镧系离子掺杂TiO2的制备及其对咪唑降解反应的光催化活性

 以TiCl4和镧系元素的氯化盐溶液为前驱体,采用溶胶-凝胶法制备了不同含量镧系离子掺杂的TiO2光催化剂,用X射线衍射(XRD)、 光致发光光谱(PLS)、 表面光电压谱(SPS)和X射线光电子能谱(XPS)对催化剂进行了表征. XRD结果表明,样品为锐钛矿和金红石的混晶相,镧系离子未进入到TiO2晶格中. PLS和SPS测定结果表明,随着掺杂离子的不同和掺杂含量的不同,样品的谱强度呈现有规律的变化. 在紫外光照射下,以咪唑为目标降解物比较了催化剂的光催化活性. 结果表明,适当含量的镧系离子掺杂可有效促进TiO2表面光生载流子的分离,从而显著提高其光催化活性.     

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.     

Ce及N共掺杂改性TiO_2光催化性能及Ce组分的作用

以钛酸正丁酯、硝酸亚铈及氨水为前驱体运用溶胶-凝胶法对TiO2进行Ce及N单一和共掺杂改性,以甲基橙光催化降解为探针考察掺杂组分对催化剂的紫外、可见光活性影响,观察到了Ce及N的单一掺杂及共掺杂催化剂紫外、可见光活性的明显提升。运用X射线衍射(XRD)、低温氮气吸附(BET)、紫外-可见漫反射吸收光谱(DRS)、程序升温氧脱附(TPD)和程序升温氧化(TPO)等表征手段从催化剂的晶体结构及形貌、比表面积、紫外及可见光响应特性、表面吸附氧量及吸附氧循环性能等方面尝试理解掺杂组分的光活性影响机制。实验结果表明掺杂改性催化剂中适量Ce组分的作用在于通过抑制催化剂的晶粒长大、团聚和锐钛结构向金红石结构的相转变,提高催化剂的光相应强度和拓展光响应范围,增加催化剂表面吸附氧容量和促进催化剂的表面氧循环,有效捕获光生载流子,衍生各类高活性自由基物种和增大催化剂比表面积等方面增进催化剂的光催化性能。     

铬和硫共掺杂二氧化钛催化剂的制备及其可见光催化性能

以钛酸四丁酯为前驱体,硝酸铬和硫脲为掺杂离子给体,通过溶胶-凝胶法成功制备了纯TiO2、不同浓度的铬掺杂和铬/硫共掺杂TiO2光催化剂.以靛红为目标污染物,进行了可见光催化降解活性测试实验.结果表明,共掺杂催化剂的活性高于未掺杂和单掺杂催化剂.当共掺杂催化剂含0.60%(原子比)的铬,1.2%(原子比)的硫,焙烧温度为500℃时具有最高的光催化降解活性.X射线衍射、N2吸附、X射线光电子能谱和紫外-可见漫反射吸收光谱表征结果显示,共掺杂催化剂为锐钛矿型,具有较高的比表面积,对可见光有较强的吸收能力.共掺杂TiO2具备较高可见光催化活性的原因可能是铬掺杂降低了TiO2的禁带宽度,拓展了可见光吸收区域,而硫掺杂能够维持体系的电荷平衡,增强催化剂对可见光的吸收.     

掺Sn的纳米TiO2表面光生束缚激子的验证及其特性

采用溶胶-凝胶法制备了不同掺杂Sn的TiO2纳米粒子，并主要利用表面光电压谱(SPS)和电场诱导表面光电压谱(EFISPS)对样品进行了表征，重点探讨了焙烧温度和掺Sn量对TiO2光生电荷性质的影响．同时揭示了样品结构与表面光生束缚激子的关系及其特性．结果表明：与束缚激子相关的光伏响应只在含有金红石相的TiO2样品中出现，且在混晶相中表现得更加显著．掺杂适量Sn不仅提高了纳米TiO2的与带带跃迁相关的SPS响应强度，同时也使与束缚激子相关的SPS响应明显增强．     

形态结构和光电特性对纳米TiO2光催化性能的影响

采用sol-gel法制备了系列纳米TiO2光催化剂,运用X射线衍射、BET比表面测定、紫外漫反射吸收光谱和表面光电压谱等手段对催化剂进行表征,并以乙烯作为光催化反应的指标反应分子,研究了TiO2纳米晶的性质对于光催化活性的影响.随着焙烧温度的升高,TiO2的晶粒逐渐增大,比表面积下降,晶相由锐钛矿向金红石转变,其吸收带边与光伏响应阈值向长波方向移动,氧化－还原能力降低,降解乙烯的转化率迅速下降.     

