TiO_2/SiO_2纳米薄膜的光催化活性和亲水性

通过 sol-gel工艺在钠钙玻璃表面制备了均匀透明的 TiO2/SiO2复合纳米薄膜 .实验结果表明 : 当 SiO2添加量较高时 , TiO2/SiO2复合纳米薄膜的光催化活性明显降低 ;当 SiO2添加量较低时 ,TiO2/SiO2复合薄膜的光催化活性无明显变化 .在 TiO2薄膜中添加 SiO2,可以抑制薄膜中 TiO2晶粒的长大 ,同时薄膜表面的羟基含量增加 , 水在复合薄膜表面的润湿角下降 , 亲水能力增强 .当 SiO2含量为 10％－ 20％（摩尔分数）时获得了润湿角为 0°的超亲水性薄膜 .     

TiO2/SiO2纳米薄膜的光催化活性和亲水性

通过sol gel工艺在钠钙玻璃表面制备了均匀透明的TiO2/SiO2复合纳米薄膜.实验结 果表明: 当SiO2添加量较高时, TiO2/SiO2复合纳米薄膜的光催化活性明显降低;当SiO2添加 量较低时,TiO2/SiO2复合薄膜的光催化活性无明显变化.在TiO2薄膜中添加SiO2,可以抑制薄 膜中TiO2晶粒的长大,同时薄膜表面的羟基含量增加, 水在复合薄膜表面的润湿角下降, 亲 水能力增强.当SiO2含量为10％－20％（摩尔分数）时获得了润湿角为0°的超亲水性薄膜.     

CoFe2O4／TiO2磁性复合薄膜的制备及表征

以钛酸丁酯和金属盐酸盐为原料,采用溶胶-凝胶工艺制备了CoFe2O4／TiO2复合薄膜,分析了不同热处理温度对复合薄膜晶粒生长及薄膜表面形貌的影响．通过XRD射线、拉曼光谱、扫描电子显微镜、偏光显微镜对薄膜热分解中物相变化过程及其表面形貌进行了观测,用振动样品磁强计（VSM）测定了样品的磁性．实验结果表明：溶胶-凝胶法制得的复合薄膜,两相组分晶体各自析出长大,CoFe2O4组分均匀地分布在TiO2基体中,随着热处理温度的升高,薄膜的磁性增强．     

W（100）c（2×2）表面的STM图像

用基于第一性原理的密度泛函理论研究了W000）c（2×2）再构表面的表面弛豫以及扫描隧道显微镜（STM）图像和衬底偏压的关系．计算所得到的表面原子沿[110]方向的畸变位移δ为0．027nm,畸变能△E为80．6meV·atom^-1,表面原子的弛豫分别为-7．6％（△d12/d0）和＋0．8％（△d23/d0）,功函数西为4．55eV．STM图像模拟表明,由于表面原子沿[110]方向的位移,会导致出现平行于[110]方向的亮暗带状条纹．STM图像中突起所对应的并不是表面或次表面的钨原子,而是zig-zag型W原子链中线位置;而STM暗区对应于原子位置畸变形成的相邻zig-zag型W原子链中间区域．当衬底负偏压时,STM针尖典型起伏高度大约在0．008-0．013nm之间;而当衬底正偏压时,针尖起伏高度在0．019—0．024nm之间变化．     

TeO2-SiO2/（z-TeO2 Composite Film Prepared by Electrochemical sol-gel Method and Its Non-linear Optical Properties

以异丙醇碲和正硅酸乙酯作为前驱体,配制了稳定的TeO2-SiO2复合溶胶;以之为电解液采用电化学-溶胶凝胶法制备了黑色的凝胶薄膜,将薄膜经热处理后得到灰白色半透明的复合薄膜.分别采用XRD和SEM-EDX研究复合薄膜的晶体结构、表面形貌及其组成,结果表明凝胶薄膜的主要成分为Si,Te,O元素,黑色的凝胶薄膜为TeO2-SiO2/Te,灰白色半透明的复合薄膜为少量Te的SiO2-TeO2/α-TeO2;α-TeO2颗粒和少量Te颗粒均匀分散在TeO2-SiO2凝胶复合薄膜中.采用Z-scan方法测试薄膜的光学性能,结果表明其三阶非线性极化率χ（3）为2.171×10-14（m V-1）2.     

