Bi3Ti4O12/α-Bi2O3/TiO2复合光催化剂的制备及其可见光催化活性研究

以工业二氧化钛(TiO2)、五水合硝酸铋(Bi(NO3)3·5H2O)为原料制备了Bi3Ti4O12/α-Bi2O3/TiO2复合光催化剂.采用X射线衍射(XRD)、透射电子显微镜(TEM)、X射线光电子能谱(XPS)、傅里叶变换红外光谱(FT-IR)、紫外-可见吸收光谱(UV-Vis)、荧光光谱(PL)等表征方法对光催化剂结构进行分析,表明复合样品中形成了Bi3 Ti4 O12/α-Bi2 O3/TiO2异质结结构,其禁带宽度减小、吸收带边红移,光催化效率有明显提高.以亚甲基蓝为目标污染物评价其光催化活性,TiO2与Bi(NO3)3·5H2O质量比为1:2.5,煅烧温度为600℃,煅烧时间为5 h时,复合样品光催化活性最佳,在12 W LED灯下,180 min后对浓度为10 mg/L的亚甲基蓝溶液的去除率达96.8;.     

V2O5/g-C3N4复合物的制备及可见光催化性能研究

以偏钒酸铵和尿素混合物为前驱体,混合煅烧制备了V2O5/g-C3N4复合物催化剂.用X射线衍射(XRD)、傅里叶红外光谱(FT-IR)、扫描电镜(SEM)、透射电镜(TEM)、紫外-可见光漫反射吸收光谱(UV-vis)、比表面积测试(BET)、光致发光谱(PL)等对其结构进行了表征.结果表明复合物中存在V2O5和g-C3N4形成异质结构,其禁带宽度减小、吸收带边红移,光催化效率有显著提高.以亚甲基蓝(MB)为目标化合物,评价了样品的光催化活性,当前躯体中尿素与NH4VO3质量比为10∶1,煅烧温度为500℃,煅烧时间为0.5h,催化剂活性最高.在60W日光灯照射40 min,对亚甲基蓝得降解率达到97.52;.     

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.     

g-C3N4/TiO2可见光催化降解磺胺二甲基嘧啶的研究

以商用TiO2颗粒和三聚氰胺为原料,采用高温煅烧法制备g-C3N4/TiO2复合光催化材料.利用X射线衍射仪(XRD)、扫描电镜(SEM)、透射电镜(TEM)、低温氮气物理吸附和紫外-可见漫反射光谱仪(UV-vis)对g-C3N4/TiO2的进行表征,并研究在可见光条件下g-C3N4/TiO2对溶液中磺胺二甲基嘧啶(Sulfamethazine,SMT)的光催化降解效果.结果表明:TiO2颗粒附着在层状结构g-C3N4/表面,形成具有孔隙结构和更大比表面积的g-C3N4/TiO2,有利于污染物的吸附.g-C3N4/TiO2的光吸收带边移动到430 nm,具有可见光响应.在可见光照射下,当g-C3N4/TiO2投加量为0.2 g/L时,初始浓度为0.5 mg/L的SMT在3h内去除率可达98.8;.在相同条件下,g-C3N4和TiO2只能分别去除57.8;和9.7;的SMT.活性物质掩蔽实验表明g-C3N4/TiO2光催化降解SMT过程中,超氧自由基(·O2-)和光生空穴(h+)在降解SMT时起主要作用.     

BiFeO3-Bi24Fe2O39复合物的制备及可见光催化性能研究

以硝酸铁(Fe(NO3)3·9H2O)硝酸铋(Bi(NO3)3·5H2O)为原料,酒石酸作络合剂,聚乙二醇6000作分散剂,用溶胶-凝胶法制备了BiFeO3-Bi24Fe2 O39复合催化剂.用XRD、FT-IR、UV-vis、PL光谱、TG-DSC等对其结构进行了表征.以亚甲基蓝为目标化合物,评价了样品的可见光催化活性.结果表明,500℃煅烧2h的复合催化剂热稳定性好,荧光强度最强,禁带宽度最小,用500 W的长弧氙灯照射6h,亚甲基蓝降解率达到93.11;.     

炭吸附Bi2O3/TiO2复合粉体的制备及其光催化性能研究

利用炭吸附溶胶凝胶法,以钛酸丁酯为钛源,氧化铋为铋源制备氧化铋含量为10;(质量分数)的纳米Bi2O3/TiO2复合粉体.通过热重/差热仪(TG-DTA)、X射线衍射仪(XRD)、透射电镜(TEM)和紫外可见光谱仪(UV-Vis)等对所得催化剂的焙烧温度、物相、微粒尺寸及光吸收性能进行表征.结果表明:炭黑的吸附有效阻止了纳米Bi2O3/TiO2复合粉体在制备、干燥以及焙烧过程的团聚和烧结,制得的粉体颗粒均匀,分散性好,团聚较少,经600℃焙烧的粉体,平均颗粒直径约为18.8 nm,比表面积约为86.52 m2/g.亚甲基蓝紫外光催化反应结果表明,在50 min内亚甲基蓝在Bi2O3/TiO2催化剂上几乎完全分解.     

