高效SnO2纳米片催化剂用于CO氧化

SnO2是一种具有丰富表面缺位氧的n型半导体,其晶格氧亦可还原.另外其熔点高达1630oC,具有较高的热稳定性能.在过去的几十年中, SnO2主要用作气敏材料.而其作为催化材料的性能,特别是用于大气污染治理则鲜见报道.在过去的几年中,本课题组系统研究了SnO2的催化化学,发现利用传统共沉淀法制备的SnO2纳米粉末,在焙烧温度高于500 oC时,其比表面积通常低于20 m2/g,因而限制了其氧化活性.在SnO2晶格中掺杂Fe、Cr、Mn、Ce和Ta等形成固溶体可有效提高其比表面积并产生更多的活性氧物种,因而其对CO和CH4的氧化活性及稳定性大幅度提高.本课题组近期研究结果表明,采用熔盐法制备的高纯SnO2纳米棒单晶比SnO2纳米颗粒和纳米微球等具有更优异的CO氧化活性,260 oC即可完全氧化CO.且在240–260 oC狭窄温度区间发生转化率突跃,表现出类似贵金属的催化行为.值得指出的是, SnO2纳米棒的比表面积(1 m2/g)远低于其他几种形貌的材料,且无活泼氧存在.但研究表明SnO2纳米棒具有优先暴露的(110)活泼晶面,是导致其活性优良的主要原因.另外,我们采用简单共沉淀法成功制备了高比表面介孔Cu-Sn复合氧化物纳米片(196 m2/g),其在140 oC即可将CO完全氧化,且具有优良的抗水失活性能.因此, SnO2的形貌是影响其催化活性的主要因素之一,但迄今未见较系统深入的研究.在上述工作基础上,本文通过水热法,不添加任何有机模板剂,成功制备了厚度约10 nm的介孔SnO2纳米片和纳米棒及纳米颗粒混合物样品;采用常规共沉淀法制备了SnO2纳米颗粒.并将以上三种不同形貌的SnO2纳米材料用于CO氧化.利用SEM、XRD、N2吸附-脱附、H2-TPR和XPS探讨了不同形貌SnO2催化剂的体相结构和表面性质及其对催化性能的影响.与SnO2纳米颗粒相比,介孔SnO2纳米片具有高的比表面积、孔体积及更活泼的氧中心,因此后者CO氧化活性远高于前者.在空速18000 mL/(g·h)时, SnO2纳米片在260 oC即可完全氧化CO.而SnO2纳米颗粒的CO完全氧化温度高于360 oC. SnO2纳米棒和纳米颗粒的混合样品虽然其比表面积和孔体积及表面活性氧的活性仅略高于SnO2纳米颗粒,但XRD定量结果表明,其具有更多的暴露(110)活泼晶面,因而活性也高于SnO2纳米颗粒. SnO2纳米片催化剂的寿命及抗水性能测试结果表明,该催化剂具有良好的稳定性,且水蒸气仅对其活性产生可恢复的影响.进一步优化其性能, SnO2纳米片有可能用于实际汽车尾气状况下的CO催化清除.     

钙钛矿型氧化物负载纳米金属催化剂结构的动态调变及其催化氧化CO反应性能

研究了钛酸钡和钛酸钙担载的Ag和Pt纳米催化剂的表面结构随氧化-还原处理过程的动态变化及其对CO完全氧化反应性能的影响.发现氧化物担载的Ag催化剂在氧化处理后其催化活性较还原处理的高; X射线衍射(XRD)和X射线光电子能谱(XPS)表征结果表明,氧化处理能够提高载体表面Ag颗粒的分散度,而还原处理导致Ag颗粒的聚集,从而降低了催化氧化CO反应的活性.氧化-还原处理改变了担载Ag纳米粒子的尺寸并影响其CO氧化反应活性.与此相反,氧化物担载的Pt催化剂在还原处理后所表现出的CO氧化反应活性较氧化处理的高; 对比研究发现,氧化和还原处理后Pt纳米粒子的尺寸基本相同,但是氧化处理的样品中Pt表面物种以氧化态为主,而还原处理后Pt表面物种主要为金属态.Pt纳米粒子表面化学状态随氧化-还原处理的调变是导致表面催化活性差异的主要原因.     

