氧化层结构对铀在CO/H_2气氛中表面反应的影响

用Ｘ射线光电子能谱（ＸＰＳ）分析研究了不同氧化层结构的铀金属试样在ＣＯ（２５℃）和Ｈ２（２００℃）气氛中的表面反应。ＣＯ和Ｈ２与铀金属表层反应后，氧化物中氧含量均减少，Ｏ／Ｕ比值随气体进气量的增加而减少。ＣＯ对铀金属表面的还原效果随铀表层氧化程度的提高而增强，并且强于Ｈ２。当表层氧化物较少、氧化程度较低时，铀试样在Ｈ２气氛中发生氢化反应。     

CO/H在Ru/SiO2和Pt/SiO2催化剂上吸附和反应的成键能研究

采用成键能判据探讨了ＣＯ／Ｈ在Ｒｕ／ＳｉＯ２和Ｐｔ／ＳｉＯ２担体金属催化剂上的吸附和反应，从成键能角度说明了ＣＯ在催化剂上吸附强弱的原因以及ＣＯ氢化活性高低的原因。     

含茂基、烷氧墓及乙酰氧基混合配位镧系金属有机化合物的合成及表征

本文通过二茂基镧系金属氯化物Ｃｐ２ＬｎＣｌ（ＣＰ＝Ｃ５Ｈ５；Ｌｎ＝Ｄｙ，Ｈｏ，Ｙｂ）与等摩尔的ＮａＯＡｃ（Ａｃ＝ＣＨ３ＣＯ）及烷基醇ＨＯＲ（Ｒ＝－ＣＨ２ＣＨ２ＣＨ３，－ＣＨ２ＣＨ＝ＣＨ２）在四氢呋喃溶剂中混合一步反应，合成了六种新的含三种不同配位基的镧系金属有机化合物。化合物的元素分析结果符合通式ＣｐＬｎ（ＯＲ）（ＯＡｃ），红外光谱显示了η＾５－Ｃｐ、ＯＲ及ＯＡｃ基团的特征吸收峰，质谱显示了化合物     

在铜基催化剂上由CO加氢合成低碳混合醇反应速率控制步骤探讨

本文应用“原位”发射红外光谱技术，在２８０℃，０．５ＭＰａ反应条件下，对于Ｃｕ／ＺｎＯ／Ａｌ２Ｏ３催化剂 ＣＯ＋Ｈ２ＣＯ＋Ｈ２＋ＣＯ２反应体系的反应过程进行了动态跟踪结果表明，ＣＯ｜Ｈ２反应体系中，ＣＯ插入表面－烷氧基的金属－碳键可能是生成碳二以上醇的反应速控步骤。     

含茂基、烷氧墓及乙酰氧基混合配位镧系金属有机化合物的合成及表征

本文通过二茂基镧系金属氯化物Ｃｐ２ＬｎＣｌ（Ｃｐ＝Ｃ５Ｈ５；Ｌｎ＝Ｄｙ，Ｈｏ，Ｙｂ）与等摩尔的ＮａＯＡｃ（Ａｃ＝ＣＨ３ＣＯ）及烷基醇ＨＯＲ（Ｒ＝－ＣＨ２ＣＨ２ＣＨ３，－ＣＨ２ＣＨ—ＣＨ２）在四氢呋喃溶剂中混合一步反应，合成了六种新的含三种不同配位基的镧系金属有机化合物．化合物的元素分析结果符合通式ＣＰＬｎ（ＯＲ）（ＯＡｃ），红外光谱显示了η５－ＣＰ、ＯＲ及ＯＡｃ基团的特征吸收峰，质谱显示了化合物的三聚碎片离子峰．基于元素分析、红外光谱及质谱数据，建议化合物可能为三聚体结构，即：［ＣｐＬｎ（ＯＲ）（ＯＡｃ）］３．     

含茂基、烷氧基及氯离子混合配镧系金属有机化合物的合成及表征

本文通过二茂基镧不金属氯化物Ｃｐ２ＬｎＣｌ（Ｃｐ＝Ｃ５Ｈ５；Ｌｎ＝Ｄｙ，Ｙｂ）与烷基醇ＲＯＨ（Ｒ＝－ＣＨ２ＣＨ２ＣＨ３，－ＣＨ２ＣＨ＝ＣＨ２）在四氢呋喃中反应，合成了四个新的含三种不同配位基的镧系金属有机化合物；元素分析，红外光谱及质谱分析表明这些化合物可能具有三聚体结构，即：［ＣｐＬｎ（ＯＲ）Ｃｌ］３。     

