The crystal structure of the molybdenum cementite Mo12Fe22C10 (ξ-phase)

The crystal structure of molybdenum cementite Mo₁₂Fe₂₂C₁₀ (-phase) has been determined by means of a single crystal x-ray diffraction study of crystal fragments. The lattice parameters were found to be:a=10.865 (3),b=7.767 (2),c=6.559 (2) Å and =120.13 (2)°, space group C2/m;Z=1. From the analysis ofPatterson maps and differenceFourier analysis the atomic parameters were derived, yielding a residual ofR=0.059. The crystal structure contains octahedral and triangular prismatic groups which accommodate the carbon atoms in their voids, as is usually found in interstitial compounds. The octahedral building group consists of four Mo- and two Fe-atoms, the triangular prism is built up by four Fe-and two Mo-atoms. The mode of filling of the metal polyhedra is discussed.

---

Die Kristallstruktur von Molybdän-Zementit, Mo₁₂Fe₂₂C₁₀ (-Phase)

Zusammenfassung Die Kristallstruktur von Molybdän-Zementit, Mo₁₂Fe₂₂C₁₀ (-Phase) wird auf Grund von Einkristall-Beugungsaufnahmen unter Anwendung vonPatterson-and DifferentialFourier-Analysen bestimmt. In der monoklinen Elementarzelle (a=1.870;b=7.67;c=6.563 Å, =120.1°) Raumgruppe C 2/m befindet sich eine Formeleinheit Mo₁₂Fe₂₂C₁₀ (oderZ=2, Mo₆Fe₁₁C₅). DerR-Wert von 6% für 1200 Reflexe unterstreicht die Richtigkeit der Struktur, die aus oktaedrischen und trigonal prismatischen Gruppen aufgebaut ist. Die Oktaedergruppe besteht aus 4 Mo- und 2-Fe-Atomen, die trigonal prismatische Gruppe aus 4 Fe- und 2 Mo-Atomen. Die Kohlenstoffatome füllen die Lücken dieser Bauelemente, wie es für typische Einlagerungscarbide (Komplexcarbide) erwartet werden kann.

     

膦、胂叶立德的化学与应用——Ⅰ.用红外光谱对膦、胂叶立德结构的研究

以78个带吸电子取代基的膦、胂叶立德的红外光谱的解析为根据,讨论了它们的结构及其与光谱的关系。     

金属四重键化合物M2X4（PMe3）4（M=Cr，Mo，W;X=F，CI，Br，I）结构和电子光谱的密度泛函理论研究

采用密度泛函理论方法，在TZ2P-STO基组水平下，对金属四重键化合物M2Cl4（PMe3）4（M=Cr，Mo，W）和Mo2X4（PMe3）4（X=F，Cl，Br，I）的几何结构进行优化，分析了电子结构，并运用TDDFT方法对其低占据激发态进行了计算．考虑相对论效应的ZORA方法能够较好地重现M2X4（PMe3）4的几何结构．M2X4（PMe3）4的电子结构分析表明其d电子的组态为σ^2π^4δ^2，前线轨道能级顺序为πlig〈πd／σd〈δd〈δd^＊．金属原子和卤素配体的改变虽然使轨道能量发生变化，但没有影响轨道的排布顺序．TDDFT方法对M2Xa（PMe3）4δd→δd^＊和π→δd^＊跃迁能量的计算较为准确，对πlig→δd^＊（LMCT）跃迁能量的计算误差较大．金属原子、卤素配体以及相对论效应对激发能的影响可以根据分子轨道能级的变化给予解释．     

双取代单酰胺与硝酸铀酰萃合物的制备与表征

合成了系列双取代单酰胺萃取剂，利用萃取方法获得了与硝酸铀酰的萃合物。利用元素分析、红外光谱、¹H NMR和¹³C NMR对萃合物进行了表征。结合实验数据初步探讨了萃合物的结构、萃取剂的结构与性能以及萃取体系的三相等问题。     

高氯酸稀土Sm(Ⅲ)开环冠醚(EO4)配合物的晶体结构

The crystal of title compounds belongs to orthorhombic system with space group P2₁2₁2₁ (No.19). The cell parmeters are a=1.432 16(3) nm, b=1.457 20(3) nm， c=3.005 85(6) nm, and V=6 273.0(2) nm³, Z=8, μ(Mo Kα)=22.21 cm^-1， D_c=1.802 g·cm^-3, F(000)=3 416.00, Finally R₁=0.033 and wR₂=0.073 (I>2.00σ(I)), S=1.023. Every center atom Sm(Ⅲ) is surrounded by the two aether chains, the title compound has ten-coordinate structure and the coordination polyhedron shows a Bicapped Square Antiprism. In the crystal, the title compound has the flack of double moleculars and non-symmetry. The anion ClO₄^- does not take part in the coordination. CCDC: 238709.     

