硫掺杂氧化锡纳米材料的固相合成及其可见光降解百草枯

以十二烷基苯磺酸钠(SDBS)为模板, 采用低温固相反应法合成了硫掺杂二氧化锡(S-SnO₂)纳米粉体材料, 并用XRD、XPS、SEM、UV-Vis、FTIR及HR-TEM等技术对材料进行了表征, 探讨了S掺杂SnO₂纳米材料对百草枯的可见光降解性能, 分析了S掺杂效应的作用机理。结果表明, 采用固相反应法所得SnO₂及S-SnO₂纳米材料的禁带宽度变窄, SDBS对材料的表面结构具有一定的调控作用。S是以S(Ⅳ)和S(Ⅵ)的形式进入SnO₂晶格形成Sn_1-xS_xO₂晶体结构而不是进入SnO₂晶格间隙, Sn-O-S键的弯曲振动峰介于930~980 cm^-1之间。S的掺杂使SnO₂纳米材料表面活性增强, 光催化降解百草枯的活性依次为SnO₂ 2(SDBS) 2 2(SDBS), 2 h内, S-SnO_2(SDBS)样品对除草剂百草枯的光催化活性达95.2%, 其主要原因是S-SnO_2(SDBS)材料表面有更多的羟基和进入SnO₂晶格的S, 有利光生电荷的有效分离。     

S、Al掺杂TiO2纳米材料的固相合成及其可见光降解性能

采用固相反应法分别合成了硫掺杂二氧化钛(S-TiO2)、铝掺杂二氧化钛(Al-TiO2)及硫和铝共掺杂二氧化钛(S-Al-TiO2)纳米材料,并对材料进行了XRD、SEM、UV-Vis、XPS、Raman、N2吸附-脱附等物相织构表征,同时研究了材料对溴甲酚绿(BCG)的可见光降解活性。结果表明,在S-Al-TiO2纳米材料中,硫以阳离子S6+进入二氧化钛晶格,铝以同晶取代方式占据TiO2晶格中Ti的位置,其晶型为锐钛矿型。S、Al共掺杂能有效地抑制TiO2晶粒的生长,其紫外-可见漫反射吸收光谱涵盖了可见光区并延伸到近红外区域。材料的光催化活性决定于掺杂元素及其掺杂量。在25℃、pH=6.5下,S-Al-TiO2纳米材料对溴甲酚绿的可见光降解具有很高的活性,并服从一级反应动力学规律。当S与Al投料物质的量的比为1∶9时,S-Al-TiO2(1S-9Al)纳米材料对BCG的可见光降解速率常数为0.03286 min-1,分别是纯TiO2、S-TiO2及Al-TiO2的5.46、2.62和4.63倍。50 min内,S-Al-TiO2(1S-9Al)纳米材料对BCG的可见光降解率达80%。     

固相反应法制备磷钼酸(H3PMo12O40)掺杂聚苯胺对其电化学活性的影响

利用固相反应法制备了磷钼酸(H3PMo12O40,简称PMA)掺杂聚苯胺,并以红外光谱(FT-IR)、X-射线衍射(XRD)、循环伏安(cyclic voltamm ogram)等测试方法对聚苯胺进行了表征。结果表明,无论是液相法还是固相法,磷钼酸掺杂于聚苯胺中,仍保持自身结构特征,与传统液相合成的磷钼酸掺杂聚苯胺相比,固相反应法合成的磷钼酸掺杂聚苯胺的晶化率和电活性略差。固相反应法制备的磷钼酸掺杂聚苯胺在对抗坏血酸(AH2)电催化氧化中,表现出比液相合成更好的电催化活性。     

