Li2O-CaO-Gd2O3-SiO2:Eu,Bi体系的结构和发光性能之间的关系

用X射线粉末衍射法研究了Li₂O-CaO-Gd₂O₃-SiO₂:Eu,Bi发光体系的物相组成随Gd₂O₃含量的变化,探讨了不同硅酸盐物种和结构对Eu³⁺和Bi³⁺发光特性的影响。结果表明,无Gd₂O₃组分时发光体是β-CaSiO₄多晶体,当Gd₂O₃/SiO₂比超过2.5%时,Ca₂Gd₈(SiO₄)₆O₂和LiGd₉(SiO₄)₆O₂物相逐渐增加,当其成为主要物相时,EU³⁺发光呈数倍增强,这2种含钆物相的结构既利于EU³⁺的红光发射又利于敏化剂向激活剂传输能量,所形成的固熔体是优良的发光基质材料。     

铸态及快淬态CeMg10Ni2合金电化学储氢热力学及动力学性能研究

为了改善CeMg₁₀Ni₂合金的电化学储氢性能,快淬技术被用来制备具有非晶纳米晶结构的CeMg₁₀Ni₂合金. 运用X射线衍射及高分辨透射电镜对合金的微观结构及其相组成进行分析. 通过恒电流充放电、高倍率放电、交流阻抗以及动电位极化测试对合金的电化学性能进行了详细研究. 研究结果表明,铸态合金由多相结构组成,经过快速凝固处理的合金内部含有大量的非晶纳米晶结构,而且增加的凝固速度可以增强合金内部的非晶纳米晶形成能力. 快速凝固处理减小了合金的热力学参数（ΔH和ΔS）,降低了合金氢化物的热稳定性,改善了电化学放电容量. 另外,快速凝固处理显著改善了合金的电化学动力学性能,合金的表观活化能变化进一步解释了这一结论.     

稀土焦绿石化合物Er-2Fe4/3W2/3O7的高温高压多形转变

F.Basile和M.A.Subramanian等人在常压高温下合成出变形的焦绿石化合物Er₂Fe_4/3W_2/3O₇,并用X射线粉末衍射法定出其结构属六方晶系。但对这种化合物的高温高压结构研究未见文献报导。我们在高压高温下进行了这种化合物的多形转变的研究。     

影响TiMnx非计量比合金储氢容量的结构因素

以TiMn_x (x = 1.4, 1.5, 1.6, 1.7)非计量比合金为对象,系统研究了储氢容量与其内在结构之间的相关性。结果表明,所有合金的主相均为C14型Laves相,但其储氢容量却存在显著差异。其中TiMn_1.4合金的储氢量约为0.65% (w,质量分数),吸/放氢平台较倾斜,且存在明显的滞后;而TiMn_1.5合金的可逆储氢量达到1.2% (w),平台较为平坦;但继续增加x,其储氢量反而降低,如x = 1.6合金的储氢量仅为0.30% (w),而x = 1.7合金则几乎不吸氢。进一步结构解析表明,上述储氢容量的迥异主要归因于部分Ti原子占据Mn(2a)位置,且其占位率随x的增加而降低,随之C14相中贮氢四面体间隙体积减小;而引起贮氢四面体间隙体积发生变化的主要因素是Ti―Ti键和Mn(2a)―Mn(2a)键的键长,其中Mn(2a)―Mn(2a)键长的增加对合金储氢容量的提升起关键作用。     

Synthesis and low temperature fluorination of the alkaline-earth palladates Ba2−xSrxPdO3 (x = 0–2)

Since the discovery of superconductivity in Sr₂CuO₂F_2+δ there has been an increased interest in ternary oxide-fluorides. Sr₂CuO₂F_2+δ is prepared via low temperature (T = 220 °C) reaction routes. Low temperature fluorination induces an interesting structural rearrangement in the parent compound Sr₂CuO₃, which is a one-dimensional material containing linear chains of vertex sharing CuO₄ squares along the crystallographic b axis. Upon fluorination, one oxide is substituted by two fluorides and Cu²⁺ becomes octahedrally coordinated by four oxides and two fluorides. The fluorinated compound Sr₂CuO₂F_2+δ displays the T-type structure (La₂CuO₄). Insertion of excess fluorine, δ, also takes place and this fluorine occupies interstitial sites in the T structure. Although the starting material Ca₂CuO₃ is isostructural to Sr₂CuO₃, Ca₂CuO₂F_2+δ displays the T′ (Nd₂CuO₄) structure due to the smaller radius of Ca²⁺ compared to that of Sr²⁺.