In离子掺杂二氧化钛纳米管可见光催化活性的研究

采用两步预掺杂方法制备出In离子掺杂二氧化钛纳米管可见光催化剂. 可见光催化降解对氯苯酚实验证明: 掺杂In离子量为3%的TiO2纳米管可见光活性最高, 是纯TiO2纳米管的2倍以上. X射线衍射(XRD), X光电子能谱(XPS)和表面光电压谱(SPS)结果表明: 当In离子掺杂浓度较小时, In离子取代晶格Ti的位置形成InxTi1－xO2取代式掺杂结构. In离子的掺杂能级与Ti离子的3d轨道形成混合价带, 使禁带宽度变窄, 增强了可见光响应. 随着In离子掺杂浓度的增加, 同时在InxTi1－xO2纳米管表面生成In2O3, 形成InxTi1－xO2/In2O3纳米管复合结构. 该复合结构有效地增加可见光响应, 促进了光生载流子的分离, 提高了光生载流子在固/液界面参加光催化反应的利用率, 使纳米管催化剂可见光催化活性显著提高.     

碳掺杂的二氧化钛纳米管的制备及其可见光催化性能

以尿素作为碳元素前驱体对TiO2纳米管进行掺杂,采用比表面积测定、X射线衍射、透射电子显微镜、能量色散X射线荧光光谱、X射线光电子能谱、固体漫反射紫外-可见吸收光谱和荧光光谱对产物进行了表征。 结果表明,以尿素作为前驱体可制备C掺杂的TiO2纳米管,C掺杂后,TiO2纳米管的可见光催化活性明显提高。 此外,研究了C掺杂量、煅烧温度、催化剂用量和pH值对TiO2纳米管光催化降解活性的影响,发现当C的掺杂量为5.3%、催化剂用量为1.5 g/L、溶液的pH值为5时,在其催化作用下,可见光光照3 h后罗丹明B的降解率可达到91%。     

过渡金属掺杂和碳纳米管（CNT）接枝双重改性TiO2光催化剂

提出了一种过渡金属掺杂和碳纳米管(CNT)双重改性TiO2的新方法:首先采用溶胶-凝胶法合成掺杂镍和铁的二氧化钛基催化剂,然后采用流化床化学气相沉积方法(FBCVD)在二氧化钛基催化剂表面接枝生长CNT,得到CNT/Fe-Ni/TiO2复合光催化剂.通过X射线衍射、扫描电子显微镜、比表面分析、拉曼光谱、紫外-可见吸收光谱、荧光光谱等方法考察了双重改性复合光催化剂CNT/Fe-Ni/TiO2的结构和性能,通过降解亚甲基蓝溶液评价了双重改性复合光催化剂的活性.结果表明,在TiO2表面接枝的CNT具有较好的石墨化结构,CNT生长过程中小部分TiO2由锐钛矿向金红石晶型转变.过渡金属和CNT双重改性有效地克服了TiO2的比表面积小、量子效率低等缺点,明显提高了TiO2的光催化活性.     

TiO2/Mo-TiO2 的制备、表征和光催化活性

 采用溶胶-凝胶法制备了掺 Mo 的 TiO2 粉末, 再由其制得 TiO2/Mo-TiO2 复合物光催化剂. 使用 X 射线光电子能谱、X 射线衍射、透射电镜、N2 吸附-脱附、紫外-可见漫反射光谱和荧光光谱等手段对催化剂进行了表征. 在紫外光照射下, 以甲基橙溶液降解为探针反应, 研究了 Mo 掺杂量对样品光催化活性的影响. 结果表明, Mo-TiO2 催化剂的活性不如纯 TiO2, 这是因为 Mo 离子促进了光生载流子的复合; 而带有 n-n 异质结半导体结构的 TiO2/Mo-TiO2 复合催化剂具有比纯 TiO2 和 Mo-TiO2 催化剂更高的光催化活性. 当 Mo 掺杂摩尔分数为 2%, TiO2:Mo-TiO2 质量比为 10:1 时, 活性是纯 TiO2 的 1.57 倍.     