NiFe2O4/g-C3N4的制备及可见光催化降解甲基橙

采用浸渍法制备不同负载量NiFe2 O4的负载型光催化剂NiFe2 O4/g-C3 N4,利用XRD、FT-IR、N2-adsorption、ICP-OES、TEM及XPS等手段表征NiFe2 O4/g-C3 N4样品,并考察其对甲基橙的可见光催化降解性能.结果表明,与NiFe2 O4和g-C3 N4样品相比,负载型NiFe2 O4/g-C3 N4样品对甲基橙具有更好的光催化降解活性,且催化活性随着NiFe2 O4负载量增大(0.5~5.0wt;)而呈现先增大再减小的趋势.NiFe2 O4负载量2.0wt;的样品2-NiFe/CN在可见光照射下对浓度5 mg·L-1的甲基橙表现出最好的降解活性和稳定性.这是因为能带宽度小(1.5 eV)的NiFe2 O4与能带宽度大(2.7 eV)的g-C3 N4形成的异质结催化剂NiFe2 O4/g-C3 N4,有效地促进光生载流子在二者界面快速传递和光生电子-空穴对的有效分离.     

金属镍掺杂g-C3N4的制备及其光降解性能

采用浸渍法制备不同掺杂量的负载型光催化剂Ni/g-C3N4,并考察其在可见光照下对亚甲基蓝的光降解性能.利用XRD、FT-IR、SEM、TEM、XPS、N2-sorption和ICP-OES等手段表征Ni/g-C3N4样品.研究表明,Ni/g-C3N4催化剂的光催化活性随着金属镍粒子掺杂量的增加而增大,随着亚甲基蓝浓度的增大而减小,其中金属镍掺杂量4.0wt;的样品4-Ni/g-C3N4表现出优异的光催化活性和光降解稳定性.这是由于4-Ni/g-C3N4样品的光降解过程中产生了超氧自由基、羟基自由基和空穴等活性物质,其中超氧自由基起主导作用.金属Ni0离子在光生电子作用下生成Ni2+,O2分子得到电子生成O2·-自由基.这些活性物质的产生有助于光生电子-空穴对的分离和抑制其复合速率,从而实现可见光下高效催化降解亚甲基蓝.     

Fe@Fe2O3/g-C3N4复合光催化剂的制备及其性能

通过高温煅烧三聚氰胺制备了石墨相氮化碳g-C3N4,再以硼氢化钠( NaBH4)为还原剂,室温下还原氯化高铁(FeCl3· 6H2O)制备出了具有核壳结构的Fe@Fe2O3纳米线.然后分别通过超声法和溶剂热法制备了Fe@Fe2 O3/g-C3N4复合光催化剂,并利用X-射线衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)等表征方法对其进行表征.所得样品的光催化性能通过在可见光下(λ≥400 nm)光催化降解罗丹明B(RhB)溶液来评估.研究表明,超声法制备的Fe@Fe2O3/g-C3N4复合催化剂具有优良的可见光催化性能,其催化活性明显高于单组分的催化活性,一般认为Fe@Fe2O3与g-C3N4之间有一定的协同作用,从而可以提高材料的催化活性.同时,研究发现该催化体系中起关键作用的主要活性物种是超氧自由基.     

g-C3N4/ZnO复合光催化剂的制备及其光催化活性

以硝酸锌、三聚氰胺、氢氧化钠为原料,采用回流法合成g-C3N4/ZnO复合光催化剂.利用傅里叶红外光谱(FTIR),X射线衍射(XRD),扫描电子显微镜(SEM),紫外可见漫反射光谱(UV-Vis DRS)及N2吸附-脱附(BET)等技术对所合成样品的组成和形貌进行表征.在模拟太阳光条件下,以亚甲基蓝为模拟污染物评价催化剂的活性.结果表明,g-C3N4加入量为5wt;,煅烧温度500℃,煅烧时间2 h条件下制备的复合光催化剂具有最佳的光催化活性.5wt;g-C3N4/ZnO复合光催化剂在反应40 min时对亚甲基蓝的降解率可达到98.5;,其光催化降解速率为纯ZnO的2.8倍.     

