不同烧结温度对PMN基铁电陶瓷B位有序度的影响

本文研究了不同烧结温度下,CuO添加对0.94PMN-0.06PT(PMN-6PT)弛豫铁电陶瓷B位化学有序度的影响。拉曼和XRD分析结果表明,不同的烧结温度下,离子取代不同,对B位有序度的影响不同。烧结温度在950℃时,主要是Cu2+进入晶格,不影响B位化学有序度;烧结温度在1 080℃时,主要是Cu1+进入晶格,B位化学有序度改变。介温测试所表现出来的弛豫特性与拉曼分析有序度的结果相一致。     

基于金纳米棒刻蚀比色法检测铁、铜离子

采用种子生长法制备金纳米棒(AuNRs)以构建光学传感器,用于 Fe³⁺和 Cu²⁺的高选择性快速可视化检测。在酸性环境中,Fe³⁺和 Cu²⁺通过与 KI溶液反应,将 I^-氧化成 I₂。I₂刻蚀 AuNRs,导致其纵向表面等离子体共振(LSPR)吸收峰蓝移,从而实现对Fe³⁺和Cu²⁺的检测。结果表明,反应温度为50℃时,添加0.8 mL 0.1 mol·L^-1 HCl、2 mL AuNRs生长液和20 mmol·L^-1 KI溶液,与 2 mL 500 μmol·L^-1 Fe³⁺或 30 μmol·L^-1 Cu²⁺反应 25或 90 min,可将 AuNRs刻蚀至 LSPR 吸收峰消失。该方法对 Fe³⁺和 Cu²⁺检测具有高选择性和准确性,对于 Fe³⁺、Cu²⁺共存体系的检测,可通过加入适量 F-与 Fe³⁺生成配合物[FeF₆]3^-完成对 Fe³⁺的化学掩蔽,消除Fe³⁺的干扰,实现共存体系中Cu²⁺的准确检测。     

Ba0.98Bi0.02(Ti0.9Zr0.1)1-xCuxO3陶瓷的介电性能、弛豫行为与结晶化学特性

采用固相合成法, Bi3+作施主掺杂A位, Cu₂₊作受主掺杂B位, 制备了Ba_0.98Bi_0.02(Ti_0.9Zr_0.1)_1-xCu_xO₃(x=0, 0.01, 0.02, 0.03)陶瓷样品。借助XRD、LCR等研究了该陶瓷的结构与介电性能。结果表明:当x=0.03时, 陶瓷样品出现第二相。通过GULP模拟, 缺陷偶极子的稳定性从低到高依次为:[2Bi_Ba^·+V_Ba"]、[2Bi_Ba^·+Cu_Ti/Zr"]、[Cu_Ti/Zr"+V_O^··], 结合实验可知:介电弛豫程度与晶体中缺陷偶极子的存在形式相关, 其中x=0.01时, 晶体中以[2Bi_Ba^·+Cu_Ti/Zr"]为主。随Cu₂₊掺杂量的增加, 介电常数增加, 介电常数与B位键价和呈反比变化、与八面体BO₆的体积呈正比变化。     

周期性密度泛函理论研究NO在Cu2O(111)表面上的吸附

运用广义梯度密度泛函理论(GGA)的PBE方法结合周期平板模型，在DND基组下，研究了NO以N端和O端两种吸附取向在Cu₂O(111)非极性表面上的吸附。通过对不同吸附位置的吸附能和几何构型参数的计算和比较发现：表面上配位不饱和的铜离子(CuCUS)为活性吸附位；NO的N端吸附比O端吸附更为有利，N端吸附时吸附能可达到113.5 kJ·mol^-1，而O端情况下只有39.7 kJ·mol^-1；NO倾斜吸附在Cu₂O(111)表面上，O端吸附时倾斜度更大。在两种吸附取向情况下，N-O键的伸缩振动频率都发生了较大的红移，N端吸附情况下红移150 cm^-1，O端时红移330 cm^-1。前线轨道分析表明，Cu与NO间的吸附作用主要是Cu的d轨道和NO的π^*轨道间的相互作用。表面弛豫的计算表明，Cu₂O(111)面的弛豫对O端吸附方式产生较大影响，考虑表面弛豫时O端吸附为很弱的化学吸附(吸附能为39.7 kJ·mol^-1)，而没有考虑弛豫时吸附能为60.5 kJ·mol^-1。     