Bi3.25La0.75Ti3O12纳米线的可见光催化性能

研究了用一步水热法制备的掺镧钛酸铋(Bi_3.25La_0.75Ti₃O₁₂, BLT)纳米线的光学和可见光催化性能, 并对其晶体结构和微观结构用X射线衍射(XRD)、透射电子显微镜(TEM)和高分辨透射电子显微镜(HRTEM)等手段进行了表征. 结果表明, 制备的纳米线为纯相的Bi_3.25La_0.75Ti₃O₁₂, 平均直径约为25 nm. 室温光致发光谱(PL)显示BLT纳米线在433和565 nm附近有较强的发射峰, 分别对应激子发射和表面缺陷发光. 紫外-可见漫反射光谱(UV-Vis DRS)表明BLT样品的带隙能约为2.07 eV. 利用可见光(λ>420 nm)照射下的甲基橙降解实验评价了BLT样品的光催化性能. 结果表明, BLT的光催化活性比商用TiO₂催化剂P25、掺氮TiO₂和纯相钛酸铋(Bi₄Ti₃O₁₂, BIT)高得多. BLT光催化剂具有更高催化活性的原因是La³⁺离子掺杂拓展了BIT对可见光的吸收范围, 同时抑制了BIT的光生电子-空穴的复合.     

可见光激发下PtⅣClx /TiO2的光诱导电子转移研究

1998年, Kisch等[1]发现PtⅣ卤化物修饰的TiO2催化剂(PtⅣClx/TiO2)具有可见光活性, 他们认为PtⅣ卤化物作为光敏化物种, 能够将电子转移到TiO2导带, 催化剂的表面吸附氧捕获电子后生成氧自由基, 继而氧化降解成对氯苯酚. 但是, 由于PtⅣ卤化物及其激发态能级的不确定, 对其反应机理研究尚未见报道.     

Optical properties of ZnO and ZnO:In nanorods assembled by sol-gel method

Self-assembled zinc oxide (ZnO) and indium-doping zinc oxide (ZnO:In) nanorod thin films were synthesized on quartz substrates without catalyst in aqueous solution by sol-gel method. The samples were characterized by x-ray diffraction (XRD), scanning electron microscope (SEM), Raman-scattering spectroscopy, room-temperature photoluminescence (PL) spectra, and temperature-dependent PL spectra measurements. XRD and Raman spectra illustrated that there were no single In2O3 phase in ZnO lattice after indium doping. The PL spectra of ZnO showed a strong UV emission band located at 394 nm and a very weak visible emission associated with deep-level defects. Indium incorporation induced the shift of optical band gap, quenching of the near-band-edge photoluminescence and enhanced LO mode multiphonon resonant Raman scattering in ZnO crystals at different temperatures. Abnormal temperature dependence of UV emission integrated intensity of ZnO and ZnO:In samples is observed. The local state emission peak of ZnO:In samples at 3.37 eV is observed in low-temperature PL spectra. The near-band-edge emission peak at room temperature was a mixture of excitons and impurity-related transitions for both of two samples.     

