一步水热法制备TiO2复合结构及光伏性能研究

采用一步水热法制备TiO₂纳米棒阵列,研究了无水乙醇作为前驱物替换去离子水对纳米棒阵列的形貌的影响。实验发现,当无水乙醇的含量达到100%的时候,在生长的TiO₂纳米棒阵列的上面获得一层以TiO₂纳米棒为基本单元的微米球, 从而制备出TiO₂复合纳米阵列薄膜。通过XRD和TEM发现,样品为单晶四方金红石结构TiO₂构成的阵列薄膜,将样品组装成染料敏化太阳能电池后,电池的开路电压和短路电流分别为V_oc=0.63 V,J_sc=10.9 mA·cm^-2,填充因子FF=56.3%,转换效率达到η=4.1%。     

P3HT/CdS/TiO2/ZnO一维有序核壳式纳米棒阵列的构制及其在杂化太阳电池中的应用研究

采用恒电位法在铟锡氧化物导电玻璃(ITO)上制备了高度有序一维ZnO纳米棒阵列,将ZnO纳米棒阵列在TiO2溶胶中采用提拉法制备出了一维TiO2/ZnO核壳式纳米棒阵列.在一维TiO2/ZnO核壳式纳米棒阵列上电沉积CdS纳米晶得到一维CdS/TiO2/ZnO核壳式纳米棒阵列,然后在一维CdS/TiO2/ZnO核壳式纳米棒阵列上电沉积聚3-己基噻吩(P3HT)薄膜得到P3HT/CdS/TiO2/ZnO核壳式纳米结构薄膜.以该纳米结构薄膜电极为光阳极制备出新型纳米结构杂化太阳电池,研究了该类电池的光电转换性能,初步探讨了该类电池的工作机理.     

ZnO纳米棒阵列在TiO2介孔薄膜上的生长及其表征

通过低温水热法成功地将ZnO纳米棒阵列定向生长在了介孔锐钛矿TiO2纳米晶薄膜上,并主要利用X射线衍射、场发射扫描电子显微镜和光致发光光谱等对其进行了表征。所制备的纳米棒具有六边形的端面,纳米棒的尺寸及端面边长分布范围窄,并且沿c轴方向(002)表现出了明显的择优化生长。此外,相比于玻璃基底或TiO2纳米颗粒薄膜,生长在介孔TiO2薄膜上的ZnO纳米棒阵列表现出了较好的取向生长,表明基底的表面结构和组成对ZnO纳米棒阵列的生长有显著的影响。根据基底有序的多孔结构,讨论了纳米棒阵列可能的生长机理。所得到的ZnO纳米棒阵列在室温下分别表现出了以370 nm为中心的强近紫外光和以530 nm为中心的弱绿光两条荧光谱带。     

TiO2/Au纳米棒阵列的制备及其光催化性能

采用电沉积和旋转涂膜相结合的方法成功制备了高度有序的TiO2/Au纳米棒阵列催化剂.扫描电镜和透射电镜结果表明,TiO2薄膜均匀地包覆在Au纳米棒的表面,形成核壳型的一维阵列结构.X射线衍射分析表明所获得TiO2为(101)晶面优先生长的锐钛矿晶相.紫外-可见漫反射光谱显示,由于Au和TiO2间肖特基结的存在造成吸收红...     