Cu2+和Cu+对原代培养的小鼠成骨细胞增殖、分化和钙化的影响

利用噻唑蓝(MTT)法、碱性磷酸酶(ALP)比活性测定、油红O染色和矿化结节染色及定量分析,研究了Cu²⁺和Cu⁺对原代培养的成骨细胞增殖、分化及钙化的影响。结果显示：Cu²⁺(1×10^-9~1×10^-6 mol·L^-1)促进成骨细胞增殖,随时间延长,促进作用变弱。Cu⁺(1×10^-7~1×10^-5 mol·L^-1)抑制成骨细胞增殖,随时间延长,浓度为1×10^-6 mol·L^-1的Cu⁺为促进作用,其余浓度则没有影响。对于成骨细胞分化,Cu²⁺和Cu⁺表现出相似的影响,浓度为1×10^-9和1×10^-6 mol·L^-1时均促进成骨细胞分化,而当浓度为1×10^-7和1×10^-5 mol·L^-1时,则抑制成骨细胞分化,随作用时间延长,大多数浓度均表现为促进作用。测试浓度下的Cu²⁺和Cu⁺均对成骨细胞向脂肪细胞的横向分化表现为促进效应。对矿化功能的影响,1×10^-5 mol·L^-1的Cu²⁺和Cu⁺表现出显著的抑制效应,但随浓度降低,抑制效应变弱。1×10^-7 mol·L^-1的Cu²⁺ 促进成骨细胞矿化结节的形成。结果提示：作用浓度、作用时间及铜离子的价态都是影响Cu²⁺和Cu⁺生物效应转变(从毒性到活性,从损伤到保护,从下调到上调)的关键因素。     

Li＋-CaxPb1－xTiO3湿敏纳米薄膜的激光拉曼光谱、晶格畸变和激光显微组织——应用“软模理论”解谱

测定了标题物Li^＋-Ca_xPb_1－xTiO₃ (缩写为Li-CPT, 其中x＝0.35, Li/Ti＝1.0%, mol/mol, 850 ℃/h)的激光拉曼光谱(LRS)和激光显微组织, 并与湿敏性能极差的纯钛酸铅PbTiO₃ (缩写为PT)以及不同钙掺杂量的钛酸铅Ca_xPb_1－xTiO₃ (缩写为CPT, x＝0.08, 0.16, 0.24, 0.32, 0.40)的LRS进行比较, Li-CPT以及CPT的LRS与PT的LRS相比有很大差别,仅在75, 125, 190, 273和585 cm^－1出现五个谱峰. 应用“软模理论”将其分别归属于PT四方晶相的五个特征单模E(1TO), A₁(1TO), E(2TO), B₁＋E和A₁(3TO)的红移及宽化, PT的其它五个特征单模在Li-CPT及CPT的谱图中完全消失或被淹没. 对于这种拉曼活性的降低, 可以根据“软模理论”与晶格畸变作用的关联加以解释. Pauling离子半径较小的Ca^2＋的掺杂, 等价取代了半径较大的Pb^2＋的晶格位置, 降低了四方晶相畸变度δ＝c/a和不对称性导致的各向异性, 不单消除了薄膜冷却时位移型相变可能引起的破裂, 而且改变了晶格中氧八面体“TiO₆”及十二面体“PbO₁₂”的几何结构和电荷分布, 改变了晶格c轴上M-O (M＝Ti, Pb)键的化学环境, 直接阻尼了M—O键的伸缩振动软模, 减小了电偶矩及其自发极化, 使Li-CPT的振动模的拉曼活性大大降低, 因此LRS提供了一种表征晶格畸变的有效方法, 反过来也佐证了“软模理论”可以用来解释拉曼光谱.     

