氮掺杂纳米多孔TiO2∶EDTA-Na2辅助水热合成及光催化性能

利用螯合剂乙二胺四乙酸二钠(EDTA-Na₂)作为致孔剂,以三氯化钛(TiCl₃)为前驱体,利用水热法直接合成了氮掺杂的纳米多孔TiO₂。通过 SEM、XRD、IR、低温N2吸附-脱附、XPS、热重分析(TG)和紫外可见(UV)光谱对样品进行了表征与分析。结果表明所合成TiO₂以锐钛矿相形式存在,氮掺在TiO₂晶面之间,具有典型的介孔结构和较高的比表面积,通过改变EDTA-Na₂的浓度,比表面积可控制在95~216 m²·g^-1之间。这种纳米多孔TiO₂在光降解甲基橙的实验中表现出很好的光催化活性,且随着EDTA-Na₂的浓度增大而逐渐增加。     

多孔TiO2的合成条件对其光催化性能的影响

利用微波辅助水热法,以十八胺作为软模板合成了多孔TiO2;对多孔的TiO2进行XRD、N2吸附脱咐等温曲线、比表面积的表征.研究了超声波的能量、温度、硝酸的浓度对多孔结构形成的影响;并以甲苯为目标污染物,考察了合成的多孔TiO2在紫外光下的光催化活性.结果表明,多孔TiO2的光催化活性要比无孔道结构的TiO2的光催化活性高.     

TiO2纳米管的模板法制备及表征

TiO2纳米材料在太阳能的储存与利用、光电转换、光致变色及光催化降解大气和水中的污染物等方面具有广阔的应用前景,成为重点研究的课题之一[1～5].目前,以TiO2纳米粉体和纳米膜的研究较为普遍,而TiO2纳米管的报道不多.由于纳米管比纳米膜具有更大的比表面积,因而具有较高的吸附能力,可望提高TiO2的光电转换效率.模板法(包括多孔阳极氧化铝膜(PAA)、光刻蚀制备的纳米模板、聚碳酸酯纳米滤膜等)在制备导电聚合物、金属、碳、无机半导体等纳米管或线型材料方面已得到广泛应用[6～9],在这些模板中,PAA膜具有均匀分布的垂直于表面的相互平行的密集纳米孔,且孔径、孔间距、膜厚可以通过电化学手段加以控制[10～13].     

光电化学水氧化用多孔单晶金红石TiO2纳米棒阵列光阳极的设计和构建

光电化学电池(如染料敏化太阳能电池、量子点敏化太阳能电池以及光电化学水分解电池)是实现太阳能转化及存储的有效手段之一.其中,光电极是光电化学电池的核心组成部分,它集光吸收、光生电荷输运及转移等决定光转化效率的关键过程于一身,因此构筑高活性半导体光电极以实现高效太阳能转化利用引起研究者广泛关注.多孔TiO2纳米颗粒堆垛薄膜光阳极因具有大的比表面积,可提供更多的染料(量子点)担载和反应活性位点,在光电化学电池中表现出优异活性而被广泛研究.然而, TiO2纳米颗粒间大量存在的晶界对光生电荷有较强的散射作用,降低了光生电荷的收集效率.英国牛津大学Snaith研究小组利用模板辅助水热过程首次获得了(001)晶面占优的多孔单晶锐钛矿TiO2微米颗粒,这种多孔单晶TiO2微米颗粒在具有大比表面积的同时,其单晶结构还能有效去除晶界对电荷的散射作用,因而具有优异的电荷输运特性.利用这种多孔单晶TiO2微米颗粒组建的光阳极用于染料敏化太阳能电池中,展现出优异的太阳能光电转化性能.受该工作启发,各种形貌的多孔单晶TiO2微米颗粒作为光催化剂和光电化学分解水用光阳极材料被广泛研究,并表现出优异活性.在单晶微米颗粒堆垛成的薄膜光电极中,虽然单个单晶微米颗粒中晶界对电荷的散射作用被有效抑制,但是单晶颗粒间的晶界仍然存在并影响光生电荷的收集效率.为了彻底抑制晶界对光生电荷的散射作用,每个单晶颗粒都应该贯穿整个薄膜,例如一维TiO2纳米棒单晶阵列薄膜.虽然一维单晶阵列薄膜能够有效提高光生电荷的收集效率,但相对于多孔薄膜具有较小的比表面积,限制了担载染料(量子点)和反应位点的数量.为了增大TiO2单晶纳米棒阵列薄膜的比表面积,目前主要的手段包括调控纳米棒长径比、表面修饰TiO2纳米颗粒以及二次生长构建TiO2枝晶阵列.本文首次提出通过制备多孔单晶TiO2纳米棒单晶阵列薄膜来获得高比表面积和高光生电荷收集效率的光阳极,提高光电化学电池的效率.在透明导电薄膜(FTO)表面利用水热生长TiO2纳米棒阵列薄膜之前,预先在FTO基体上沉积一层SiO2球密堆模板, TiO2纳米棒单晶阵列在从FTO表面向上生长过程中,会将SiO2球模板包裹进TiO2纳米棒中,再通过碱溶液将SiO2球模板溶解,首次在FTO基体上原位生长出多孔单晶TiO2纳米棒阵列薄膜.将所得多孔单晶金红石TiO2纳米棒阵列薄膜作为光电化学分解水电池光阳极,其光电化学分解水活性相对于实心单晶金红石TiO2纳米棒阵列提高了2.6倍.多孔单晶金红石TiO2纳米棒阵列光阳极性能的提升可归因于：(1)多孔结构赋予多孔单晶金红石TiO2纳米棒阵列薄膜更大的比表面积,可提供更多的反应活性位点;(2)多孔结构能够有效缩短单晶金红石TiO2纳米棒中光生电荷体相输运距离,提高光生电荷的收集效率;(3)多孔结构通过对光多次反射吸收可有效增强光吸收,产生更多光生电荷参与水分解反应;(4)在制备过程中引入Si掺杂,导致多孔单晶金红石TiO2纳米棒带隙扩大了0.1 eV,带隙增大归因于导带位置负移0.1 eV,光生电子具有更强的还原能力,光电流起始电位相应负移约0.1 V.     

