CeO2—TiO2复合纳米晶多孔膜的光电化学行为

用溶胶凝胶法制备了CeO2－TiO2复合纳米晶多孔膜电极，并用XRD及原子力显微镜（AFM）进行表征．通过光电化学研究，发现了CeO2-TiO2复合纳米晶电极光响应的p型和n型转换现象．结果表明，随着CeO2含量的不同及外电场的变化，CeO2－TiO2复合纳米晶电极可以呈现不同的光响应．     

铜电极在含苯并三唑的硼砂-硼酸缓冲溶液中的光电化学行为研究

用光电化学方法研究了铜电极在含苯并三唑(BTA)的硼砂-硼酸缓冲溶液中的光电化学行为。BTA能使铜电极的光响应由p-型转变为n-型。产生光响应的原因是铜电极表面的Cu2O膜。当BTA存在时由于BTA的作用致使电极表面Cu2O膜中共存着p-型和n-型区域, 电位正移和频率增加导致电极显示n-型光响应。     

铜电极在含苯并三唑的硼砂-硼酸缓冲溶液中的光电化学行为研究

用光电化学方法研究了铜电极在含苯并三唑(BTA)的硼砂—硼酸缓冲溶液中的光电化学行为.BTA能使铜电极的光响应由p-型转变为n-型.产生光响应的原因是铜电极表面的Cu_2O膜, 当BTA存在时由于BTA的作用致使电极表面Cu_2O膜中共存着P-型和n-型区域,电位正移和频率增加导致电极显示n-型光响应.     

纳米结构ZnO/染料/聚吡咯光阳极的光电化学性质

用光电化学方法研究了染料RuL2 (NCS) 2 (L =2 ,2′ bipydine 4,4′ dicarboxylicacid) (简写为Dye)、聚吡咯 (PPy)敏化氧化锌 (ZnO)纳米晶电极以及用RuL2 (NCS) 2 和PPy复合敏化ZnO纳米晶膜电极的光电化学行为 .实验表明 ,ZnO/PPy纳米多孔膜电极为双层n 型半导体结构 .PPy和RuL2(NCS) 2 都可对ZnO纳米晶膜产生敏化作用 ,ZnO/RuL2 (NCS) 2 /PPy复合多孔膜电极产生的光电流远大于ZnO/PPy纳米多孔膜电极和ZnO/Dye多孔膜电极产生的光电流 .讨论了该电极的光生电子的机理 ,初步测定了ZnO/RuL2 (NCS) 2 /PPy电极作为光阳极的光电化学电池的工作特性曲线 ,测得该电池的光电转换效率为 1 .3% ,填充因子为 0 .75 .     

多孔炭载聚钴酞菁修饰电极用于苯二酚的电催化及检测

以二氧化硅纳米球为模板,通过葡萄糖的水热聚合反应制备了具有三维结构的多孔炭(PC)。采用电化学聚合方法将单体钴酞菁聚合在多孔炭修饰的玻碳电极(PC/GC)表面,制备了多孔炭载聚钴酞菁的修饰电极(Co-TAPc/PC/GC)。通过循环伏安法(CV)研究了间苯二酚、邻苯二酚和对苯二酚在此修饰电极的电化学响应。结果表明,相对于裸玻碳电极、多孔炭或聚钴酞菁单独修饰的电极,该修饰电极对3种同分异构体的酚类物质均有更好的电催化活性。利用计时安培技术,该修饰电极对间苯二酚、邻苯二酚及对苯二酚分别在5.0×10-6～5.0×10-4 mol/L,6.0×10-6～2.5×10-4 mol/L和2.0×10-6～8.0×10-4 mol/L范围内具有较好的线性响应。此修饰电极具有制备简单、响应灵敏、稳定性好等优点。     

TiO2修饰的镍基光电极的制备及光电化学性能

通过溶胶 凝胶法，直接在导电的金属镍基上制备多孔TiO2纳米薄膜，利用STM观察电极的表面形貌，所制TiO2粒径约为20～80 nm，随着烧结温度的升高，TiO2纳米薄膜表面孔的数量增多、孔径增大.用循环伏安法分析了电极的光电化学性能，结果表明，电极的光电响应随烧结温度的升高和薄膜厚度的增加而增大.     