预处理气氛对CuO/CeO2/γ-Al2O3催化剂表面性质及“NO+CO”反应性能的影响

用不同的预处理气氛制备了CeO₂/γ-Al₂O₃载体以调节表面Ce的价态,并以Cu(CH₃COO)₂为前驱体制备了CuCeAl催化剂。XRD和H₂-TPR的结果表明在还原气氛下处理的CeO₂/γ-Al₂O₃载体具有更多的活性氧原子,因此相应的CuCeAl催化剂表面有更多分散态的Cu²⁺/Cu⁺物种。NO+CO反应的结果表明分散态的Cu²⁺/Cu⁺是NO转化的活性物质,而Cu⁰在低温下具有较好的N₂选择性。因此,同时含有分散态Cu²⁺/Cu⁺和少量晶相Cu⁰的催化剂具有最好的催化性能。     

金属离子对CdS量子点/聚酰胺-胺树形分子纳米复合材料光致发光性能的影响

以聚酰胺-胺树形分子为模板制备了分散好、尺寸均匀的CdS量子点，并用分光光度滴定法研究了Cd²⁺、Zn²⁺、Pb²⁺、Cu²⁺、Mn²⁺几种金属离子对其光致发光性能的影响。发现不同离子对CdS量子点的发光性能影响不同:Cd²⁺和Zn²⁺使量子点荧光增强，Pb²⁺、Cu²⁺和Mn²⁺使其荧光有不同程度淬灭。这归因于金属离子对CdS量子点表面的修饰作用。Cd²⁺能减少由S^2-悬键构成的非辐射复合中心，增强树形分子对量子点表面缺陷的钝化作用，并能在量子点周围形成类肖特基能垒，从而显著增大CdS量子点的光致发光效率。由于ZnS与CdS的晶格参数非常接近，Zn²⁺能起到与Cd²⁺类似的作用，使CdS量子点的发光效率大大增强。Pb²⁺和Cu²⁺能取代Cd²⁺在CdS量子点表面生成窄带隙的壳层，对其发光有很强的淬灭作用。由于块体PbS的带隙比块体CuS窄，故Pb²⁺的淬灭能力强于Cu²⁺。Mn²⁺能破坏Cd²⁺与PAMAM树形分子的配位键，降低树形分子对CdS量子点表面缺陷的钝化作用，且其本身在量子点表面构成了新的荧光淬灭中心，但Mn²⁺也能形成较弱的类肖特基能垒，故对量子点的发光淬灭作用较弱。     

以9-蒽醛为荧光基团的吡唑啉衍生物荧光探针对Fe3+和Cu2+的检测

以9-蒽醛为荧光基团,吗啉环和吡唑环为识别基团,合成了一种新型荧光探针1,5-二苯基-3-（10-（吗啉甲基）蒽-2-基）吡唑啉（PMAP）,利用¹H NMR、¹³C NMR和单晶衍射表征其结构,通过荧光发射光谱和紫外可见吸收光谱研究其离子识别性能。结果表明,探针PMAP对Fe³⁺、Cu²⁺具有良好的识别效果,荧光量子产率分别从0.14降到0.05和0.04,溶液颜色从淡黄色变为蓝色。PMAP与Fe³⁺/Cu²⁺以1∶1的化学计量比形成配合物,检测限约为1 μmol·L^-1。同时,干扰实验表明PMAP具有良好的抗干扰性能。在实际样品中的应用表明,PMAP传感器能有效地检测实际水样中的Cu²⁺和Fe³⁺。另外,根据Fe³⁺、Cu²⁺和H+不同组合时PMAP的量子产率构建了分子水平上的三输入NOR逻辑门电路。     