三维有序介孔/大孔TiO2微球的制备、表征及光催化性能

以聚甲基丙烯酸甲酯微球为模板,分别以钛酸四丁酯和四异丙醇钛为钛源,通过溶胶-凝胶法辅助模板法制得TiO2纳米微球前驱体,并用程序升温控制其焙烧温度,最终成功制得了具有三维有序介孔/大孔复合结构的TiO2微球.以罗丹明B(RhB)为模型污染物,探索了以不同钛源制备得到的介孔/大孔复合TiO2微球的光催化性能;并采用XRD、SEM、TEM、UV-vis DRS、比表面积测试、光催化性能测试等对样品的晶粒尺寸、物相、形貌、光吸收、比表面积及性能等进行了分析.结果表明,运用溶胶凝胶法辅助模板法能够合成结晶度高、形貌规整、比表面积大、光催化活性良好的锐钛矿相TiO2微球.     

N掺杂TiO_2纳米管阵列的制备及可见光光催化性能研究

分别以氨水、乙二胺、丁胺为氮源,利用阳极氧化法和湿化学法合成氮掺杂的二氧化钛(TiO2)纳米管阵列.通过扫描电镜(SEM)、X射线衍射(XRD)、X射线光电子能谱(XPS)等表征方法对氮掺杂TiO2纳米管形貌,晶型和氮元素掺杂方式进行分析,并通过可见光光催化降解六氯苯(HCB)废水,研究氮元素掺杂方式与可见光光催化活性的关系.结果表明有序排列的TiO2纳米管阵列垂直生长在钛基底表面,管长500nm左右,管径100nm左右.氮元素掺杂阻碍了TiO2晶粒的增长,抑制了锐钛矿向金红石相的转变.无机氮比有机氮更加利于氮元素进入TiO2晶格,取代态氮比间隙态氮表现出更高的可见光光催化活性.     

多孔二氧化钛微球的制备、表征及其光催化性能

以Lutensol TO(异构十三醇聚氧乙烯醚)系列非离子表面活性剂为辅助剂,采用溶胶-凝胶法制备了比表面积高、孔径分布窄的锐钛矿型TiO2多孔微球,并用透射电镜、扫描电镜、热重-差热分析、X射线衍射和氮吸附进行了表征.以亚甲基蓝降解为模型反应评价了其光催化性能,并与商品化TiO2Degussa P25进行了比较.实验结果表明,样品在425℃焙烧后,形成具有孔状结构的锐钛矿型TiO2微球,粒径为0.7~1.0μm,比表面积为70.5 m2/g,总孔容为0.12 cm3/g,平均孔径为4.26nm,晶粒尺寸为12 nm.这种多孔TiO2微球具有较高的催化活性,与Degussa P25纳米TiO2的催化活性相当.     

La2O3掺杂低温合成介孔锐钛矿相二氧化钛

采用非离子型表面活性剂EO20PO70EO20(P123)为模板剂,钛酸丁酯为钛源,La2O3为促进剂,无水乙醇为萃取剂,使用溶胶-凝胶法合成了具有锐钛矿相介孔结构和高比表面积的纳米TiO2.XRD,BET,IR和HRTEM等表征表明,La2O3的掺杂量对TiO2锐钛矿相的形成具有明显影响,当La2O3掺杂量为0.1%(摩尔分数)时,合成的TiO2锐钛矿相晶型最好,且为介孔结构,孔径大小均一,比表面积达到367.7 m2·g-1.     

HNdNb2O7/(Pt,TiO2)的制备和光催化性能的研究

利用层间插入反应,合成HNdNb2O7/(Pt,TiO2 )层状光催化纳米复合材料.采用X射线衍射、紫外-可见光漫反射、比表面积测定分析等分析手段对所制备的材料进行了表征.通过光照分解水,考察了所制备的材料的光催化性能,结果表明所制备的HNdNb2O7 /(Pt ,TiO2 )纳米复合材料具有较高的光催化分解水效率并且其光催化活性稳定.     

酸法纳米纤维素模板剂合成介孔TiO2及光催化活性

以生物可再生资源的酸法纳米纤维素为模板剂,四氯化钛为钛源,采用液相水解-沉淀法制备了具有介孔结构的TiO2光催化剂。采用低温N2物理吸附-脱附、透射电镜(TEM)、X射线衍射(XRD)、热重-量热扫描(TG/DSC)、傅里叶变换红外(FTIR)、X射线光电子能谱(XPS)等对介孔TiO2进行了表征,并以甲基橙为模型物,考察了介孔TiO2光催化活性。结果表明,以酸法纳米纤维素为模板剂合成的TiO2光催化活性显著提高,且具有良好的孔隙结构,平均孔径5.03 nm、总孔容积0.35 cm3.g-1、比表面积192m2.g-1;纤维素模板剂合成的TiO2表面羟基数量降低;纤维素长链分子结构之间的羟基与TiO2表面羟基的键合,可有效限制TiO2前驱体的生长和团聚,并抑制锐钛矿相TiO2向金红石相转变。     

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.