室温下制备以{211}晶面为主的Ti1-xVxO2薄膜及其可见光催化性能

以金属Ti和V作为靶材,采用直流反应共溅射技术在室温下制备了以{211}晶面为主的锐钛矿相Ti_1-xV_xO₂薄膜,研究了不同V靶功率对Ti_1-xV_xO₂薄膜的薄膜成分、晶相结构和可见光催化性能的影响。研究表明,Ti_1-xV_xO₂薄膜的晶相结构为锐钛矿相,择优取向为(211),而结晶度受V靶功率的影响。随着V靶功率的增加,薄膜中V元素含量逐渐增加,同时,晶粒和沉积速率也逐渐增加。另外,当V靶功率为150 W时,薄膜的表面粗糙度值有一个最大值。V的掺杂导致薄膜的能带间隙变窄,对光的吸收向可见光区偏移,从而有效地改善了薄膜的可见光催化能力。当V靶功率为150 W时,Ti_1-xV_xO₂薄膜的能带间隙值为 2.82 eV,其在2 h的可见光照射下分解了80%的RhB染料。这被归结于能带间隙窄,高能晶面{211}和结晶度高的共同作用。     

室温下制备以{211}晶面为主的Ti1-xVxO2薄膜及其可见光催化性能

以金属Ti和V作为靶材,采用直流反应共溅射技术在室温下制备了以{211}晶面为主的锐钛矿相Ti_1-xV_xO₂薄膜,研究了不同V靶功率对Ti_1-xV_xO₂薄膜的薄膜成分、晶相结构和可见光催化性能的影响。研究表明,Ti_1-xV_xO₂薄膜的晶相结构为锐钛矿相,择优取向为(211),而结晶度受V靶功率的影响。随着V靶功率的增加,薄膜中V元素含量逐渐增加,同时,晶粒和沉积速率也逐渐增加。另外,当V靶功率为150W时,薄膜的表面粗糙度值有一个最大值。V的掺杂导致薄膜的能带间隙变窄,对光的吸收向可见光区偏移,从而有效地改善了薄膜的可见光催化能力。当V靶功率为150W时,Ti_1-xV_xO₂薄膜的能带间隙值为2.82eV,其在2h的可见光照射下分解了80%的RhB染料。这被归结于能带间隙窄,高能晶面{211}和结晶度高的共同作用。     

Fabrication and characterization of multi-metal co-doped titania films for a water-splitting reaction

Anchored visible-light-absorbing TiO(2) films have been synthesized by the layer-by-layer method on a quartz slide substrate as a new class of visible light-sensitive photocatalyst. UV-vis, XRD and XPS spectra show that W and Mn enter the TiO(2) lattices and partially substitute for Ti, and that W appears to have a solubility limit into the anatase structure. The Mn and W dopants cause new electronic states above the valence-band edge of pure TiO(2), and the new electronic states may be directly related to the visible-light absorption of doped TiO(2) films. A constant H(2) generation rate is obtained for long periods of time for all the investigated TiO(2) films, and the H(2) production rates for titania films doped with 0.74 at% W (relative to Ti) are 4.1 and 3.3 times higher than that of non-doped TiO(2) under UV and visible light, respectively, as the dopant atoms not only restrict the band gap to the visible region, but also facilitate the detrapping of charge carriers to the surface of the catalyst.     

Photocatalytic H2 evolution under visible-light irradiation over band-structure-controlled (CuIn)xZn2(1-x)S2 solid solutions

(CuIn)(x)Zn2(1-x)S2 solid solutions between a ZnS photocatalyst with a wide band gap and CuInS(2) with a narrow band gap showed photocatalytic activities for H(2) evolution from aqueous solutions containing sacrificial reagents SO(3)(2-) and S(2-) under visible-light irradiation (lambda >/= 420 nm). Pt (0.5 wt %)-loaded (CuIn)(0.09)Zn(1.82)S(2) with a 2.3-eV band gap showed the highest activity for H(2) evolution, and the apparent quantum yield at 420 nm amounted to 12.5%. H(2) evolved at a rate of 1.5 L h(-1) m(-2) under irradiation with a solar simulator (AM 1.5). Diffuse reflection and photoluminescence spectra of the solid solutions shifted monotonically to a long wavelength side, as the ratio of CuInS(2) to ZnS increased in the solid solutions. The photocatalytic H(2) evolution depended on the composition as well as the photophysical properties. DFT calculations suggested that the visible-light response should be derived from the contribution of Cu 3d and S 3p orbitals to the valence band and that of In 5s5p and Zn 4s4p orbitals to the conduction band, respectively. The contribution of these orbitals to the energy bands affected the photophysical and photocatalytic properties.     

