偏压控制Cu2O和Cu在TiO2表面的生长及其光电化学性质

基于TiO2/Ti电极在含Cu2+溶液中的循环伏安图,调节电沉积的沉积电压,我们在TiO2平整表面制备出Cu2O和/或Cu颗粒.通过扫描电镜(SEM)、X射线衍射(XRD)和X射线光电子能谱(XPS)表征,发现Cu2O和Cu有不同的生长机制:Cu2O颗粒在TiO2表面分散结晶,而Cu颗粒是在已生长的颗粒上成核,从而形成堆积颗粒结构.这是由于在Cu2O/TiO2界面和Cu/TiO2界面形成不同的能带结构,使得电子的转移方式不同.与纯TiO2光阳极比较,可以观察到Cu2O/TiO2和Cu/TiO2异质结构的光电流均有显著增强.特别地,存在一个电压区间使得Cu2O和Cu同时生长在TiO2表面,此时对应的光电流比较稳定并且能达到最大.紫外-可见(UV-Vis)漫反射光谱、电化学阻抗谱(EIS)和光电流-电压特性曲线均显示,Cu2O和Cu明显有助于光的可见光吸收,同时Cu/TiO2在光电转换过程中显示更宽波段的可见光利用率.此外,开路电压的增加、有效的电荷分离和电极/电解质界面上载流子的快速迁移也增强了材料的光电化学性质.     

Au/PATP/PANI膜电极和Au/PATP/PANI/TiO2膜电极的光电化学

聚苯胺（PANI）是一种结构、 性质不同于聚乙炔和聚吡咯的新型导电高聚物,有着十分广泛的应用[1,2].近年来利用光电化学研究聚苯胺的电子结构、 掺杂情况引起人们的重视[3～5].在酸性溶液中电聚合制备聚苯胺的循环伏安曲线上出现两对氧化还原峰,其峰值电位分别为E11/2=0.13 V和E21/2=0.7 V(对饱和甘汞电极).通过改变电极电位,可获得部分氧化态、还原态、氧化态等3种状态的聚苯胺.部分氧化态具有金属导电性,还原态和氧化态均为绝缘体.本文测量3种状态聚苯胺膜电极的光电响应,首次得到其光电流谱,发现聚苯胺一些新的光电化学实验结果.提出了覆盖绝缘体的金属内发射的光电化学模型.同时,在聚苯胺膜上电沉积纳米TiO2微粒膜,得到广谱区的复合光电材料.     

叶绿素敏化二氧化钛纳米管电极光电性能及其增强机理

为了研究叶绿素的敏化机理,本文以菠菜叶片叶绿素的乙醇浸提液敏化纳米管TiO_2电极,在Na2SO4水溶液电解液中测定其光电性能。敏化电极的光电流响应曲线显示,叶绿素浸提液敏化纳米管TiO_2电极时会显著改变电极的光电流值,而敏化Ti电极时则产生光电流极小。电极的循环伏安曲线则表明,叶绿素浸提液使电极上的氧化反应更容易发生。测定不同浓度的叶绿素浸提液敏化纳米管TiO_2电极的单色光光电转化效率(IPCE)图谱,结果表明,合适的叶绿素浓度(7.123~71.23μg/L)使电极IPCE平均增加2倍以上,但浓度增大至7123μg/L时,其敏化电极IPCE则明显降低;同时发现叶绿素的敏化作用未明显改变TiO_2电极IPCE图谱的特征谱峰位置。根据实验数据和结果,得出在水溶液中叶绿素改变纳米管TiO_2光电性能的机理,主要是通过叶绿素分子与TiO_2电极中的光生空穴发生反应,进而减少光生电子与空穴的复合,使电极有效光生电子数量增加,光电流密度增大,最终提高TiO_2电极的IPCE。     

Ru(bpy)2(NCS)2染料敏化CdS/Zn2+TiO2复合半导体纳米多孔膜的光电化学

采用水热法合成了Zn²⁺离子掺杂的TiO₂纳米粒子[Zn²⁺掺杂量0.5%(物质的量的比)],并用光电化学方法研究了经Ru(bpy)₂(NCS)₂(bpy=2,2′bipyridine₄,4′dicarboxylicacid)分别敏化的掺杂Zn²⁺的TiO₂电极(简写为Zn²⁺-TiO₂)和CdS/Zn²⁺-TiO₂复合半导体纳米多孔膜电极的光电化学行为.实验证明Ru(bpy)₂(NCS)₂敏化CdS/Zn²⁺-TiO₂复合半导体纳米多孔膜电极比单独敏化Zn²⁺-TiO₂电极的光电转换效率高,且敏化Zn²⁺TiO₂电极和敏化CdS/Zn²⁺TiO₂复合半导体纳米多孔膜电极比Zn²⁺-TiO₂电极的光电流产生的起始波长都向长波方向移动.在360600nm范围内,Ru(bpy)₂(NCS)₂敏化CdS/Zn²⁺-TiO₂复合半导体纳米多孔膜电极光电转换效率最好.     