微波辅助溶剂热合成In-Si共改性TiO_2的增强光催化性能

利用微波辅助溶剂热法合成了In-Si共改性的TiO2光催化剂.粉末X射线衍射(XRD)、激光拉曼(Raman)光谱、N2吸脱附(BET)、X射线光电子能谱(XPS)、光致发光(PL)光谱和紫外-可见漫反射光谱(UV-Vis DRS)等实验表明,尽管掺杂和改性后TiO2结晶度略有降低,但不影响光催化剂锐钛相的形成.Si掺杂入TiO2晶格使颗粒变小,比表面积变大.In不能进入TiO2晶格,在TiO2表面形成了In2O3.罗丹明B(RhB)降解实验显示,In-Si共改性TiO2表现出很高的紫外和可见光催化活性,Si:In:Ti的摩尔比为0.03:0.02:1的样品(IST-2)光催化活性最高,紫外光下3 min即可将RhB降解完全,可见光下120 min RhB降解率为97%,这是由材料的高表面积,In2O3-TiO2复合半导体之间高效电荷转移及染料敏化等共同作用所致.对于苯酚,光催化降解则相对缓慢,700 min内尚不能降解完全.     

二氧化钛与针铁矿复合光催化材料的制备与光催化性能

以四氯化钛为钛源,针铁矿(α-FeOOH)为载体,采用水解沉淀法制备了金红石相二氧化钛(Ti₂O)与α-FeOOH的复合光催化材料,并采用X射线衍射、扫描电子显微镜、透射电子显微镜、X射线能量散射谱和X射线光电子能谱对样品进行了表征.结果表明,低温下,金红石相Ti₂O包覆于α-FeOOH表面,并形成复合结构;较高温下,铁离子进入金红石相Ti₂O晶格,并形成铁掺杂金红石相Ti₂O纳米管;中温下,样品兼有复合和掺杂两者特征.在室温下以甲基橙为降解对象,采用钨灯+氘灯(波长200~800nm)为光源,对样品的光催化活性进行了测试.结果表明,样品对甲基橙的光催化降解效果良好;与纯α-FeOOH和金红石相Ti₂O相比,不同结构样品的光催化活性均有所提高,其中,复合兼掺杂型样品的光催化活性最高.由此可见,与α-FeOOH复合和铁掺杂是提高Ti₂O光催化活性的有效途径.     

F~-离子对C掺杂Nb_2O_5纳米粒子生长及光催化性能的影响

在合成C掺杂Nb2O5的基础上,通过引入F-离子合成出具有更高光催化活性的C,F共掺杂Nb2O5光催化材料,对合成样品进行了分析、表征并测试了其光降解罗丹明B的活性,研究了F-离子对C掺杂Nb2O5纳米粒子生长及光催化性能的影响.结果表明,在合成过程中引入F-离子能够促进Nb2O5纳米晶的生长,尤其是沿[001]方向的生长.实验结果还表明,F未进入Nb2O5纳米晶的晶格内部,而是以F-离子的形式分散在Nb2O5纳米结构中,通过促进Nb2O5表面·OH自由基的产生,起到提高合成样品光催化活性的作用.     

H_6P_2W_(18)O_(62)/SiO_2:用模板剂制备及光催化降解二甲酚橙的性能

分别采用非离子表面活性剂(C_3H_6OC_2H_4O)_x(P123),阴离子表面活性剂C_(12)H_(25)NaO_4S(SDS)和C_(18)H_(29)NaO_3S(SDBS)作为模板剂,通过溶胶-凝胶再结合程序升温溶剂热一步法制备了一系列固载杂多酸光催化材料-H_6P_2W_(18)O_(62)/SiO_2。通过傅立叶-红外光谱(FTIR)、X-射线衍射(XRD)、电感耦合等离子体原子发射光谱(ICP-AES)、氮气吸附-脱附测定、透射电子显微镜(TEM)以及扫描电子显微镜配合X-射线能量色散谱仪(SEM-EDS)等测试手段对不同模板剂作用下合成产物进行了对比表征分析。结果表明,不同模板剂作用下的系列固载杂多酸-H_6P_2W_(18)O_(62)/SiO_2产物中母体多酸的Dawson基本结构均未发生明显变化,但固载后比表面积显著不同,其中,经模板剂P123和SDS作用合成的H_6P_2W_(18)O_(62)/SiO_2(P123)和H_6P_2W_(18)O_(62)/SiO_2(SDS)的比表面积高达916和634m~2·g~(-1),且显示为有序介孔材料。以二甲酚橙为模型分子,在微波场作用下,该系列固载多酸光催化性能研究结果显示,它们的光催化活性可被微波显著增强,其中,采用P123作用合成产物的光催化活性最高,60 min内对二甲酚橙的降解率达99%以上。     

