CdSe/TiO2复合薄膜的制备及光电性能研究

以SeO2,CdCl2.5/2H2O,H2SO4为原料,采用三电极体系,分别在ITO玻璃和TiO2纳米管阵列基底上沉积CdSe薄膜。研究了不同沉积电压(-0.6,-0.7,-0.8,-0.9V,均相对于SCE)下制备的复合薄膜的晶体结构和微观形貌,并测试了其光电性能。结果表明:制备出的纳米粒子呈不均匀团聚状态;随沉积电压的增大,光吸收增强,光响应电流增大,在沉积电压为-0.8V时复合薄膜的光响应电流达到最大值,但此沉积电压下的薄膜容易剥落。综合考虑薄膜质量和光响应电流,沉积电压为-0.7V时制备的复合薄膜最佳。     

阴极电沉积法同时制备TiO2薄膜和颗粒

采用阴极电沉积法电解钛酸四丁酯同时制备TiO2膜和颗粒,并讨论沉积条件对产物的影响。pH值是控制产物的主要参数。对比在紫外灯光照下不同产物不同时间下的光催化性能,比较其差异得出,酸性在pH值为1-2(加浓硫酸2-3mL)时的产物效果最好,光催化性能最好。并横向比较了加入硫酸体积相等的条件下,颗粒和薄膜的光催化效率。     

纳米Ag2S/TiO2异质复合薄膜的制备和光电性能

以异丙醇钛(C12H28O4Ti)为主要原料合成氧化钛(TiO2)前驱体溶胶,并结合230℃水热处理得到TiO2溶胶,利用电流体动力学(EHD)技术在掺氟氧化锡导电(FTO)玻璃基片上镀膜,450℃高温煅烧制备具有多级结构锐钛矿TiO2纳米薄膜.以硝酸银(AgNO3)及硫化钠(Na2S)分别为银源和硫源,采用化学浴沉积...     

TiO2-SiO2双组分膜结构与光催化性能的研究

采用溶胶-凝胶法制备了不同Si／Ti比的TiO2-SiO2双组分膜．用紫外光照射亚甲基蓝的分解实验比较薄膜的光催化性能．通过XRD、FTIR、HRTEM、FE—SEM、AFM以及UV—VS—NIR分光光度计等分析手段对薄膜的结构和光学性能进行了表征．结果表明：适量SiO2的引入，显著提高了TiO2薄膜的光催化活性，Si／Ti比为0．2时薄膜的光催化活性为最佳．SiO2引入TiO2薄膜后，生成了Ti—O—Si玻璃相和无定形SiO2，这两种物相聚集在TiO2晶界周围，有效地阻止了TiO2的晶粒长大，提高了锐钛矿相向金红石相的转变温度，使复合薄膜经过500℃热处理后，只有锐钛矿相存在，有利于薄膜的光催化活性的提高．     

Cu2O薄膜的制备与表征

以透明导电玻璃ITO和铜片为工作电极,用0.1mol/L乙酸铜和0.02mol/L乙酸钠的混合溶液作为电解液,通过两电极电化学沉积方法制备了Cu2O薄膜。讨论了pH值和沉积电位对Cu2O薄膜的影响,利用X射线衍射仪(XRD)、场发射扫描电子显微镜(SEM)、X射线光电子能谱(XPS)对薄膜进行表征。结果表明,两电极电化学沉积法制备Cu2O薄膜最佳的pH值为5.7～5.9,沉积电位为1.1～1.3V。此外,分析了沉积电位对Cu2O薄膜形貌的影响。     

自组装单层膜表面的Bi2Ti2O7薄膜制备与表征

以硝酸铋和钛酸四丁酯为原料,以三氯十八烷基硅烷(OTS)为模板,采用自组装单层膜(self-as-sembled monolayers,SAMs)技术,在玻璃基板上成功制备了Bi2Ti2O7晶态薄膜。借助X射线衍射(XRD)、场发射扫描电子显微镜(FE-SEM)、X射线能谱(EDS)及原子力显微镜(AFM)等测试手段对Bi2Ti2O7薄膜进行了表征。结果表明,以OTS为模板利用自组装技术,经540℃煅烧2h可成功制得立方相Bi2Ti2O7晶态薄膜,且薄膜表面平整光滑,均匀致密。     

TiO2/CuInS2复合纳米棒阵列的制备及其光电性能

采用两步溶剂热法在氧化氟锡(FTO)导电玻璃基底上制备了CuInS2敏化TiO2纳米棒阵列复合薄膜光阳极.利用X射线衍射仪(XRD)和扫描电子显微镜(SEM)表征了复合阵列薄膜的晶体结构和表面形貌,同时采用紫外可见吸收分光光度计(UV-Vis)及光电流电压(I-V)曲线研究了CuInS2敏化TiO2纳米阵列薄膜的光学及光电化学性质.研究结果表明,TiO2纳米棒阵列薄膜被CuInS2敏化后在可见光区的吸收有明显的增强.在模拟太阳光照射下(100 mW/cm2),利用这种复合薄膜作为光阳极组装的量子点敏化太阳能电池的开路电压为0.29 V,短路电流密度为0.15 mA/cm2,具有一定的光电转换能力.     

