纳米复合Sb_2O_3/TiO_2的光催化性能研究

采用溶胶-凝胶法制备复合纳米 Sb2O3/TiO2。 Sb2O3掺入浓度越大,催化剂中锐钛矿相含量越高,晶粒直径与颗粒直径越小,比表面积越大。在 380～ 460nm范围内, Sb2O3/TiO2的反射率则减弱,表明光吸收增强。 XPS分析表明：掺入 2％ Sb2O3,出现新的 Ti2p3/2峰,对应于 Ti3＋,占 9.13％;锑以 Sb3＋、 Sb5＋两种形式存在, Sb5＋占 84.42％、 Sb3＋占 17.58％。以亚甲基蓝溶液光催化降解为模型反应,掺入 2％、 5％ Sb2O3,亚甲基蓝溶液的光催化脱色降解一级动力学常数与总有机炭（ TOC）去除率增大。发射光谱证明： Sb2O3的最佳比例为 2％,当其比例大于 2％时,其电子空穴对的复合率升高,光催化活性下降。     

Sb_xSn_(1-x)O_2固溶体系电学性能与导电机制研究

本文报道以均匀共沉淀法制得 Sbx Sn1 -x O2 体系半导体气敏材料 ,研究了固溶体组成与电导的变化规律 ,并对导电机制进行了讨论。结果表明 :x<0 .30时均可生成固溶体。微量 Sb(x=0 .0 4 )的掺入即能提高 Sn O2 电导一个数量级 ,在 x≤ 0 .0 4区间电导都呈上升趋势 ,其后一直到固溶范围内随着 X增加 ,电导反而缓慢下降。根据体系中存在的 Sb°Sn和 Sb′Sn两种缺陷 ,讨论了其电导变化和导电机制。认为平衡 Sb°Sn 2 e′=Sb′Sn对上述导电机制起决定作用。XPS分析对 Sb5 、Sb3 的含量进行了确认 ,交流阻抗谱的测试结果从另一角度对电导行为加以证实。     

纳米复合Sb2O3/TiO2的光催化性能研究

采用溶胶－凝胶法制备复合纳米Sb2O3/TiO2Sb2O3掺入浓度越大,催化剂中锐钛矿相含量越高,晶粒直径与颗粒直径越小,比表面积越大,在380－460nm,范围内,Sb2O3/TiO2的反射率则减弱,表明光吸收增强,Sb^5＋,占48．42％、Sb^ 占17．58％,以亚甲基蓝溶液光催化降解为模型反应,掺入2％,5％Sb2O3,亚在蓝溶液的光催化脱色降解一致动力学常数与总有机炭（TOC）去除率增大,发射光谱证明,Sb2O3的最佳比例为2％,当其比例大于2％时,其电子空穴对的复合率升高,光催化活性下降。     

α-Fe2O3掺杂对In2O3电导和气敏性能的影响

用化学共沉淀法制备了α Fe2O3掺杂的In2O3纳米晶微粉,研究了α Fe2O3掺杂对In2O3电导和气敏性能的影响. 结果表明, α Fe2O3和In2O3间可形成有限固溶体In2－xFexO3(0≤x≤0.40); Fe3＋对In2O3晶格中In3＋格位的部分取代,大大增强了阴阳离子间的结合力,导致材料中氧空位VO×数骤降、 自由电子的浓度变稀和电导下降. n(Fe3＋):n(In3＋)=5 :5的共沉淀粉于800 ℃下灼烧4 h所得的α Fe2O3掺杂In2O3传感器元件,对45 μmol•L－1 C2H5OH的灵敏度达54.0,为相同浓度干扰气体汽油的8倍多.     

Y2O3薄膜/锡掺杂玻璃光波导气敏元件及其气敏性

采用溶胶-凝胶法将氧化钇(Y2O3)敏感膜固定在锡掺杂玻璃光波导表面,研制出了Y2O3薄膜/锡掺杂玻璃光波导气敏元件,并对挥发性有机气体进行了检测.通过XRD测试对敏感薄膜的结构及晶粒尺寸进行了表征.实验结果表明,在室温下Y2O3薄膜/锡掺杂玻璃光波导气敏元件对二甲苯、氯苯气体有较好的选择性响应,其响应浓度范围为l×10-3 ～1×10-5(V/V).Y2O3薄膜/锡掺杂玻璃光波导气敏元件具有灵敏度高、成本低、响应速度快、制作工艺简单和可逆性好等优点.     