光电化学水氧化用多孔单晶金红石TiO2纳米棒阵列光阳极的设计和构建

光电化学电池(如染料敏化太阳能电池、量子点敏化太阳能电池以及光电化学水分解电池)是实现太阳能转化及存储的有效手段之一.其中,光电极是光电化学电池的核心组成部分,它集光吸收、光生电荷输运及转移等决定光转化效率的关键过程于一身,因此构筑高活性半导体光电极以实现高效太阳能转化利用引起研究者广泛关注.多孔TiO2纳米颗粒堆垛薄膜光阳极因具有大的比表面积,可提供更多的染料(量子点)担载和反应活性位点,在光电化学电池中表现出优异活性而被广泛研究.然而, TiO2纳米颗粒间大量存在的晶界对光生电荷有较强的散射作用,降低了光生电荷的收集效率.英国牛津大学Snaith研究小组利用模板辅助水热过程首次获得了(001)晶面占优的多孔单晶锐钛矿TiO2微米颗粒,这种多孔单晶TiO2微米颗粒在具有大比表面积的同时,其单晶结构还能有效去除晶界对电荷的散射作用,因而具有优异的电荷输运特性.利用这种多孔单晶TiO2微米颗粒组建的光阳极用于染料敏化太阳能电池中,展现出优异的太阳能光电转化性能.受该工作启发,各种形貌的多孔单晶TiO2微米颗粒作为光催化剂和光电化学分解水用光阳极材料被广泛研究,并表现出优异活性.在单晶微米颗粒堆垛成的薄膜光电极中,虽然单个单晶微米颗粒中晶界对电荷的散射作用被有效抑制,但是单晶颗粒间的晶界仍然存在并影响光生电荷的收集效率.为了彻底抑制晶界对光生电荷的散射作用,每个单晶颗粒都应该贯穿整个薄膜,例如一维TiO2纳米棒单晶阵列薄膜.虽然一维单晶阵列薄膜能够有效提高光生电荷的收集效率,但相对于多孔薄膜具有较小的比表面积,限制了担载染料(量子点)和反应位点的数量.为了增大TiO2单晶纳米棒阵列薄膜的比表面积,目前主要的手段包括调控纳米棒长径比、表面修饰TiO2纳米颗粒以及二次生长构建TiO2枝晶阵列.本文首次提出通过制备多孔单晶TiO2纳米棒单晶阵列薄膜来获得高比表面积和高光生电荷收集效率的光阳极,提高光电化学电池的效率.在透明导电薄膜(FTO)表面利用水热生长TiO2纳米棒阵列薄膜之前,预先在FTO基体上沉积一层SiO2球密堆模板, TiO2纳米棒单晶阵列在从FTO表面向上生长过程中,会将SiO2球模板包裹进TiO2纳米棒中,再通过碱溶液将SiO2球模板溶解,首次在FTO基体上原位生长出多孔单晶TiO2纳米棒阵列薄膜.将所得多孔单晶金红石TiO2纳米棒阵列薄膜作为光电化学分解水电池光阳极,其光电化学分解水活性相对于实心单晶金红石TiO2纳米棒阵列提高了2.6倍.多孔单晶金红石TiO2纳米棒阵列光阳极性能的提升可归因于：(1)多孔结构赋予多孔单晶金红石TiO2纳米棒阵列薄膜更大的比表面积,可提供更多的反应活性位点;(2)多孔结构能够有效缩短单晶金红石TiO2纳米棒中光生电荷体相输运距离,提高光生电荷的收集效率;(3)多孔结构通过对光多次反射吸收可有效增强光吸收,产生更多光生电荷参与水分解反应;(4)在制备过程中引入Si掺杂,导致多孔单晶金红石TiO2纳米棒带隙扩大了0.1 eV,带隙增大归因于导带位置负移0.1 eV,光生电子具有更强的还原能力,光电流起始电位相应负移约0.1 V.     

TiO2纳米片/巢状分级结构纳米阵列薄膜的制备及其在染料敏化太阳能电池中的应用

采用水热合成法在氟掺杂二氧化锡(FTO)导电玻璃基底上得到TiO2纳米阵列薄膜,并进一步通过NaOH溶液水热处理制备了由巢状纳米阵列及纳米片覆盖层构成的TiO2纳米阵列分级结构一体化薄膜.采用场发射扫描电镜(FE-SEM),X射线衍射(XRD),紫外-可见(UV-Vis)漫反射光谱和吸收光谱技术对TiO2薄膜的结构和性质进行表征.FE-SEM结果表明:分级结构TiO2薄膜膜厚为1.5μm,薄膜由一层纳米片覆盖层(约0.2μm高)和一层巢状纳米阵列层(约1.3μm高)组成.XRD谱图表明TiO2薄膜为锐钛矿相.UV-Vis光谱显示分级结构TiO2薄膜具有较强的光捕获能力和染料吸附能力.TiO2纳米片/巢状分级结构纳米阵列薄膜作为光阳极,可有效地提高染料敏化太阳能电池的光电转换效率,其短路电流(Jsc)为7.79mA·cm-2,开路电压(Voc)为0.80V,填充因子(FF)为0.40,光电转换效率(η)为2.48%,其光电转换效率较TiO2纳米阵列薄膜提高了近10倍.     

单晶二氧化钛纳米棒阵列的修饰及其在量子点敏化太阳电池中的应用(英文)

使用TiCl4溶液对单晶TiO2纳米棒阵列(TNRs)进行修饰,通过在TiO2纳米棒表面合成TiO2纳米颗粒来提高TNRs的表面积,提高TNRs对量子点的吸附能力,并在此基础上研究了TiCl4修饰时间对基于单晶TNRs的CdS/CdSe量子点敏化太阳电池光伏性能的影响,同时结合强度调制光电流谱(IMPS)研究了TiO2纳米棒阵列的电子传输性能.结果表明:TiCl4修饰可以大幅提高基于单晶TNRs的CdS/CdSe量子点敏化太阳电池的光伏性能,在TiCl4修饰时间为60 h时,其短路电流密度和光电转换效率分别由修饰前的(2.93±0.07)mA·cm-2和0.36%±0.02%提高至(8.19±0.12)mA·cm-2和1.17%±0.07%.同时,IMPS测试表明电子在单晶TiO2纳米棒阵列中的传输速率高于在TiO2纳米颗粒薄膜中的传输速率,证明了单晶TiO2纳米棒阵列在电子传输方面的优越性.     