Zn_2SnO_4纳米材料制备及光致发光特性

以ZnO、SnO2和活性炭的混合物为原料,通过碳热还原热蒸发法无催化剂成功制备出Zn2SnO4纳米材料.借助X射线衍射仪(XRD)、拉曼光谱和扫描电子显微镜(SEM)对样品物相和形貌进行了表征,结果显示样品为面心立方结构的Zn2SnO4纳米链状棒,同时含有少量的ZnO物相.利用X射线光电子能谱(XPS)对Zn2SnO4样品表面各元素的化学状态及相互作用方式进行了测试,结果表明:样品中Zn和Sn分别是以+2价和+4价氧化态形式存在,其中Zn2p3/2电子有两个结合能,分别来自ZnO和Zn2SnO4,Zn2SnO4中Sn4+占据不同的格点位置.室温下光致发光谱(PL)结果显示,样品在紫外区域(320-450nm)和可见区域存在很强的发光带,其中紫外区域的宽发光带,经过高斯拟合可分为358和385nm两个发光峰,与同条件下制备得到的纯ZnO纳米材料发光谱比较,确认358nm发光峰是来自于Zn2SnO4的近带边复合发光.     

氧化石墨烯的制备及低温还原研究

用化学氧化法制备氧化石墨烯,并用一种新型的低温化学还原方法将其还原。用红外光谱、拉曼光谱、X射线衍射、X射线光电子能谱、扫描电镜、原子力显微镜等多种手段表征氧化石墨烯和还原氧化石墨烯的结构与形貌。结果表明,即使在低温条件下,壳聚糖依然可以还原氧化石墨烯,从而预示,在低温条件下,能够在同一环境下实现氧化石墨烯的还原和石墨烯的应用。     

氧化铈的结构对其热稳定性及催化丙烷氧化脱氢反应性能的影响

采用湿化学法制备了低维氧化铈的纳米棒和纳米颗粒,通过原位X射线粉末衍射、透射电镜和N2物理吸附等技术研究了氧化铈纳米结构对其热稳定性的影响.结果表明,氧化铈纳米棒的稳定性更高.采用浸渍法制备了氧化铈负载的氧化钒催化剂,并用于丙烷氧化脱氢反应中,发现以氧化铈纳米棒为载体的催化剂表现出更高的丙烯选择性,这可能是由于棒状结构的开放性有利于产物丙烯的直接扩散.     

α-Fe2O3表面结构对NH3选择性催化还原NO活性的影响

通过水热法合成了两种具有不同形貌的α-Fe2O3纳米棒和纳米立方体,并探索了它们的中温NH3选择性催化还原(NH3-SCR)NO的活性.NH3-SCR测试表明α-Fe2O3纳米棒具有更高的催化活性.X射线粉末衍射(XRD)、场发射扫描电镜(FE-SEM)和高分辨透射电镜(HRTEM)结构分析表明:α-Fe2O3纳米棒暴露有高表面能的{110}活性面,而纳米立方体暴露的主要是低表面能的{012}晶面.H2程序升温还原(H2-TPR)和NO程序升温脱附(NO-TPD)结果证明纳米棒比纳米立方体具有更高的氧化还原性能.因此,α-Fe2O3纳米棒由于暴露高表面能的活性面具有比纳米立方体更高的NH3-SCR性能.     

CO氧化反应中的二氧化铈晶面效应

二氧化铈(CeO2)因其具有较强的储放氧能力,被用作氧化还原反应的催化材料.自2005年,研究者制备出形貌可控的CeO2纳米棒、纳米立方块和纳米多面体,在CeO2形貌控制及构效关系研究方面取得长足发展.各种结构表征手段包括原位拉曼(in situ Raman)、原位傅里叶变换红外光谱(in situ DRIFTS)、核磁共振(NMR)和电镜等被用来研究不同形貌CeO2的表面结构和在催化反应中的活性差异.一般的活性规律为CeO2纳米棒({110}/{100})>纳米立方块({100})>纳米多面体({111}/{100}).近年来,负载型CeO2催化剂因其能稳定分散金属,通过金属-载体相互作用调控界面电子结构并表现出优异的催化活性而引起广泛关注,其中晶面效应在负载型CeO2催化体系中显得较为复杂.铜铈催化剂被认为是非常经济有效的CO氧化催化剂,然而由于制备和测试条件差异导致的CeO2晶面对铜铈催化剂催化CO氧化活性的影响规律并不统一.我们之前的研究工作发现纳米棒CeO2-{110}晶面上的Cu-[Ox]-Ce结构不利于形成Cu((40)),而纳米颗粒CeO2-{111}晶面上的CuOx团簇很容易形成Cu((40)),从而对CO催化氧化极为有利,这与纯载体CeO2的规律并不一致.与此同时,对于铜负载的CeO2纳米棒(NR)及纳米立方体(NC)所体现的性质及活性差异缺少系统深入的研究.在上述工作基础上,我们采用沉积沉淀法在CeO2 NR及CeO2 NC上负载1%wt的铜分别得到1Cu CeNR和1Cu CeNC,并对所合成催化剂的结构和吸附性能进行了表征.高分辨透射电镜(HRTEM)照片显示,CeO2纳米棒主要暴露{110}晶面,而CeO2纳米立方体以{100}晶面为主.催化测试结果表明,1Cu CeNC在130℃时CO已完全转化为CO2,而相同温度下1Cu Ce NR只有50%转化.进一步通过氢气程序升温还原(H2-TPR)和一氧化碳程序升温脱附(CO-TPD)分析发现, 1Cu Ce NC催化剂具有较强的还原性且表面氧物种含量高.此外, X射线光电子能谱(XPS)和in situ DRIFTS研究表明, 1Cu Ce NC促进Cu((40))位点生成,导致活性Cu((40))-CO物种增多,这些优异的化学性质导致其具有较高的催化CO氧化活性.     