The alkaline-earth palladates with the general formula A₂PdO₃ (A = Ba, Sr) are isostructural with the A₂CuO₃(A = Ca, Sr) materials. We prepared the Ba_2−xSr_xPdO₃ (x = 0–2) series and performed low temperature fluorination, which led to the synthesis of the series Ba_2−xSr_xPdO₂F_2+δ (0 ≤ x ≤ 1.5). All the compounds in the Ba_2−xSr_xPdO₂F_2+δ series show T′ structure (Ca₂CuO₂F_2+δ). Similarities and differences with Sr₂CuO₂F_2+δ and Ca₂CuO₂F_2+δ will be discussed.     

Thermal stability of osmium mixed oxides I. CaOsO3 decomposition products: A new orthorhombic phase Ca2Os2O7

The thermal decomposition of CaOsO₃ by differential thermal analyses, thermogravimetry and X-ray powder diffraction has been studied. In nitrogen CaOsO₃ decomposes at 880 ± 10°C into CaO, osmium metal and oxygen due to the reaction CaOsO₃ → CaO + Os + O₂. In static air the decomposition occurs in three stages: 2CaOsO₃ + 1/2O₂ → Ca₂Os₂O₇ (in region 775–808°C), Ca₂Os₂O₇ → Ca₂Os₂O_6,5 + 1/4O₂ (at a temperature interval of 850–1000°C) and in the third stage Ca₂Os₂O_6,5 → 2CaO + OsO₄ ÷ 1/4 O₂ (at 1005 ± 5°C). The first intermediate Ca₂Os₂O₇ is isostructural with orthorhombic Ca₂Nb₂O₇ and its cell parameters are: a₀ = 3.745 Å, b₀ = 25.1 Å, c₀ = 5.492 Å, Z = 4, space group Cmcm or Cmc2. Ca₂Os₂O₇ exhibits metallic conductivity and its electrical resistivity is 4.6 × 10⁻² ohm-cm at 296K.     

Gd2ZnTiO6∶Dy3+, Eu3+单基质白光荧光粉的制备与发光性能

采用溶胶-凝胶法制备出Dy³⁺, Eu³⁺共掺杂Gd₂ZnTiO₆白光荧光粉. 通过X射线衍射(XRD)、 扫描电子显微镜(SEM)、 光致发光(PL)光谱对荧光粉的物相、 形貌及荧光性质进行了表征. 结果表明, 所制备的样品均为双钙钛矿结构, 属于单斜晶系(空间群: P2₁/n), 形貌为2~5 μm无规则形状的颗粒. 在392 nm近紫外光的激发下, Gd₂ZnTiO₆∶Dy³⁺,Eu³⁺荧光粉展现出Dy³⁺的蓝光、 黄光发射以及Eu³⁺的特征红光发射. 此外, 通过调节Dy³⁺和Eu³⁺的掺杂浓度, 可实现低色温的暖白光发射. 基于样品优异的荧光性能, 该荧光粉在近紫外激发白光LED中具有一定的开发潜力.     

制备方法对Nd_2O_3上过氧物种光诱导生成的影响

分别采用水解、水热和燃烧法制备了三种主要物相均为立方Nd_2O_3的样品。以325 nm激光为激发源,在室温和空气气氛下对上述样品上过氧物种的光诱导生成情况进行了比较考察。经Raman光谱仪的激光束照射后,三种样品上均可检测到过氧物种的生成,但燃烧法制备的样品上过氧的生成速率显著大于其他两种样品。O_2-和CO_2-TPD(程序升温脱附)的表征结果表明,与水解和水热法制备的立方Nd_2O_3相比,燃烧法制备的样品表面含有更多的低配位晶格氧物种,晶格氧的碱性也更强,因而更有利于在光诱导下与分子氧反应生成过氧物种。     

