（ＯＥｔ）２」＾－）和Ｍｏ３Ｓ４（ＤＴＰ）３（ｍａｌｏｎａｔｅ）（Ｐｙ）（Ｂ）的红外吸收光谱,对Ｍｏ－Ｓ键及配体的主要吸收峰进行了归属和讨论,并与化合物Ｍｏ３Ｓ４（ＤＴＰ）４（Ｐｙ）（Ｃ）的谱图进行了比较。结果表明,通过对这类复     

六方氮化硼的振动光谱与立方氮化硼的合成

 以X射线衍射分析作参比，分析了高度三维有序到近乱层结构的9种六方氮化硼的红外和拉曼光谱，并进行了立方氮化硼的高温高压合成。光谱分析表明，随着晶性的降低，六方氮化硼的低频红外吸收峰的位置及拉曼谱线等基本振动光谱发生明显的特征性的变化，并伴随出现各自不同的次级光谱结构。合成结果表明，在触媒作用下，立方氮化硼的形成需要六方氮化硼原料有一定的结晶度，但立方氮化硼合成效果与六方氮化硼结晶度并非是简单的单调关系。对振动光谱和合成试验的结果进行了讨论。     

两种含铋的杂多化合物的光谱研究

在水热条件下合成了两个含铋的杂多化合物：Co₅[Bi₂Co₂W₂₀O₇₀(H2O)₆]·44H₂O(Ⅰ)和Na₃H₂[Ce₃(H₂O)₁₈Bi₂W₂₂O₇₆]·23H₂O(Ⅱ),通过用FTIR, NIR FT-Raman和UV-Vis DRS光谱研究了它们的结构和性能的关系。ν_as(MO_d)和ν_s(M—Ob—M)的特征振动频率和材料的结构相关。ν_as(M—O_b—M)振动频率可说明当W原子被Co原子取代时氧化活性增强。在化合物Ⅰ和Ⅱ的UV-Vis DRS谱中,分别存在254,319和220,310 nm的(O_d→W),(O_b, c→W)的荷移跃迁特征峰,化合物Ⅰ还在529 nm处出现宽而弱的Co2+的d-d跃迁吸收谱带。最后,文章还对化合物Ⅰ进行了量子化学计算,用于说明其结构特征。     

Vibrational spectroscopic investigation of the hydrates of manganese(II) oxalate

The three known hydrates of manganese(II) oxalate, α‐MnC₂O₄ · 2H₂O, γ‐MnC₂O₄ · 2H₂O and MnC₂O₄ · 3H₂O were synthesized by known procedures and characterized by X‐ray powder diffractometry. Their infrared (IR) and Raman spectra were recorded and discussed on the basis of its structural peculiarities allowing to establish some interesting relations between them and with other, previously investigated, oxalate complexes. The IR spectra of partially deuterated samples of α‐MnC₂O₄ · 2H₂O were also discussed, reinforcing some of the performed assignments. Copyright © 2009 John Wiley & Sons, Ltd.     

121Sb Mössbauer spectroscopic study of a series of organoantimony(III) compounds

A systematic study of organoantimony(III) compounds, SbR₃, was attempted in view of the effect on Mössbauer parameters of the substituent on the aromatic ring. The Mössbauer parameters obtained in frozen organic solutions reflected the electronic effect caused by the characteristics of the substituents, electron donative or attractive, at the para position on the aromatic ring.     

Vibrational spectroscopic investigation of the phase diagram of a biomimetic lipid monolayer

The phase behavior of a biomimetic monolayer consisting of diphospholipid molecules on water is investigated using vibrational sum-frequency generation and fluorescence microscopy. In addition to the transition from the-molecularly disordered-liquid phase to the highly ordered and oriented con-densed phase, a novel, extremely sharp transition is observed at low compression, which is attributed to the uncurling of the hydrophobic alkane chains upon compression.     

Vibrational modes of oxygen on W(110)

Electron energy loss measurements of the vibrational modes of oxygen on W(110) as a function of coverage up to 0.5 monolayer are presented and analyzed. A single loss at 67 meV is observed initially; with increasing exposure this loss shifts to 72 meV and another loss appears at 47 meV. These data indicate coexistence of two species on the surface with a coverage-dependent conversion. Angular profiles of the specular elastic beam show a dramatic increase in width with initial oxygen coverage; this is possibly due to an oxygen-induced static disordering of the W surface layer.     