Metal powder addition effect on the photocatalytic reactions and the photo-generated electric charge collected at an inert electrode in aqueous TiO2 suspensions

The photocatalytic reaction in an aqueous TiO₂ suspension has been found to be enhanced by the additiona of some metal powders such as copper, silver, nickel and cobalt into the suspension. Just mixing a metal powder into the suspension gave nearly the same efficiency as metal-loading on the semiconductor particles. The effect is attributed to the rapid transfer of the photogenerated electrons from the TiO₂ to the metal particles, resulting in the effective separation of the electrons and holes.

The photo-current measurements were performed using inert collecting electrodes in the suspensions of TiO₂, where formate was added as a hole scavenger, with and without a metal powder. Higher anodic photocurrent was obtained in the presence of a metal than in its absence, indicating that the metal-mediated electron transfer reaction occurs more effectively from the electron-rich TiO₂ particles to the collecting electrode than the direct discharge of the electron-rich TiO₂ on the collecting electrode.     

CdS/CdSe/TiO2多级空心微球光阳极中量子点覆盖度的提高

TiO₂多级空心微球(THHSs)具有高的比表面积、强的光散射效应以及良好的电子传输性质,以此作为光阳极材料,可以显著提升CdS/CdSe敏化太阳能电池(QDSSCs)的性能。但基于化学浴沉积方法获得的这一类电池中量子点在光阳极表面的覆盖度通常不高(50%左右),本文发展了一种基于表面选择性吸附原理的多步沉积方法,选取特定分子(正十二硫醇)限制已有量子点的生长,通过二次沉积成功提高了CdS/CdSe在TiO₂多级空壳微球表面的覆盖度。使用此方法最终得到高达85.4%的覆盖度。结果表明,量子点覆盖度的增加有效提高了电池对太阳光的利用率,使得光电流获得了明显的增加。同时,二氧化钛空白表面积的减小还可以抑制电子和空穴的复合。优化后的电池光电流密度为15.69 mA·cm^-2,填充因子为0.583,电压为0.605 V,最高光电转换效率为5.30%。     

The role of n–p junction electrodes in minimizing the charge recombination and enhancement of photocurrent and photovoltage in dye sensitized solar cells

The composite electrode comprising n-type TiO₂ and p-type NiO oxides when sensitized with Ru-dye showed short-circuit photocurrent (I_sc) of 17 mA/cm² and open-circuit photovoltage (V_oc) of 730 mV compared to I_sc of 12 mA/cm² and 700 mV for TiO₂ electrodes. Formation of a n–p junction between TiO₂ and NiO oxide layers contributes to the enhanced photocurrent, photovoltage, fill factor and efficiency. In addition to the junction effect, NiO acts as a barrier for charge recombination leading to higher cell performance. The efficiency of the NiO coated TiO₂ solar cell is 30% more than that of bare TiO₂. The negative shift of the flat-band potential of the NiO coated TiO₂ electrode compared to TiO₂ also could be one of the reasons for higher photovoltage observed for TiO₂/NiO electrode. The highest cell efficiencies were obtained immersing TiO₂ thin films in Ni²⁺ solution and converting them to NiO by firing and the optimum NiO coating thickness was found to be only a few angstroms. The energy levels of the excited dye and the band positions of TiO₂ and NiO suggest that the electron transfer from the excited dye to the underlying n-type oxide layer occurs by tunneling through the p-type NiO layer.     

对电极性能对染料敏化太阳电池动力学过程的影响

借助电化学阻抗谱(EIS)和强度调制光电流谱(IMPS)/强度调制光电压谱(IMVS)技术, 采用不同纳米TiO₂多孔薄膜对电极研究了染料敏化太阳电池(DSC)内部2个主要电荷输运过程的内在联系, 并探讨了载Pt材料对DSC界面动力学过程及电池宏观性能的影响机理. 借助等效电路模型分析了基于不同对电极材料电池的填充因子变化原因. 结果表明, 对电极材料的电极电荷交换过程制约光阳极膜内电子传输, 进而影响电池光伏性能; 同时对电极催化反应速率主要与催化剂活性、 载Pt材料电导率和催化反应面积有关.     

