单壁AlAs(111)纳米管结构和电子性质的密度泛函理论研究

通过卷曲立方AlAs(111)单层片(sheets)构造了一系列(n,0)和(n,m)一维单壁纳米管。用周期性密度泛函理论(DFT)计算并比较了不同类型AlAs纳米管在几何结构、能量及电子性质等方面的差别。计算结果表明锯齿型和椅型纳米管应变能均为负值,并随着管径变大而逐渐变小。然而,它们的带隙相当不同:椅型纳米管为间接带隙,随着管径的增大而带隙减小;锯齿型纳米管为直接带隙,管径为1.87 nm时存在着一个极大带隙值(2.11 eV)。这种不同主要源于锯齿型纳米管铝原子间3p轨道的耦合贡献。     

氟掺杂TiO2纳米管的可见光催化活性及第一性原理计算

作为光催化技术的核心, 提高TiO₂的光催化活性和对可见光的利用率是当前光催化研究中最重要的研究课题. 为了提高TiO₂纳米管的可见光催化活性, 采用化学气相沉积法对TiO₂纳米管进行了氟掺杂. 扫描电子显微镜(SEM)结果表明退火温度对于TiO₂纳米管的形貌完整性有较大影响, 当样品在550和700 °C下退火, 氟掺杂TiO₂纳米管结构受损; X射线衍射(XRD)分析表明氟掺杂对TiO₂由锐钛矿相转化为金红石相有阻碍作用; X射线光电子能谱(XPS)测试表明化学气相沉积能有效地对TiO₂纳米管进行非金属掺杂, 且该方法安全、操作简单. 氟掺杂TiO₂纳米管对甲基橙有较高的可见光催化降解活性. 第一性原理计算结果表明氟掺杂对TiO₂带隙无显著影响, 费米能级附近的F 2p轨道电子位于价带底部, 与O 2p交联作用较小, 因此对TiO₂光吸收带边影响不大. 氟掺杂能促进表面氧空穴的产生, 增加表面酸度与Ti³⁺, 有利于减少电子-空穴复合率, 从而提高其光催化活性.     

TiO2-MoO3复合纳米管阵列薄膜的制备及其可见光活性

通过阳极氧化的方法制备TiO₂纳米管薄膜, 在MoO₃存在的条件下对该薄膜进行热处理得到TiO₂-MoO₃复合纳米管阵列薄膜. 利用X射线衍射(XRD), 扫描电子显微镜(SEM), X射线光电子能谱(XPS), 电化学阻抗谱(EIS), Mott-Schottky 及光电化学方法对得到的薄膜进行了表征. XRD结果表明, TiO₂-MoO₃复合纳米管薄膜中的TiO₂主要为锐钛矿晶型. SEM实验证实了薄膜纳米管结构的存在, 样品中的MoO₃均匀地分散在TiO₂纳米管表面. 利用XPS方法分析了TiO₂-MoO₃复合纳米管薄膜元素的组成, 结果表明, MoO₃在TiO₂表面形成TiO₂-MoO₃复合纳米管薄膜. 研究了热处理温度以及热处理时间对样品的光电化学性能的影响, 相对于单纯TiO₂纳米管薄膜, 适量引入MoO₃提高了样品在可见光区的光电响应能力, 样品的平带电位负移. 在450 °C热处理60 min制得的TiO₂-MoO₃复合半导体纳米管阵列薄膜光电响应活性最高.     

微含水量电解液中高管径比TiO2纳米管阵列的制备

通过阳极氧化法在微含水量为0.5wt%的NH₄F/乙二醇/H₂O酸性电解质体系中制备了管径大、高管径比的二氧化钛（TiO₂）纳米管阵列。采用SEM、XRD等测试手段对TiO₂纳米管阵列形貌及晶相进行表征,探讨了不同氧化时间、电压对纳米管阵列形貌的影响,微含水量下氧化电压可以适当增加,更容易得到规整的长纳米管阵列;通过测定样品的光电流和紫外-可见光漫反射吸收光谱,研究分析了含水量以及超声工艺对纳米管光吸收及光电流特性,微含水量下得到的纳米管阵列可见光吸收边红移至420nm,对480~700nm可见光有明显的光吸收,光电流显著增大;丙酮作为超声介质可有效去除纳米管阵列表面的集束,能进一步提高纳米管阵列的光电性能。     