球形分枝结构Pt纳米催化剂的合成、纯化及电催化性能

以非离子型表面活性剂Brij-35为稳定剂,以水为溶剂,在常温、常压条件下利用抗坏血酸还原K2PtCl4制备了Pt纳米催化剂,采用透射电子显微镜、能量弥散X射线谱、X射线粉末衍射、热重及循环伏安扫描对催化剂进行了表征.结果表明,所制Pt纳米催化剂为尺寸均一的球形分枝结构,平均粒径为36.9nm,其中每一个Pt分枝的直径为2～4nm,长度为4～6nm.为去除表面活性剂Brij-35和副产物,开发了一种简单的多次水洗法以纯化所制Pt纳米催化剂.表征结果证明,该法可有效去除表面活性剂和副产物,所得催化剂纯度与商业Pt黑(99.9%)相当,且电化学活性比表面积更高,在氧还原反应和甲醇氧化反应中表现出更高的电催化活性.     

氮掺杂还原氧化石墨烯负载铂催化剂的制备及甲醇电氧化性能

采用高温热解聚苯胺修饰的氧化石墨烯（PANI-GO）,得到了氮掺杂的还原氧化石墨烯碳材料（N-RGO）,以其负载Pt 制备了Pt/N-RGO纳米结构电催化剂. 采用透射电镜（TEM）、X射线光电子能谱（XPS）、X 射线衍射（XRD）谱及拉曼光谱等技术对N-RGO和Pt/N-RGO的形貌及结构进行了表征,用循环伏安、计时电流等电化学技术研究了Pt/N-RGO电极催化剂对CO溶出反应和甲醇电氧化反应的催化性能. 结果表明：高温热解PANIGO可同时实现GO的还原及其氮掺杂的过程,氮掺杂引起还原氧化石墨烯碳材料表面缺陷结构和导电性的增加;与相应的未掺杂氮样品Pt/RGO相比较,Pt/N-RGO样品上Pt 颗粒的分散更均匀,显示出更强的抗CO毒化能力和更高的甲醇电氧化催化活性及稳定性.     

SnO2-TiO2薄膜载体对Au-Pt纳米颗粒电化学性能的影响

采用真空镀膜法在玻碳(GC)电极表面修饰SnO2-TiO2薄膜, 在SnO2-TiO2/GC复合电极表面组装Au-Pt双金属纳米颗粒, 制得Au-Pt/SnO2-TiO2/GC复合电极. 通过循环伏安法(CV)研究了SnO2-TiO2薄膜载体对Au-Pt双金属纳米颗粒电化学性能的影响; 采用扫描电镜(SEM)及X射线光电子能谱(XPS)对Au-Pt在SnO2-TiO2薄膜沉积的形貌及结构进行了表征. 研究结果表明, 10 nm的Au-Pt双金属纳米颗粒均匀地组装于SnO2-TiO2薄膜表面; SnO2-TiO2薄膜载体改善了复合电极抗CO中毒能力; Au-Pt双金属合金的形成提高了Pt 对甲醇氧化的电催化能力, SnO2-TiO2薄膜载体又使Pt纳米粒子d空轨道增多, 提高了Au-Pt双金属纳米颗粒的稳定性和催化性能.     