清洁及氧修饰Cu（100）表面上CO2加氢制甲醇反应的能量学

分别以清洁及氧悠Ｃｕ（１００）表面作为金属态铜和部分氧化态铜的表面模拟，用键级守恒－Ｍｏｒｅｓ势法研究了两种表面上ＣＯ２加氢制甲醇反应的能量学，计算结果表明，在两种表面上，ＣＯ２加氢制甲醇反应的优势反应途径均为“ＣＯ２，ｓ→ＨＣＯＯｓ→Ｈ２ＣＯｓ→ＣＨ３Ｏｓ→ＣＨ３ＯＨｓ”与清洁铜表面上的相应基元步骤相比，在Ｃｕ（１００）－ｐ（２×２）Ｏ表面上甲醇合成反应各基元步骤具有更低的活化能；ＨＣＯＯｓ是含     

Ni/Al_2O_3催化剂上CH_4部分氧化制合成气机理的IR研究(英文)

在２．９％（ｗｔ）Ｎｉ／Ａｌ２Ｏ３催化剂上用ｉｎｓｉｔｕＦＴＩＲ研究了ＣＨ４部分氧化制合成气的反应机理。结果表明，催化剂表面的活性碳物种与化学吸附的Ｏ原子反应生成ＣＯ；ＣＨ４／Ｏ２（２：ｌ）混合气在催化剂表面吸附的ＩＲ谱图表明只有Ｈ２Ｏ和ＣＯ２存在，说明ＣＨ４和ＣＯ２的重整反应没有发生。因此，我们认为ＣＯ和Ｈ２是一级产物。     

三元体系Y(ClO4)3·3H2O—B15C5—CH3OH(25℃)的半微量相平衡研究

采用半微量相平衡方法研究了三元体系Ｙ（ＣｌＯ４）３．３Ｈ２Ｏ－Ｂ１５Ｃ５－ＣＨ３ＯＨ在２５℃的溶解度，测定了各饱和溶液的折光率。该体系在２５℃生成三种化学计量的配合物，其组成分别为：４Ｙ（ＣｌＯ４）３．３Ｂ１５Ｃ５．１２Ｈ２Ｏ．１２Ｃｈ３ＯＨ（Ｉ），Ｙ（ＣｌＯ４）３．２Ｂ１２Ｃ５．３Ｈ２Ｏ．Ｃｈ３ＯＨ（Ⅲ），其中配合物（Ｉ）和（Ⅱ）是溶解不一致化合物。在甲醇溶剂中，分离制备了配合物（Ⅲ），在６９－     

取代型钨镓杂多配合物的导电性及其磁性

合成了过渡金属取代的钨镓杂多配合物α－Ｎａ７「ＧａＷ１１Ｃｏ（Ｈ２Ｏ）Ｏ３９」．１６Ｈ２Ｏ，α－Ｎａ７Ｈ２「ＧａＷ１０Ｃｏ２（Ｈ２Ｏ）２Ｏ３９」．１６Ｈ２Ｏ和α－ＮａｎＨｍ「ＧａＷ９ＭＥ（Ｈ２Ｏ）３Ｏ３７」．１６Ｈ２Ｏ「Ｍ＝Ｃｏ（Ⅱ），Ｎｉ（Ⅱ，）Ｖ（Ⅴ）」，通过红外，紫外，ＩＣＰ，ＴＧ－ＤＴＡ，ＥＰＲ，ＸＰＳ，＾１８３ＷＮＭＲ，极谱等手段进行了表征。     

Sol-gel synthesis of K3InF6 and structural characterization of K2InC10O10H6F9, K3InC12O14H4F18 and K3InC12O12F18