BiOCl/In2S3复合可见光催化剂制备及性能研究

氯氧化铋（BiOCl）较大的禁带宽度使得其只能对紫外光产生响应,严重制约了其进一步光催化应用。为实现BiOCl对可见光的利用,以In2S3为可见光光敏剂,并基于高效实用的机械研磨手段构建BiOCl/In2S3复合可见光催化剂。通过扫描电子显微镜(SEM)、X射线衍射(EDS)、X射线衍射(XRD)、红外光谱(FT-IR)和紫外-可见漫反射光谱(UV-Vis DRS)等方法对催化剂的形貌和结构进行表征。选择盐酸四环素（TC）可见光催化降解为评价模型,系统研究了BiOCl/In2S3复合比例对光催化活性的影响。结果表明两者复合比例为1:1时具有最佳的光催化活性,在可见光照射下对TC的降解效率高达91.4%,且经3次循环降解效率仍保持在87.3%。机理研究表明,In2S3被可见光激发产生电子注入BiOCl的导带(CB),能有效提升载流子的分离效率,而h+和?O2-是光降解过程中的主要活性物质。该项研究工作充分表明了In2S3对BiOCl的高效光敏活性,展示了物理复合法在新型高效可见光催化体系构建中的重要意义。     

全有机S型异质结PDI-Ala/S-C3N4光催化剂增强光催化性能

Organic photocatalysts have attracted attention owing to their suitable redox band positions, low cost, high chemical stability, and good tunability of their framework and electronic structure. As a novel organic photocatalyst, PDI-Ala (N, N'-bis(propionic acid)-perylene-3, 4, 9, 10-tetracarboxylic diimide) has strong visible-light response, low valence band position, and strong oxidation ability. However, the low photogenerated charge transfer rate and high carrier recombination rate limit its application. Due to the aromatic heterocyclic structure of g-C₃N₄ and large delocalized π bond in the planar structure of PDI-Ala, g-C₃N₄ and PDI-Ala can be tightly combined through π–π interactions and N―C bond. The band structure of sulfur-doped g-C₃N₄ (S-C₃N₄) matched well with PDI-Ala than that with g-C₃N₄. The electron delocalization effect, internal electric field, and newly formed chemical bond jointly promote the separation and migration of photogenerated carriers between PDI-Ala and S-C₃N₄. To this end, a novel step-scheme (S-scheme) heterojunction photocatalyst comprising organic semiconductor PDI-Ala and S-C₃N₄ was prepared by an in situ self-assembly strategy. Meanwhile, PDI-Ala was self-assembled by transverse hydrogen bonding and longitudinal π–π stacking. The crystal structure, morphology, valency, optical properties, stability, and energy band structure of the PDI-Ala/S-C₃N₄ photocatalysts were systematically analyzed and studied by various characterization methods such as X-ray diffraction, transmission electron microscopy, energy dispersive X-ray spectrometry, X-ray photoelectron spectroscopy, ultraviolet visible diffuse reflectance spectroscopy, electrochemical impedance spectroscopy, and Mott-Schottky curve. The work functions and interface coupling characteristics were determined using density functional theory. The photocatalytic activities of the synthesized photocatalyst for H₂O₂ production and the degradation of tetracycline (TC) and p-nitrophenol (PNP) under visible-light irradiation are discussed. The PDI-Ala/S-C₃N₄ S-scheme heterojunction with band matching and tight interface bonding accelerates the intermolecular electron transfer and broadens the visible-light response range of the heterojunction. In addition, in the processes of the PDI-Ala/S-C₃N₄ photocatalytic degradation reaction, a variety of active species (h⁺, ·O₂^-, and H₂O₂) were produced and accumulated. Therefore, the PDI-Ala/S-C₃N₄ heterojunction exhibited enhanced photocatalytic performance in the degradation of TC, PNP, and H₂O₂ production. Under visible-light irradiation, the optimum 30%PDI-Ala/S-C₃N₄ removed 90% of TC within 90 min. In addition, 30%PDI-Ala/S-C₃N₄ displayed the highest H₂O₂ evolution rate of 28.3 μmol·h^-1·g^-1, which was 2.9 and 1.6 times higher than those of PDI-Ala and S-C₃N₄, respectively. These results reveal that the all organic photocatalyst comprising PDI-based supramolecular and S-C₃N₄ can be efficiently applied for the degradation of organic pollutants and production of H₂O₂. This work not only provides a novel strategy for the design of all organic S-scheme heterojunctions but also provides a new insight and reference for understanding the structure–activity relationship of heterostructure catalysts with effective interface bonding.      