Synthesis,characterization, and biosensing application of ZnO/SnO2 heterostructured nanomaterials

In this work, zinc oxide/tin oxide (ZnO/SnO₂) heterostructured nanomaterials were synthesized by hydrothermal method. Transmission electron microscopy, scanning electron microscopy, energy-dispersive X-ray spectroscopy, and X-ray diffraction measurements revealed that the product was composed of ZnO nanowires and SnO₂ nanobranches. The novel ZnO/SnO₂ heterostructured nanocrystals were for the first time used as a supporting matrix to explore a novel immobilization and biosensing platform of redox proteins. UV–visible absorption investigation indicated that hemoglobin (Hb) intercalated well in the ZnO/SnO₂ heterostructured nanocrystals retained its native structure. Comparative experiments have confirmed that the ZnO/SnO₂-based biosensor not only had enhanced direct electron transfer capacity but also displayed excellent electrocatalytic properties such as higher sensitivity and wider linear range to the detection of hydrogen peroxide in comparison with the ZnO- and SnO₂-based biosensors.     

Size-controlled synthesis of SnO2 nanoparticles using reverse microemulsion method

Tin oxide nanoparticles were prepared using an ionic surfactant (sodium dodecyl sulfate) and tin (IV) chloride as an inorganic precursor via the reverse microemulsion method. The size of the nanoparticles is controlled by variation of water-to-surfactant ratio. Eliminating of surfactant in prepared nanoparticles was confirmed by the infrared spectroscopy after sequential calcinations. Transmission electron microscopy, surface area, pore volume, average pore diameter, pore size distribution and X-ray diffraction results were used for evaluation of size distribution, shape and structure of prepared SnO₂ nanoparticles. Transmission electron micrographs confirmed that the obtained materials are spherical nanoparticles. The X-ray diffraction results show the crystalline phases of all samples are SnO₂ with tetragonal structured crystal. In addition, the X-ray diffraction and transmission electron microscopy data showed that the size of SnO₂ nanoparticles decreased with decreasing the water-to-surfactant ratio.     

Synthesis and gas sensitivities of SnO2 nanorods and hollow microspheres

SnO₂ urchin-like structures composed of nanorods with diameters of 10-15 nm and lengths of 50-70 nm have been hydrothermally synthesized via a H₂O₂-assisted route without any surfactant, using SnCl₂ as raw material. With the addition of methenamine (HMT), SnO₂ hollow microspheres with diameters of 2-3 μm and shell thickness of 60-140 nm were also prepared. The as-obtained products were examined using diverse techniques including X-ray powder diffraction (XRD), Raman spectroscopy, field-emission scanning electron microscopy (FE-SEM), transmission electron microscopy (TEM), selected-area electron diffraction (SAED), high-resolution TEM and photoluminescence spectra. The gas sensitivity experiments have demonstrated that the as-synthesized SnO₂ materials exhibit good sensitivity to alcohol vapors, which may offer potential applications in gas sensors.     

High visible light-driven photocatalytic activity of large surface area Cu doped SnO<Subscript>2</Subscript> nanorods synthesized by novel one-step microwave irradiation method

The paper investigates the structural, optical and photocatalytic activity of large surface area single crystalline copper (Cu) doped SnO₂ nanorods (NRs) synthesized by a novel one-step microwave irradiation method. Powder X-ray diffraction (XRD) analysis confirms that both pure and Cu doped SnO₂ are tetragonal rutile type structure (space group P42/mnm) formed during the microwave process within 10 min without any post annealing treatment. Transmission electron microscopy (TEM) reveals that the as synthesized Cu doped SnO₂ samples exhibited rod-like shape and the length was less than 80 nm and diameter was about few nanometers. Typical selected-area electron diffraction (SAED) pattern indicates that, the growth direction of Cu–SnO₂ nanorod is along [110] direction. The variety of phonon interaction in the pure and Cu doped SnO₂ is observed by Raman spectroscopy. Electron paramagnetic resonance and X-ray photoelectron spectroscopy (XPS) confirms that the presence of copper and tin as Cu²⁺ and Sn⁴⁺ in state, respectively. The photocatalytic activity was monitored via the degradation of methylene blue (MB) and Rhodamine B (RhB) dyes and the Cu–SnO₂ showed better photocatalytic activity than that of pure SnO₂. This could be attributed to the effective electron–hole separation by surface modification.     