K₃InF₆ is synthesized by a sol-gel route starting from indium and potassium acetates dissolved in isopropanol in the stoichiometry 1:3, with trifluoroacetic acid as fluorinating agent. The crystal structures of the organic precursors were solved by X-ray diffraction methods on single crystals. Three organic compounds were isolated and identified: K₂InC₁₀O₁₀H₆F₉, K₃InC₁₂O₁₄H₄F₁₈ and K₃InC₁₂O₁₂F₁₈. The first one, deficient in potassium in comparison with the initial stoichiometry, is unstable. In its crystal structure, acetate as well as trifluoroacetate anions are coordinated to the indium atom. The two other precursors are obtained, respectively, by quick and slow evaporation of the solution. They correspond to the final organic compounds, which give K₃InF₆ by decomposition at high temperature. The crystal structure of K₃InC₁₂O₁₄H₄F₁₈ is characterized by complex anions [In(CF₃COO)₄(OH_x)₂]^(5−2x)− and isolated [CF₃COOH_2−x]^(x−1)− molecules with x=2 or 1, surrounded by K⁺ cations. The crystal structure of K₃InC₁₂O₁₂F₁₈ is only constituted by complex anions [In(CF₃COO)₆]³⁻ and K⁺ cations. For all these compounds, potassium cations ensure only the electroneutrality of the structure. IR spectra of K₂InC₁₀O₁₀H₆F₉ and K₃InC₁₂O₁₂F₁₈ were also performed at room temperature on pulverized crystals.     

Li2O-TiO2-SiO2-P2O5和Li2O-TiO2-Al2O3-P2O5体系锂离子固体电解质的制备及性能研究

一些具有NASICON型网格结构的固体电解质具有高的电导率和好的稳定性,NASICON的意思是Na Super Ionic Conductor[1]。当NaZr2(PO4)3中P5 被Si4 部分取代时便可以得到具有NASICON结构的Na1 xZr2SixP3-xO12体系,其具有高的钠离子电导率。然而有相同结构的Li1 xZr2SixP3-xO12体系的离子电导率却很低,这是因为Li 半径太小,而NASICON三维网格结构的离子通道太大,两者不匹配而使电导率下降[2]。但当LiZr2(PO4)3中Zr4 被离子半径小些的Ti4 取代,所得LiTi2(PO4)3的通道就与Li 半径相匹配,适合于锂离子的迁移,从而使其电导率…     

Magnetic properties of Ca2F2-xMnxO5

Magnetic susceptibility of Ca₂F_2-xMn_xO₅ members crystallizing in two different structures, one having octahedral (O), tetrahedral (T) and square-pyramidal (SP) coordination of transition metal atoms (OTSP structure) and the other having octahedral and tetrahedral coordination (OT structure), has been investigated. Susceptibility behaviour of the oxides with OTSP structure is different from that of the oxides with OT structure. Ca₂Fe_1-33Mn_0-67O₅ with OTSP structure shows an antiferromagnetic ordering while the corresponding oxide with OT structure shows weak ferromagnetism. Contribution No. 398 from the Solid State and Structural Chemistry Unit     

Structure Study of Bi2.5Na0.5Ta2O9 and Bi2.5Nam−1.5NbmO3m+3 (m=2-4) by Neutron Powder Diffraction and Electron Microscopy

The crystal structures of Bi_2.5Na_0.5Ta₂O₉ and Bi_2.5Na_m-1.5Nb_mO_3m+3 (m=3,4) have been investigated by the Rietveld analysis of their neutron powder diffraction patterns (λ=1.470 Å). These compounds belong to the Aurivillius phase family and are built up by (Bi₂O₂)²⁺ fluorite layers and (A_m-1B_mO_3m+1)^2- (m=2-4) pseudo-perovskite slabs. Bi_2.5Na_0.5Ta₂O₉ (m=2) and Bi_2.5Na_2.5Nb₄O₁₅ (m=4) crystallize in the orthorhombic space group A2₁am, Z=4, with lattice constants of a=5.4763(4), b=5.4478(4), c=24.9710 (15) and a=5.5095(5), b=5.4783(5), c=40.553(3) Å, respectively. Bi_2.5Na_1.5Nb₃O₁₂ (m=3) has been refined in the orthorhombic space group B2cb, Z=4, with the unit-cell parameters a=5.5024(7), b=5.4622(7), and c=32.735(4) Å. In comparison with its isostructural Nb analogue, the structure of Bi_2.5Na_0.5Ta₂O₉ is less distorted and bond valence sum calculations indicate that the Ta-O bonds are somewhat stronger than the Nb-O bonds. The cell parameters a and b increase with increasing m for the compounds Bi_2.5Na_m-1.5Nb_mO_3m+3 (m=2-4), causing a greater strain in the structure. Electron microscopy studies verify that the intergrowth of mixed perovskite layers, caused by stacking faults, also increases with increasing m.     