ITO/TiO2-xNx/NiO复合电极制备及其光电化学性能

以三乙胺为氮源,钛酸丁酯为钛源,采用溶胶-凝胶法制备氮掺杂TiO2,并用旋涂法制备ITO导电玻璃为基材的氮掺杂TiO2薄膜,经300℃、400℃、500℃处理制得ITO/TiO2-xNx薄膜。采用XRD、XPS、SEM和UV-Vis吸收光谱等对样品进行表征,并进行光电化学性能测定,结果表明500℃处理制得的ITO/TiO2-xNx薄膜具有最佳的光电催化性能。进一步采用化学沉积法在ITO/TiO2-xNx薄膜表面上沉积多孔NiO薄膜,制得ITO/TiO2-xNx/NiO复合薄膜,研究表明该复合薄膜具有很好的光电致色特性及储放电性能,可应用于光电致变色和光电能量储存领域。     

电沉积液初始pH值对电沉积制备钽基RuO2·nH2O薄膜的影响

以RuCl3·2H2O水溶液为电沉积液,通过恒流电沉积法在钽箔上电沉积一层RuO2·nH2O薄膜;研究了电沉积液初始pH值对制备RuO2·nH2O薄膜的影响.分别采用SEM、EDS、XRD、粒度分析仪(DELSA 440SX analyzer control)对薄膜的形貌、薄膜元素、溶胶的Zeta电位及薄膜的物相进行观察与测试.结果表明,电沉积液初始pH值越高,RuO2·nH2O薄膜越疏松,龟裂纹越大,与基体结合力也越差.初始pH值为2.3时,薄膜的孔隙率最佳,综合性能指标最好.     

染料敏化太阳能电池中CuO/TiO2薄膜制备及应用

采用普通直流电沉积和超声直流电沉积制备Cu∕TiO2纳米管阵列∕Ti基复合薄膜,而后在NaOH溶液中用电氧化的方法将Cu单质氧化成CuO,制备了CuO∕TiO2纳米管阵列∕Ti基复合薄膜。利用扫描电子显微镜(SEM)和X射线衍射仪(XRD)对两种复合薄膜电极的形貌和结构进行了表征,详细考察了电镀工艺参数(电流密度)和超声波对复合薄膜形貌的影响。同时通过稳态光电响应技术对复合薄膜电极组成的染料敏华太阳能电池(DSSC)的光电性能进行了研究,结果表明:通过普通直流电沉积在工艺参数(3mA/cm2、5min)处制备的复合薄膜组装的DSSC具有该体系下的最佳光电性能(Jsc=9.00mA/cm2、Voc=0.664V、FF=0.512、η=3.06%);在同等条件下通过超声辅助直流电沉积制备的复合薄膜组装的DSSC的最佳光电性能(Jsc=15.50mA/cm2、Voc=0.688V、FF=0.505、η=5.39%)出现在工艺参数为(6mA/cm2、5min)处。对比可知超声条件下的光电性能较好,且最佳光电性能工艺参数发生了后移。     

VLE data for CO2-CF2Cl2, N2-CO2, N2-CF2Cl2 and N2-CO2-CF2Cl

Knowledge about vapour-liquid (VLE) is required as a basis of reliable calculations for separation processes. Correlations available for the prediction of T, p, x, y data are less accurate for mixtures at high pressures and mixtures containing supercritical components. The results of VLE experiments are reported and compared with data calculated with equations of state.     

Thermal diffusion in binary mixtures H2-CCl2F2 and H2-CHClF2

Thermal diffusion coefficients were measured in two gaseous mixtures, in which one component was close to the critical temperature, in the pressure range (19.6–127.4)·10⁴ N/m² and at a freon concentration of 0.25–0.8.     

Preparation of ZrO2-CeO2 and HfO2-CeO2 nanopowders

We prepared weakly agglomerated powders of ZrO₂-CeO₂ and HfO₂-CeO₂ solid solutions 5–8 nm in particle size, consisting of monoclinic and tetragonal phases. After heat treatment at 1200°C, the crystallite size was 30 and 14 nm, respectively. We also examined the effect of precipitate freeze drying on the crystallization of hafnia-based solid solutions containing up to 20 mol % CeO₂.     