可见光响应的硫掺杂TiO2的制备、表征及其光催化活性

采用溶胶-凝胶法制备了硫掺杂TiO2光催化剂粉末.光催化降解罗丹明B实验结果表明,钛酸四丁酯与硫脲的摩尔比Ti/S=2.7∶ 1,经600℃热处理后光催化活性最佳.通过紫外可见漫反射吸收光谱(DRS)、X-射线衍射(XRD)、X-射线光电子能谱(XPS)、傅立叶变换红外光谱(FT-IR)以及表面光电压谱(SPS)等研究结果表明,适量的硫掺杂导致TiO2有效地抑制晶相转变.在热处理过程中由S2-被氧化为S4+并进入TiO2晶格中取代部分Ti4+,发生晶格畸变,带隙变窄,使催化剂吸收光谱红移至550 nm,诱发可见光活性.     

纳米SnO2／TiO2的制备及光催化臭氧化活性

用沉积-沉淀法制备了一系列不同Sn/Ti比例的纳米催化剂SnO2/TiO2, 以糖蜜酒精废水的脱色降解为探针反应, 研究了在紫外光条件下Sn/Ti比和焙烧温度对其臭氧化活性的影响. 结果表明, 在Sn掺杂量为5%(mol)时, 焙烧温度773K时, SnO2/TiO2催化活性最好. XRD、TPR显示, 部分Sn4+可能掺入到TiO2的晶格之中, 形成了Sn-O-Ti键. 紫外漫反射光谱显示, 复合SnO2/TiO2对光的吸收明显增加, 催化活性的提高应归因于SnO2/TiO2表面的臭氧吸附. SnO2/TiO2光催化臭氧化降解糖蜜酒精废水的活性与臭氧在催化剂表面的吸附分解有很大的关系, 光的作用只是强化催化臭氧化的氧化效果.     

锡掺杂Bi2O3可见光响应光催化剂的制备及性能

以硝酸铋和四氯化锡为原料,采用浸渍法制备了纯Bi2O3和Sn掺杂Bi2O3光催化剂。利用X射线光电子能谱、X射线荧光光谱、X射线衍射、扫描电子显微镜、紫外-可见吸收光谱和光致发光光谱对样品进行了表征。在可见光下,利用2,4-二氯苯酚水溶液的光催化降解作为探针反应,考察了样品的可见光催化活性。结果表明,浸渍法能较好地实现Sn的掺杂,催化剂中掺杂剂Sn的价态为+4价,以锡的氧化物形式存在于Bi2O3晶格间隙或晶粒表面。并且掺杂适量的Sn,可有效抑制Bi2O3晶相由四方相向单斜相的转变,拓宽了Bi2O3的可见光响应范围,有效阻止了光生电子和空穴的复合,从而提高了Bi2O3的可见光催化活性。当Sn的掺杂量为2%时(物质的量的分数),Bi2O3具有最好的可见光催化活性。     

Li_(1.3)Ti_(1.7)Al_(0.3)(PO_4)_3,Na_(1.3)Ti_(1.7)Al_(0.3)(PO_4)_3的离子交换研究

研究了在不同温度下的NaNO3和AgNO3水溶液中Li1.3Ti1.7Al0.3(PO4)3和Na1.3Ti1.7Al0.3(PO4)3离子交换行为.实验表明Li1.3Ti1.7Al0.3(PO4)3和Na1.3Ti1.7Al0.3(PO4)3均显示出了高选择性与Na+和Ag+进行离子交换的特征,且对Ag+的选择性高于Na+.升高温度可显著提高Ag/Li和Ag/Na的交换反应速度.     