TiO2-B纳米管负载过渡金属氧化物的电化学嵌锂性能

采用碱性条件下的水热法合成了质子钛酸盐纳米管,在此基础上采用化学沉淀方法制备了负载过渡金属(Co,Ni和Cu)氢氧化物的纳米管材料,然后在300 ℃氩气氛下烧结后得到负载过渡金属(Co,Ni和Cu)氧化物TiO₂-B纳米管。采用XRD和TEM等对其结构与形态进行了表征,采用恒电流充放电、循环伏安以及交流阻抗测试研究了其电化学嵌/脱锂性能。结果表明,TiO₂-B纳米管通过负载过渡金属(Co,Ni和Cu)氧化物纳米颗粒之后,改善了TiO₂-B纳米管的高倍率放电性能和循环稳定性。其中,负载NiO和CuO的TiO₂-B纳米管的高倍率放电性能和循环稳定性较为突出。研究还表明,负载过渡金属氧化物纳米颗粒后,有助于保持TiO₂-B纳米管在动态反应条件下的拟电容反应控制特征,并不同程度地减小了TiO₂-B纳米管的表面电荷转移电阻,这是TiO₂-B纳米管的电化学性能改善的主要原因。     

浸渍-分解法制备高可见光催化活性的Bi2O3/TiO2纳米管阵列

用浸渍-分解法将Bi₂O₃纳米颗粒沉积在TiO₂纳米管壁上, 制备了Bi₂O₃/TiO₂纳米管阵列. 用电感耦合等离子体发射光谱(ICP-AES)测定了Bi₂O₃/TiO₂ 纳米管阵列的化学组分, 利用X 射线衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)和紫外-可见(UV-Vis)吸收光谱表征了所制备的样品. 通过在可见光下(λ>400 nm)降解甲基橙(MO)水溶液来评价样品的光催化活性. 结果表明, Bi₂O₃纳米颗粒均匀地沉积在TiO₂纳米管中. Bi₂O₃/TiO₂纳米管阵列具有比纯Bi₂O₃膜和N-TiO₂纳米管阵列高得多的可见光催化活性. Bi₂O₃/TiO₂纳米管阵列活性的增强是其强可见光吸收和Bi₂O₃与TiO₂之间形成的异质结的协同作用的结果.     

热处理气氛对 TiO2 纳米管阵列薄膜光电催化性能的影响

 采用原位阳极氧化法在 Ti 基底上制备了高度有序的 TiO₂ 纳米管阵列薄膜, 分别在 O₂, 空气, Ar 和 H₂ 气氛中于 500 oC 进行结晶热处理, 考察了热处理气氛对 TiO₂ 纳米管阵列薄膜光电催化降解亚甲基蓝 (MB) 反应性能的影响. 结果表明, 在这些气氛中热处理得到的锐钛矿晶型的纳米管阵列薄膜对 MB 降解满足一级反应, 其速率常数分别为 4.967, 3.127, 1.989 和 1.625 h^-1 (0.5 V). 电化学阻抗分析表明, TiO₂ 纳米管的光电催化性能受控于光生电荷的传递特性. 在 O₂ 中热处理, TiO₂ 纳米管的光吸收及激发性能得以改善, 且电荷传递阻抗降低, 因而其光电催化性能最好.     