La3Ru8B6 and Y3Os8B6, new members of a homologous series R(A)nM3n−1B2n

Two new compounds, La₃Ru₈B₆ and Y₃Os₈B₆, were synthesized by arc melting the elements. Their structural characterization was carried out at room temperature on as-cast samples by using X-ray diffractometry. According to X-ray single-crystal diffraction results these borides crystallize in Fmmm space group (no. 69), Z=4, a=5.5607(1) Å, b=9.8035(3) Å, c=17.5524(4) Å, ρ=8.956 Mg/m³, μ=25.23 mm⁻¹ for La₃Ru₈B₆ and a=5.4792(2) Å, b=9.5139(4) Å, c=17.6972(8) Å, ρ=13.343 Mg/m³, μ=128.23 mm⁻¹ for Y₃Os₈B₆. The crystal structure of La₃Ru₈B₆ was confirmed from Rietveld refinement of X-ray powder diffraction data. Both La₃Ru₈B₆ and Y₃Os₈B₆ compounds are isotypic with the Ca₃Rh₈B₆ compound and their structures are built up from CeCo₃B₂-type and CeAl₂Ga₂-type structural fragments taken in ratio 2:1. They are the members of structural series R(A)_nM_3n−1B_2n with n=3 (R is the rare earth metal, A the alkaline earth metal, and M the transition metal). Structural and atomic parameters were also obtained for La_0.94Ru₃B₂ compound from Rietveld refinement (CeCo₃B₂-type structure, P6/mmm space group (no. 191), a=5.5835(9) Å, c=3.0278(6) Å).     

The crystal chemistry of Bi6TP2O15+x, T=Fe, Ni, Zn: Isomorphism and polymorphism, structural relationship to Bi6TiP2O16

The crystal structures of compounds with nominal compositions Bi₆FeP₂O_15+x (I), Bi₆NiP₂O_15+x (II) and Bi₆ZnP₂O_15+x (III) were determined from single-crystal X-ray diffraction data. They are monoclinic, space group I2, Z=2. The lattice parameters for (I) are a=11.2644(7), b=5.4380(3), c=11.1440(5) Å, β=96.154(4)°; for (II) a=11.259(7), b=5.461(4), c=11.109(7) Å, β=96.65(1)°; for (III) a=19.7271(5), b=5.4376(2), c=16.9730(6) Å, β=131.932(1)°. Least squares refinements on F² converged for (I) to R1=0.0554, wR₂=0.1408; for (II) R₁=0.0647, wR₂=0.1697; for (III) R₁=0.0385, wR₂=0.1023. The crystals are complexly twinned by 2-fold rotation about , by inversion and by mirror reflection. The structures consist of edge-sharing articulations of OBi₄ tetrahedra forming layers in the a-c plane that then continue by edge-sharing parallel to the b-axis. The three-dimensional networks are bridged by Fe and Ni octahedra in (I) and (II) and by Zn trigonal bipyramids in (III) as well as by oxygen atoms of the PO₄ moieties. Bi also randomly occupies the octahedral sites. Oxygen vacancies exist in the structures of the three compounds due to required charge balances and they occur in the octahedral coordination polyhedron of the transition metal. In compound (III), no positional disorder in atomic sites is present. The Bi-O coordination polyhedra are trigonal prisms with one, two or three faces capped. Magnetic susceptibility data for compound (I) were obtained between 4.2 and 350 K. Between 4.2 and 250 K it is paramagnetic, μ_eff=6.1 μ_B; a magnetic transition occurs above 250 K.     