用2-(对磺基苯偶氮)变色酸胶束增溶光度法测定微量镁

在混合表面活性剂（CPB＋OP）存在下，镁（Ⅱ）和2－（对磺基苯偶氮）变色酸（SPADNS）的络合反应发生显著的增敏作用，其λmax为606nm，比无混合表面活性剂时红移33nm，灵敏度提高近11倍，表观摩尔吸光系数（ε'）达1．23×105·mol-1·cm－1.测量的pH范围为10．0～11．3，镁浓度在0～200μg／L内符合比尔定律．Fe3＋、Al3＋等干扰离子可用TEA－甘露醇联合掩蔽。用拟定的方法测定了铝合金中的镁，结果满意．     

Sr2+-TiO2薄膜的制备及超亲水性

以钛酸丁酯作为前驱物,采用溶胶-凝胶法及浸渍-提拉法在载玻片上制备SrO-TiO2薄膜。通过X射线衍射和红外光谱等测试技术表征了SrO-TiO2粉末的结构,用紫外可见分光光度计测定薄膜的透光率,用接触角测试仪测定水与薄膜的接触角。结果表明,掺杂适量Sr2+后,SrO-TiO2粉末中TiO2晶粒的尺寸变小,SrO-TiO2薄膜表面吸附的羟基含量增多且稳定,可提高TiO2薄膜的超亲水性。经紫外光照１ｈ或自然光照５ｈ后,掺杂Sr2+（摩尔分数））为1.0％的SrO-TiO2薄膜与水的接触角接近于0°,表现出良好的亲水性。     

微乳-水热法制备具有自清洁功能的TiO2薄膜

采用热陈化微乳液及浸渍-提拉技术,制备了具有自清洁功能的TiO2薄膜。 考察了微乳液中表面活性剂十二烷基苯磺酸（DBS）的用量对TiO2薄膜的表面形态和微观结构的影响。 进而对合成的TiO2薄膜的光催化活性、光致亲水性能及实际环境中的自清洁效果进行了测试评价。 随着表面活性剂DBS用量的增加,微乳液中的分散质点尺寸减小,但热陈化后所获得的TiO2粒子表现出凝集现象。 在DBS用量为0及58 mg/L时,所获得薄膜表面较为平整,由15~20 nm大小的TiO2粒子组成。 这些薄膜在无紫外光照射时,水接触角增大的速度较慢,并且在紫外光照射下能迅速恢复其超亲水性能。 将薄膜置于室外25 d后其表面无灰尘粘结,水接触角由原来的0°增大至14°~18°。 当DBS用量为580 mg/L以上时,薄膜表面起伏不平,粗糙度过大,对应TiO2薄膜光致亲水性能较差,室外放置25 d后,水接触角由原来的0°增大至46°~48°。     

纳米金/3-氨丙基-三乙氧基硅烷修饰传感器电化学检测NO-2

将3-氨丙基-三乙氧基硅烷（ATS）修饰在玻碳电极表面,再自组装一层纳米金,制备了一种新型NO2^-的电化学传感器。该修饰电极对NO2^-有较好的催化作用。在pH为3时,NO2^-的氧化峰电流与其浓度在5．0×10^-7～1．0×10^-3mol／L范围内呈良好的线性关系,检出限可达2．0×10^-7mol／L。方法具有较高的灵敏度和较好的重现性。     

固体超强酸S2O8^2-／ZrO2-CeO2催化剂的结构与性能表征

用共沉淀法制备了固体超强酸S2O8^2-／ZrO2-CeO2催化剂,通过XRD,FTIR,BET,TEM,DSC／TG等分析手段对其结构进行了表征,并考察了其对乳酸丁酯合成反应的催化活性。结果表明．Ce的引入可以有效地抑制ZrO2晶粒由四方相向单斜晶相转变和催化剂表面含硫物种的流失;当焙烧温度高于500℃时,体系内部有四方相Ce0.16Zr0.84O2固溶体形成,最佳焙烧温度为600℃。在n（乳酸）：n（正丁醇）=1．0：3．0,。（S2O8^2-／ZrO2-CeO2）=12．0％,反应温度145℃,反应时间2．0h的条件下,S2O8^2-/ZrO2-CeO2催化剂对乳酸的酯化率达96．6％。     

Sc2MgGa2 and Y2MgGa2

Scandium magnesium gallide, Sc₂MgGa₂, and yttrium magnesium gallide, Y₂MgGa₂, were synthesized from the corresponding elements by heating under an argon atmosphere in an induction furnace. These intermetallic compounds crystallize in the tetragonal Mo₂FeB₂‐type structure. All three crystallographically unique atoms occupy special positions and the site symmetries of (Sc/Y, Ga) and Mg are m2m and 4/m, respectively. The coordinations around Sc/Y, Mg and Ga are pentagonal (Sc/Y), tetragonal (Mg) and triangular (Ga) prisms, with four (Mg) or three (Ga) additional capping atoms leading to the coordination numbers [10], [8+4] and [6+3], respectively. The crystal structure of Sc₂MgGa₂ was determined from single‐crystal diffraction intensities and the isostructural Y₂MgGa₂ was identified from powder diffraction data.     

