CdS/TiO2纳米管阵列的制备及光催化性能

采用阳极氧化法在纯钛箔上制备出TiO2纳米管阵列,再通过化学水浴沉积法在TiO2纳米管阵列上负载CdS纳米颗粒.利用XRD、FESEM和UV-Vis分光光度计对样品的晶体结构、微观形貌和光学性质进行表征,并研究了不同含量CdS负载的复合薄膜对光催化降解气相苯性能的影响.结果表明,CdS纳米颗粒均匀沉积到TiO2纳米管阵列上,所制备的复合薄膜光吸收带边均扩展到了可见光区.CdS的修饰大幅度提高了TiO2纳米管阵列对气相苯的光催化降解活性,其中负载CdS质量分数为3;的TiO2纳米管阵列光催化活性最佳,80 min内对气相苯的去除率为80;,终产物CO2的浓度为640 mg/m3.     

阳极氧化工艺制备TiO2纳米管阵列及其碳包覆改性

首先采用阳极氧化工艺制备了TiO2纳米管阵列,然后利用水热工艺对其进行C包覆改性,探讨了热处理温度、F-浓度、阳极氧化电压、阳极氧化时间等参数对TiO2纳米管阵列形貌及性能的影响,并初步研究了其生长机理.通过实验得到TiO2纳米管阵列的最佳制备条件:F-浓度0.5wt;;阳极氧化电压30 V;阳极氧化时间1h;热处理温度450℃.C包覆改性后的TiO2纳米管阵列对可见光的吸收明显增强,尿素浓度为20wt;时制得的TiO2纳米管阵列对亚甲基蓝的光降解率高达92.7;,相较于未进行C包覆改性的TiO2纳米管阵列提高了7.9;,说明C包覆改性可以显著提高TiO2纳米管阵列的光催化性能.     

PAN/TiO2复合微粒的制备与表征

采用沉淀法合成聚丙烯腈(PAN),并通过化学吸附法制备得到PAN/TiO2纳米复合微粒.采用透射电镜(TEM)、X射线衍射(XRD)、红外光谱(IR)、X射线光电子能谱(XPS)、紫外可见漫反射吸收光谱(DRS)等方法对复合微粒的结构和性能进行了分析表征.结果表明,复合微粒的形貌、晶型和粒径和纯二氧化钛比较基本没有发生改变;PAN/TiO2纳米复合微粒在可见光区的光吸收能力增强.对甲基橙降解实验研究结果表明,所制备的PAN/TiO2纳米复合微粒具有良好的光催化降解性能,其14 h对甲基橙的降解去除率可以达到86.5;.     

Sm2O3/TiO2对亚甲基蓝染料的光催化降解行为研究

采用浸渍法制备Sm2O3掺杂TiO2的负载型光催化剂Sm2O3/TiO2,考察其在紫外可见光区对亚甲基蓝的光降解行为.利用XRD、N2吸附、SEM、TEM、XPS和ICP-OES等手段表征Sm2O3/TiO2样品,考察Sm2 O3掺杂量和亚甲基蓝浓度对亚甲基蓝紫外光降解活性的影响和催化剂Sm2O3/TiO2的催化稳定性.结果表明,Sm2O3/TiO2对亚甲基蓝的紫外光降解活性高于TiO2,这归因子掺杂Sm2O3引起TiO2的晶体缺陷.这种晶体缺陷作为光生电子和空穴的陷阱实现光生电子-空穴对的有效分离,从而提高Sm2O3/TiO2的光催化活性.Sm2O3/TiO2对亚甲基蓝的光降解活性随着Sm2O3掺杂量的增加先增大后减小,随着亚甲基蓝浓度的增大而减小.Sm2 O3掺杂量5.0wt;的Sm2O3/TiO2对亚甲基蓝紫外光降解的7次循环实验未出现明显失活.     

Ag3PO4/TiO2复合催化剂的制备及光催化性能研究

为提高纳米TiO2的光催化降解性能和稳定性,采用两步水热法制备具有高催化性能的Ag3PO4/TiO2复合催化剂,采用XRD、SEM、EDS、XPS、TEM等仪器对其表面微观形貌和形态大小、表面元素组成、物相结构等进行表征,并研究了TiO2的比表面积和Ag3PO4颗粒尺寸大小对Ag3PO4/TiO2光催化性能的影响.以亚甲基蓝(MB)和苯酚为目标降解物来考察复合光催化剂的光催化性能.结果表明:1h后Ag3PO4、TiO2、Ag3PO4/TiO2对亚甲基蓝的降解率为25;、42;、92;;复合光催化剂Ag3PO4/TiO2经过5次光催化降解实验后,对亚甲基蓝的降解率仍可达78;.     