添加NaBF4对阳极氧化法制备TiO2纳米管光催化剂的影响

在阳极氧化电解液中添加NaBF₄制得了具可见光活性的B掺杂TiO₂纳米管阵列（B/TNTs）。采用扫描电镜（FE-SEM）、能谱仪（EDS）、X射线衍射（XRD）、傅立叶红外光谱（FTIR）、紫外-可见漫反射光谱（UV-Vis DRS）以及X射线光电子能谱（XPS）对样品进行表征,以亚甲基蓝（MB）的光催化降解为目标反应评价其光催化活性。结果表明：添加NaBF₄后,TiO₂纳米管表面形貌变化较大;B掺入到TiO₂晶格中形成B-O-Ti键;B掺杂使得TiO₂纳米管表面羟基量增加、光学带隙能减小、光吸收阀值红移,且B掺杂量越多,其相应值的变化量越大;B掺杂能促进TiO₂锐钛矿相的发育,纳米管经550℃煅烧后仍保持未掺杂样品的锐钛矿相结构;NaBF₄的最佳添加量为0.6%（w/w）时,所得样品光催化活性最佳,可见光下光催化降解MB的4 h降解率由未添加的39.90%提高至75.15%,且反复使用10次后其光催化性能基本保持不变;总有机碳（TOC）分析结果表明,MB在可见光下能被B/TiO₂有效矿化。     

Fe2O3/TiO2纳米管阵列的制备及其光催化性能

在钛基体上采用阳极氧化法制备了TiO₂纳米管阵列,采用化学浴方法在TiO₂纳米管阵列上修饰了Fe₂O₃纳米颗粒.利用扫描电镜、X射线衍射和紫外可见漫反射光谱等手段对材料进行了表征,同时测试了材料的光电化学性能及其光催化降解亚甲基蓝染料废水的性能.结果表明,Fe₂O₃纳米颗粒的修饰将TiO₂纳米管阵列的光响应拓宽至可见光区域,提高了光电流,Fe₂O₃/TiO₂纳米管阵列的光电流是未修饰的TiO₂纳米管阵列的9倍.而在光催化反应中,亚甲基蓝最高降解率可达80%,比未修饰的TiO₂纳米管阵列高出30%.     

CdS/TiO2纳米管复合结构的制备与光电性能研究

利用阳极氧化法在钛金属基体表面制备一层TiO₂纳米管阵列薄膜, 然后通过水热反应在TiO₂纳米管上负载CdS纳米粒子, 形成CdS/TiO₂纳米管的复合结构。利用SEM、XRD、XPS、UV-Vis等手段对其形貌和结构进行表征。进一步考察了CdS/TiO₂纳米管的光电性能和光催化活性, 结果表明, 相比于TiO₂纳米管, CdS/TiO₂纳米管复合结构在紫外光和可见光下都具有更好的光催化活性及光电性能。     

Investigation of the silicon concentration effect on Si-doped anatase TiO2 by first-principles calculation

A first-principles calculation based on the density functional theory (DFT) was used to investigate the energetic and electronic properties of Si-doped anatase TiO₂ with various silicon concentrations. The theoretical calculations showed that with Si-doping the valence band and conduction band of TiO₂ became hybrid ones with large dispersion, which could benefit the mobility of the photo-generated carriers. This result is in agreement with the experimental reports. At lower doping levels, the band gap of Si-doped anatase TiO₂ decreases about 0.2 eV. With the increase of silicon concentration, the band gap increases gradually and larger formation energies are required during the synthesis of Si-doped TiO₂.     

三维有序结构In掺杂TiO_2薄膜的可见光催化活性

采用自组装生长聚苯乙烯胶体模板和溶胶-凝胶法,制备出三维(3D)有序结构In掺杂TiO2(IO-TiO2-In)薄膜可见光催化剂.光催化实验证明,IO-TiO2-In薄膜降解甲醛的可见光活性是TiO2和三维有序结构TiO2(IOTiO2)薄膜的5倍.利用X射线电子衍射(XRD)谱、X射线光电子能谱(XPS)、扫描电子显微镜(SEM)和紫外-可见(UV-Vis)漫反射吸收光谱确定了催化剂的晶相结构、表面微结构和能带结构.结果表明,IO-TiO2-In薄膜具有锐钛矿型三维有序结构,与TiO2相比,增加了比表面积,提高光的利用率;掺入的In离子在薄膜表面形成In2O3和O-In-Clx(x=1,2)物种,既增强可见光的吸收,又有效地促进了光生载流子的分离,提高了光生载流子在固/气界面参加光催化反应的利用率,使催化剂的可见光催化活性显著提高.     