均匀沉淀法制备纳米氧化锡粒子

以 CO(NH2 ) 2 、Sn Cl4· 5 H2 O为原料 ,采用均匀沉淀法制备了纳米 Sn O2 粒子。以 TG-DTA、XRD、TEM等测试手段 ,对纳米 Sn O2 的粒子结构和形貌进行了研究。结果表明 ,在 6 0 0℃下热处理得到的粒子结晶性能良好。改变反应条件 ,制备出了粒径分布窄、分散性良好的纳米 Sn O2 粒子 ,其平均粒径为 15 nm。同时对均匀沉淀法形成纳米 Sn O2 粒子的机理进行了初步探讨     

Fe~(3 )/TiO_2/SiO_2复合纳米微粒的合成及光催化降解NO_2~-

采用溶胶 -凝胶法制备了 Ti O2 / Si O2 和不同浓度 Fe3 掺杂的 Fe3 / Ti O2 / Si O2 复合纳米粉末 ,并利用XRD、BET、UV-vis等手段研究了 Ti O2 / Si O2 及掺铁形成的 Fe3 / Ti O2 / Si O2 复合微粒的表面结构形态变化 ,以及对污染物 NO- 2 光催化降解的影响 .结果表明 ,Fe3 / Ti O2 / Si O2 (ω( Fe3 ) =1 .5 % ,m( Ti)∶ m( Si) =2∶ 1 )具有最佳活性 ,样品呈晶化度较低的锐钛矿结构 .Fe3 掺杂导致晶粒的增大 ,稳定性降低 ,大大提高了半导体的光催化活性 ,有利于对低浓度 NO- 2 的光催化降解     

制备方法对新型锡锆固溶体催化剂结构及其选择催化一氧化氮还原性能的影响

 固定SnO2含量为60％，采用不同沉淀方法和在不同沉淀条件下制备了锡锆固溶体催化剂Sn0．45Zr0．55O2，考察了沉淀过程对其结构和性能的影响．控制尿素浓度为总金属离子（Sn4＋＋Zr4＋）浓度的20倍，采用均相沉淀法制备的锡锆固溶体Sn0．45Zr0．55O2对催化NO还原具有最高活性和较好的重复性，在350℃下最大NO转化率达到74％．XRD，Raman，XPS，BET比表面测定和孔结构分析表明，沉淀条件不同，沉淀物的成核及生长过程不同，对SnO2与ZrO2之间的固溶度、催化剂表面元素分布、比表面和孔道结构以及催化活性都有较大的影响．ZrO2在SnO2（r）晶格中较高的固溶度、Sn在催化剂表面一定程度的偏析以及催化\r\n剂较大的孔径均有利于提高对NO还原反应的催化活性．     

稀土掺杂PbO2电极的制备及催化性能研究

以SnCl4.5H2O,Sb2O3,La（NO3）3（或Nd（NO3））为前驱体（摩尔比分别为Sn∶Sb∶La（Nd）=100∶6∶（0.5,1,2）,制备稀土（La,Nd）掺杂Sn,Sb溶胶,以钛电极为基体,用溶胶-凝胶法制备稀土（La,Nd）掺杂SnO2中间层,热处理温度为450和500℃,热处理时间共5 h;采用电沉积法制备PbO2表面层,得到改性PbO2阳极,优化了制备改性PbO2电极的稀土掺杂量。以含油污水为目标有机物,借助于CODCr去除情况分析电极的电催化氧化能力;分析了电极结构与电催化特性之间的关系。采用SEM和XRD分析了制备电极的表面形貌、晶体结构并通过电化学工作站对其析氧电位进行了表征分析。结果表明,中间层掺杂La元素的电极,掺杂比为Sn∶Sb∶La=100∶6∶1时电极性能最好;而中间层掺杂Nd元素,掺杂比为Sn∶Sb∶Nd=100∶6∶2时电极的性能最好,此比例时电极对目标有机物CODCr去除率分别为91.90%和90.93%。     