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%.     

Mo掺杂对纳米TiO2结构和活性的影响

利用Mo6 的掺杂在TiO2中引入缺陷,从而扩大TiO2催化剂的光谱响应范围。运用UV-Vis、XRD、XPS、TG-DTA等测试技术考察了钼离子掺杂浓度对于TiO2光催化剂吸收光谱范围、晶型、晶胞和晶粒的影响,分析了钼进入TiO2品格的方式、价态和掺杂催化剂在热处理过程中发生的物理和化学变化。以亚甲蓝溶液的光催化降解为模型反应,考察了掺杂量对这种新型光催化剂的光催化活性的影响。结果表明,Mo6 可进入TiO2晶格中形成杂质缺陷,引起TiO2品格膨胀,Mo6 的掺杂量影响TiO2晶粒尺寸和晶相转化。Mo6 掺杂的质量分数为4．5％时,样品的吸收带边可达460 nm,对40 mg/L亚甲蓝反应2 h的降解率为58．3％,矿化率为52．5%。而Mo6 的掺杂质量分数为3．0％和6．0％时,形成的TiO2晶粒尺寸较小,TiO2晶粒中锐钛矿相与金红石相的比例接近4:1时,对亚甲蓝降解率分别为56．6％和52．0％,矿化率分别为49．2％和44．2％。     

Synthesis and Visible-light Photocatalytic Performance of C-doped Nb2O5 with High Surface Area

C-doped Nb₂O₅ with abundant mesopores has been successfully synthesized through a facile solvothermal synthetic strategy followed by calcination treatment. The resulting C-doped Nb₂O₅ displayed the highest BET surface area(345 m²/g) and large mesopore size(ca. 4.2 nm), capable of offering more accessible active sites as well as faster mass transfer for catalysis. Besides, the doping of C(2.21%, molar fraction) at the O sites in Nb₂O₅ lattice greatly enhanced visible-light response by lowering the band gap, thereby making the material a photocatalyst under visible-light irradiation. Typically, the C-doped Nb₂O₅ exhibited a high H₂ evolution rate of ca. 39.10 μmol·g^-1·h^-1 and also degraded RhB dye completely after 30 min of visible light exposure, which turned out to be much better than Degussa P25 and pure Nb₂O₅ catalysts.     

Photophysical properties and photocatalytic activities of bismuth molybdates under visible light irradiation

Aurivillius structure Bi(2)MoO(6) (BG: 2.70 eV) that is a low-temperature phase showed an intense absorption band in the visible light region and photocatalytic activity for O(2) evolution from an aqueous silver nitrate solution under visible light irradiation, among various bismuth molybdates (Bi(2)MoO(6), Bi(2)Mo(2)O(9), and Bi(2)Mo(3)O(12)) synthesized by solid-state and reflux reactions. Bi(2)Mo(3)O(12) (BG: 2.88 eV) also showed photocatalytic activity for O(2) evolution under full-arc irradiation of a Xe lamp (lambda > 300 nm). The photocatalytic activity of the Aurivillius structure Bi(2)MoO(6) prepared by the reflux method was dependent on the annealing temperature after the preparation. The crystallinity was the important factor for the activity. Calculation by the density functional method indicated that the conduction band of Aurivillius structure Bi(2)MoO(6) was made up of Mo 4d orbitals. It turned out that the visible-light absorption of this photocatalyst was due to the transition from the valence band consisting of O 2p orbitals to the conduction band. The corner-sharing structure of the MoO(6) octahedra contributed to the visible light response and the photocatalytic performance because excitation energy and/or photogenerated electron and hole pairs began to migrate easily in the Aurivillius structure.     