Crystal growth, structure determination, and optical properties of new potassium-rare-earth silicates K3RESi2O7 (RE=Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu)

Single crystals of K₃RESi₂O₇ (RE=Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu) were grown from a potassium fluoride flux. Two different structure types were found for this series. Silicates containing the larger rare earths, RE=Gd, Tb, Dy, Ho, Er, Tm, Yb crystallize in a structure K₃RESi₂O₇ that contains the rare-earth cation in both a slightly distorted octahedral and an ideal trigonal prismatic coordination environment, while in K₃LuSi₂O₇, containing the smallest of the rare earths, lutetium is found solely in an octahedral coordination environment. The structure of K₃LuSi₂O₇ crystallizes in space group P6₃/mmc with a=5.71160(10) Å and c=13.8883(6) Å. The structures containing the remaining rare earths crystallize in the space group P6₃/mcm with the lattice parameters of a=9.9359(2) Å, c=14.4295(4) Å, (K₃GdSi₂O₇); a=9.88730(10) Å, c=14.3856(3) Å, (K₃TbSi₂O₇); a=9.8673(2) Å, c=14.3572(4) Å, (K₃DySi₂O₇); a=9.8408(3) Å, c=14.3206(6) Å, (K₃HoSi₂O₇); a=9.82120(10) Å, c=14.2986(2) Å, (K₃ErSi₂O₇); a=9.80200(10) Å, c=14.2863(4) Å, (K₃TmSi₂O₇); a=9.78190(10) Å, c=14.2401(3) Å, (K₃YbSi₂O₇). The optical properties of the silicates were investigated and K₃TbSi₂O₇ was found to fluoresce in the visible.     

Near infrared study of aqueous rare-earth ethylsulfates

The near infrared spectra of aqueous solutions of the ethylsulfates of La, Nd, Gd, Tb, Er, Yb, Lu, Y, and Na have been determined from about 0.2 mol-dm^–3 to nearly saturation. The extinction coefficients of water have been calculated taking into account the absorption of ethylslfate anions determined in separate experiments. Their values appeared to be nearly the same as that of pure water. The relative contents of free OH groups in 0.5 and 0.7M solutions have been estimated from the absorbances at 1160 nm. They were lower in solutions of the heavy rare-earth ethylsulfates (Tb, Er, Yb, Lu) than in equimolar solutions of the lighter ones (La, Nd), confirming our previous view that secondary hydration of the heavy trivalent rare-earth cations is distinctly stronger than that of the lighter ones. A comparison of the spectra of these aqueous ethylsulfates with those of perchlorates shows that the structure-breaking ability of the C₂H₅SO ₄ ^– ion is much smaller than that of perchlorate anion.     

Structural studies of five layer Aurivillius oxides: A2Bi4Ti5O18 (A=Ca, Sr, Ba and Pb)

The room temperature structures of the five layer Aurivillius phases A₂Bi₄Ti₅O₁₈ (A=Ca, Sr, Ba and Pb) have been refined from powder neutron diffraction data using the Rietveld method. The structures consist of [Bi₂O₂]²⁺ layers interleaved with perovskite-like [A₂Bi₂Ti₅O₁₆]²⁻ blocks. The structures were refined in the orthorhombic space group B2eb (SG. No. 41), Z=4, and the unit cell parameters of the oxides are a=5.4251(2), b=5.4034(1), c=48.486(1); a=5.4650(2), b=5.4625(3), c=48.852(1); a=5.4988(3), b=5.4980(4), c=50.352(1); a=5.4701(2), b=5.4577(2), c=49.643(1) for A=Ca, Sr, Ba and Pb, respectively. The structural features of the compounds were found similar to n=2-4 layers bismuth oxides. The strain caused by mismatch of cell parameter requirements for the [Bi₂O₂]²⁺ layers and perovskite-like [A₂Bi₂Ti₅O₁₆]²⁻ blocks were relieved by tilting of the TiO₆ octahedra. Variable temperature synchrotron X-ray studies for Ca and Pb compounds showed that the orthorhombic structure persisted up to 675 and 475 K, respectively. Raman spectra of the compounds are also presented.     

