多元金属掺杂改性ZnO/ZSM-5紫外光降解罗丹明B印染废水研究

运用溶胶-凝胶法将纳米ZnO负载于ZSM-5制光催化剂,用Ag、Fe、Cu掺杂改性ZnO/ZSM-5光催化性能并探究光催化剂ZnO/ZSM-5降解罗丹明B(RhB)模拟印染废水性能。以SEM和XRD分析手段对材料进行表征;探究溶液pH、底物初始浓度、光催化剂的用量及光强等因素对ZnO/ZSM-5降解RhB效果的影响。结果表明:ZnO/ZSM-5降解RhB印染废水最佳条件:ZnO/ZSM-5用量0.1 g·L~(-1)、初始浓度5 mg·L~(-1)、pH为7的RhB溶液、在紫外光源20 W的条件下降解RhB速率高达98.8%;Ag、Fe、Cu掺杂量分别:5%Ag-ZnO/ZSM-5、3%Fe-ZnO/ZSM-5、0.01%Cu-ZnO/ZSM-5时RhB的降解率分别高达97.52%、90.07%、87.12%;Ag、Fe、Cu共同掺杂的3%Fe-0.1%Cu-5%Ag-ZnO/ZSM-5催化效果优于单种金属元素掺杂改性材料。     

Fe(Ⅲ)螯合掺杂对g-C3N4光催化性能和活性位的影响(英文)

元素掺杂是一种简单有效的光催化剂改性方法.已有诸多文献报道采用非金属元素(B、P、S)或金属元素(Na⁺, Ni³⁺,Co³⁺, Cu²⁺)对g-C₃N₄进行掺杂改性,但目前对金属掺杂的模型和影响机理尚不清晰.g-C₃N₄作为层状材料,它的表面和边缘有大量的胺基,它对光生载流子的传输起到重要作用.此外,胺基可以与金属通过配位键形成螯合物;与胺基螯合的金属由于其功函数较小,可以捕获半导体的光生电子,并有利于降低光生载流子的复合.本文选用Fe(Ⅲ)对g-C₃N₄进行掺杂改性, SEM-EDS表明, C和N元素均匀分布在g-C₃N₄整个骨架上,而Fe元素主要分布在g-C₃N₄边缘部分;FTIR结果发现,掺杂Fe后, N-Hx伸缩振动峰强度随着掺杂量的增加而降低,证明Fe(Ⅲ)与g-C     

Fe3+-TiO2/SiO2光催化降解罗丹明B的研究

以硅胶为载体,采用溶胶-凝胶法制备了不同掺杂量的Fe3+-TiO2/SiO2光催化剂,并采用SEM,Raman和DRS等手段对其进行了分析和表征.以氙灯为光源,通过对可溶性染料罗丹明B的降解反应,考察了Fe3+-TiO2/SiO2催化剂的光催化活性,探讨了光催化反应中溶液pH值和起始浓度对催化反应的影响.     

F-和Fe3+掺杂对Ti基PbO2阳极性能的影响

采用热分解-电镀法制备了Ti基PbO2,阳极(Ti/PbO2),F-掺杂PbO2阳极(Ti/F-PbO2),Fe3+掺杂PbO2阳极(TiP/Fe-PbO2)和F-,Fe3+共掺杂PbO2,阳极(Ti/F-Fe-PbO2).采用XRD和EDX测试对电极进行了表征,应用加速电解寿命测试和电催化降解4-氯苯酚(4-CP)污水,考察了F-掺杂,Fe3+掺杂和F-,Fe3+共掺杂对PbO2阳极稳定性及电催化活性的影响.结果表明,Ti/F-PbO2和Ti/FePbO2阳极有相近的电催化降解活性,但与Fe3+掺杂相比,F-掺杂大大提高了PbO2阳极的加速电解寿命.对Ti/F-Fe-PbO2阳极,Fe3+掺杂改善了其导电性能.同时F-掺杂提高了阳极的稳定性能,使其有较长的电解寿命.与Ti/PbO2,Ti/F-PbO2和Ti/Fe-PbO2阳极相比,Ti/F-Fe-PbO2阳极的电催化降解活性显著提高,这不仅与其导电性能的改善有关,更与F-掺杂和Fe3+掺杂对4-CP降解的表面协同作用有关.     

磁性Fe3O4/ZnO核壳材料的制备及降解四环素类抗生素

利用共沉淀及退火处理两步法,合成了具有核壳结构的磁性Fe3O4/ZnO纳米材料。采用X射线衍射仪、红外光谱仪、透射电子显微镜及振动样品磁强计(VSM)等技术对材料的组分、形貌及磁力性质进行表征,并以氙灯为光源,以四环素(TC)、强力霉素(DC)和盐酸土霉素(OTC)3种四环素类抗生素为降解目标,模拟测试样品在日光下的光催化活性,并通过改变Zn2+浓度,调节包覆结构从而得到最佳光催化效果。研究表明,ZnO包覆在Fe3O4表面并随Zn2+浓度增大逐渐形成尺寸在100 nm的锥形结构,当Zn2+浓度为0.5 mol/L时,样品对TC、DC和OTC的降解率最大,分别为85%、78%和64%。基于以上的研究显示,合成的磁性Fe3O4/ZnO核壳材料可应用去除水中抗生素,是一种具有高催化活性且能回收利用的新型复合光催化剂。     