Pu在Gd2Zr2O7基质中的模拟固化: (Gd1-xCex)2Zr2O7+x的热物理性能研究

采用高温固相反应,以NaF作助熔剂,在1000 ℃的温度下合成了锕系元素Pu的模拟固化体(Gd_1-xCe_x)₂Zr₂O_7+x (0 ≤ x ≤ 0.7).研究了模拟固化体的物相、热膨胀系数(TEC)、热导率(TC)随温度及组成的变化规律.粉末X射线衍射(XRD)测试结果表明: Gd₂Zr₂O₇基质本身呈弱有序烧绿石结构,而用Ce⁴⁺取代Gd³⁺的模拟固化体都呈缺陷萤石结构. (Gd_1-xCe_x)₂Zr₂O_7+x的Ce(3d) X射线光电子能谱(XPS)有六个峰,结合能分别位于881.7, 888.1, 897.8, 900.4, 907.1, 916.1 eV处,与CeO2的XPS图谱非常相似,说明Ce为四价.随着温度的升高,所有样品的热膨胀系数总体上呈增大趋势.在室温至750 ℃附近,大部分样品的热导率随温度的升高而降低,之后热导率又呈小幅上升.在相同温度下,固化体(Gd_1-xCe_x)₂Zr₂O_7+x (0 ≤ x ≤ 0.7)的热膨胀系数及热导率随组成变化呈相同趋势:在0 ≤ x ≤ 0.1范围内随x的增大而增大,随后在x = 0.1-0.7时逐渐减小.     

高功率镍氢电池La1-xMgx(NiCoAl)3.6金属氢化物电极的电化学性能研究

MH-Ni电池具有电化学比能量高、耐过充/放电性能好、无记忆效应和环境友好等优点而得到广泛应用.金属氢化物电极是MH-Ni电池的核心材料,其研究工作主要集中在稀土AB₅系、钛系、锆系和镁基等合金作为MH-Ni电池金属氢化物电极方面.但这些体系合金的电化学容量低.     

Ce1-xGdxO2-x/2的溶胶-凝胶法合成及其性质

利用溶胶-凝胶法合成了Ce₁-xGdxO_2-x/2(x=0.1～0.6)系列固体电解质,系统地研究了其结构、热膨胀系数和导电性.XRD结果表明,160℃即完全形成立方萤石结构.由于溶胶-凝胶法合成的物质粒度均匀,颗粒小,故在较低温度(1300℃)时即可形成高致密样品,此温度明显低于传统的高温固相法烧结温度(1600～1650℃).高温X射线衍射测得Ce_0.8Gd_0.2O_1.9的热膨胀系数为8.125×10^-6K₁.阻抗谱表明,溶胶-凝胶法合成可减少或消除固体电解质的晶界电阻,600℃时Ce_0.8Gd_0.2O_1.9的电导率为5.26×10^-3S/cm,活化能E_a=0.82eV.     