改性PTFE纤维金属配合物的制备及其光催化降解性能

使用聚丙烯酸接枝改性聚四氟乙烯(PAA-g-PTFE)纤维分别与Fe³⁺及其与Cu²⁺的混合物反应制备改性PTFE纤维铁和铁铜双金属配合物, 并分别使用傅里变换叶红外(FTIR)光谱和紫外-可见(UV-Vis)漫反射光谱(DRS)对两种配合物的化学结构和光吸收性能进行表征. 然后将两种配合物分别作为非均相光Fenton 反应催化剂应用于典型偶氮染料活性蓝222氧化降解反应中, 考察和比较了二者在不同pH介质中对降解反应的催化作用. 结果表明, 在有或无Cu²⁺的存在条件下, 一个Fe³⁺能够与三个PAA-g-PTFE表面的6个羧基发生反应形成配合物, 并且它们在紫外和可见光区表现出好的光吸收特性. 当两种金属离子共存时Cu²⁺比Fe³⁺更容易与PAA-g-PTFE发生配位反应形成铁铜双金属配合物. 在可见光辐射下PAA-g-PTFE铁配合物对不同pH水溶液中染料降解反应均表现出显著的催化作用, 但是溶液pH的升高不利于配合物催化活性的发挥. 而配合物中铁离子含量提高特别是引入Cu²⁺作为助金属离子能够较大幅度地改善其在高pH范围内的催化活性和重复利用性.     

The Crystal Structures of Zr3Al3C5, ScAl3C3, and UAl3C3and Their Relation to the Structures of U2Al3C4and Al4C3

Single crystals of Zr₃Al₃C₅—a carbide previously reported with the formula ZrAlC_2−x—were isolated from a sample prepared by reaction of ZrC with an excess of aluminum. The carbides ScAl₃C₃and UAl₃C₃were synthesized from the elemental components by arc-melting. The crystal structures of these three compounds were redetermined from four-circle X-ray diffractomter data. In the original structure determination of ZrAlC_2−x, the metal positions were found to form close-packed layers in the space groupP6₃/mmc, while the carbon atoms were assumed to occupy 5/6 of the octahedral voids at random. The present structure determination in the space groupP6₃/mc(R=0.024 for 519 structure factors and 23 variable parameters) shows that all carbon positions are fully occupied and one has a trigonal bipyramidal aluminum coordination. The structures of ScAl₃C₃and UAl₃C₃also have originally been determined in the space groupP6₃/mmc. The present structure refinements in the space groupP6₃mc(ScAl₃C₃:R=0.031 for 282Fvalues and 16 variables; UAl₃C₃:R=0.029 for 217Fvalues and 16 variables) essentially confirms the structures with the exception of one aluminum site. In all of these structures the metal atoms are arranged in close-packed layers and together with the previously reported structure of U₂Al₃C₄they form a homologous series with the general formulaT_1+nAl₃C_3+n, wheren=0, 1, 2 for ScAl₃C₃, U₂Al₃C₄, and Zr₃Al₃C₅, respectively. The packing of the metal atoms is represented by the Zhdanov symbols (4)₂, (5)₂, and (6)₂. The arrangement of the aluminum atoms is very similar to that of the binary carbide Al₄C₃, while the other metal atoms form a cubic stacking sequence, as it is found in the binary carbidesTC with NaCl type structure.     

Phase diagram of the In3As2Se6-In3As2S3Se3 system

The In₃As₂Se₆-In₃As₂S₃Se₃ system has been investigated by methods of physicochemical analysis (DTA, X-ray powder diffraction, MSA) and by microhardness and density measurements. The phase diagram of the system, which is the quasi-binary section of the As-In-S-Se quaternary system, has been constructed. The region of the In₃As₂Se₆-based solid solutions is extended to 7 mol %, and the In ₃As₂S₃Se₃-based region to 15 mol %. A new quaternary compound In₆As₄S₃Se₉ is found in the system. Original Russian Text ? I.I. Aliev, R.S. Magammedragimova, A.A. Farzaliev, Dzh. Veliev, 2009, published in Zhurnal Neorganicheskoi Khimii, 2009, Vol. 54, No. 4, pp. 691–694.     