具有不同Bi/Ti摩尔比的BiOI/TiO2 (A)光催化剂的结构与性能

在室温条件下通过沉积法制备了BiOI敏化纳米锐钛矿TiO₂ (A)光催化剂. 用X射线衍射(XRD),X射线光电子能谱(XPS), 光致发光(PL)光谱和紫外-可见漫反射(UV-Vis DRS)等手段对其进行了表征. 通过罗丹明B(RhB)催化降解实验评价了其光催化活性. 随BiOI含量增加, BiOI/TiO₂ (A)在370-630 nm的吸收强度增强, 吸收带边红移增加, 紫外和可见光催化活性先增加, 当BiOI含量约为1.7% (质量分数)时, 各自达到最大值, 然后随BiOI含量的进一步增加而减小. 1.7% BiOI/TiO₂ (A)的可见光活性明显高于P25, 它的紫外光活性也略高于P25. 在BiOI含量相近时, BiOI/TiO₂ (A)比BiOI/P25具有更低的光催化活性. 和TiO₂ (A)相比, 1.7% BiOI/TiO₂ (A)明显具有更高的紫外和可见光催化活性, 这归功于它在370-630 nm的强吸收、吸收带边红移明显以及光生电子和空穴的有效转移, 减少了电子-空穴对的复合.     

Controlled synthesis of highly dispersed TiO2 nanoparticles using SBA-15 as hard template

Highly dispersed TiO2 nanoparticles were successfully synthesized by a wet impregnation method using SBA-15 as hard template for confining the growth of TiO2 nanocrystals, and then calcined at 550 degrees C in muffle furnace for 2 h. The as-synthesized samples were characterized with Fourier transform infrared spectra (FTIR), Raman spectroscopy, diffuse reflectance UV-visible spectroscopy (UV-vis), powder X-ray diffraction (XRD), small-angle X-ray diffraction (SAXRD), nitrogen adsorption, transmission electron microscopy (TEM) and photoluminescence spectra (PL). It was found that SBA-15 contained abundant silanol groups after removal of triblock copolymers by ethanol extraction and could easily adsorb a great number of titanium alkoxide via chemisorption. After subsequent hydrolysis of the anchored Ti complexes and calcination of the amorphous TiO2, anatase TiO2 nanocrystals with spherical shape and uniform particle diameter of about 6 nm were formed. A blue shift was observed in UV-vis absorption spectra due to the quantum size effect of TiO2 nanoparticles. Moreover, the as-prepared TiO2 nanoparticles showed a high PL intensity due to an increase in the recombination rate of photogenerated electrons and holes under UV light irradiation.     

蓝色磷光材料FIrpic的发光特性

研究了掺杂浓度及热退火对磷光材料双(4,6-二氟苯基吡啶-N,C2?)吡啶甲酰合铱(FIrpic)发光性能的影响.不同掺杂浓度的薄膜及有机电致发光器件(OELDs)的发光颜色都随FIrpic浓度的增大由蓝色逐渐变化到黄绿色.纯FIrpic薄膜的吸收光谱和光致发光(PL)光谱在440-480nm范围内有明显的光谱重叠,476nm处的发光强度随FIrpic掺杂浓度增大而降低主要是由自吸收效应引起的.测量了不同激发密度下的光致发光光谱和不同掺杂浓度下的电致发光(EL)光谱,发现530nm处的发光强度随激发强度或掺杂浓度的增大而增强,证实了530nm处的发光是来源于FIrpic分子间的激基缔合物发光.通过比较热退火前后薄膜微观形貌及电致发光器件光谱的变化,进一步证实了热退火促进FIrpic分子聚集,增强了FIrpic分子间的辐射跃迁发光.通过调控FIrpic掺杂浓度和优化器件结构,并对器件进行热退火处理得到一系列发光颜色从蓝色逐渐变化到黄绿色的有机电致发光器件.     

Indium and aluminium-doped ZnO thin films deposited onto FTO substrates: nanostructure,optical, photoluminescence and electrical properties

The microstructure, optical, photoluminescence and electrical properties of ZnO based films deposited onto FTO glass substrates by ultrasonic spray pyrolysis have been investigated. For comparison and a better understanding of physical properties of indium- and aluminum-doped ZnO and undoped ZnO thin films, X-ray diffraction analysis, photoluminescence spectra, optical, SEM texture and electrical conductivity analyses were performed. The AZO and IZO films exhibit the nanofiber structure with diameters 260 and 400 nm. X-ray diffraction showed all samples to be polycrystalline with hexagonal ZnO. The optical band gaps of the films were varied by Al and In dopants. The photoluminescence spectra of the films show a weak broad in the visible range and shifted to green emission for indium doping and to the green blue emission for aluminum as dopant. The width of the PL spectra for aluminum-doped films is too large compared to those of the indium-doped ones. The electrical conductivity of the ZnO film changes with Al and In dopants. The position of donor levels changes with In and Al dopants and approaches the conduction band level with the metal dopants. The obtained results suggest that the metal doping has a clear effect upon the growth, optical, photoluminescence and electrical conductivity properties of the ZnO films.     