电感耦合等离子体光谱法(ICP-AES)测定银精矿中铜、铅、锌、砷、镉、钙、镁、锰含量

针对银精矿样品复杂,难消解的特点,研究了不同酸溶法和碱熔法对样品的消解情况,建立了硝酸,盐酸,氢氟酸,高氯酸消解银精矿的方法。根据元素灵敏度和抗干扰性,选定各元素的测定波长。通过酸溶样和碱熔样测定结果比对,验证了方法准确性。建立了四酸消解-电感耦合等离子体光谱法测定银精矿中铜、铅、锌、砷、镉、钙、镁、锰含量的方法,元素的线性相关系数均在0.9999以上。通过共存元素干扰实验,确定了银精矿中高含量元素(铜、铅、锌、铁、锑、铋等)对测定元素结果没有影响。方法检出限：Cu 0.0063 mg/L, Pb 0.0159 mg/L ,Zn 0.0090 mg/L,As 0.0192 mg/L, Cd 0.0093 mg/L ,Ca 0.0084 mg/L, Mg 0.0075 mg/L, Mn 0.0081 mg/L。测定下限：Cu 0.0105mg/L,Pb 0.0265 mg/L, Zn 0.0150 mg/L, As 0.0320 mg/L, Cd 0.0155 mg/L, Ca 0.0140 mg/L, Mg 0.0125 mg/L,Mn 0.0135 mg/L。3个样品的相对标准偏差在0.87%~3.56%之间,加标回收率在95.00%~103.56%之间。方法流程短,操作简单,快速,灵敏度和再现性高,结果准确可靠,可以满足银精矿中铜、铅、锌、砷、镉、钙、镁、锰含量的测定。     

The crystal chemistry of Bi6TP2O15+x, T=Fe, Ni, Zn: Isomorphism and polymorphism, structural relationship to Bi6TiP2O16

The crystal structures of compounds with nominal compositions Bi₆FeP₂O_15+x (I), Bi₆NiP₂O_15+x (II) and Bi₆ZnP₂O_15+x (III) were determined from single-crystal X-ray diffraction data. They are monoclinic, space group I2, Z=2. The lattice parameters for (I) are a=11.2644(7), b=5.4380(3), c=11.1440(5) Å, β=96.154(4)°; for (II) a=11.259(7), b=5.461(4), c=11.109(7) Å, β=96.65(1)°; for (III) a=19.7271(5), b=5.4376(2), c=16.9730(6) Å, β=131.932(1)°. Least squares refinements on F² converged for (I) to R1=0.0554, wR₂=0.1408; for (II) R₁=0.0647, wR₂=0.1697; for (III) R₁=0.0385, wR₂=0.1023. The crystals are complexly twinned by 2-fold rotation about , by inversion and by mirror reflection. The structures consist of edge-sharing articulations of OBi₄ tetrahedra forming layers in the a-c plane that then continue by edge-sharing parallel to the b-axis. The three-dimensional networks are bridged by Fe and Ni octahedra in (I) and (II) and by Zn trigonal bipyramids in (III) as well as by oxygen atoms of the PO₄ moieties. Bi also randomly occupies the octahedral sites. Oxygen vacancies exist in the structures of the three compounds due to required charge balances and they occur in the octahedral coordination polyhedron of the transition metal. In compound (III), no positional disorder in atomic sites is present. The Bi-O coordination polyhedra are trigonal prisms with one, two or three faces capped. Magnetic susceptibility data for compound (I) were obtained between 4.2 and 350 K. Between 4.2 and 250 K it is paramagnetic, μ_eff=6.1 μ_B; a magnetic transition occurs above 250 K.     