Y2O3包覆LiCo1/3Ni1/3Mn1/3O2的电化学性能

通过在硝酸钇水溶液浸渍并焙烧的简单工艺, 在LiCo1/3Ni1/3Mn1/3O2材料表面包覆了一层Y2O3. 采用X射线衍射(XRD), 扫描电子显微镜(SEM), 透射电子显微镜(TEM), 循环伏安(CV)和恒流充放电对包覆和未包覆的LiCo1/3Ni1/3Mn1/3O2进行了测试分析. 结果表明, Y2O3包覆并没有改变LiCo1/3Ni1/3Mn1/3O2的晶体结构, 只存在于LiCo1/3Ni1/3Mn1/3O2的表面; 与未包覆的材料相比, Y2O3包覆后的材料在高电位下具有更好的容量保持率和放电容量. CV测试表明, 包覆层的存在有效抑制了材料层状结构的转变及电极与电解液的负反应.     

Luminescence properties of efficient X-ray phosphors of YBa3B9O18, LuBa3(BO3)3, α-YBa3(BO3)3 and LuBO3

The samples of YBa₃B₉O₁₈, LuBa₃(BO₃)₃, α-YBa₃(BO₃)₃ and LuBO₃ powders have been synthesized by the solid-state reaction methods at high temperature and their X-ray excited luminescent properties were investigated. All the studied materials show a broad emission band in the wavelength range of 300-550 nm with the peak centers at about 385 nm for YBa₃B₉O₁₈ and LuBa₃(BO₃)₃, 415 nm for α-YBa₃(BO₃)₃ and 360 nm for LuBO₃ powders, respectively. Even though those compounds have the different atomic structures, they have the common structural feature of each yttrium or lutetium ion bonded to six separate BO₃ groups, i.e., octahedral RE(BO₃)₆ (RE=Lu or Y) moiety. This octahedral RE(BO₃)₆(RE=Lu or Y) moiety seems to be an important structural element for efficient X-ray excited luminescence of those compounds, as are the edge-sharing octahedral TaO₆ chains for tantalate emission.     

Structural and magnetic properties of Ba3La3Mn2W3O18

A quaternary phase, Ba₃La₃Mn₂W₃O₁₈, was synthesized in reduced atmosphere (5% H₂/Ar) at 1200 °C and characterized by using powder X-ray diffraction, electron diffraction and high resolution TEM. Ba₃La₃Mn₂W₃O₁₈ crystallizes in rhombohedral space group with the cell parameters, and , and can be attributed to the n=6 member in the B-site deficient perovskite family, A_nB_n−1O_3n. The structure can be described as close-packed [La/BaO₃] arrays in the sequence of (hcccch)₃, wherein the B-site cations, W and Mn, occupy five octahedral layers in every six octahedral layers, which leave a vacant octahedral layers separating the 5-layer perovskite blocks. The B-cation layers in the perovskite block alternate along the c-axis in a sequence of W⁶⁺-Mn²⁺-W⁵⁺-Mn²⁺-W⁶⁺. The bond valence calculation and optical reflection spectrum confirm the presence of W⁵⁺. This compound behaves paramagnetically in wide temperature range and weak antiferromagnetic interaction only occurs at low temperatures.     

Computation of the complexation energies of BH3NH3 and BH3PH3

Extended basis set computations on SCF and CEPA level were performed for BH₃NH₃ and BH₃PH₃ to determine the complexation energy ΔE and the equilibrium distance r(BX) between the “heavy” atoms. Our CEPA results (SCF in parentheses): ΔE(BH₃NH) = ?27(?21.3) kcal/mol, ΔE(BH₃PH₃) = ?17(?11.8) kcal/mol, r(BN) = 1.65(1.68) Å, r(BP) = 1.95(1.99) Å indicate a marked influence of electron correlation on these properties.     