(Na1/2Bi1/2)TiO3-(Na1/2Bi1/2)(Zn1/3Nb2/3)O3无铅压电陶瓷的介电特性研究

采用固相合成法制备了(1-x)(Na1/2Bi1/2)TiO3-x(Na1/2Bi1/2)(Zn/23Nb2/3)O3(简写为(1-x)NBT-xNBZN)无铅压电陶瓷.研究了该体系陶瓷晶体结构、弥散相变特征与介电弛豫行为.X射线衍射分析表明,所研究的组成均能够形成纯钙钛矿(ABO3)型固溶体.当x≥0.5%摩尔分数时,该体系陶瓷具有三方、四方共存的晶体结构.材料的介电常数-温度曲线显示陶瓷具有两个介电反常峰Tf和Tm.修正的居里-外斯公式较好的描述了陶瓷弥散相变特征,弥散指数随x的增加而增加.x≤0.5%摩尔分数的陶瓷仅在低温介电反常峰Tf附近表现出明显的频率依赖性,随x的增加,陶瓷材料在室温和低温介电反常峰Tf之间都表现出明显的频率依赖性.根据有序-无序转变和宏畴.微畴转变理论探讨了该体系陶瓷介电弛豫特性的机理.     

Pb(In1/2Nb1/2)O3-Pb(Ni1/3Nb2/3)O3-PbTiO3压电陶瓷的介电、铁电和压电性能

采用两步法制备了0.30Pb(In1/2 Nb1/2)O3-(0.70-x)Pb(Ni1/3Nb2/3)O3-xPbTiO3(PIN-PNN-PT,x=0.33,0.35,0.37,0.39)压电陶瓷.研究了PIN-PNN-PT压电陶瓷的相结构、介电、铁电和压电性能.研究表明位于准同型相界(MPB)的组分0.30PIN-0.33PNN-0.37PT具有最佳电学性能,其居里温度TC、压电系数d33、平面机电耦合系数kp、自由介电常数ε二介电损耗tanδ、剩余极化Pr、矫顽场EC分别为200℃、386 pC/N、50;、2692、0.045、34 μC/cm2、18 kV/cm.结果 显示PIN-PNN-PT三元系相比于PNN-PT有更高的居里温度,同时保持了优异的压电性能.     

Precipitation of In2O3 nano-crystallites from glasses in the system Na2O/B2O3/Al2O3/In2O3

Glasses in the system Na₂O/B₂O₃/Al₂O₃/In₂O₃ were melted and subsequently tempered in the range from 500 to 700 °C. Depending on the chemical composition, various crystalline phases were observed. From samples without Al₂O₃, In₂O₃ could not be crystallized from homogeneous glasses, because either spontaneous In₂O₃ crystallization occurred during cooling, or other phases such as NaInO₂ were formed during tempering. The addition of alumina, however, controlled the crystallization of In₂O₃. Depending on the crystallization temperature applied, the crystallite sizes were in the range from 13 to 53 nm. The glass matrix can be dissolved by soaking the powdered glass in water. This procedure can be used to prepare nano-crystalline In₂O₃-powders.     

Optical Properties of Bi2O3-TeO2-B2O3 Glasses

Glasses of the Bi₂O₃-TeO₂-B₂O₃ ternary system were developed and their linear and nonlinear optical properties were investigated. The absorption edges of these glasses were found to be 367-384 nm with a good transmittance in visible wavelength, although they exhibit the refractive indices as high as 1.98-2.12 at 633 nm. The absorption edges are quite steep and they are analyzed by the Urbach theory. The obtained Urbach energies of these glasses are 73-79 meV which are comparable to silica glasses. The high refractive index and its glass composition dependency are discussed according to the basics of the electronic polarizability and optical basicity. The high third order nonlinear susceptibility χ⁽³⁾ = 2.0 × 10^− 12 esu at 800 nm was also obtained in the 36Bi₂O₃-18TeO₂-46B₂O₃ glass.     

Spectroscopic properties of Er-doped Na2O-Sb2O3-B2O3-SiO2 glasses

Spectroscopic properties of Er³⁺-doped Na₂O-Sb₂O₃-B₂O₃-SiO₂ glasses have been investigated for developing 1.5-μm broadband fiber amplifiers. An intense 1.5-μm near infrared emission with a broad full width at half maximum (FWHM) of 88 nm has been obtained for Er³⁺-doped 5Na₂O-20Sb₂O₃-35B₂O₃-40SiO₂ glass upon excitation with a 980 nm laser diode. The obtained emission cross-section of the ⁴I_13/2 → ⁴I_15/2 transition and the lifetime of the ⁴I_13/2 level of Er³⁺ ions are 6.8 × 10⁻²¹ cm² and 0.36 ms, respectively. It is noted that the product of the emission cross-section and the FWHM of the glass, σ_e × FWHM, is as great as 598.4 × 10⁻²¹ cm² nm, which is comparable or higher than that of Er³⁺-doped bismuth-based and tellurite-based glasses. These special optical properties encourage in identifying them as important materials for potential applications in high performance optics and optical communication networks.     