TiO2/P3HT纳米复合材料光催化降解甲基橙的动力学研究

用化学氧化聚合法制备了导电聚合物聚3-己基噻吩(P3HT).用聚3-己基噻吩改性纳米二氧化钛,合成TiO2/P3HT纳米复合微粒.对其光催化降解甲基橙的反应动力学进行了分析,测定了反应的表观活化能.结果表明,纯纳米TiO2和TiO2/P3HT纳米复合微粒光催化降解甲基橙的反应均为一级反应;纳米TiO2经聚3-己基噻吩(P3HT)修饰后在可见光下的光催化活性得到提高,且提高降解温度有利于提高甲基橙的降解率,纳米TiO2经P3HT修饰后降解甲基橙的表观活化能由23.44 KJ/mol下降到19.36 kJ/mol.     

Ce/TiO2纳米管阵列的制备及光催化性能的研究

采用电化学阳极氧化法在钛表面制备TiO2纳米管阵列,并用稀土铈对其修饰改性.以甲基橙为目标降解物,考察了Ce3+溶液浓度、甲基橙溶液的初始浓度和初始pH对铈改性的TiO2纳米管光催化活性的影响.结果表明:Ce3+溶液的浓度存在一个最佳值,当Ce3+溶液浓度为0.01 mol/L,在10 mg/L,pH =3的甲基橙溶液中光催化活性最好.光照4h后,甲基橙的降解率达83％.     

生物质改性纳米TiO2的制备及其结构表征

采用溶胶-凝胶法制备了系列生物质改性复合纳米TiO2.以亚甲基蓝溶液为模拟污染物,考察了其可见光催化活性,并确定了最佳制备工艺.通过X射线光电子能谱(XPS)、X射线衍射(XRD)、场发射扫描电镜(FESEM)、紫外-可见漫反射光谱(UV-Vis-DRS)、荧光光谱(PL)等手段对催化剂样品进行了表征.实验结果表明,催化剂对亚甲基蓝的光催化降解适应一级反应动力学,复合TiO2和纯TiO2的反应速率常数分别为0.4990 h-1和0.0305 h-1,且复合催化剂实现了C、N、S、P、K等多元素的共掺杂.相比纯TiO2,复合TiO2的比表面积增大,结晶度升高,光生载流子复合率降低,吸收边带红移,禁带宽度窄化了0.09 eV.     

稀土Sm掺杂对纳米TiO2结构和可见光催化性能的影响

采用溶胶-凝胶法制备了纯TiO2和稀土Sm掺杂TiO2纳米粉体( Sm-TiO2),通过XRD、XPS、FT-IR、UV-Vis-DRS、PL和Nano-sizer纳米粒度仪等对样品进行表征,以亚甲基蓝( MB)的光催化降解为探针反应,探讨稀土Sm掺杂对纳米TiO2的结构和可见光催化性能的影响。结果表明,Sm掺入TiO2后在表面存在Sm3+和Sm2+两种价态, Sm掺杂抑制了TiO2从锐钛矿向金红石的相转变,阻碍纳米晶粒生长,增加了纳米粉体表面羟基含量;适量的Sm掺杂能使TiO2吸收光谱的阈值波长红移,有效降低光生e-/h+的复合率,提高TiO2光催化活性。热处理温度500℃时,掺杂1.0wt;Sm的纳米TiO2样品在普通日光灯下对MB在6 h内的光催化降解效率达97;,明显高于同等条件下Degussa公司产品P25的降解率56;。     

电解液温度对二氧化钛纳米管阵列结构及光电性能的影响

以氟化铵(NH4F)、乙二醇溶液为电解液,在不同的电解液温度(0～50℃)条件下,采用电化学阳极氧化法制备二氧化钛(TiO2)纳米管阵列.采用扫描电子显微镜(SEM)、X射线衍射仪(XRD)、紫外-可见分光光度计(UV-Vis)对TiO2纳米管阵列的形貌、结构和光学性能进行表征.结果表明,电解液温度高于20℃均能制备出纳米管阵列.光照下电解液温度40℃时制备的TiO2纳米管阵列具有最高光电流密度(Iph)0.2408 mA/cm2.以活性艳红X-3B为目标降解物,在室温、紫外光照射条件下考察了电解液温度对光催化活性的影响,结果显示电解液温度40℃时制备的TiO2纳米管阵列具有最高的光催化活性.     

(C2N2H10)2Mg(HP2O7)2·2H2O synthesis and crystal structure

(C₂N₂H₁₀)₂Mg(HP₂O₇)₂·2H₂O, is a new inorganic organic hybrid structure. It has been synthetized using wet chemistry. Its crystal structure consists of cis- and trans-edge sharing [MgO₄(H₂O)₂] octahedra resulting in chains, which are linked via [HP₂O₇] units to form [Mg(HP₂O₇)₂(H₂O)₂]⁴⁻ layers. The Mg²⁺ cations and the ethylendiammonium cations are located on centers of inversion. The ethylendiammonium cations are alternately located in the interlayer space. The cohesion of the crystal is well ensured by coulombic interactions between anions and cations and by several hydrogen bonds. The diphosphate anion shows an eclipsed conformation.     