Ag/Ag2MoO4/Bi2MoO6复合光催化剂的制备及其光催化性能

采用水热、化学沉积和原位光还原的方法成功制备了新型Ag/Ag₂MoO₄/Bi₂MoO₆三元复合光催化剂。通过X射线粉末衍射（XRD）、扫描电子显微镜（SEM）、X射线光电子能谱（XPS）和紫外可见漫反射光谱（UV-Vis DRS）等技术对材料的组成、形貌、光吸收特性和光电化学性能等进行系统分析。以四环素为目标污染物,研究Ag/Ag₂MoO₄/Bi₂MoO₆在可见光下的光催化性能。研究结果表明,相比于纯Ag₂MoO₄和Bi₂MoO₆,Ag的表面等离子体共振（SPR）效应显著拓宽了催化体系对可见光的吸收能力及响应范围。当Ag₂MoO₄理论负载量（质量分数）为24.6%时,Ag/Ag₂MoO₄/Bi₂MoO₆复合材料在20 min内可将四环素完全降解,且5次循环使用后仍保持较高的催化活性,表现出良好的循环稳定性。     

Ag/Ag2MoO4/Bi2MoO6复合光催化剂的制备及其光催化性能

采用水热、化学沉积和原位光还原的方法成功制备了新型Ag/Ag₂MoO₄/Bi₂MoO₆三元复合光催化剂。通过X射线粉末衍射(XRD)、扫描电子显微镜(SEM)、X射线光电子能谱(XPS)和紫外可见漫反射光谱(UV-Vis DRS)等技术对材料的组成、形貌、光吸收特性和光电化学性能等进行系统分析。以四环素为目标污染物,研究Ag/Ag₂MoO₄/Bi₂MoO₆在可见光下的光催化性能。研究结果表明,相比于纯Ag₂MoO₄和Bi₂MoO₆,Ag的表面等离子体共振(SPR)效应显著拓宽了催化体系对可见光的吸收能力及响应范围。当Ag₂MoO₄理论负载量(质量分数)为24.6%时,Ag/Ag₂MoO₄/Bi₂MoO₆复合材料在20 min内可将四环素完全降解,且5次循环使用后仍保持较高的催化活性,表现出良好的循环稳定性。     

一维纳米Co_3O_4,Ag/Co_3O_4及CuO/Co_3O_4的合成与电催化性能(英文)

采用水热合成法制备了Co3O4及复合Ag/Co3O4、CuO/Co3O4一维纳米产品。用XRD,FE-SEM和TEM手段对产品进行了表征。采用循环伏安法研究了合成产品修饰的玻碳电极在碱性溶液中对对硝基苯酚的电催化还原性能。与裸玻碳电极相比,1mmol·L-1的对硝基苯酚在用Co3O4、特别是CuO/Co3O4修饰的玻碳电极上还原的峰电流明显增大,用Ag/Co3O4(Ag/Co原子比分别为1∶5和2∶5)修饰的玻碳电极催化还原对硝基苯酚时,尽管还原峰电流增大不是太大,但其峰电位明显降低(分别降低0.265和0.371V)。     

Synthesis and structural characterization of Al7C3N3-homeotypic aluminum silicon oxycarbonitride, (Al7−xSix)(OyCzN6−y−z) (x∼1.2, y∼1.0 and z∼3.5)

A new aluminum silicon oxycarbonitride, (Al_5.8Si_1.2)(O_1.0C_3.5N_1.5), has been synthesized and characterized by X-ray powder diffraction (XRPD), transmission electron microscopy (TEM), energy dispersive X-ray spectroscopy (EDX) and electron energy loss spectroscopy (EELS). The title compound is hexagonal with space group P6₃/mmc and unit-cell dimensions a=0.322508(4) nm, c=3.17193(4) nm and V=0.285717(6) nm³. The atom ratios of Al:Si and those of O:C:N were, respectively, determined by EDX and EELS. The initial structural model was successfully derived from the XRPD data by the direct methods and further refined by the Rietveld method. The crystal is most probably composed of four types of domains with nearly the same fraction, each of which is isotypic to Al₇C₃N₃ with space group P6₃mc. The existence of another new oxycarbonitride (Al_6.6Si_1.4)(O_0.7C_4.3N_2.0), which must be homeotypic to Al₈C₃N₄, has been also demonstrated by XRPD and TEM.