Comparison of the Electronic Structures of La2CuO4, Sr2CuO2Cl2, and Sr2CuO2F2

First-principles cluster calculations are reported of the local electronic structure of the three compounds: La₂CuO₄, Sr₂CuO₂Cl₂, and Sr₂CuO₂F₂. The copper ${\text{3d}}_{x^2 - y^2 } $ and the planar oxygen 2p _σ atomic orbitals exhibit a similar degree of covalency. The out-of-plane orbitals, however, are quite different with the ${\text{3}}d_{3z^2 - r^2 } $ atomic orbital lowered significantly in energy for chlorine and fluorine apical positions.     

Radial GRIN glasses in Li2O-Na2O-Al2O3-TiO2-SiO2 systems

A series of GRIN glass rods have been developed in Li2O-Na2O-Al2O3-TiO2-SiO2 systems. Negative radial refractive index profiles were generated by exchanging Na+ for Li+ ions in these glass rods. It has been observed that TiO2 plays a vital role in increase in the profile depth and maximum change in the refractive index because of its ambivalent nature. Change in the refractive index can be further increased by increasing the concentration of exchanging cation in the base glass.     

Elastic and Electronic Properties of Superconducting CaPd 2 As 2 and SrPd 2 As 2 vs. Non-superconducting BaPd 2 As 2

The first-principles calculations were performed to predict the elastic and electronic properties of the superconducting ThCr₂Si₂-type phases CaPd₂As₂ and SrPd₂As₂ in comparison with the non-superconducting CeMg₂Si₂-type phase BaPd₂As₂. Besides, the same properties were compared for CeMg₂Si₂- and ThCr₂Si₂-type polymorphs of BaPd₂As₂. We found that all these phases are mechanically stable and belong to soft materials with low hardness. The near-Fermi region is formed by the valence states of the blocks [Pd₂As₂] with decisive contributions of Pd 4d states. The values of N(E _F) increase in the sequence: CaPd₂As₂ < SrPd₂As₂ < BaPd₂As₂, i.e. in the reverse sequence relative to the transition temperatures T _C. Thus, the change in T _C cannot be explained by the electronic factor, i.e. by the simple correlation T _C～N(E _F). Most likely the decrease in T _C in the sequence CaPd₂As₂ → SrPd₂As₂ and the absence of a superconducting transition in BaPd₂As₂ are related to the structural factors and the peculiarities of the electron–phonon coupling mechanism.     

Si_2N_2O-Al_2O_3-La_2O_3和Si_2N_2O-Al_2O_3-CaO系统的亚固相关系

本文给出了 Si_2N_2O-Al_2O_3-La_2O_3和 Si_2N_2O-Al_2O_3-CaO 系统的亚固相图。实验结果表明:在 Si_2N_2O-Al_2O_3-CaO 系统中有一个未知结构的新化合物 CaO·Si_2N_2O,在3CaO·Si_2N_2O 和3CaO·Al_2O_3两化合物之间形成连续立方固溶体。而 Si_2N_2O-Al_2O_3-La_2O_3系统中则没有发现新化合物。在两个系统的富 Si_2N_2O区,过量的 Si_2N_2O 与 La_2O_3和 CaO 分别反应形成 Si_3N_4与 La_(10)[SiO_4]_(?)N_2(H-相)(和 CaSiO_3。所研究的这两个三元系统中,分别形成了如下几个四元相容性区。在 Si_2N_2O-Al_2O_3-La_2O_3系统内有:H-Si_3N_4-La_2O_3·Si_2N_2O-La_2O_3·Al_2O_3;H-Si_3N_4-La_2O_3·Al_2O_3-La_2O_3·11 Al_2O_3;H-Si_3N_4-La_2O_3·11 Al_2O_3-Al_2O_3;H-Si_3N_4-Al_2O_3-O′s.s;H-Si_3N_4-O′s.s-Si_2N_2O在 Si_2N_2O-Al_2O_3-CaO 系统内有:Si_3N_4-CaSiO_3-CaO·Si_2N_2O-3CaO·Al_2O_3;Si_3N_3-CaSiO_3-3CaO·Al_2O_3-2CaO·Al_2O_3·SiO_(?);Si_(?)N_(?)-CaSiO_3-2CaO·Al_2O_3·SiO_2-Al_2O_3;Si_3N_4-CaSiO_3-Al_2O_(?)-O′s.s;Si_3N_4-CaSiO_3-O′s.s-Si_(?)N_(?)O