AAO模板对液相沉积TiO2纳米阵列结构的影响

采用液相沉积法(LPD),在不同的阳极氧化铝(AAO)模板上原位合成高度有序的TiO2纳米阵列.实验结果表明,经过400℃热处理后,制备出的薄膜是锐钛矿相的TiO2纳米阵列,草酸AAO模板中Al2O3的体积分数大于0.71,薄膜由TiO2纳米棒组成,外径约为100 nm左右;而磷酸AAO模板中Al2O3的体积分数小于0.71,液相沉积后获得TiO2纳米管,管外径达200 nm左右,内径约为100 nm左右.     

异形复层结构TiO2纳米棒薄膜的水热合成及性能

本文采用水热反应法,通过改变合成条件,经XRD和FESEM表征,证实合成了四方金红石相异形复层(阵列-团簇)结构的TiO2薄膜。合成薄膜的下层是TiO2的阵列,上层是团簇状的TiO2,并且构成阵列和团簇的每个方柱又由多根纳米棒(25~65 nm)组成。上层团簇的生成量和厚度可以通过改变反应物的初始浓度、反应时间和生长基片的角度进行调控。将这种异形复层结构薄膜试用于染料敏化太阳能电池(DSSC)光阳极,发现其光电转化效率比单层阵列TiO2薄膜提高了2.6倍。由此表明TiO2这种以纳米棒为单元结构的异形复层薄膜,上层团簇结构有利于产生采光作用以及吸附微粒的作用,下层阵列结构有利于载流子的定向快速传输,其复合结构的形成,致使光电转换效果明显提高。     

4.81%光电转换效率的全固态致密PbS量子点薄膜敏化TiO_2纳米棒阵列太阳电池（英文）

利用TiO_2纳米棒阵列和在旋涂辅助连续离子层吸附反应过程中使用乙二硫醇的策略,成功地在TiO_2纳米棒阵列上获得了致密PbS量子点薄膜,组装了新颖结构的全固态致密PbS量子点薄膜敏化TiO_2纳米棒阵列太阳电池。研究了TiO_2纳米棒阵列长度对全固态致密PbS量子点薄膜敏化太阳电池光伏性能的影响,发现TiO_2纳米棒阵列长度为290、540和1040 nm时,相应太阳电池的光电转换效率分别是2.02%、4.81%和1.95%。对于组装全固态量子点敏化太阳电池,综合考虑空穴传输长度和量子点担载量的平衡是获得较高光电转换效率的关键所在。     

Phase equilibria in the solid state in the V9Mo6O40-Cr2O3 system

Phase equilibria have been established in the solid state in the V₉Mo₆O₄₀-Cr₂O₃ system. The results obtained have permitted to state that the system of interest, in the subsolidus area, is not a real two-component system in the whole component concentration range.

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Zusammenfassung Im Festzustand des Systemes V₉Mo₆O₄₀-Cr₂O₃ wurden Phasengleichgewichte ermittelt. Die erhaltenen Resultate lassen darauf schließen, daß das fragliche System im Subsolidus-Gebiet über den gesamten Konzentrationsbereich kein reelles Zweikomponentensystem ist.

     

The deviation of the true heating rate with respect to the programmed one

The paper deals with the influence of the deviation of the true heating rate with respect to the programmed one on the values of non-isothermal kinetic parameters for the solid-gas thermal decompositions of CaC₂O₄.H₂O and [Ni(NH₃)₆]Br₂. An original method, based on integration over small ranges of the variables and making use of local heating rates, was applied in order to determine the non-isothermal kinetic parameter values. The results show significant differences between values of non-isothermal kinetic parameters obtained by using true local heating rates and those obtained by using the programmed heating rate.     

On the reduction of Cr3+ during the thermal decomposition of fluorochromates(III) with nitrogen containing cations

The thermal decomposition of [CO(NH₂)₂H]CrF₆·H₂O, (C₃N₆H₈)CrF₅·H₂O and the solid state reaction of CrF₃ and melamine are investigated under non-reciprocal quasi-static conditions and compared with the thermal behaviour of other fluorochromates(III) ([Cr(NH₃)₆]CrF₆, (NH₄)₃CrF and [C(NH₂)₃]₃CrF₆). The comparison of the results shows that the amount of chromium(II) in the final product is determined by the thermal stability and consequently by the decomposition temperature of the intermediates. Neither bonding properties in the starting materials nor the absolute amount of generated NH₃ influence the composition of the final product.     