二氧化钛纳米晶溶胶内渗透电极对染料敏化太阳能电池的光伏性能的提高

以自制的过氧钛酸(PTA)水溶液为前驱体,用水热法制备了透明锐钛矿相二氧化钛溶胶.无需有机添加剂可得到直径小于7 nm的棒状二氧化钛纳米晶溶胶.通过将溶胶内渗透到染料敏化太阳能电池(DSSCs)的多孔二氧化钛电极后,消除了多孔电极内的大孔并改善了电极内纳米晶之间的连通性.用扫描电子显微镜(SEM)和光学轮廓仪对溶胶内渗透后的光阳极进行了表征.结果表明:小颗粒棒状二氧化钛纳米晶附着在多孔的二氧化钛表面,填充了电极由于烧结产生的大孔,并在多孔的二氧化钛内部形成了有利于电子传输的网络结构.与未经处理的多孔电极相比,改性后的光阳极组装成染料敏化太阳能电池后光电转化效率提高了64%.     

自组装分子印迹单层膜修饰电极对L-丝氨酸的检测

以电沉积多孔金膜为基底,L-丝氨酸为模板分子,L-半胱氨酸为功能单体构建了信号放大的自组装分子印迹单层膜修饰电极.电极对L-丝氨酸浓度响应的线性范围为5.0×10-6～2.0×10-4 mol/L,检出限为4.8×10-7 mol/L,灵敏度为215 mA·L·mol-1.由于多孔金膜有效增加了模板分子的固定量,印迹电极响应性能较无多孔金膜修饰的印迹电极有明显提高.     

n-型多孔Si/TiO2纳米线异质结构的制备及光电化学性能

采用光辅助电化学腐蚀法制备了n-型多孔硅衬底, 再采用水热法在其表面生长TiO₂纳米线制得了三维n-型多孔Si/TiO₂纳米线异质结构. 通过X射线衍射、 扫描电子显微镜和X射线能量散射等表征证实了n-型多孔Si/TiO₂纳米线异质结构的形成. 紫外-可见漫反射光谱测试结果表明, n-型多孔硅与TiO₂纳米线的复合提高了紫外-可见波段的光吸收. 光电性能测试结果表明, 3个样品中n-型多孔Si/TiO₂纳米线异质结作为光电极的光电流最高, 这说明n-型多孔Si/TiO₂纳米线作为光电极具有更高的光电化学分解水性能.     

双染料复合敏化SnO2纳米多孔膜光电极的研究

光电化学;光电转换;双染料复合敏化SnO2纳米多孔膜光电极的研究     

掺镁氧化铁电极光响应n-p型转换的研究

Electrodes were prepared with heating commercial pure iron chips buried in Mgo powder and showe dboth n-and p-type photoresponses.The photoresponses were so weak that in fact they were totally buried inthe noise.Hence asignal averager was used. After 1000 cycles'summation the signal to noise ratio was greatly improved and we obtained a wave form series showing the conversion of n-type, p-type photoresponses for the first time. Fig.1(a): E=0.261V. The absolute peak-to-peak photovoltagevalue (ΔV_(ph)) equals 13.4 mV and shows a typical n-type photoresponse. (b); E=-0.04 V, ΔV_(ph)=1.24 mV, still an -n-type response, but when light is chopped off, the electrode potential reaches its stable value much faster than in (a). (c): When E=-0.076 V, which is only 0.036 V more negative than in (b), in the latter 85% part of illuminating period, electrode potential tends to increase, demonstrating some p-type character. (d): As E=-0.09 V, the magnitude of p-type response almost equals that of n-type. (e): As E=-0.12 V, the main response belongs to p-type, and ΔV_(ph) is only 0.634 mV. This electrode potential is much more positive than the flat band potential of the undoped iron oxide electrode (E_(fb) is about -0.5 V). (f): E=-0.17 V. There is still a small n-type response at the beginning of every illuminating period, and the whole curve appears to be p-type responnse. (g): E=-0.36 V. Typical p-type response appears. ΔV_(ph)=2.05 mV. (h) and (i): E=-0.40 V and -0.45 V. ΔV_(ph) drop to 1.55 mV and 1.05 mV respectively. the above data were reproducible, no retardation of photoresponse was observed when potential was changed.An XPS surface analysis was performed thereafter on the same electrode. A peak of Mg1S at 1305 eV(BE) is apparent. Huge amount of Mg exists on the surface layer. the relative atomic concentration (s compared with Fe) reaches 15-20 AT%. After Ar~+ etching, the amount of Mg decreases. Fig.2 is the result after 9 minutes′ Ar~+ etching. A possible explanation of these experimental facts based on model of energy band of semiconductors was given.     