X-ray spectroscopic investigation of some chromium compounds

The intensity distribution of theKα doublet in chromium metal and some of its compounds, CrB, CrSb, Cr₂Te₃, K₂CrO₄, and CaCrO₄, has been investigated by means of a high resolution X-ray spectrometer provided with a bent topaz crystal (radius one meter). From the results obtained it seems that the bonding of Cr is largely metallic in CrB while it is largely covalent in the CaCrO₄ and Cr₂Te₃ compounds. On the other hand, the bonding is essentially ionic in K₂CrO₄ while it is both ionic and covalent in CrSb. The line width of the six valence compounds are found to be larger than that of chromium metal. This shows that the 2p— 3d electrons interaction is not mainly responsible for the large line width found. It may probably be attributed to the crystal field.     

Vibrational spectroscopic and force field studies of copper(II) chloride and bromide compounds,and crystal structure of KCuBr3

Vibrational spectroscopic and force field studies have been performed of 15 related copper(II) chloride and copper(II) bromide compounds, including hydrated salts crystallizing in ternary aqueous systems with alkali and ammonium halides. For halocuprates with distorted octahedral coordination characteristic stretching Raman wavenumbers, corresponding to symmetric stretching Cu^II X modes in the equatorial plane, were found in the ranges 247–288 cm⁻¹ for X = Cl, and 173–189 cm⁻¹ for X = Br, while the low‐wavenumber stretching modes for the weaker axial Cu X interactions varied considerably. The tetrahedral coordination for Cs₂CuCl₄ and Cs₂CuBr₄ leads to somewhat lower Cu X symmetric stretching wavenumbers, 295 and 173 cm⁻¹, respectively. The assignments of the copper–ligand stretching vibrations were performed with the aid of normal coordinate calculations. Correlations between force constants, averaged Cu X stretching wavenumbers and bond distances have been evaluated considering the following aspects: (1) Jahn–Teller tetragonal distortion (axial elongation) of the octahedral copper(II) coordination environment, (2) differences between terminal and bridging halide ligands (3) effects of coordinated water and the influence of outer‐sphere cations. Force constant ratios for terminal and bridging metal–halide bonds reveal characteristic differences between planar and tetrahedrally coordinated M₂X₆ species. In the hydrated copper(II) halide complexes, the halide ligands are more strongly bound than coordinated water molecules. The crystal structure of KCuBr₃ (K₂Cu₂Br₆), which was determined to provide structural information for the force field analyses, contains stacks of planar dimeric [Cu₂Br₆]²⁻ complexes held together by weak axial Cu Br interactions. Copyright © 2007 John Wiley & Sons, Ltd.     

若干具有[（PO4）4Mo6^VO15]^12^-簇骼的化合物的光谱研究

Five novel organic-molybdenum phosphates with [(PO4)4Mo6(V)O15]12- cluster, Na x (H4TETA)3 x (H3O)5 x {Zn[(HPO4)2(PO4)2Mo6O15]2} (2), (H2en)7 x (H3O)4 x {Cu[(HPO4)2(PO4)2Mo6O15]2} x H2O (3), (H3DETA)2 x (H3O)3 x {Co0.5[(HPO4)2(PO4)2Mo6O15]} x H2O (4), [Co(H3TETA)]2{Co0.5[(HPO4)(PO4)3Mo6O15] x 3.5H2O (5) and (H3DETA) x (H3O)4 x {Co1.5 [(HPO4)2(PO4)2Mo6O15]} x 0.5H2O (6), have been synthesized. The relationship between their properties and structures was studied by using FTIR, NIR FT-Raman, UV-Vis DRS and fluorescence etc. In these compounds, every two [(PO4)4Mo6O15] clusters are coordinated by a metal atom to form a {M[(PO4)4Mo6O15]2} dimer. In compound 2, 3 and 4, {M[(PO4)4Mo6O15]2} dimers are hydrogen-bonded by the organic molecules and water molecules to form a three-dimensional expended framework, respectively. In compound 5 and 6, {Co[(PO4)4Mo6O15]2} dimers are coordinated by [Co(H3TETA)] groups and [CoO4] tetrahedra to form a network, respectively. These characteristic vibrational frequencies of the molybdenum phosphates are related to the structure of these compounds. Three characteristic bands in UV-Vis DRS spectra of these compounds have to be attributed to the absorptions of O(d) --> Mo, O(mu) --> Mo and O --> M charge transfer, respectively. These compounds exhibit strong fluorescence emission bands at about 410 nm when excited by 240 nm, which are caused by O(mu) --> Mo charge transfer.