基于MWCNT/TiO2对电极和硫醇盐/二硫化物非碘氧化还原电对的染料敏化太阳能电池性能

采用水热法合成出多壁纳米碳管/二氧化钛(MWCNT/TiO₂)复合物, 并作为染料敏化太阳能电池(DSSC)中对电极材料并组装成电池. 通过场发射扫描电子显微镜(FE-SEM)、傅里叶变换红外(FTIR)光谱、X射线粉末衍射(XRD)、同步热重-差示扫描量热(TGA-DSC)、拉曼(Raman)光谱和光电子能谱(XPS)等方法对其形貌、组成和结构进行表征. 结果表明, 酸化MWCNT表面―COOH与水热生长出的锐钛矿TiO₂表面―OH之间, 通过形成类似于O＝C―O―Ti 或者C―O―Ti 的结构, 能有效地增强复合物薄膜层与导电玻璃基底之间的相互作用. 通过循环伏安(CV)、电化学阻抗谱(EIS)、塔菲尔曲线(Tafel)和电池的伏安特性曲线等方法研究了该类对电极对硫醇盐/二硫化物(T-/T₂)非碘氧化还原电对的光电化学特性. 结果表明: 当MWCNT与TiO₂质量比为3:1时, 基于该复合物对电极与T-/T₂非碘氧化还原电对所组装DSSC的开路电压为0.63 V, 短路电流为15.81 mA·cm^-2, 填充因子为0.65, 光电转换效率达到6.47%.     

钛片热氧化法制备光敏电极的研究

本文研究了以钛片为基底的TiO₂多晶薄膜电极的制备条件。发现在钛片热氧化和TiO₂膜的还原时,在气流中添加少量的水蒸气可解决TiO₂膜与基底结合不良的问题。制备了不同膜厚的光敏电极,研究了膜厚和光电流的关系。用热导法观察了氢气气氛下还原TiO₂的现象,研究了半导体化温度对光电流的影响。用制得的电极在日光下分解水制氢,能量转换效率为1.2%。     

Preparation and photoelectrochemical characterization of nano-particulate TiO2 and polyaniline composite films on Au

TiO₂ and polyaniline(PANI) composite film was obtained by electrochemical methods^[1] and investigated for solar energy conversion application. A strong rectifying effect was found in the cyclic voltammogram of the film in dark when the scan speed was slow enough (5 mV/s) and a quasi-reversible voltammogram of the film was observed when the scan speed was fast (100 mV/s). The results of both the cyclic voltammograms and the SEM images of the composite film show that the PANI film is almost completely covered with nano-particulate TiO₂. Two anodic photocurrent bands and a cathodic band was observed in the spectra of the photocurrent of the TiO₂/PANI/PATP(p-aminothiophenol)/Au film in 0.05 mol/L Fe(CN)₆^3-/Fe(CN)₆^4- solution. The band at 300~400 nm (3.1~4.1 eV) can be ascribed to the photocurrent band of TiO₂ particles and the bands at 450~730 nm (1.7~2.8 eV) can be ascribed to those of the PANI. The partially-oxidized PANI has internal photoemission function and the insulating matrix of PANI is verified to be reduced PANI with a 3.33 eV bandgap energy. The flat-band potentials of partially-oxidized PANI and TiO₂/PANI composite film in 1.0 mol/LHClO₄ solution are determined as 0.87 V and 0.09(SHE) from Mott-Schottky plots, respectively.     

Post-modification using aluminum isopropoxide after dye-sensitization for improved performance and stability of quasi-solid-state solar cells

In this study, dye-sensitized TiO₂ electrodes were immersed into a solution of aluminum isopropoxide and after hydrolysis quasi-solid-state solar cells were fabricated. The interaction between the dye and the resulting Al₂O₃ overlayer was investigated by ultraviolet–visible (UV–vis) spectrum, Fourier transform infrared (FTIR) spectrum and X-ray photoelectron spectrum (XPS). The current density–voltage (I–V) characteristics showed that the overlayer increased the photovoltage and decreased the photocurrent under low intensity irradiation, and increased both the photovoltage and photocurrent under AM 1.5 irradiation. The Al₂O₃ overlayer at the dye/electrolyte interface resulted in a 28% improvement in overall photo-to-electrical conversion efficiency from 2.60 to 3.32%. Dark current measurements showed that Al₂O₃ acted as an insulator barrier to retard recombination between the TiO₂ and dye/quasi-solid-state electrolyte interface. Without encapsulation, dye-sensitized solar cells with Al₂O₃ coating after sensitization also exhibited improved stability compared to cells without coating.     