氧化铁电极的半导体性能和光电化学 Ⅴ.烧结掺锌氧化铁电极的光电响应

Somorjai等曾报道在不同电势下,测得掺MgO氧化铁光电极具有n,p两种类型的光响应^[1]。最近本实验室首次报道了在同一电势下,热形成的掺MgO-Fe₂O₃光电极具有n,p型双重光响应共存现象^[2],由于其在电催化等中可能的应用价值引起了较广泛的兴趣。     

3D porous V_2O_5 architectures for high-rate lithium storage

The discovery of novel electrode materials promises to unleash a number of technological advances in lithium-ion batteries. V_2O_5 is recognized as a high-performance cathode that capitalizes on the rich redox chemistry of vanadium to store lithium. To unlock the full potential of V_2O_5, nanotechnology solution and rational electrode design are used to imbue V_2O_5 with high energy and power density by addressing some of their intrinsic disadvantages in macroscopic crystal form. Here, we demonstrate a facile and environmental-friendly method to prepare nanorods-constructed 3D porous V_2O_5 architectures(3 D-V_2O_5)in large-scale. The 3D porous architecture is found to be responsible for the enhanced charge transfer kinetics and Li-ion diffusion rate of the 3D-V_2O_5 electrode. As the result, the 3D-V_2O_5 surpasses the conventional bulk V_2O_5 by showing enhanced discharge capacity and rate capability(delivering 154 and127 m Ah g~(-1) at 15 and 20 C, respectively).     

Annealing sequence dependent open-circuit voltage of inverted polymer solar cells attributable to interfacial chemical reaction between top electrodes and photoactive layers

The ability to laminate and delaminate top metal contacts during the processing and testing of inverted polymer solar cells has led us to uncover the peculiar dependence of their open-circuit voltage (V(oc)) on the annealing sequence. Specifically, thermally annealing inverted polymer solar cells having bulk-heterojunction photoactive layers after top electrode deposition above 100 °C leads to lower V(oc) compared to analogous devices with unannealed photoactive layers or photoactive layers that have been annealed prior to metal electrode deposition. This reduction in V(oc), however, can be reversed when the top electrodes are replaced. This observation is thus a strong indication that such changes in V(oc) with annealing sequence are manifestations of changes at the top electrode-photoactive layer interface, and not structural changes in the bulk of the photoactive layer. Electronic characterization conducted on the photoactive layers and metal contacts after dissection of the polymer solar cells via delamination suggests the reduction of V(oc) on thermal annealing in the presence of the metal top contacts to stem from an interfacial chemical reaction between the photoactive layers and the metal electrodes. This chemically generated interfacial layer is removed upon electrode delamination, effectively reverting the V(oc) to its original value prior to thermal annealing when the top electrodes are replaced.     

Origin of enhancement in open-circuit voltage by adding ZnO to nanocrystalline SnO2 in dye-sensitized solar cells