Struktur‐ und magnetochemische Untersuchungen an KCuGaF6

Structural and Magnetochemical Studies on KCuGaF₆ The crystal structure of KCuGaF₆ was determined on the base of X‐ray single crystal data (wR₂ = 0.084 for 2476 independent reflections). The compound crystallizes with a = 728.56(4), b = 989.51(6), c = 676.27(3) pm, β = 93.120(5)°, Z = 4 in space group P2₁/c of the pyrochlore related KCuCrF₆ type. The octahedral coordinations [GaF₆] and [CuF₆] are slightly resp. strongly distorted (mean values Ga‐F: 188.2 pm resp. Cu‐F: 188.2/200.1/227.6 pm). The longest distances Ga‐F and the shortest ones Cu‐F are found within octahedral chains of these two kinds of atoms, running along [100] and [001], resp., and being mutually bridged as well (M‐F‐M in between 114 and 145°). The magnetic mole susceptibilities measured at powders and at a single crystal follow the isotropic Heisenberg model for S = ¹/₂, if effects of chain disrupture are considered in the form of some paramagnetic portion. No indication of threedimensional magnetic order is observed down to T = 2 K and low magnetic fields H < 100 G. KCuGaF₆ (J/k = —71 K for the powder) is distinguished this way from the chain structure compounds KCuAlF₆ und Na₂CuScF₇ (J/k = —76 resp. —59 K) which were also magnetically studied and yield similar antiferromagnetic exchange constants J/k.     

含羧酸配体的鼓形有机锡氧簇合物：六聚苯基锡氧3-吲哚丁酸酯的合成及晶体结构

利用Ph3SnOH和3-吲哚丁酸以1：1摩尔比反应，合成了新型含羧酸配体的鼓形 有机锡氧簇合物：六聚苯基锡氧3-吲哚西酸酯。通过元素分析、红外光谱和X射线 单晶衍射对其结构进行了表征。测试结果表明：该化合物为三斜晶系，空间群P1， a=1.1722(6),b=1.5694（8）nm，c=1.7227(9)nm，α=116.251（8）°，β=100. 854（10）°，γ=95.606（9）°，Z=1，V=2.732(3)nm^3，Dc=1.554g·cm^-3，μ =1.420mm^-1，F(000)=1276，R=0.0630，ωR=0.0762。晶体结构中，六配位的锡原 子呈畸变的八面体构型。     

CuO/γ-Al2O3单分散催化剂的XAFS研究

采用XAFS方法研究浸渍法制备并于低温焙烧的CuO/γ-Al2O3催化剂的局域结构.对于CuO负载量小于单层分散阈值的CuO/γ-Al2O3(0.4mmol/100m2),结果表明,CuO物种是以层状分散的孤立原子簇存在于γ-Al2O3载体表面,其第一近邻Cu-O配位环境的结构与晶态CuO的相似,键长和配位数分别为0.195nm和4.对于CuO负载量等于单层分散阈值的CuO/γ-Al2O3(0.8mmol/100m2),已有少量的CuO纳米颗粒生成.对于CuO负载量大于单层分散阈值的CuO/γ-Al2O3(1.2mmol/100m2),其结构与多晶CuO的相近.基于CuO在γ-Al2O3载体上的三种不同分散状态的结构特点,我们提出了CuO/γ-Al2O3催化剂的结构模型.     

碱性水蒸气处理的ZSM-5沸石酸性质及孔结构的影响

 采用XRD，NH3－TPD，比表面积和孔结构测定等研究了在不同温度下用含10％NH3的水蒸气处理时HZSM－5沸石n（Si）／n（Al）＝25）酸性质及孔结构的变化规律．结果表明，随着处理温度的提高，HZSM－5的结构未发生明显的变化；样品的总酸量下降很快，但弱酸分布量相对提高，而强酸分布量相对下降；提高处理温度，样品的比表面积和微孔体积减小，二次孔或中孔体积及外表面积有增大的趋势．     

(μ3-S)FeCo2(CO)7(dppfe)的合成和晶体结构

通过简单取代反应,合成了一个新的混金属簇合物(μ3-S)FeCo2(CO)7(dppfe) (2) (dppfe=Ph2PC5H4FeC5H4PPh2).利用IR,1H NMR,MS 和 X-ray单晶衍射的方法对簇合物2进行了结构表征.簇合物2的晶体属于三斜晶系,空间群为Pī.晶胞参数: a=1.132 4(15) nm, b=1.3670(17) nm, c=1.5769(2) nm,α=114.646(2)°,β=100.340(2)°,γ=100.113(3)°, V=2.0953(5) nm3.