Synthesis of nano-TiO2 assisted by diethylene glycol for use in high efficiency dye-sensitized solar cells

The performance of dye-sensitized solar cells(DSSCs) consisting of anatase TiO_2 nanoparticles that were synthesized via a hydrothermal method was studied.The synthesized TiO_2 nanoparticles were characterized by X-ray diffraction(XRD),nitrogen sorption analysis,scanning electron microscopy(SEM),high resolution transmission electron microscopy(HRTEM),and UV-vis spectroscopy.Then the J-Vcurve,electrochemical impedance spectroscopy(EIS),and open-circuit voltage decay(OCVD) measurement were applied to evaluate the photovoltaic performance of DSSCs.Compared with the commercial TiO_2nanoparticles(P25),the synthesized-TiO_2 nanoparticles showed better performance.By adding diethylene glycol(DEG) before the hydrothermal process,the synthesized TiO_2 nanoparticles(hereafter referred to as TiO_2-DEG particles) shows narrower size distribution,larger specific surface area,higher crystallinity,and less surface defects than TiO_2(DEG free) particles.The analysis of photovoltaic properties of DSSCs based on TiO_2-DEG particles showed that the recombination of electron-hole pairs was decreased and the trapping of carries in grain boundaries restrained.It was believed that the photoelectrode fabricated with the as-prepared TiO_2 nanoparticles improved the loading amount of dye sensitizers(N719).and enhanced the photocurrent of the DSSCs.As a result,the TiO_2-DEG particle based cells achieved a photo-to-electricity conversion efficiency(η) of 7.90%,which is higher than 7.53%for the cell based on TiO2(DEG free) and 6.59%for the one fabricated with P25.     

基于催化发卡自组装和 Ru(NH3)63+ 的核酸光电化学灵敏分析

基于催化发卡自组装反应（CHA）和电活性材料[Ru(NH₃)₆]Cl₃,发展了一种“信号增强”型光电化学生物传感器,实现了核酸的灵敏检测. 首先,采用逐层离子吸附法（SILAR）将CdS 固定于TiO₂/ITO 电极表面. 光电材料CdS 不仅能够将TiO₂ 的吸收范围从紫外光区拓展到可见光区,而且还能提高光电转换效率. 之后,通过Cd-S 键将捕获DNA（C-DNA）固定于CdS/ TiO₂/ITO 电极表面. 与此同时,将Au 结合的发卡DNA 探针1（Au-HP1）,发卡DNA 探针2（HP2）和目标DNA（T-DNA）混合物于溶液中进行CHA 反应,得到大量的Au-HP1:HP2 复合物. 再通过Au-HP1:HP2 复合物与C-DNA 的杂交反应将大量的双链DNA 引入到电极表面. 最后,将电活性物质Ru(NH₃)₆³⁺嵌入DNA 的磷酸骨架中,从而使得光电流大幅度的增强. 该光电生物传感器检测核酸的线性范围为10 fmol·L^-1 到 1500 fmol·L^-1,检测线为6.19 fmol·L^-1,在生物分析、新药筛选以及疾病的早期诊断等方面具有潜在的应用前景.     

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.     

TiO2多孔薄膜电极的制备、微结构及光电化学性能研究

近年来,半导体纳晶多孔薄膜作为一类重要的纳米结构材料,其光电化学性质及功能特性的研究受到人们广泛关注。由于量子尺寸效应及介电限域效应,它们的光物理、光电化学性质以及电荷传输机理明显异于多晶及单晶体材料。通过简便快捷的涂敷、浸涂或溅射等方法,半导体纳晶多孔薄膜可以在导电衬底上形成。这些薄膜具有高度多孔性、大比表面,易于用有机功能分子或半导体超微粒进行表面修饰^[1-2],在太阳能转换^[2]、光电子器件或电子变色器件^[3]及光催化治理环境污染^[4]等方面具有潜在的应用前景。因此,在光电化学、半导体物理及材料科学领域里研究十分活跃。本文采用涂敷及浸涂提拉方法制备了四种具有不同多孔率及比表面的TiO₂薄膜电极,并对其晶型、表面形貌微结构及光电化学性能进行了研究。     