内嵌金属碳氮化物团簇富勒烯的稳定性与生成机理

Fullerene molecules have nano-scale cavities in which various metal or metal clusters of different sizes can be embedded to form metallofullerenes with unique core-shell structures. The physical and chemical properties of metallofullerenes can be modified through the interaction between the encapsulated metals and the fullerene cages. As such, the investigation of metallofullerenes with novel structures has been a principal research focus in the field of fullerenes. In this study, we investigated the size matching effect between encapsulated clusters and fullerene cages for the endohedral metal carbonitride clusterfullerenes in order to discover new metallofullerenes. The stability and electronic structure of the metallofullerenes formed by encapsulating M₃NC clusters (M = Y, La, Gd) into D₂(186)-C₉₆ and D₂(35)-C₈₈ fullerenes were studied using quantum chemical calculations. It was found that the fullerene cages formed stable structures by accepting six electrons transferred from the encapsulated clusters. The change in configuration of the encapsulated clusters was clarified by a comparison with the corresponding M₃N@C_2n metal nitride clusterfullerenes; the size matching effect between M₃NC cluster and fullerene cage was elucidated on the basis of the calculated results and previous studies on Sc₃NC@I_h(7)-C₈₀. For the D₂(186)-C₉₆ fullerene, the Gd₃NC cluster was found to have smaller changes in the configuration as compared with the La₃NC cluster, proving that Gd₃NC is more suitable than La₃NC for encapsulation in the D₂(186)-C₉₆ fullerene cage. In addition, it was determined that the La₃NC cluster requires a large structural change to maintain its planar configuration. For the D₂(35)-C₈₈ fullerene cage, the Y₃NC cluster is more suitable than Gd₃NC for encapsulation owing to the smaller size of the Y₃NC cluster. The spatial distribution of the highest occupied and lowest unoccupied molecular orbitals (HOMO and LUMO) of Gd₃NC@D₂(186)-C₉₆ were found to be similar to those of Gd₃N@D₂(186)-C₉₆. However, a unique endohedral cluster-based occupied molecular orbital was found for Gd₃NC@D₂(186)-C₉₆. This orbital is derived from the interaction between the NC unit and the Gd atoms. The spatial distribution of the HOMO of Y₃NC@D₂(35)-C₈₈ is similar to that of Y₃N@D₂(35)-C₈₈, while the LUMO of Y₃NC@D₂(35)-C₈₈ has a much larger contribution from the endohedral cluster as compared to Y₃N@D₂(35)-C₈₈. Thus, the addition of a carbon atom in the cluster has a remarkable impact on the electronic structure of the metallofullerenes. With respect to structural characteristics, we found that the three fullerene cages, D₂(186)-C₉₆, D₂(35)-C₈₈, and I_h(7)-C₈₀, have a uniform distribution of five-membered carbon atom rings; these fullerenes can be greatly stabilized in the form of C_2n^6- anions. However, the formation mechanism of fullerenes and metallofullerenes, at present, is poorly understood. Based on the structural analysis, we propose a direct mechanism for the formation of fullerenes without the Stone-Wales isomerization, i.e., the rearrangement of five-membered rings through the addition of carbon atoms and the transformation into larger carbon cages while maintaining stable structural units.     

A New Tubular Borate Built by[B14O24(OH) 6]12- Cluster Units

Anew mixed alkali and alkaline-earth metal borate Na₄Ca₂[B₁₄O₂₂(OH)₆]·2H₂O(1) has been made under a mild solvothermal condition and characterized by single-crystal X-ray diffraction, infrared(IR) spectroscopy, UV-Vis diffuse reflectance spectroscopy, powder X-ray diffraction and thermogravimetric analysis, respectively. Compound 1 features a 1D tube based on[B₁₄O₂₄(OH)₆]^12-({B₁₄}-1) oxo-boron clusters. Such a tube built by {B₁₄}-1 units has been discovered for the first time in borate system. These tubes are arranged orderly to generate 2D layers and a further 3D supramolecular network through hydrogen bond interactions. UV-Vis diffuse reflectance spectrum reveals that compound 1 is a wide band-gap semiconductor and has potential application in UV region.     

Lanthanide and Transition Metal Coordination Polymers via Hydrothermal Reaction

Studies on the syntheses, structures and properties of lanthanide-transition metal complexes are of current great interest, because they can provide good models for investigation of the nature of magnetic exchange interaction between 3d and 41metal ions in the magnetic materials containing rare earth metals. Many of such studies were focused on discrete complexes which were synthesized from the conventional self-assembly reactions in solution. Although several infinite lanthanide-transition metal complexes containing organic ligands have been obtained by conventional solution synthetic method, the polymeric complexes have been poorly explored. Recently we try to use organic ligands for designing magnetic complexes comprising lanthanide and transition metal ions, especially Gd-Cu, Gd-Zn and Gd-Ag couple,with infinite structures, and hope to provide useful messages for the modeling of the magnetic exchange in magnetic materials. Herein reported are a series of lanthanide and transition metal polymeric complexes[{Gd₂M₃(pydc)₆(H₂O)₁₂}·4H₂O]_n and[{Gd₄M₂(pydc)₈(H₂O)₁₂}·4H₂O]_n (M=Cu, Ag,Zn) with 1D chain and 3D wave-like structure, which were prepared from the hydrothermal reactions of Gd₂O₃, pyridine-2,5-dicarboxylic acid (H₂pydc) and Zn(OAc)₂ or MO, respectively.     