High Temperature Reactions in the MoO3-Ag2O System

High-temperature reactions were investigated in the MoO₃-Ag₂O system by means of X-ray, DTA and scanning microscopy methods, and a model was proposed according to which first an Ag₂Mo₄O₁₃ phase was formed at the MoO₃ and Ag₂O (or metallic Ag) interface. Subsequently, at the Ag₂Mo₄O₁₃-Ag₂O contact area a layer of Ag₂Mo₂O₇ appeared. If the amount of silver oxide is sufficiently high, a layer of Ag₂MoO₄ is formed between the Ag₂O and Ag₂Mo₂O₇ phases. This revised version was published online in July 2006 with corrections to the Cover Date.     

Kinetics of the decomposition of calcium carbonate in the presence of Bi2O3

Former studies concerning the formation of the compounds in the pseudobinary systems of Bi₂O₃-MO type (M =Ca, Sr, Ca+Sr) have shown that the reaction which occurs with the highest rate is that between Bi₂O₃ and CaO. In the present work CaCO₃ was used as CaO source. We carried out an investigation of the thermal decomposition of CaCO₃ in the presence of Bi₂O₃ in comparison with the decomposition of pure CaCO₃.The presence of Bi₂O₃ exerts a complex influence on the CaCO₃ decomposition acting on the nucleation as well as on the diffusion of CO₂. The decomposition of the samples with low Bi₂O₃ content follows the mechanism of a contracting sphere. A change from surface nucleation to bulk nucleation is recorded for higher amounts of Bi₂O₃.     

Phase equilibria up to the solidus line in the system Fe2O3−Fe8V10W16O85

Phase equilibria up to the solidus line in the system Fe₂O₃?Fe₈V₁₀W₁₆O₈₅ were determined by means of X-ray phase powder diffraction and differential thermal analysis. This system is one of the intersections of the three-component system Fe₂O₃?V₂O₅?WO₃. The studies revealed that this is not a real binary system, even in the solid state.     

Phase equilibria up to the solidus line in the system Fe2WO6−Fe8V10W16O85

Phase equlibria in the solid state in the system Fe₂WO₆?Fe₈V₁₀W₁₆O₈₅ were studied by means of X-ray phase powder diffraction and differential thermal analysis, This system is one of the intersections of the three-component system Fe₂O₃?V₂O₅?WO₃. The investigation demonstrated that the system is not a real two-component system even below the solidus line.     

Characteristics of the structure and crystallochemical criteria for the existence of compounds of the type AnBnO3n+2

The calculated (models of the ideal layered perovskite-like structures (LPS)) and experimental values of the unit cell parameters of compounds of the A_nB_nO_3n+2 type were analyzed. The interconnection between the peculiarities of the distortion of the LPS in these compounds, the number of layers of BO₆ octahedra in the perovskite-like blocks, and the limits of the morphotropic transitions were established. __________ Translated from Teoreticheskaya i éksperimental’naya Khimiya, Vol. 42, No. 2, pp. 92–95, March–April, 2006.     

Optimization of the Sintering Process by DSC for the Preparation of High-Temperature Superconductors

The optimum calcination and sintering conditions for the preparation of the desired phases with the proper stoichiometry of the bulk high-temperature superconductors YBa₂Cu₃O_7-x (YBCO) and Bi₂Sr₂CaCu₂O_y> (BSCCO) were investigated by differential scanning calorimetry. DSC analysis on the corresponding superconducting coatings, electrophoretically deposited, indicated that the sintering and annealing procedure was suitable for the production of stable, strong and adherent coatings. X-ray diffraction analysis, Raman spectroscopy and magnetic measurements confirmed the improved properties of the superconducting powders and coatings obtained. This revised version was published online in July 2006 with corrections to the Cover Date.     

Electrochromism in Materials Prepared by the Sol-Gel Process

Electrochromism is defined as the persistent but reversible optical change (usually transmission) produced electrochemically. The preparation by the sol-gel process of thin films made of amorphous or crystalline nanoparticles of WO₃, V₂O₅, Nb₂O₅, TiO₂, CeO₂, Fe₂O₃ and mixed compounds such as WO₃−TiO₂, CeO₂−TiO₂, CeO₂−SnO₂, have opened remarkable new opportunities for obtaining electrochromic layers exhibiting large optical transmission variation in the UV, visible or infrared range and acceptable kinetics under H⁺ or Li⁺ insertion. In this paper we give an overview of what has been recently achieved in this field, with emphasis for cathodic electrochromic coatings of Nb₂O₅ and TiO₂ composition. Finally we stress the future developments in this fast growing field.