柔性不锈钢基底上一维TiO_2纳米线薄膜的制备及表征

采用直流磁控溅射的方法在柔性不锈钢基底(50μm)上沉积纯钛薄膜,后在NaOH碱溶液中经水热法制备了非钛基大长径比的一维TiO2纳米线薄膜,并通过场发射扫描电子显微镜(FESEM)、X射线衍射(XRD)、透射电子显微镜(TEM)以及光电化学的方法对不锈钢基一维TiO2纳米线薄膜进行了表征.结果表明,纯钛薄膜的致密度、结晶性能以及与基底的结合强度均随衬底温度的升高而加强;在10mol·L-1NaOH浓度下,生长一维TiO2纳米线结构的适宜温度为130-150℃;TiO2纳米线长度达到几个微米,直径在10-30nm之间,并且相互交叉生长,构成一个三维网络结构.此外,在Na2SO4溶液中对TiO2纳米线薄膜进行了线性扫描和瞬态光电流测试,结果表明,一维TiO2纳米线薄膜电极较TiO2纳米颗粒电极表现出更优异的光电化学性能.这种磁控溅射与水热反应相结合的方法,为非钛异质基底上制备一维TiO2纳米线薄膜提供了新的思路.     

Hierarchical TiO2 Flower-spheres with Large Surface Area and High Scattering Ability: an Excellent Candidate for High Efficiency Dye Sensitized Solar Cells

Hierarchical TiO₂ flower-spheres assembled from porous nanosheets-stacked of nanoparticles were synthesized by a simple hydrothermal method with one-step. The as-prepared TiO₂ flower-spheres showed a diameter range from 200 nm to 550 nm and a large surface area of 188 m²/g. A double layer photoanode made of P25 nanoparticles and as-prepared TiO₂ flower-spheres was fabricated for the dye sensitized solar cells(DSSCs). The efficient light scattering and dye absorption of the photoanode can be attributed to the top-layer of hierarchical TiO₂ flower-spheres. DSSCs based on the double layers photoanode exhibit a higher energy conversion efficiency of 8.11% with a short-circuit photocurrent density of 17.87 mA/cm², indicating that there is an increase of 38% in the conversion efficiency compared to those based on electrode P25(5.91%, 14.09 mA/cm²).     

RGO-TiO2纳米管阵列的制备及其光电性能

采用阳极氧化的方法,通过调节阴、阳两电极间距制备不同壁厚的TiO₂纳米管阵列. 采用脉冲电还原沉积的方法将RGO负载于TiO₂纳米管阵列表面合成了RGO-TiO₂纳米管阵列. 相较于负载在薄壁TiO₂纳米管阵列上的RGO,负载于厚壁TiO₂纳米管阵列上的RGO得以充分还原,覆盖率大幅度提高,并显示出良好的光吸收性质和较低的电荷传输电阻,光电流大幅度增加.     

PHOTOCONDUCTIVITY AND PHOTOVOLTAIC EFFECTS IN LANGMUIR-BLODGETT FILMS OF CHLOROPHYLL-a

The DC photoconductivity and photovoltaic effect in Langmuir films of Chlorophyll- a (Chi a ) of precisely controlled thickness formed between Al and Au electrodes have been extensively investigated. The dark conductivity and dark voltage are almost abolished in a N₂ atmosphere. The action spectrum of the photocurrent closely resembles the monolayer absorption spectrum of Chl indicating that the primary event in photoconduction is the generation of singlet excited states. Thicknessdependence studies on the photoconductivity indicate that carrier generation is a surface process and that the mean diffusion length of the excited state is approximately 20 nm. In short (˜1 s) light exposures the photocurrent always increases linearly with both the applied voltage and the light intensity. In continuous light the current-voltage characteristics are highly non-linear and the photocurrent shows a square-root intensity dependence at high intensities and small applied potentials. These results are interpreted in terms of second-order recombination and charge-trapping processes at high carrier densities. The photovoltage usually shows a logarithmic intensity dependence at high intensities and its maximum value in thick films is 800 mV with the Al electrode acquiring a negative polarity. This behaviour, together with some observations on the asymmetry of photocurrent-voltage characteristics and the effect of substituting an aqueous top electrode for Au, further suggest that the photoactive surface is a p-n junction between the Chl and Al₂O₃ layers.