Probing the electronic structures of ternary perovskite and pyrochlore oxides containing Sn(4+) or Sb(5+)

Experimental and computational studies were performed to understand the electronic structure of ternary perovskites (ASnO(3), A = Ca, Sr, Ba, Cd), pyrochlores (RE(2)Sn(2)O(7), RE = Y, La, Lu; Cd(2)Sb(2)O(7)), and defect pyrochlore oxides (Ag(2)Sb(2)O(6)) containing the main group ions Sn(4+) and Sb(5+). In all compounds, the lowest energy states in the conduction band arise primarily from the antibonding Sn/Sb 5s-O 2p interaction. In the alkaline-earth stannate perovskites (BaSnO(3), SrSnO(3), and CaSnO(3)) the conduction bandwidth decreases strongly in response to the octahedral tilting distortion triggered by the decreasing size of the alkaline-earth cation. This in turn leads to a corresponding increase in the band gap from 3.1 eV in BaSnO(3) to 4.4 eV in CaSnO(3). The band gap of CdSnO(3) is relatively small (3.0 eV) considering the large octahedral tilting distortion. The origin of this apparent anomaly is the mixing between the empty Cd 5s orbitals and the antibonding Sn 5s-O 2p states. This mixing leads to a widening of the conduction band and a corresponding decrease in the band gap. The participation of the normally inert A-site cation in the electronic structure near the Fermi level can be considered an inductive effect, as it utilizes substitution on the A-site to directly modify the electronic structure of the SnO(3)(2)(-) framework. While the pyrochlore structure is more complicated, the energy level and width of the lowest energy conduction band can be analyzed in a manner similar to that utilized on the perovskite structure. The Sn-O-Sn and Sb-O-Sb bonds are highly distorted from linear geometry in pyrochlore, leading to a relatively narrow conduction band and a wide band gap. In Cd(2)Sb(2)O(7) and Ag(2)Sb(2)O(6) the Cd(2+) and Ag(+) ions exhibit a strong inductive effect that widens the conduction band and lowers the band gap significantly, very similar to the effect observed in the perovskite form of CdSnO(3).     

Role of complex defects in photocatalytic activities of nitrogen-doped anatase TiO(2)

Deep impurity states associated with a substitutional nitrogen at an oxygen site (N(O)) are believed to be the source of the visible-light absorption of nitrogen-doped titanium dioxide (TiO(2)). Our comprehensive study using density functional theory (DFT) plus onsite Coulomb interaction (U) reveals that a titanium atom at an interstitial site (Ti(i)) is highly mobile and strongly binds with N(O). Hybridizations of N p with Ti d states of Ti(i) give rise to a new band at the valence band edge, eliminating the hole-trapping centers originated from the deep N(O) states. The suggested mechanism explains the photocatalytic oxidation reactions as well as the visible-light absorption observed on N-doped anatase TiO(2).     

Theoretical study of the structure and optical properties of carbon-doped rutile and anatase titanium oxides

The structure and optical properties of carbon-doped titanium oxides, TiO2, in the rutile and anatase forms have been investigated theoretically from first principles. Two possible doping sites were studied, carbon at an oxygen site (anion doping) and carbon at a titanium site (cation doping). The calculated structures suggest that cation-doped carbon atoms form a carbonate-type structure, whereas anion-doped carbon atoms do not invoke any significant structural change. A density-of-states analysis revealed three in-gap impurity states for anion doping. The optical properties of anion-doped cells qualitatively agree with the experimentally reported visible-light absorbance values. We ascribe part of the absorption to transitions from the valence band to one of the impurity states. These transitions should be able to promote photocatalytic reactions, because electron holes in the valence band are considered to be crucial for this process. Neither in-gap impurity states nor visible-light absorbance were observed in the case of cation doping. The effect of oxygen vacancies was also investigated. Introduction of oxygen vacancies into anion-doped TiO2 populates the impurity states and thus suppresses photocatalysis. The interaction of a doped carbon atom with an oxygen vacancy at a finite spatial separation was also carried out. The possibility of either a carbon-oxygen vacancy pair or higher carbon-oxygen vacancy complex existing is discussed.     