高氯酸二甘氨酸十二水合二铒的晶体结构

在水溶液中合成了甘氨酸铒配合物[Er₂(Gly)₂(H₂O)₁₂](ClO₄)₆·4H₂O单晶,并测定了其晶体结构。该晶体属单斜晶系,P2₁/n空间群。晶胞参数:a=1.0571(2)nm,b=1.0837(2)nm,c=1.7728(4)nm,β=90.09(3)°,V=2.0309(7)nm²,Z=2,D_c=2.239g/cm³.最终偏差因子R=0.055,R_w=0.061.每2个Er³⁺离子由2个甘氨酸羧基桥联成双核结构。Er³⁺离子还与6个水分子的氢原子配位,形成畸变的四方棱柱型配位多面体。     

Ab initio investigation of the magnetic states of Ca2MnO4 and Ca2MnO3.5

An analysis of the electronic and magnetic properties of Ca₂MnO₄ and Ca₂MnO_3.5 is carried out within local spin density functional theory using the augmented spherical wave method. From energy differences between the hypothetic magnetic configurations both systems are found to be insulating antiferromagnets in the ground state with a 1 eV gap. However we identify an intermediate half metallic ferromagnetic state with the Hund’s rule expected moments for Mn^IV (3 μ_B) and Mn^III (4 μ_B, high spin HS configuration), respectively. The latter result of moment magnitude finds support in recent experimental evidence of Mn^III bismuth oxide as a ferromagnet in its ground state. This is characterized by a small density of states (DOS) magnitude of itinerant states in spin (↑) channel pointing to a metallic-like behavior as it is experimentally evidenced. For both Ca₂MnO₄ and Ca₂MnO_3.5 the chemical bonding characteristics are resolved for the two spin channels. Relationship to colossal magnetoresistive compounds is proposed.     

水合肼对锂离子正极材料LiNi_(0.5)Mn_(1.5)O_4性能的影响

以NiSO4和MnSO4为原料,在用共沉淀法经二次干燥制备锂离子电池正极材料LiNi0.5Mn1.5O4的前驱体时,加入水合肼进行还原处理.实验结果发现:经还原处理的前驱体制备正极材料LiNi0.5Mn1.5O4的充放电比容量远远高于同样条件下不经水合肼还原处理的前驱体制备的正极材料的充放电比容量,而且处理前驱体制备的正极材料在高倍率放电条件下电化学行为更好.粉末X射线衍射(XRD)和扫描电镜(SEM)测试结果表明,用还原剂水合肼处理的前驱体合成的样品为单一的尖晶石结构,晶粒呈规则的八面体形貌,没有杂质相,而未处理前驱体合成的样品则含有少量的杂质相.这种杂质相是在前驱体的制备过程中由于Mn(OH)2被O2氧化而形成难溶Na0.55Mn2O4.1.5H2O化合物,最终转变为Na0.7MnO2.05.     

From condensed coordination structure to open-framework by modifying acid ligand

The preparation, crystal structure and properties of a novel 3D coordination polymer Er₂(abdc)₃·5.5H₂O are reported. The rare earth Er²⁺ ion centers are in the 8-member coordination environment. Carboxylic groups bridge erbium atoms to form these building blocks in a bis-monodentate mode, which expands to construct a 3D framework with two channels intersecting each other. The sorption of these channels was studied.     

Ca3Al2Ge3O12:Cr3+的光谱性质及晶场参数计算

为了解Cr3+离子在钙铝锗酸盐Ca₃Al₂Ge₃O₁₂:石榴石中的光谱性质, 合成了Ca₃Al₂Ge₃O₁₂:Cr³⁺多晶材料；测量了其X射线衍射图, 漫反射光谱, 激发、发射光谱等；分析了Cr3+离子在钙铝锗酸盐中的发光特性；计算了其晶场强度(Dq/B), Stokes位移(ΔEs)及黄昆-里斯因子(S)等. 在450 nm激发下, Ca₃Al₂Ge₃O₁₂:Cr³⁺室温发射光谱主要由三个宽带及附加其上的弱R线构成, 分别对应于Cr3+离子的4T1、 4T2、2T2到 4A2 能级跃迁. 低温时R线变得强而锐. 通过计算, Dq/B=2.43, ΔEs=1884 cm-1, S=5.21. 表明在Ca₃Al₂Ge₃O₁₂中Cr³⁺离子处于较弱的晶场强度, 电子-声子耦合较强, 为发展可调谐激光材料提供重要线索.