The Preparation and Characterization of La Doped TiO2 Nanotubes and Their Photocatalytic Activity

La-doped TiO₂ nanotubes (La/TiO₂ NTs) were prepared by the combination of sol-gel process with hydrothermal treatment. The prepared samples were characterized by using transmission electron microscopy, x-ray diffraction, x-ray photoelectron spectra, and ultraviolet-visible spectra. The photocatalytic performance of La/TiO₂ NTs was studied by testing the degradation rate of methyl orange under ultraviolet (UV) irradiation. The results indicated La/TiO₂ NTs calcined at 300°C consisted of anatase as the unique phase. The absorption spectra of the La/TiO₂ NTs showed a stronger absorption in the UV range and a slight red shift in the band gap transition than that of pure TiO₂ nanotubes. The photocatalytic performance of TiO₂ NTs could be improved by the doping of lanthanum ions, which is ascribed to several beneficial effects the formation of Ti-O-La bond and charge imbalance, existing of oxygen defects and Ti³⁺ species, stronger absorption in the UV range and a slight red shift in the band gap transition, as well as higher equilibrium dark adsorption of methyl orange. 0.75 wt% La/TiO₂ NTs had the best catalytic activity.     

Cu掺杂TiO2纳米管可见光催化矿化甲苯

采用低温水热法制备氢钛酸管, 通过吸附-煅烧法制备Cu掺杂TiO₂纳米管(Cu-TNT)催化剂. 利用X射线衍射(XRD)、电感耦合等离子体-原子发射光谱(ICP-AES)、X射线光电子能谱(XPS)、透射电镜(TEM)、紫外-可见漫反射光谱(UV-Vis-DRS)和电化学测试手段对样品进行表征, 并进行平面波赝势密度泛函理论(DFT)计算. 结果表明, 样品中Cu/Ti原子比接近理论值, Cu掺杂进入TiO₂晶格内部, 诱发催化剂可见光活性. 掺Cu后,Cu 3d轨道和O 2p轨道杂化形成价带顶, 价带负向偏移, 样品禁带宽度减小为2.50-2.91 eV, 具有可见光响应.以甲苯为模型污染物研究催化剂对挥发性有机化合物(VOCs)的催化去除和矿化效果. 未掺杂的TNT可见光催化活性较差; Cu掺杂量超过0.1%(Cu/Ti原子比)时, 样品催化活性也减弱; Cu掺杂量为0.1%的催化剂具有最佳可见光催化氧化能力, 7 h内甲苯的去除率达77%, 甲苯的矿化率达59%.     

Gd-N共掺杂SrTiO3/TiO2复合纳米纤维制备及光催化性能

以静电纺丝技术制备的TiO_2纳米纤维为基质和反应物,结合一步水热法制得Gd-N共掺杂SrTiO_3/TiO_2复合纳米纤维光催化剂。利用X射线衍射(XRD)、扫描电子显微镜(SEM)、高分辨透射电镜(HRTEM)、X射线光电子能谱(XPS)、紫外-可见漫反射(UV-Vis DRS)和荧光光谱(PL)等方法对其微观结构、形貌和光学性能进行表征。结果表明:SrTiO_3和TiO_2形成异质结能够使光生电子和空穴得到很好的分离,而Gd-N共掺杂产生新带隙,可以拓宽光谱响应范围至可见光区,并引起晶格缺陷,成为光生电子-空穴对的浅势捕获阱。Gd-N共掺杂与异质结的协同作用有效提高了SrTiO_3/TiO_2复合纳米纤维的可见光催化活性。     

Preparation and characterization of SiO2/TiO2 composite microspheres with microporous SiO2 core/mesoporous TiO2 shell

SiO₂/TiO₂ composite microspheres with microporous SiO₂ core/mesoporous TiO₂ shell structures were prepared by hydrolysis of titanium tetrabutylorthotitanate (TTBT) in the presence of microporous silica microspheres using hydroxypropyl cellulose (HPC) as a surface esterification agent and porous template, and then dried and calcined at different temperatures. The as-prepared products were characterized with differential thermal analysis and thermogravimetric (DTA/TG), scanning electron microscopy (SEM), X-ray diffraction (XRD), nitrogen adsorption. The results showed that composite particles were about 1.8 μm in diameter, and had a spherical morphology and a narrow size distribution. Uniform mesoporous titania coatings on the surfaces of microporous silica microspheres could be obtained by adjusting the HPC concentration to an optimal concentration of about 3.2 mmol L⁻¹. The anatase and rutile phase in the SiO₂/TiO₂ composite microspheres began to form at 700 and 900 °C, respectively. At 700 °C, the specific surface area and pore volume of the SiO₂/TiO₂ composite microspheres were 552 and 0.652 mL g⁻¹, respectively. However, at 900 °C, the specific surface area and pore volume significantly decreased due to the phase transformation from anatase to rutile.     