Electrochemical study of (NEt4)2Cl2FeS2MoS2 and (NEt4)2Cl2FeS2MoS2FeCl2

Summary The ability of [MoS₄]^2–, anions to be used as ligands for transition metal ions has been widely demonstrated, especially with Fe²⁺. The present study has been restricted to linear complexes such as (NEt₄)₂ [Cl₂FeS₂MoS₂] and (NEt₄)₂[Cl₂FeS₂MoS₂FeCl₂]. Their electrochemical properties are described: upon electrochemical reduction, these compounds yield MoS₂, as a black precipitate, and an iron complex in solution, assumed to be [SFeCl₂]^2–. The electrochemical reduction goes through two electron transfers, coupled with the breakdown of the molecular skeleton: a DISPl and an ECE mechanism. Depending on the solvent, the following equilibrium may be observed: [Cl₄Fe₂MoS₄]^2–[Cl₂FeMoS₄]^2–+FeCl₂. The equilibrium constant, K_D, was evaluated by differential pulse polarography. K_D is tightly related to the donor number of the solvent.     

The alkali hypophosphites KH2PO2, RbH2PO2 and CsH2PO2

The structures of the hypophosphites KH₂PO₂ (potassium hypophosphite), RbH₂PO₂ (rubidium hypophosphite) and CsH₂PO₂ (caesium hypophosphite) have been determined by single‐crystal X‐ray diffraction. The structures consist of layers of alkali cations and hypophosphite anions, with the latter bridging four cations within the same layer. The Rb and Cs hypophosphites are isomorphous.     

Zur Kenntnis der Dialkalimetalldichalkogenide β-Na2S2, K2S2, α-Rb2S2, β-Rb2S2, K2Se2, Rb2Se2, α-K2Te2, β-K2Te2 und Rb2Te2

On Dialkali Metal Dichalcogenides β-Na₂S₂, K₂S₂, α-Rb₂S₂, β-Rb₂S₂, K₂Se₂, Rb₂Se₂, α-K₂Te₂, β-K₂Te₂ and Rb₂Te₂ The first presentation of pure samples of α- and β-Rb₂S₂, α- and β-K₂Te₂, and Rb₂Te₂ is described. Using single crystals of K₂S₂ and K₂Se₂, received by ammonothermal synthesis, the structure of the Na₂O₂ type and by using single crystals of β-Na₂S₂ and β-K₂Te₂ the Li₂O₂ type structure will be refined. By combined investigations with temperature-dependent Guinier-, neutron diffraction-, thermal analysis, and Raman-spectroscopy the nature of the monotropic phase transition from the Na₂O₂ type to the Li₂O₂ type will be explained by means of the examples α-/β-Na₂S₂ and α-/β-K₂Te₂. A further case of dimorphic condition as well as the monotropic phase transition of α- and β-Rb₂S₂ is presented. The existing areas of the structure fields of the dialkali metal dichalcogenides are limited by the model of the polar covalence.     

Formal [(2+2)+2] and [(2+2)+(2+2)] nonconjugated dienediyne cascade cycloadditions

[reaction: see text] Fluoranthene 2 and heptacycle 3 are easily accessible from the reaction of diyne 1 and norbornadiene (NBD) in the presence of the rhodium catalyst. The unusual [(2+2)+(2+2)] adduct 3 was confirmed by the X-ray crystal structure analysis.     

Crystal Structures of [Bu2Sn(O2PPh2)2], [Ph2Sn(O2PPh2)2], and [PhClSn(O2PPh2)OMe]2. Raman Spectra of [Ph2Sn(O2PPh2)2] and [PhClSn(O2PPh2)OMe]2

[(n‐Bu)₂Sn(O₂PPh₂)₂] ( 1 ), and [Ph₂Sn(O₂PPh₂)₂] ( 2 ) have been synthesized by the reactions of R₂SnCl₂ (R=n‐Bu, Ph) with HO₂PPh₂ in Methanol. From the reaction of Ph₂SnCl₂ with diphenylphosphinic acid a third product [PhClSn(O₂PPh₂)OMe]₂ ( 3 ) could be isolated. X‐ray diffraction studies show 1 to crystallize in the monoclinic space group P2₁/c with a = 1303.7(1) pm, b = 2286.9(2) pm, c = 1063.1(1) pm, β = 94.383(6)°, and Z = 4. 2 crystallizes triclinic in the space group , the cell parameters being a = 1293.2(2) pm, b = 1478.5(4) pm, c = 1507.2(3) pm, α = 98.86(3)°, β = 109.63(2)°, γ = 114.88(2)°, and Z = 2. Both compounds form arrays of eight‐membered rings (SnOPO)₂ linked at the tin atoms to form chains of infinite length. The dimer 3 consists of a like ring, in which the tin atoms are bridged by methoxo groups. It crystallizes triclinic in space group with a = 946.4(1) pm, b = 963.7(1) pm, c = 1174.2(1) pm, α = 82.495(6)°, β = 66.451(6)°, γ = 74.922(6)°, and Z = 1 for the dimer. The Raman spectra of 2 and 3 are given and discussed.     

Die Photoionenspektren von SCl2, S2Cl2 und S2Br2

Photoionization Mass Spectra of SCl₂, S₂Cl₂, and S₂Br₂ Photoionization mass spectra of SCl₂, S₂Cl₂, and S₂Br₂ have been measured. Heats of formation, bond energies, and ionization potentials of fragments have been calculated from appearance potentials.