Li+,Zn2+共掺杂对Gd2O3:Eu3+纳米粉结构和发光性能的影响

采用燃烧法制备出Li^＋,Zn^2＋掺杂的Gd2O3：Eu^3＋纳米荧光粉,研究了掺杂离子对Gd2O3：Eu^3＋的结晶性能、晶粒形貌和光致发光特性的影响.以X射线衍射（XRD）、透射电子显微镜（TEM）、发射光谱和衰减时间谱等手段表征材料性能.结果表明,Li^＋,Zn^2＋掺杂可显著提高Gd2O3：Eu^3＋纳米粉在611 nm处的发光强度,最大可达到未掺杂时的2.5倍.发光增强的主要原因可归结为3个方面： （1）使晶粒由单斜相向更利于发光的立方相转变; （2）氧空位的敏化剂作用; （3）掺杂离子的助熔剂效应,使晶粒的结晶性能提高、粒径增大,从而降低表面态引起的发光猝灭.     

CO gas sensing by ultrathin tin oxide films grown by atomic layer deposition using transmission FTIR spectroscopy

Ultrathin tin oxide films were deposited on SiO2 nanoparticles using atomic layer deposition (ALD) techniques with SnCl4 and H2O2 as the reactants. These SnO(x) films were then exposed to O2 and CO gas pressure at 300 degrees C to measure and understand their ability to serve as CO gas sensors. In situ transmission Fourier transform infrared (FTIR) spectroscopy was used to monitor both the charge conduction in the SnO(x) films and the gas-phase species. The background infrared absorbance measured the electrical conductivity of the SnO(x) films based on Drude-Zener theory. O2 pressure was observed to decrease the SnO(x) film conductivity. Addition of CO pressure then increased the SnO(x) film conductivity. Static experiments also monitored the buildup of gas-phase CO2 reaction products as the CO reacted with oxygen species. These results were consistent with both ionosorption and oxygen-vacancy models for chemiresistant semiconductor gas sensors. Additional experiments demonstrated that O2 pressure was not necessary for the SnO(x) films to detect CO pressure. The background infrared absorbance increased with CO pressure in the absence of O2 pressure. These results indicate that CO can produce oxygen vacancies on the SnO(x) surface that ionize and release electrons that increase the SnO(x) film conductivity, as suggested by the oxygen-vacancy model. The time scale of the response of the SnO(x) films to O2 and CO pressure was also measured by using transient experiments. The ultrathin SnO(x) ALD films with a thickness of approximately 10 A were able to respond to O2 within approximately 100 s and to CO within approximately 10 s. These in situ transmission FTIR spectroscopy help confirm the mechanisms for chemiresistant semiconductor gas sensors.     

Microstructural control and selective C2H5OH sensing properties of Zn2SnO4 nanofibers prepared by electrospinning

Microstructural evolution of spinel Zn(2)SnO(4) nanofibers was manipulated via an in situ phase separation process of inorganic precursors and a matrix polymer during electrospinning and calcination. Chemiresistive gas sensors using porous Zn(2)SnO(4) fibers exhibited superior C(2)H(5)OH sensing response.     

二氧化锡中空微球用于快速灵敏检测硫化氢

以氨基酚醛树脂球作模板,通过一种简单的模板法制备了具有中空微球(HMS)结构的二氧化锡;将其涂覆于氧化铝陶瓷管金电极表面,制得一种新型薄膜式硫化氢传感器.采用X射线衍射(XRD)及透射电子显微镜(TEM)表征了材料的微观结构和形貌,并考察了二氧化锡中空微球(Sn O2HMS)的气敏性能.结果表明,二氧化锡中空微球对硫化氢气体表现出良好的气敏特性.在最佳工作温度(200℃)下,所制作的传感器对142.6 mg/m3硫化氢的响应值高达97.13%,响应时间为22 s.该传感器对硫化氢的响应线性范围为0.2852~142.6 mg/m3,相关系数为0.9931,检出限达到0.1549 mg/m3,且几乎不受环境湿度和温度的影响,具有良好的重现性和选择性.对养殖场中硫化氢气体连续监测10个月后,传感器响应信号衰减了5.4%,表明该传感器具有长期稳定的使用寿命,可实现远程监测的实际应用.     