Carbon nanotube assisted synthesis of CeO2 nanotubes

CeO₂ nanotubes have been synthesized facilely using carbon nanotubes (CNTs) as templates by a liquid phase deposition method. The properties of the CeO₂ nanotubes were characterized by scanning electron microscopy (SEM), transmission electron microscopy (TEM), X-ray diffraction (XRD), X-ray photoelectron spectrum (XPS) as well as thermogravimetry and differential thermal analysis (TG-DTA). The obtained CeO₂ nanotubes with a polycrystalline face-centered cubic phase have a uniform diameter ranging from 40 to 50 nm. The CeO₂ nanotubes are composed of many tiny interconnected nanocrystallites of about 10 nm in size. The pretreatment of CNTs and calcination temperature were confirmed to be the crucial factors determining the formation of CeO₂ nanotubes. A possible formation mechanism has been suggested to explain the formation of CeO₂ nanotubes.     

Preparation and spectroscopic characterization of visible light sensitized N doped TiO2 (rutile)

Nitrogen doped TiO₂ represents one of the most promising material for photocatalitic degradation of environmental pollutants with visible light. However, at present, a great deal of activity is devoted to the anatase polymorph while few data about rutile are available. In the present paper we report an experimental characterization of N doped polycrystalline rutile TiO₂ prepared via sol-gel synthesis. Nitrogen doping does not affect the valence band to conduction band separation but, generates intra band gap localized states which are responsible of the on set of visible light absorption. The intra band gap states correspond to a nitrogen containing defect similar but not coincident with that recently reported for N doped anatase.     

Photocatalytic Crystalline and Amorphous TiO2 Nanotubes Prepared by Electrospinning and Atomic Layer Deposition

In this work core/shell composite polymer/TiO₂ nanofibers and from those TiO₂ nanotubes were prepared. First, poly(vinyl alcohol) (PVA) and poly(vinylpyrrolidone) (PVP) fibers were synthetized by electrospinning. They were covered with a 100 nm thick amorphous TiO₂ layer by atomic layer deposition at 50 °C. Later the polymer core was removed by two different methods: dissolution and annealing. In the case of dissolution in water, the as-prepared TiO₂ nanotubes remained amorphous, while when annealing was used to remove the polymers, the TiO₂ crystallized in anatase form. Due to this, the properties of amorphous and crystalline TiO₂ nanotubes with exactly the same structure and morphology could be compared. The samples were investigated by SEM-EDX, ATR-IR, UV-Vis, XRD and TG/DTA-MS. Finally, the photocatalytic properties of the TiO₂ nanotubes were studied by decomposing methyl-orange dye under UV light. According to the results, crystalline anatase TiO₂ nanotubes reached the photocatalytic performance of P25, while amorphous TiO₂ nanotubes had observable photocatalytic activity.     

Preparation of a new pyrochlore-type compound Na0.32Bi1.68Ti2O6.46(OH)0.44 by hydrothermal reaction

A new pyrochlore-type Na_0.32Bi_1.68Ti₂O_6.46(OH)_0.44 with the cubic cell of a=10.339(5) Å was prepared by hydrothermal reaction using TiO₂ (anatase) and Bi₂O₃ in NaOH solution. This compound was obtained when the molar ratio of NaOH/TiO₂ was above 2 and the reaction temperature was above 240 °C. The TG-curve of as-prepared sample showed a mass loss of 0.8 mass% which was caused by release of OH group. This compound decomposed to a pyrochlore-type compound and a layered-type Na_0.5Bi_4.5Ti₄O₁₅ above 800 °C. The optical band gap of Na_0.32Bi_1.68Ti₂O_6.46(OH)_0.44 was estimated to be 2.5 eV.