Pb(Sc1/2Nb1/2)O3-Pb(Mg1/3Nb2/3)O3-PbTiO3-PbZrO3弛豫铁电晶体的生长及表征

采用高温溶液法生长了准同型相界(MPB)四元弛豫铁电单晶Pb(Sc1/2Nb1/2) O3-Pb(Mg1/3 Nb2/3)O3-PbTiO3-PbZrO3,得到较大尺寸且具有规则外形的立方单晶.研究结果表明所生长的晶体为钙钛矿结构,立方晶粒平整的暴露面均为(001)面;晶体以层状方式生长,生长机制为搭桥生长;所生长晶体的矫顽场Ec～3.52kV/cm,三方四方相变温度Tr-t～104℃,居里温度Tc～149.5℃,压电常数d33～1089 pC/N,剩余极化强度Pr～25.4 μC/cm2;随着频率增加,晶体的相变弥散度减小.     

Optical properties of and concentration quenching in Bi2O3-B2O3-Ga2O3 glasses

Er₂O₃-doped Bi₂O₃-B₂O₃-Ga₂O₃ glasses were prepared by the conventional melt-quenching method, and the Er³⁺:⁴I_13/2 → ⁴I_15/2 fluorescence properties are studied for different Er³⁺ concentrations. when the Er₂O₃ concentration increases from 0.03 to 3.0 mol%, the measured lifetime of Er³⁺:⁴I_13/2 level decrease from 2.24 to 0.9 m s, and from 0.25 to 0.20 m s for the Er³⁺:⁴I_11/2 level. The fast energy migration among Er³⁺ ions cause the reduction of lifetime of the ⁴I_13/2 level, whereas the change in the ⁴I_11/2 level is mainly due to a cooperative upconversion process (⁴I_11/2, ⁴I_11/2) → (⁴F_7/2, ⁴I_15/2). Based on the dipole-dipole interaction theory, the interaction parameter, C_Er,Er, for the migration rate of Er³⁺:⁴I_13/2 ↔ ⁴I_13/2 was calculated to be 32 × 10⁻⁴⁰ cm⁶ s⁻¹.     

Thermo-optic properties of B2O3 doped Li2O-Al2O3-SiO2 glass-ceramics

Reduction in the temperature coefficient of the optical path length, dS/dT of Li₂O-Al₂O₃-SiO₂ glass-ceramics with near-zero thermal expansion coefficient was attempted using control of the temperature coefficient of electronic polarizability, ?, and the thermal expansion coefficient, α. The dS/dT value of 2.6 mol% B₂O₃-doped glass-ceramic was 12.5  × 10⁻⁶/°C, which was 0.9 ×  10⁻⁶/°C smaller than that of B₂O₃-free glass-ceramic. On the other hand, reduction in dS/dT through B₂O₃ doping was not confirmed in precursor glasses. Results showed that reduction in dS/dT of the glass-ceramic through B₂O₃ doping is caused by the reduction in ?. The reduction in ? from B₂O₃ doping was probably attributable to numerical reduction in non-bridging oxide ions with larger ? value by the concentration of boron ions in the residual glass phase. In addition, application of hydrostatic pressure during crystallization was effective to inhibit precipitation of β-spodumene solid solution, which thereby decreases dS/dT. The dS/dT value of B₂O₃-doped glass-ceramic crystallized under 196 MPa was 11.7 ×  10⁻⁶/°C. That value was slightly larger than that of silica glass. The α value of this glass-ceramic was smaller than that of silica glass.     

Effect of Al2O3 on phase separation and crystallization in ZnO---Al2O3---B2O3---SiO2 glasses

The effect of alumina on the phase separation and the crystallization of the glasses of composition (mol%) 18ZnO·30B₂O₃·52SiO₂ and O-40 Al₂O₃ was studied using an electron microscope and IR spectroscopy. The main crystalline phase appears in the microphase for which the compositions are not nearer to the crystal stoichiometry than the mean. The addition of Al₂O₃ suppresses the immiscibility but enhances the crystallizability.     

Quenched glasses in the systems of Li2O with Al2O3, Ga2O3 and Bi2O3

By rapid quenching in a twin roller apparatus, glass was found to occur widely in the systems of Li₂O with Al₂O₃, Ga₂O₃, Bi₂O₃ and in mixed systems. Examination of the resulting flakes by X-ray powder diffraction, differential thermal analysis, and capacitance data revealed the occurrence of glass, glass transitions, crystallization exotherms and the nature of some of the crystallization paths.The log ionic conductivity of the glasses was found to follow a linear relationship with the Li concentration. Evidence was observed for three new metastable crystalline phases, one in the Li₂OAl₂O₃ system and two in the Li₂OBi₂O₃ system. The latter system also showed evidence for the occurrence of two glasses at almost all compositions.