Fe3+改性纳米ZnO光催化降解壬基酚聚氧乙烯醚

采用氨浸法制备了不同Fe3 含量的Fe3 /ZnO光催化剂,并用X射线衍射、N2吸附、X射线光电子能谱和紫外-可见漫反射光谱对纳米Fe3 /ZnO进行了表征.以壬基酚聚氧乙烯醚(NPE-10)为模型污染物,分别在紫外光和可见光下考察了纳米Fe3 /ZnO的光催化活性.结果表明,该方法能成功地将Fe掺杂到ZnO晶体上,且随着Fe3 添加量的增加,ZnO的晶粒尺寸逐渐减小,比表面积逐渐增大.与纳米ZnO样品相比,Fe3 /ZnO中Fe2p结合能减小,而Zn2p和O1s结合能增大,ZnO表面的羟基氧和吸附氧含量增加,光催化活性提高.当Fe3 的添加量大于0.5%时,Fe3 /ZnO样品的吸收光谱发生红移,在可见光区出现吸收.光催化降解结果显示,0.5?3 /ZnO样品的光催化活性最高,在紫外光和可见光照射3h后对NPE-10的降解率分别比纯ZnO提高18%和69%.     

水热合成Fe3+掺杂ZnO复合材料及其光催化活性

以Zn(Ac)2·2H2O、Fe(NO3)3·9H2O和NaOH为原料,采用水热法合成了Fe3+掺杂ZnO复合材料. 并用X射线衍射和扫描电子显微镜测试技术对合成样品的结构和形貌进行了表征. 结果表明,Fe3+掺杂ZnO合成产物为直棒状,直径为500 nm,长度为3 μm左右. 样品的紫外可见漫反射分析结果表明,在300～500 nm紫外可见光区域均有强的吸收. Fe3+掺杂ZnO作为光催化剂降解有机染料性能优于纯ZnO材料.     

Fe3+-TiO2/SiO2薄膜催化剂的结构对其光催化性能影响

以硅胶为载体,采用溶胶-凝胶法制备了掺杂不同量Fe3+的TiO2光催化剂(Fe3+-TiO2/SiO2),以氙灯为光源,罗丹明B为目标降解物,对其光催化活性进行了研究.结果表明,Fe3+-TiO2/SiO2比TiO2纳米粉有更好的催化活性,Fe3+的最佳掺入量为0.03％.罗丹明B在粉体和膜催化剂的作用下遵循不同的光催化反应机理.根据XRD,SEM,Raman,XPS和FTIR的表征结果可认为,TiO2在SIO2表面薄膜化和Ti-O-Si键的形成是催化活性提高和降解机理不同的主要原因.     

Er3+/Yb3+共掺纳米In2O3的制备及上转换发光

用低温溶剂热法以乙二醇为溶剂合成了Er3+和Yb3+共掺的In2O3纳米晶。用X射线衍射(XRD)、透射电镜(TEM)、漫反射光谱和上转换发光光谱对样品进行了分析。XRD和TEM结果表明,产物为纯的立方相In2O3结构,粒径约为30 nm;漫反射光谱显示了In2O3∶Er3+,Yb3+纳米晶在522、653和975 nm附近有3个吸收带;在980 nm近红外光激发下,样品发射出中心波长为525及555 nm的绿光和662 nm的红光,分别对应于Er3+的2H11/2→4I15/2、4S3/2→4I15/2和4F9/2→4I15/2跃迁;研究了Er3+和Yb3+离子的不同掺杂浓度对发光强度的影响,确定了Yb3+和Er3+离子的最佳掺杂浓度均为3%;双对数曲线显示绿光和红光的发射过程均为双光子吸收过程,对样品的上转换发光机制进行了初步讨论。     

Li+共掺杂对Er3+-Yb3+∶TiO2紫外、可见和红外发光同步增强研究

采用溶胶-凝胶(Sol-gel)法制备了Li+共掺杂的Er3+-Yb3+∶TiO2粉末。976 nm激光激发下在波长350~1700 nm范围内观察到了紫外、蓝色、绿色和红色上转换发光和红外下转换发光。随着Li+共掺杂浓度由0增大到20mol%,Er3+-Yb3+∶TiO2的紫外、可见和红外发光强度同步增强。低Li+共掺杂浓度引起的Li+固溶以及高Li+共掺杂浓度引起的相变过程相继破坏了Er3+的晶体场对称性,导致紫外、可见和红外发光显著增强。结果表明共掺杂Li+是一种提高Er3+掺杂材料发光性能的有效方法。     

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.     

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.     

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.     

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.     

Nitrato- and fluoroboracites M3B7O13NO3 and M3B7O13F

New boracites containing nitrato- or fluoroanions that appear to be true low-pressure phases have been synthesized at superatmospheric pressures. The M₃B₇O₁₃NO₃ compounds (M = Co, Ni, Cu, Zn, Cd) transform rapidly and reversibly in the temperature region 300–500°C between probable orthorhombic and face centered cubic symmetry, while the M₃B₇O₁₃F compounds (M = Mg, Mn, Fe, Co, Zn) appear to maintain rhombohedral symmetry up to their decomposition temperatures of 800–900°C. True high-pressure boracite-like phases containing F and Cr, Mn, Fe, or Co that decompose upon heating to M₃B₇O₁₃F have also been isolated.     

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).     

Phase states in the Bi4Ti3O12-BiFeO3 section in the Bi2O3-TiO2-Fe2O3 system

Specific features of the thermal behavior of Bi _{m + 1}Fe _m−3Ti₃O_{3m + 3} layered perovskite-like compounds (where m takes integer and some fractional values between 3 and 9) were considered, and the temperature limits of stability of these compounds were determined. The phase diagram of the Bi₄Ti₃O₁₂-BiFeO₃ section through the Bi₂O₃-TiO₂-Fe₂O₃ system was constructed.