Preparation and Optoelectronic Property of a SnO2/CdS Nanocomposite Based on the Flowerlike Clusters of SnO2 Nanorods

A SnO₂/CdS nanocomposite based on the flowerlike clusters of SnO₂ nanorods was prepared and characterized with x-ray diffraction (XRD), transmission electron microscope (TEM), scanning electron microscopy (SEM) and EDX analysis. The SEM and TEM images show the nanocomposite is composed of CdS nanoparticles and flowerlike clusters of SnO₂ nanorods. The UV–vis spectrum of the nanocomposite displays a new absorption band in the region of 350 to 530 nm, compared with that of the flowerlike clusters of SnO₂ nanorods. The measurement of optoelectronic property indicates that the photoresponse of the composite is extended into the visible region and the incident photon-to-current conversion efficiency (IPCE) of the composite is up to 6.5 in the range of 400 to 440 nm. These phenomena ought to be ascribed to the special nanostructure of the SnO₂/CdS composite obtained.     

Fabrication and photocatalytic properties of SnO2 double-shelled and triple-shelled hollow spheres

SnO₂ double-shelled and triple-shelled hollow spheres were tailored by adjusting concentration of tin (IV) chloride solution during the process of the tin (IV) ions infused carbonaceous spheres. The structures of these SnO₂ multi-shelled hollow spheres were examined by X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), and their possible formation mechanism were also discussed. In virtue of triple-shelled hollow porous structure and higher specific surface area, SnO₂ triple-shelled hollow spheres exhibited enhanced photocatalytic properties compared to SnO₂ double-shelled hollow spheres.     

Fabrication of CoO nanorods via thermal decomposition of CoC2O4 precursor

Cobalt oxide (CoO) nanorods were synthesized by annealing CoC₂O₄ precursor. The nanorods were identified by Transmission electron microscopy (TEM), X-ray diffraction (XRD), high-resolution transmission electron microscopy (HRTEM) and other methods. The results showed that the nanorods are composed of cubic CoO with diameter of 10–80 nm, and lengths ranging from 1 to 3 μm. The mechanism of formation of CoO nanorods was also discussed.     

Boron and nitrogen-codoped TiO2 nanorods: Synthesis, characterization, and photoelectrochemical properties

Boron and nitrogen codoped TiO₂ nanorods (BNTRs) were synthesized via two-step hydrothermal reactions using TiN as a starting material. The as-prepared samples were characterized by X-ray diffraction, field-emission scanning electron microscope (SEM), transmission electron microscopy and X-ray photoelectron spectroscopy techniques. The results showed that TiO₂ nanorods with the diameter of approximately 50–100 nm and the length of several micrometers were doped by the interstitial N and B. The nanorods were firstly formed in the hydrothermal synthesis of nitrogen doped TiO₂. The growing process of nanorods was observed by SEM and a most probable formation mechanism of the trititanate nanorods was proposed. The BNTRs showed a higher photocatalytic activity and a bigger photocurrent response than N–TiO₂ nanorods under visible light irradiation.     

Synthesis,Characterization and Photocatalytic Application of TiO<Subscript>2</Subscript>/SnO<Subscript>2</Subscript> Nanocomposite Obtained Under Non-thermal Plasma Condition at Atmospheric Pressure

A plasma-assisted synthesis of TiO₂/SnO₂ nanocomposite is described. In this approach, a precursor containing a mixture of [TiCl₃ and SnCl₂] exposed to electric discharge was oxidized by plasma-generated reactive species (HO^·/H₂O = 2.85 eV/SHE). SnO₂ microstructures with a diameter of 10–40 µm were coated by thin layers TiO₂ nanorods with mean diameter of 6–8 nm. The obtained TiO₂/SnO₂ nanocomposite was characterized by transmission and scanning electron microscopy, X-ray diffraction and Fourier transform infrared. TiO₂/SnO₂ nanocomposite was found to be a promising new material for the photocatalytic discoloration of aqueous Remazol Brilliant Blue-R dye under daylight and UVA light sources, due to the combined effects of large specific surface area and heterojunction which efficiently separates the electron–hole pairs delaying the charge recombination. The leaching test indicated that the nanocomposite is stable easily reusable.     

Characterization of h-WO3 nanorods synthesized by hydrothermal process

Hexagonal tungsten oxide nanorods have been synthesized by hydrothermal strategy using Na₂WO₄·2H₂O as tungsten source, aniline and sulfate sodium as structure-directing templates. Techniques X-ray diffraction (XRD), scanning electron microscopy (SEM), transmission electron microscopy (TEM), high-resolution transmission electron microscopy (HRTEM), Fourier transform infrared spectroscopy (FTIR) and Raman spectroscopy have been used to characterize the structure, morphology and composition of the nanorods. The h-WO₃ nanorods are up to 5 μm in length, and 50–70 nm in diameter.