WOx/TiO2光催化剂的可见光催化活性机理探讨

采用磁控溅射技术在用浸渍提拉法制得的TiO2薄膜上，溅射氧化钨层,通过气相反应中光催化降解二甲苯的实验表明，WOx/TiO2薄膜具有可见光活性.通过UV-Vis吸收光谱、X射线光电子能谱（XPS）等方法对其可见光活性的机理进行探索.UV-Vis吸收光谱表明WOx,TiO2对可见光响应的范围有一定的扩展,吸收强度增加.XPS表明WOx/TiO2薄膜表面形成了明显的W杂质能级和Ti缺陷能级,这是WOx/TiO2在可见光范围有一吸收的主要原因,也是光催化剂具有可见光活性的必要条件之一，同时杂质能级的存在使半导体费米能级上移,载流子增加,光催化效率提高.     

Bi_(20)TiO_(32)/聚丙烯腈复合纳米纤维的制备及其对异丙隆的光催化降解性能

采用溶剂热法制备了可见光响应型光催化剂Bi_(20)TiO_(32),为了实现该光催化剂的固定化负载,进一步以Bi_(20)TiO_(32)和聚丙烯腈(PAN)为原料,通过同轴静电纺丝法制备了不同光催化剂含量的Bi_(20)TiO_(32)/PAN复合纳米纤维。通过这一途径一方面可以便于光催化剂的回收利用,另一方面纳米纤维结构可以提高光催化剂与有机污染物反应的接触面积。采用X射线衍射(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)、紫外-可见漫反射光谱(UV-Vis DRS)和氮气吸附-脱附法对样品的物相组成、形貌结构、光谱吸收和比表面积等进行表征。研究了在可见光照射下Bi_(20)TiO_(32)/PAN复合纳米纤维膜对苯脲类农药异丙隆的光催化降解性能。结果显示,制备的Bi_(20)TiO_(32)光催化剂禁带宽度为2.35 eV,属于典型的可见光响应型光催化剂。制备的Bi_(20)TiO_(32)/PAN复合纳米纤维直径在600~700 nm,Bi_(20)TiO_(32)可以在纳米纤维表面均匀负载,复合纳米纤维膜对可见光具有明显的响应性,对异丙隆具有很好的光催化降解效果,其中光催化剂质量分数为25.7%的样品S3对异丙隆的降解率最高可达到87%。这一研究表明,通过同轴静电纺丝法将光催化剂负载于有机纳米纤维表面,可以保持光催化剂原有光催化效果,是实现光催化剂固定化一条较好的途径。     