表面配体调控的CH3NH3PbBr3纳米片的聚集自组装

采用热注入的方法合成了CH3NH3Pb Br3纳米片,荧光光谱分析发现稀释一定的倍数会使荧光光谱由451 nm红移到531nm。TEM及XRD分析表明,发光红移是由CH3NH3Pb Br3纳米片聚集自组装导致的颗粒变大引起的。进一步的对比实验表明,油胺在纳米片聚集自组装的过程中起到了至关重要的作用,由此结合XRD和TEM表征,阐述了CH3NH3Pb Br3纳米片聚集自组装的机理。     

Alignment of acentric MoO3F3 anions in a polar material: (Ag3MoO3F3)(Ag3MoO4)Cl

(Ag₃MoO₃F₃)(Ag₃MoO₄)Cl was synthesized by hydro(solvato)thermal methods and characterized by single-crystal X-ray diffraction (P3m1, No. 156, Z=1, a=7.4488(6)Å, c=5.9190(7) Å). The transparent colorless crystals are comprised of chains of distorted fac-MoO₃F₃³⁻ octahedra and MoO₄²⁻ tetrahedra anions, as suggested by the formulas Ag₃MoO₃F₃ and Ag₃MoO₄⁺, and are connected through Ag⁺ cations in a polar alignment along the c-axis. One Cl⁻ anion per formula unit serves as a charge balance and connects the two types of chains in a staggered fashion, offset by . In MoO₄²⁻, the Mo atom displaces towards a single oxide vertex, and in MoO₃F₃³⁻, the Mo displaces towards the three oxide ligands. The ordered oxide-fluoride ligands on the MoO₃F₃³⁻ anion is important to prevent local inversion centers, while the polar organization is directed by the Cl⁻ anion and interchain dipole-dipole interactions. The dipole moments of MoO₃F₃³⁻ and MoO₄²⁻ align in the negative c-axis direction, to give a polar structure with no cancellation of the individual moments. The direction and magnitude of the dipole moments for MoO₃F₃³⁻ and MoO₄²⁻ were calculated from bond valence analyses and are 6.1 and 1.9 debye (10⁻¹⁸ esu cm) respectively, compared to 4.4 debye for polar NbO₆ octahedra in LiNbO₃, and 4.5 debye for polar TiO₆ octahedra in KTiOPO₄ (KTP).     

Sm2O3Ga2O3 and Gd2O3Ga2O3 phase diagrams

Four definite compounds exist in the Sm₂O₃Ga₂O₃ binary phase diagram, namely: Sm₃GaO₆, Sm₄Ga₂O₉, SmGaO₃, and Sm₃Ga₅O₁₂. The $\text{3}\text{1}$ compound is orthorhombic (space group Pnna - Z.4) with the cell parameters: a = 11.40₀Å, b = 5.51₅Å, c = 9.07Å and belongs to the oxysel family. Sm₃GaO₆ and SmGaO₃ melt incongruently at 1715 and 1565°C; Sm₄Ga₂O₉ and Sm₃Ga₅O₁₂ have a congruent melting point at 1710 and 1655°C. With regard to the Gd₂O₃Ga₂O₃ system three definite compounds have been identified: Gd₃GaO₆, Gd₄Ga₂O₉, and Gd₃Ga₅O₁₂. Only the garnet melts congruently at 1740°C with the following composition: Gd_3.12Ga_4.88O₁₂. Gd₃GaO₆, and Gd₄Ga₂O₉ melt incongruently at 1760 and 1700°C. GdGaO₃ is only obtained by melt overheating which may yield an equilibrium or a metastable phase diagram.     

Non-centrosymmetric Ba3Ti3O6(BO3)2

The compound previously reported as Ba₂Ti₂B₂O₉ has been reformulated as Ba₃Ti₃B₂O₁₂, or Ba₃Ti₃O₆(BO₃)₂, a new barium titanium oxoborate. Small single crystals have been recovered from a melt with a composition of BaTiO₃:BaTiB₂O₆ (molar ratio) cooled between 1100°C and 850°C. The crystal structure has been determined by X-ray diffraction: hexagonal system, non-centrosymmetric space group, a=8.7377(11) Å, c=3.9147(8) Å, Z=1, wR(F²)=0.039 for 504 unique reflections. Ba₃Ti₃O₆(BO₃)₂ is isostructural with K₃Ta₃O₆(BO₃)₂. Preliminary measurements of nonlinear optical properties on microcrystalline samples show that the second harmonic generation efficiency of Ba₃Ti₃O₆(BO₃)₂ is equal to 95% of that of LiNbO₃.