A selective optical sensor for antimony based on hexagonal mesoporous structures

Mesostructured materials show promise in fabricating ordered sensing systems in a reproducible manner. Here, the fabrication of optically selective and sensitive sensors up to subnanomolar concentrations of Sb(III) ions was reported via simple and reproducible techniques in which the hexagonal mesoporous silicas in powder and monolith forms were used as probe carriers. Evidence of successful fabrication of the optical sensors was investigated by extensive characterizations using powder X-ray diffraction, nitrogen adsorption/desorption isotherms, 29Si NMR spectroscopy, and transmission electron microscopy. The mesostructured features allowed high adsorption capacity and accessibility of probe molecules and efficient transport of toxic species via much more direct and easier diffusion to the network sites without significant alteration of their physical characteristics, leading to excellent sensing systems in terms of stability and sensitivity with rapid response time of detection. In addition, the high performance of the hexagonal sensors was dependent on key factors such as the number of support-based sensors, the reaction temperature, and the pH value that led to possible naked-eye detection of Sb(III) ion concentration with a detection limit as low as 3x10(-9) mol/dm3 and a wide detection range of 1 ppb-2 ppm. Of particular interest was that our mesostructured sensor design provided control over the retention of the potential functionality of the naked-eye sensing system of Sb(III) ions upon the storage and even after several regeneration and reuse cycles, indicating large-scale reversibility of sensing systems.     

Porous tin oxide nanostructured microspheres for sensor applications

We have sought to enhance the sensitivity of conductometric gas microsensors through the design and fabrication of porous, three-dimensional tin oxide nanoparticle structures. Electrostatically controlled layer-by-layer processing in aqueous solutions was used to decorate sacrificial latex microspheres with Sb:SnO2 nanoparticles. To evaluate their sensing performance, these structures were then deposited as films, via micropipetting, on MEMS micro-hot-plate platforms with interdigitated electrodes. Prior to gas testing, rapid heating of the micro-hot-plates was used to remove the sacrificial latex templates, thereby revealing a 3-D structure composed of interconnected spherical tin oxide nanoparticle shells with porous ultrathin walls. Changes in film conductance, caused by exposure to test gases (methanol, carbon monoxide, benzene, water) in a dry air background, were measured at different temperatures. Hollow nanoparticle microsphere films exhibited partial selectivity for these different gases, good dynamic range at different temperatures and gas concentrations, and good repeatability and stability over long runs. These films also yielded approximately 3-fold and 5-fold increases in sensitivity to methanol when compared to SnO2 polycrystalline chemical vapor deposition films and Sb:SnO2 microporous nanoparticle films, respectively. Gains in sensitivity are attributed to the multiscale porous architecture of the hollow microsphere films. This architecture promotes gas diffusion and increases the active surface area.     

Interplay between O2 and SnO2: oxygen ionosorption and spectroscopic evidence for adsorbed oxygen.

Tin dioxide is the most commonly used material in commercial gas sensors based on semiconducting metal oxides. Despite intensive efforts, the mechanism responsible for gas-sensing effects on SnO(2) is not fully understood. The key step is the understanding of the electronic response of SnO(2) in the presence of background oxygen. For a long time, oxygen interaction with SnO(2) has been treated within the framework of the "ionosorption theory". The adsorbed oxygen species have been regarded as free oxygen ions electrostatically stabilized on the surface (with no local chemical bond formation). A contradiction, however, arises when connecting this scenario to spectroscopic findings. Despite trying for a long time, there has not been any convincing spectroscopic evidence for "ionosorbed" oxygen species. Neither superoxide ions O(2)(-), nor charged atomic oxygen O,(-) nor peroxide ions O(2)(2-) have been observed on SnO(2) under the real working conditions of sensors. Moreover, several findings show that the superoxide ion does not undergo transformations into charged atomic oxygen at the surface, and represents a dead-end form of low-temperature oxygen adsorption on reduced metal oxide.     