Improved optical and electrical properties of sol–gel-derived boron-doped zinc oxide thin films

Sol–gel spin-coating was used to grow zinc oxide (ZnO) thin films doped with 0–2.5 at.% B on quartz substrates. The structural, optical, and electrical properties of the thin films were investigated using field-emission scanning electron microscopy, X-ray diffraction (XRD), photoluminescence (PL), ultraviolet–visible spectroscopy, and van der Pauw Hall-effect measurements. All the thin films had deposited well onto the quartz substrates and exhibited granular morphology. The average crystallite size, lattice constants, residual stress, and lengths of the bonds in the crystal lattice of the thin films were calculated from the XRD data. The PL spectra showed near-band-edge (NBE) and deep-level emissions, and B doping varied the PL properties and increased the efficiency of the NBE emission. The optical transmittance spectra for the undoped ZnO and boron-doped zinc oxide (BZO) thin films show that the optical transmittance of the BZO thin films was significantly higher than that of the undoped ZnO thin films in the visible region of the spectra and that the absorption edge of the BZO thin films was blue-shifted. In addition, doping the ZnO thin films with B significantly varied the absorption coefficient, optical band gap, Urbach energy, refractive index, extinction coefficient, single-oscillator energy, dispersion energy, average oscillator strength, average oscillator wavelength, dielectric constant, and optical conductivity of the BZO thin films. The Hall-effect data suggested that B doping also improved the electrical properties such as the carrier concentration, mobility, and resistivity of the thin films.     

Characterizations of lanthanum trivalent ions/TiO2 nanopowders catalysis prepared by plasma spray

Lanthanum trivalent ions (La(3+)) doped titanium dioxide (TiO(2)) nanopowders in the range of 20-60 nm were prepared successfully by plasma spray in the self-developed plasma spray equipment. The photocatalytic activity of samples at different doping concentrations in photocatalytic degradation of methyl orange was discussed. The nanopowders prepared were characterized by transmission electron microscopy, X-ray diffraction, ultraviolet-visible spectra, photoluminescence (PL) and X-ray photoelectron spectroscopy. The results show that La(3+) doping increased the photocatalytic activity of TiO(2) greatly, the optimal doping concentration was 0.5 at%. The La(3+) doping decreases the particle size and the distribution of particle sizes becomes more uniform. The doped powders were the mixture of anatase and rutile phase. The contents of anatase phase decreased firstly and then increased with an increase in the contents of La(3+). The intrinsic absorption band of La(3+) doped TiO(2) nanopowders appears red shift from that of pure TiO(2) nanopowders. The intensity of PL spectra increases and then decreases with increasing the content of La(3+). The PL spectral intensity reaches its peak when the ratio of La(3+)/TiO(2) is 0.2 at%. There are O, Ti, C and La elements in the prepared La(3+) doped TiO(2) nanopowders, La element still exists in trivalent and Ti element always exists in tetravalent.     

δ-MnO2对TiO2光催化降解甲基橙的抑制作用

采用动力学方法研究了在水悬浮液中δ-MnO2颗粒物对P-25 TiO2光催化降解甲基橙活性的影响, 并利用紫外-可见漫反射光谱(DRS)和光致发光光谱(PL)对受δ-MnO2污染前后的TiO2样品进行了表征. 动力学研究结果表明, 在3种不同初始pH值条件下, δ-MnO2对TiO2光催化剂都具有明显的致毒效应, 共存δ-MnO2的浓度越大, 致毒效应越明显. 表征结果表明, 由于δ-MnO2 与TiO2之间的界面接触, 使得TiO2吸收带边蓝移, 紫外光区的吸收强度降低, 光致发光信号(PL)明显减弱. 因此, δ-MnO2导致TiO2的禁带宽度增大, 光利用率降低, 并且是光生电子与空穴的复合中心.