Preparation of ZrO2-TiO2-CeO2 and Its Application in the Selective Catalytic Reduction of NO with NH3

TiO₂,ZrO₂-TiO₂,andZrO₂-TiO₂-CeO₂ were prepared by co-precipitation method and characterized by X-ray diffraction (XRD), specific surface area measurements (BET), temperature programmed desorption (NH₃-TPD), oxygen storage capacity (OSC), and temperature programmed reduction (H₂-TPR). The results showed that ZrO₂-TiO₂-CeO₂ exhibited large number of surface strong acid, possessed some oxygen storage capacity, and strong redox property. The three materials were used as supports and the monolith catalysts were prepared with 1% (w) V₂O₅ and 9% (w)WO₃ for selective catalytic reduction (SCR) of NO with ammonia in the presence of excessive O₂, and the results of catalytic activity showed that the catalyst used ZrO₂-TiO₂-CeO₂ as support yielded nearly 100% NO conversion at 275 °C at a gas hourly space velocity (GHSV) of 10000 h⁻¹, and it had the best catalytic activity and showed great potential for practical application.     

B2O3-Bi2O3-ZnO-Al2O3玻璃助烧剂对BaTiO3陶瓷烧结条件、晶体结构和介电性能的影响

通过调节B₂O₃-Bi₂O₃-ZnO-Al₂O₃(BBZA)玻璃的添加量研究其对钛酸钡(BaTiO₃)陶瓷烧结条件、晶体结构和介电性能的影响。结果表明：添加适量的BBZA玻璃能够有效地将BaTiO₃陶瓷烧结温度由1 350℃降至950℃,并使其致密化。同时,添加BBZA玻璃后,BaTiO₃的晶体结构随着烧结温度的升高而发生转变(立方相→四方相)。另外,BBZA玻璃的引入使BaTiO₃陶瓷的居里峰得到了有效的抑制和拓宽。陶瓷微观形貌显示,玻璃相均匀分布在BaTiO₃晶粒表面。优化的BaTiO₃陶瓷制备条件如下：BBZA添加量(质量分数)为2.0%,烧结温度为950℃。在该条件下制备的BaTiO₃陶瓷介电常数达到1 364,介电损耗低至1.2%。     

The Phase Relations in the System In2O3–TiO2–MgO at 1100 and 1350°C

The phase relations in the system In₂O₃–TiO₂–MgO at 1100 and 1350°C are determined by a classical quenching method. In this system, there are four pseudobinary compounds, In₂TiO₅, MgTi₂O₅ (pseudobrookite type), MgTiO₃ (ilmenite type), and Mg₂TiO₄ (spinel type) at 1100°C. At 1350°C, in addition to these compounds there exist a spinel-type solid solution Mg_2−xIn_2xTi_1−xO₄ (0≤x≤1) and a compound In₆Ti₆MgO₂₂ with lattice constants a=5.9236(7) Å, b=3.3862(4) Å, c=6.3609(7) Å, β=108.15(1)°, and q=0.369, which is isostructural with the monoclinic In₃Ti₂FeO₁₀ in the system In₂O₃–TiO₂–MgO. The relation between the lattice constants of the spinel phase and the composition nearly satisfies Vegard's law. In₆Ti₆MgO₂₂ extends a solid solution range to In₂₀Ti₁₇Mg₃O₆₇ with lattice constants of a=5.9230(5) Å, b=3.3823(3) Å, c=6.3698(6) Å, β=108.10(5)°, and q=0.360. The distributions of constituent cations in the solid solutions are discussed in terms of their ionic radius and site preference effect.     

Microstructures of Some Bi-W-Nb-O Phases

Microstructures of three Bi-W-Nb-O phases have been examined by using high-resolution transmission electron microscopy. Bi₁₇W₂Nb₃O₃₉ and Bi₁₇WNb₃O₃₆ have incommensurate superstructures derived from the defect fluorite-type δ-Bi₂O₃ and can be regarded as intermediate phases between the type II solid solutions in the Bi-Nb-O and Bi-W-O systems. Bi₈W₂Nb₂O₂₃ has a Bi₂WO₆-like subunit cell with a stepped superstructure. Formation mechanisms of various superstructures are discussed.