Co-MOF作为电子供体用于提高g-C3N4纳米片的可见光催化还原CO2性能（英文）

作为温室效应的主要气体CO2浓度持续上升,已经成为全球环境问题.将CO2光催化还原成可再生能源不仅可以解决CO2带来的温室效应,而且可以将太阳能转化为燃料物质而取代传统意义上的化石能源.实际上光催化的研究可以追溯到1979年,自从Inoue首次报道了光催化CO2和水制取甲酸、甲烷等有机物,人们一直在努力开发高效的CO2转化光催化剂.近年来,随着光催化技术的快速稳定发展,各种半导体光催化剂,如Zn2Ge O4,CdS,Fe3O4,g-C3N4和SrTiO3等,已被开发用于光催化还原二氧化碳.在这些半导体中,有的材料具有较大的带隙导致较低的可见光活性,有的材料具有毒性引起额外的环境问题.因此,寻求具有适度带隙且环境友好的半导体材料是解决全球变暖问题的关键.近年来,g-C3N4因其带隙(约2.7e V)较窄,具有一定的可见光吸收性能,无污染,以及化学和热稳定性良好等特点,被视为理想的可见光响应光催化材料之一.但是,g-C3N4光吸收有限、光生电子空穴复合率较高等缺点严重限制了其光催化活性.为了进一步提高g-C3N4的CO2可见光催化还原活性,国内外研究者开发了许多方法来提高电荷分离效率,进而提高g-C3N4光催化剂的总体活性.在这些策略中,将g-C3N4与具有合适导带位置的其他材料偶联以促进电子空穴分离是提高光催化性能的有效方法之一.由于Co-MOF具有较窄的带隙且导带位置与g-C3N4匹配,我们选择Co-MOF与g-C3N4复合来克服g-C3N4的缺点,进而达到提高其光催化活性的目的.作为电子供体的Co-MOF能够将最低未占分子轨道(LUMO)上的光生电子转移到g-C3N4的导带以促进电荷分离,同时水被g-C3N4价带上的空穴氧化,最终生成氧气,从而提高光催化还原CO2的性能.制备的Co-MOF/g-C3N4纳米复合材料在可见光照射下具有优异的光催化还原CO2性能,约为纯g-C3N4的光催化活性的2倍.一系列分析表明,Co-MOF的引入不仅拓宽了可见光的吸收范围,而且促进了电荷分离,有利于提高g-C3N4的光催化活性.特别是在590nm单波长照射下进行的羟基自由基实验进一步证明了Co-MOF的LUMO上的光生电子可以转移到g-C3N4.该研究结果为基于g-C3N4的光催化体系的合理构建提供了新思路.     

β-AgAl(1-x)Ga(x)O2 solid-solution photocatalysts: continuous modulation of electronic structure toward high-performance visible-light photoactivity

A series of β-AgAl(1-x)Ga(x)O(2) solid-solution materials were explored as novel visible-light-sensitive photocatalysts. These Ag-based solid solutions crystallize in a homogeneous crystal structure with orthorhombic symmetry but possess continuously modulated band gaps from 2.19 to 2.83 eV by decreasing the ratios of Ga/Al. Their photoactivities for iso-propanol degradation were found to be dependent on the variation of chemical compositions. Among them, the β-AgAl(0.6)Ga(0.4)O(2) sample showed the highest photocatalytic performance, which simultaneously exhibited 35 and 63 times higher activities than two terminus materials, β-AgAlO(2) and β-AgGaO(2), respectively. The apparent quantum efficiency of this sample for iso-propanol photodegradation achieved up to 37.3% at the wavelength of 425 ± 12 nm. The theoretical calculation based on density functional theory demonstrated that the levels of valence band maximum of β-AgAl(1-x)Ga(x)O(2) are similar, but the levels of conduction band minimum are gradually negatively shifted with the increase of the ratio of Ga/Al, thereby continuously narrowing the band gap. Nevertheless, the highest activity observed on β-AgAl(0.6)Ga(0.4)O(2) may be attributed to its optimized band structure, which adapts the balance between effective visible-light absorption and adequate redox potentials.     