SnO2 + ZnO working electrodes for dye-sensitized solar cells were made by mixing a nanocrystalline SnO2 colloidal dispersion with ZnO or Zn(CH3COO)2. Addition of ZnO or Zn(CH3COO)2 enhanced the open-circuit voltage (V(oc)) of the cells with respect to cells containing only SnO2. Dependence of the electron lifetime in the electrodes on short-circuit photocurrent density (J(sc)) gave evidence against the assumption that the suppression of back electron transfer to the electrolyte is the origin for the V(oc) enhancement by addition of Zn. V(oc) dependence on temperatures indicated a decrease in the combined capacitance of the mixed electrode. The slope of the V(oc) dependence versus the logarithm of J(sc) indicated that the contribution of unpinning of the band to the enhancement of V(oc) could be neglected. From the cyclic voltammograms of the electrodes, the combined capacitance of the mixed electrode was 1 order of magnitude smaller than that of SnO2. The decrease in the combined capacitance in the mixed electrode could be explained by the decrease in the chemical capacitance of SnO2, thus the shift of the conduction band position toward the vacuum level. X-ray photoelectron spectra of Sn 3d(5/2) peaks showed a shift toward lower binding energy with an increasing amount of added Zn. This was attributed to an increase in the surface potential toward the negative direction, which might have resulted from a dipole moment formed by Zn on the surface of SnO2.     

冠醚部花青的合成及其光电化学性能

部花青类化合物是一种光敏材料,由于它的结构比较稳定,吸收光谱范围可以调节以及容易做成薄膜电极等优点,用部花青染料做光伏器件的研究引起了人们的注视.Ghosh报道了用青类化合物做成高效率Schottky太阳能电池,光电转换效率达到1%.     

铅电极在硫酸溶液中的光电化学行为

研究了铅电极在阳极氧化过程中光响应的产生机制。结果表明，Ｐｂ电极在光照氧化时存光活化过程，且光经过程须在电位高于０Ｖ时才能发生。采用现场测量光电压技术研究了Ｐｂ电极在硫酸溶液中的恒电流极化过程。     

二氧化钛和三氧化二铁复合纳米晶电极的光电化学性质

研究了以不同方式相互修饰的Fe2 O3和TiO2 纳米晶电极的光电化学行为 (包括离子的相互掺杂 ) .在不同的入射光波长下 ,瞬态光电流谱显示Ti4 掺杂的Fe2 O3电极呈现n型半导体的特性(阳极光电流 ) ;以不同方式经Fe2 O3包覆的TiO2 电极由于能级的不匹配 ,在整个的波长测量范围内没有光响应 ;而对Fe3 离子掺杂的TiO2 电极和经TiO2 修饰 (包覆或偶联 )的Fe2 O3纳米晶电极则呈现出p n共存特性 ,甚至个别的电极表现出纯粹的p型半导体的特性 .这些现象可以从p型微区的形成得到解释 .     

光电催化氧化甲醇电极

直接甲醇燃料电池 (DMFC)可直接利用甲醇 ,无须中间转化装置 ,具有系统结构简单、体积能量密度高、燃料补充方便等优点 .从提高电流密度和稳定催化剂本征活性这两方面来看 ,DMFC需要解决的关键问题是使甲醇直接氧化的阳极材料 .近年来有关此类阳极材料的制备与催化性能的研究报道日益增多 [1,2 ] ,但都是单纯地从光催化或电催化的角度出发 .本文提出一种利用 Ti O2 为光催化剂 ,Pt- Ru为电催化剂 ,试图将光催化与电催化反应发生于一体 ,使甲醇能得到联合的催化氧化作用 ;同时为了能进一步增加Ti O2 的光催化氧化能力 ,改变 Ti O2 - n…     

粘结剂聚四氟乙烯乳液经过乙醇预处理后对气体扩散电极性能的影响

在气体扩散电极的制作工艺中,加入乙醇对粘结剂聚四氟乙烯(PTFE)进行预处理.通过伞自动微孔物理化学吸附仪对气体扩散电极进行BET比表面积、Langmuir比表面积、孔分布等进行测试,并用扫描电子显微镜(SEM)检测观察电极表观形貌.以锌电极作为负极组装成锌空气电池,检测在不同的电流密度下气体扩散电极相对锌电极的电位变化,研究PTFE乳液经过乙醇预处理后对电极性能的影响.结果显示,PTFE乳液经过乙醇处理后,先膨胀后收缩,能够增加催化层和气体扩散层的孔隙结构和比表面积,从而使得电极有效电化学反应场所相应增多,减低电极在大电流密度条件下放电时的极化过电位.