Single-crystalline Sb-doped SnO2 nanowires: synthesis and gas sensor application

The synthesis of semiconducting Sb-doped SnO2 nanowires in mass production by an in situ doping approach are reported, and the ethanol sensing results demonstrated that Sb-doped SnO2 nanowires have a promising application for the fabrication of gas sensors with low resistance, and quick response and recovery times.     

钠离子取代对气相分子氢氘交换反应的影响

用质谱学方法测定分子的氢氘交换反应过程和结果是研究蛋白质分子等生物体系的分子构象,如蛋白质折叠状态的常用方法之一．本文利用线型离子阱．飞行时间质谱技术,在气相中测定了由不同个数钠离子所取代的简单多肽分子——五联丙氨酸（5Ala-nH＋nNa）．H^＋,,n=2,3,4,5的氢氘交换反应情况,得到了由不同个数钠离子取代的分子离子的氢氘交换反应速度以及交换的氢氘数量等,并研究了钠离子个数对分子氢氘交换反应的影响．结果表明,在本工作的实验条件下,钠离子的取代将影响分子离子的氢氚交换反应．当钠离子数为2时,（5Ala-2H＋2Na）．H^＋分子离子很难发生氢氘交换反应;当钠离子数增加时,对于（5Ala-3H＋3Na）．H^＋,（5Ala-4H＋4Na）．H^＋,和（5Ala-5H＋5Na）．H^＋等,分子的氢氘交换反应速度会加快．这可能是由于钠离子的取代导致了分子离子的构型以及分子的质子亲和势发生了显著的改变,因此影响它们的氢氘交换反应．此外,我们还研究了线型四极场的q值对离子氢氘交换反应的影响,发现对于某种离子,当其对应的四极场q值低于0．8时,对各种离子的交换反应速度影响不大,但当q值接近第一稳定区图的边界点,即当q接近0．908时,对某些离子的交换反应速度影响很明显．q值对离子的交换反应速度影响可以用离子的运动速度加快而导致碰撞反应能量增加来解释．     

An Au clusters related spill-over sensitization mechanism in SnO(2)-based gas sensors identified by operando HERFD-XAS, work function changes, DC resistance and catalytic conversion studies

The role of Au additives in SnO(2)-based thick film gas sensors was investigated by a combination of operando investigation techniques, namely spectroscopic high energy resolved fluorescence detected X-ray absorption spectroscopy (HERFD-XAS) and simultaneous DC resistance and work function change measurements. The results have shown that the Au is present in the form of small metallic particles at the surface of the host metal oxide without changing its bulk or surface electronic properties. The sensitization effect of Au can therefore be attributed to the "spill-over effect", meaning that the Au particles enrich the surface of the active metal oxide with oxygen species which consequently react with reducing gases such as CO and H(2). This is in contrast to the effect of Pd and Pt promoters which were found to be distributed at an atomic level on the surface and in the bulk of the supporting sensing material and therefore have a tremendous effect on its bulk and surface electronic properties.     

热处理对LiFe1-0.01xY0.005xAg0.005xPO4薄膜光波导传感元件气敏性的影响

以FeSO4.7H2O,H3PO4,LiOH.H2O,AgNO3及Y(NO3)3.6H2O为原料,利用水热法一步合成出了LiFe1-0.01xY0.005xAg0.005xPO4粉体(x=0.5,1.0),并将该材料作为敏感试剂,用旋转-甩涂法做成纳米薄膜固定在锡掺杂玻璃光波导表面,在不同温度下进行热处理。采用紫外-可见分光光度计、测厚仪以及自组装的玻璃光波导气敏测试仪研究了热处理对LiFe1-0.01xY0.005xAg0.005xPO4薄膜光学及气敏特性的影响。研究结果表明:在450℃下进行热处理的薄膜元件具有良好的光学透明及较好的气敏特性。相同浓度的不同挥发性有机气体中,该传感元件对二甲苯气体有很好的选择性响应,其检测响应范围为1×10-7～1×10-3(V/V),响应-恢复时间分别小于5和100 s。