Crystal structure of Rb2[GeO2(OH)2]·2H2O

Single crystals of Rb₂[GeO₂(OH)₂] · 2H₂O are studied by X-ray diffraction. The crystals belong to the orthorhombic system, sp. gr. Pna2₁, a = 13.523(6) Å, b = 8.143(4) Å, c = 13.407(6) Å, Z = 8, R ₁ = 0.0506. In [GeO₂(OH)₂]^2? anions, the Ge-O distances (1.71–1.73(1) Å) are shorter than the Ge-OH distances (1.76–1.80(1) Å). Anions are linked to each other by pairs of hydrogen bonds to form infinite chains. The chains are linked by hydrogen bonds involving water molecules to form a 3D structure. The assignment of the bands in the IR spectrum of the compound under study is performed.     

Elastic properties of the dithionates Na2S2O6 · 2 H2O,K2S2O6, Rb2S2O6, CaS2O6 · 4H2O and SrS2O6 · 4 H2O

Single crystals of the title compounds having optical quality and dimensions of several cm were grown from aqueous solutions. The elastic and thermoelastic constants were determined from ultrasonic resonance frequencies of thick plates. The true point symmetry of K₂S₂O₆ and Rb₂S₂O₆, which is screened by a hexagonal hypermorphy, could be clearly revealed to be trigonal (32) by the existence of the elastic constant c₁₄. In the case of CaS₂O₆ · 4H₂O and SrS₂O₆ · 4H₂O the constant c₁₄ of the specimens appeared too small to confirm the trigonal symmetry group required from electrooptic and non-linear optic effects unambiguously. The isotypy of K₂S₂O₂ and Rb₂S₂O₆ as well as that of CaS₂O₆ · 4H₂O and SrS₂O₆ · 4H₂O is confirmed by their elastic behaviour. The mean elastic stiffness of dithionates is closely related to that of the corresponding sulphates. In the vicinity of the second-order phase transition of K₂S₂O₆ near 235 K weak anomalies of the temperature derivatives of the longitudinal elastic stiffnesses are observed.     

Optical properties of the germanate melilites Sr2MgGe2O7, Sr2ZnGe2O7 and Ba2ZnGe2O7

Refractive indices and their dispersion in the wavelength range from 365 nm to 2325 nm and transmission ranges of the tetragonal melilite‐type germanates Sr₂MgGe₂O₇, Sr₂ZnGe₂O₇ and Ba₂ZnGe₂O₇ were determined. The uniaxial positive crystals Sr₂MgGe₂O₇ and Ba₂ZnGe₂O₇ both offer the possibility for phase matched second harmonic generation, a detailed analysis of phase matching conditions is given. The refractive indices of Sr₂ZnGe₂O₇ show an isoindex (isotropic) point at 467 nm. The investigation was performed on Czochralski grown large single crystals. The crystal structure of all three germanates were determined by means of X ‐ray diffraction. The results corroborate unmodulated melilite‐type structures at room temperature. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Crystal structure of bis 4-benzyl piperidinium monohydrogenmonophosphate pentahydrate, [C6H5CH2CHCH2CH2NH2CH2CH2]2HPO4·5H2O

The salt bis 4-benzyl piperidinium monohydrogenmonophosphate pentahydrate is orthorhombic with the following unit cell dimensions: a = 11.235(2) Å, b = 27.924(6) Å, c = 9.321(4) Å space group Pca2₁ with Z = 4. The structure was solved by the Patterson method and refined to final R value of 0.049 for 1802 independent reflections. The flack parameter is 0.14 with an e.s.d. of 0.23. The structure consists of infinite parallel two-dimensional [110] planes built of mutually connected ions and water molecules by strong O—H,...,O and N—H,...,O hydrogen bonding. There are no contacts other than normal van der Waals interactions between the layers.     

Optical Properties of MnIn2S2Se2 Single Crystals

Optical transmittance and reflectance spectra of MnIn₂S₂Se₂ single crystals are measured in the wavelength range from 0.5 to 30 μm. The interference method is used to determine the refractive index of the compound for wavelengths between 0.8 and 12 μm. From an analysis of the absorption spectrum it follows that the fundamental edge is due to forbidden indirect transitions between parabolic bands for the polarization E ⊥ c with a gap energy of 1.50 eV at room temperature.     