具有SPR效应的Ag/Ag2MoO4材料在可见光区的光催化性能研究

作为一类新兴的光催化材料,钼酸盐纳米材料具有高表面能、多活性位点和高选择性等优点,在可见光催化降解污染物方面有着重要应用,近年来受到广泛关注.作为钼酸盐家族重要的一员,钼酸银在杀菌、表面增强拉曼光谱、气敏材料等方面均有重要应用,但其光催化性能却鲜见报道.这是由于它的光谱响应范围窄和广生载流子分离效率低所致.虽然近来有少量基于钼酸银的复合材料的光催化研究,但催化效果不佳.众所周知,作为自由电子体系,诸多金属纳米粒子,如贵金属、碱金属等,存在表面等离子体共振效应(SPR),使得贵金属,特别是Ag,Au等纳米粒子在可见区域有较强的吸收.利用这一特性,Awazu等将Ag纳米颗粒沉积在TiO2表面,创造性地将SPR应用于光催化反应,开发出在可见光谱区具有宽光谱吸收特征的Ag/TiO2.随后陆续合成出基于SPR效应的Ag@AgCl,Ag/Ag3PO4材料均具有良好的光催化性能.基于此,本文在十二烷基硫酸钠(SDS)的存在下,采用水热法一步合成了具有SPR效应的Ag/Ag2MoO4可见光催化材料,并利用X射线粉末衍射(XRD)、紫外可见漫反射(DRS)、X射线光电子能谱(XPS)和扫描电子显微镜(SEM)等技术对材料进行了表征.系统地探讨了体系pH值、反应时间、表面活性剂用量对产物的晶相和微观形貌等的影响.此外,还利用罗丹明B降解实验考察了上述合成条件对材料可见光催化活性的影响,并通过捕获剂实验深入地研究了起催化作用的活性物种.XRD结果表明,体系的pH值对材料的晶型有极大影响,随着pH由酸性变至中性、碱性,最终得到的钼酸银也由Ag2Mo2O7过渡到Ag2MoO4.SEM图显示在最优条件(pH为7,加入0.5 g SDS,160oC下水热14 h)下制得的钼酸银为八面体的Ag2MoO4,且其表面均匀地分布着Ag纳米颗粒,与XPS图谱结果一致.另外表面活性剂SDS的用量对所合成材料的形貌影响很大.本文可一步得到以八面体Ag2MoO4为主的Ag/Ag2MoO4复合材料,是因为SDS的疏水长链可以诱导Ag2MoO4的各向异性生长.DRS结果表明,Ag2MoO4八面体上Ag颗粒的引入使其在可见光区的吸收明显加强,因而它在可见光下催化降解罗丹明B降解反应活性增加.捕获剂实验结果表明,起决定性作用的活性物种是光生空穴,另外?OH也起了一定作用.     

Synthesis and visible-light photocatalysis capability of BiFeO3–(Na0.5Bi0.5)TiO3 nanopowders by a sol–gel method

Multiferroic BiFeO₃–(Na_0.5Bi_0.5)TiO₃ (BFO–NBT) nanopowders were successfully synthesized by a sol–gel method, and the visible-light photocatalytic and magnetic properties of BFO–NBT nanopowders were investigated. X-ray diffraction results indicated that the adding of NBT and the excess of natrium source could suppress the formation of secondary phases and made it easier to obtain single perovskite phase. High photoactivity of this catalyst for Rhodamine B (RhB) degradation under visible-light irradiation was detected, which is due to narrow band gap energy of 2.08 eV, higher surface area and pure phase compounds with no or less amounts of impurities. The BFO–NBT nanopowders showed a weak ferromagnetic order at room temperature, which should be attributed to the size-confinement effects of the nanostructures. It is suggested that BFO–NBT is a kind of new narrow band gap semiconductor visible-light photocatalyst with broad application prospects, in addition to potential applications for novel magnetoelectric devices.     

Ce-doped ZnO (Ce(x)Zn(1-x)O) becomes an efficient visible-light-sensitive photocatalyst by co-catalyst (Cu2+) grafting

We have fabricated an efficient visible-light-sensitive Cu(2+)-grafted Ce-doped ZnO photocatalyst (Cu(2+)-Ce(x)Zn(1-x)O) by adopting a metal ion doping and co-catalyst modification. Impurity states were formed below the conduction band (CB) edge in Ce(x)Zn(1-x)O, and these impurity states induce the visible-light absorption. Ce(x)Zn(1-x)O without a Cu(2+)-co-catalyst showed negligible visible-light activity due to the low reduction power of electrons in impurity levels. Surprisingly, Cu(2+)-modification over Ce(x)Zn(1-x)O drastically increased its visible-light activity. Excited electrons in impurity states can transfer to the Cu(2+)-ions on the surface and form Cu(2+)/Cu(+) redox couples, which cause the efficient oxygen reduction through a multi-electron reduction process. One of the striking features of the present study is that the metal doped semiconductors which were inactive due to their impurity states become efficient visible-light photocatalysts upon co-catalyst modification. The successful strategy used here for designing a highly active visible-light photocatalyst would provide numerous opportunities to develop an efficient metal-ion based visible-light photocatalyst.