Identification of a new family of diphosphate compounds, AI2BII3(P2O7)2: Structures of Ag2Co3(P2O7)2, Ag2Mn3(P2O7)2, and Na2Cd3(P2O7)2

Syntheses and single-crystal X-ray structural results are reported for three new mixed diphosphates of the family A^I ₂B^II ₃(P₂O₇)₂; Ag₂Co₃(P₂O₇)₂ (I), Ag₂Mn₃(P₂O₇)₂ (II), and Na₂Cd₃(P₂O₇)₂ (III). All crystallize in the triclinic system, space group P1 bar: (I) a = 5.351(4), b = 6.375(4), c = 16.532(4) Å, = 80.83(6) = 81.45(4), = 72.87(5)°, V = 528.9(6) ų, Z = 2, D _calc = 4.649 mg/m³, R/Rw = 0.0428/0.0548 for 3949 obs. reflns; (II) a = 5.432(7), b = 6.619(6), c = 16.51(3) Å, = 80.78(8) = 82.43(9), = 72.82(7)°, V = 557.7(13) ų, Z = 2, D _calc = 4.338 mg/m³, R/Rw = 0.0679/0.1303 for 2100 obs. reflns and (III) a = 5.67(3), b = 7.08(4), c = 7.90(4) Å, = 77.0(2), = 82.5(2), = 67.8(2)°, V = 286(3) ų, Z = 2, D _calc = 4.249 mg/m³, R/Rw = 0.0307/0.0342 for 1945 obs. reflns. (I) and (II) are isostructural but (III) is of a different type. All three structures are characterized by layers of P₂O₇ groups alternating with layers of mixed metal atoms. Differences are seen in the conglomerate bonding patterns of B atoms and in the irregular geometry of Ag in (I) and (II) compared to the octahedral bonding seen for Na in (III). The differences in structure may be understood in terms of the ratios of the ionic radii of A and B atoms.     

Oxygen-conducting compounds with La2Mo2O9 structure in the ternary system La2Mo2O9-Sm2W2O9-Sm2Mo2O 9 + : Synthesis and properties

Polycrystalline samples in the ternary system La₂Mo₂O₉-Sm₂W₂O₉-Sm₂Mo₂O ₉ ⁺ were synthesized in air. The region of the existence of compounds with the lanthanum molybdate (La₂Mo₂O₉) structure in this system was determined. The polymorphism of the synthesized compounds was studied. Doping with samarium or with samarium and tungsten was shown to lead to the suppression of the transition between the monoclinic and cubic phases α → β and the appearance of the transition β _ms → β between two cubic phases. In samples with a high samarium content, the phase transition β _ms → β manifests itself as significant anomalies in the temperature dependences of the dielectric permeability and electric conductivity. An increase in the concentration of samarium in the samples leads to a substantial decrease in the conductivity compared with the nondoped compound La₂Mo₂O₉.     

Synthesis and characterization of (NH4)2CuBr2Cl2·2H2O crystals

Single crystals of a new compound, (NH₄)₂CuBr₂Cl₂.2H₂O, were grown from saturated aqueous solution at room temperature by slow evaporation method. The grown crystals were characterized through elemental, powder XRD, thermal and DSC analyses and FTIR and far IR spectra. The elemental analysis and the decomposition pattern formulated using the TG‐DTG studies confirm the stoichiometry of the compound. The crystallinity of the compound is confirmed from the powder XRD pattern. A preliminary single crystal X‐ray diffraction structural analysis reveals that the title compound belongs to the orthorhombic system with a = 7.7466 Å, b = 7.783 Å and c = 8.1211 Å. The low temperature DSC shows thermal anomalies at –161.1, –156.5, –152.4, –145.2, –134, –18.5, and 1.4°C during the heating run and at –4.3, –54.8, –66.1, –90.6, –109.7 and –147.2 °C during the cooling run. The thermal hysterses indicate first order phase transitions in the title compound at these temperatures. The FTIR spectra were used to assign the characteristic vibrational frequencies due to NH₄⁺, CuX₄^2– ions and other chemical bonds. The effect of substitution of two bromine atoms on the phase transitions of a closely related crystal, diammonium tetrachloro cuprate dihydrate is also discussed. (© 2005 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Structure of {Pb[S2CN(C2H5)2]2(1,10-phenanthroline)}2

Lead (II) nitrate reacts with 1,10-phenanthroline and sodium diethyldithiocarbamate in water to produce yellow bisdiethyldithiocarbamata 1,10-phenanthroline lead(II). Crystals from water are triclinic, space group $P\bar 1$ (#2),a=10.53(2) Å,b=11.050(12)Å,c=24.74 (3) Å, α=94.71 (9)⁰, β=98.15(11)^o, γ=114.11(9)^o,V=2569(6) ų,Z=2. Each lead atom has approximate pentagonal pyramid coordination geometry through the nitrogens of a phenathroline and sulfurs of two dithiocarbamates. Additionally, complexes form loose dimers in which lead atoms are weakly coordinated to a sulfur in an adjacent complex. IR and proton nmr spectrum of the complex are consistent with the solid state structure.