Electrochemical Studies and Selective Detection of Thioridazine Using a Carbon Paste Electrode Modified with ZnS Nanoparticles and Simultaneous Determination of Thioridazine and Olanzapine

A novel ZnS nanoparticle‐modified carbon paste electrode (ZnSNP‐MCPE) was fabricated and used to study the electrooxidation of thioridazine (TR) using cyclic voltammetry (CV) and differential pulse voltammetry (DPV). The determination conditions, such as accumulation time, pH of solution, and modifier amount were optimized. The mechanism of the electrooxidation process on the surface of the modified electrode was studied electrochemically. A linear range of 0.1–36.0 µM with detection limit of 65.0 nM was obtained for TR. In a mixture containing TR and olanzapine (OLZ), the DPV peaks of two compounds can be well separate from each other with a potential difference of 425 mV. Finally, this method was successfully applied to determinate the TR content in real samples.     

一维ZnE(E=S,Se)网状微米晶须的化学气相合成及生长机理研究

以Zn粉为原料,在CuE(E=S, Se)微米球的辅助下,采用化学气相沉积(CVD)法在Si衬底上成功制备出微米级ZnE(E=S, Se)网状晶须.用XRD,EDS,SEM和PL谱分别对产物的结构、成分、形貌和结晶质量进行了测试和分析.结果表明:生长的ZnS和ZnSe微米晶须均为立方闪锌矿结构,长度达300 μm以上,具有接近理想化学计量比的成分和较高的结晶质量.ZnE微米晶须的生长符合氧化还原反应下的气-液-固生长机制,Cu3Zn合金充当了实际的微米晶须生长催化剂,在晶须生长过程中Cu3Zn合金汇聚在一起使ZnE微米晶须形成交叉网状结构.     

水热法制备ZnS∶Cu,Al纳米X射线发光粉及其光谱特性

采用水热法低温(200 ℃)处理12 h直接制备ZnS∶Cu, Al纳米晶, 并探讨其光致(PL)和X射线激发(XEL)光谱特性及后续退火处理的影响. XRD和TEM分析表明, 水热法直接制备的ZnS∶Cu, Al粒径约为15 nm, 尺寸分布窄, 分散性好, 具有纯立方相的球形结构. 其PL和XEL光谱均为宽带谱, n(Cu)/n(Zn)=3×10^-4和n(Cu)/n(Al)= 0.5时PL和XEL光谱强度最大, XEL峰值在470 nm处. 在此条件下, 水热处理3 h直接合成的纳米晶在氩气保护下于800 ℃退火1 h后样品的XEL发光进一步增强. XEL光谱强度约是退火前样品的8倍, 此时峰值波长在520 nm, 团聚形成径为200～500 nm的类球形六方相结构. 发光强度增强, 但粒径很小, 对提高成像系统分辨率非常有意义. 通过比较样品的XEL和PL光谱, 讨论了XEL和PL光谱的发光机理和激发机制及退火对其特性的影响.     

硫化锌纳米粒子的乳液合成

纳米材料被人们认为是新型的功能材料^[1]。作为过渡金属硫化物,硫化锌（ZnS)材料显示出许多特异光电性能,在许多领域有着广泛的应用^[2],因而一直被应用和研究。     

ZnS-based visible-blind UV detectors: Effects of isoelectronic traps

The aim of this study is to reveal the underlying cause of the gradual turn-on characteristic of low Te containing ZnSTe Schottky barrier photodiodes. The results of photoresponse studies on ZnS, ZnSSe and ZnSTe diodes indicate that the Te isoelectronic trapping effect is responsible for the gradual turn-on characteristic of low Te containing ZnSTe Schottky barrier photodiodes. The results also reveal that the ZnSSe diode, having the advantage of being free of isoelectronic centers, is a more suitable choice for applications requiring high visible rejection power. It is demonstrated that highly UV sensitive responsivity with an abrupt long wavelength cutoff tailored to lie between 340–400 nm can be achieved in the ZnSSe diode system.     

Highly‐efficient Cd‐free CuInS2 thin‐film solar cells and mini‐modules with Zn(S,O) buffer layers prepared by an alternative chemical bath process

Recent progress in fabricating Cd‐ and Se‐free wide‐gap chalcopyrite thin‐film solar devices with Zn(S,O) buffer layers prepared by an alternative chemical bath process (CBD) using thiourea as complexing agent is discussed. Zn(S,O) has a larger band gap (E_g = 3·6–3·8 eV) than the conventional buffer material CdS (E_g = 2·4 eV) currently used in chalcopyrite‐based thin films solar cells. Thus, Zn(S,O) is a potential alternative buffer material, which already results in Cd‐free solar cell devices with increased spectral response in the blue wavelength region if low‐gap chalcopyrites are used. Suitable conditions for reproducible deposition of good‐quality Zn(S,O) thin films on wide‐gap CuInS₂ (‘CIS’) absorbers have been identified for an alternative, low‐temperature chemical route. The thickness of the different Zn(S,O) buffers and the coverage of the CIS absorber by those layers as well as their surface composition were controlled by scanning electron microscopy, X‐ray photoelectron spectroscopy, and X‐ray excited Auger electron spectroscopy. The minimum thickness required for a complete coverage of the rough CIS absorber by a Zn(S,O) layer deposited by this CBD process was estimated to ∼15 nm. The high transparency of this Zn(S,O) buffer layer in the short‐wavelength region leads to an increase of ∼1 mA/cm² in the short‐circuit current density of corresponding CIS‐based solar cells. Active area efficiencies exceeding 11·0% (total area: 10·4%) have been achieved for the first time, with an open circuit voltage of 700·4 mV, a fill factor of 65·8% and a short‐circuit current density of 24·5 mA/cm² (total area: 22·5 mA/cm²). These results are comparable to the performance of CdS buffered reference cells. First integrated series interconnected mini‐modules on 5 × 5 cm² substrates have been prepared and already reach an efficiency (active area: 17·2 cm²) of above 8%. Copyright © 2006 John Wiley & Sons, Ltd.     

原子吸收硫化锌法间接测定半胱氨酸络合反应的机理研究

通过编程计算半胱氨酸和锌离子在不同pH条件下的各种存在形式,通过分析拟合分布图,研究了硫化锌法原子吸收间接测定半胱氨酸时的pH对原子吸收的影响及络合反应的机理。经对不同形态的半胱氨酸与金属锌离子的共存区域的各种离子的组合探讨,发现在最佳测定条件下的半胱氨酸是以负一价荷电形态的半胱氨酸基Cys-与Zn(OH)₂形成了可溶性络合离子_２Zn(OH)_２。结果表明,理论分析计算的结果与实验数据得到了很好的吻合。     

ZnS/CuInS2/Mo/钠钙玻璃衬底上射频溅射ZnO∶Al薄膜的SEM研究

结合ZnO薄膜在Cu-III-VI2基薄膜太阳电池上的应用，采用射频磁控溅射技术以陶瓷ZnO∶Al2O3为靶材在ZnS/CuInS2/Mo/钠钙玻璃衬底上于固定沉积条件下低温（200℃）制备了铝掺杂氧化锌（ZnO∶Al）薄膜. 运用扫描电子显微镜研究了底层材料特别是ZnS和CuInS2的生长参数对沉积的ZnO∶Al薄膜的表面形貌的影响. 实验发现，衬底材料中硫含量的增加（无论来自ZnS还是来自CuInS2) ，都会引起沉积ZnO∶Al薄膜结晶质量的提高，而金属含量的增大将有利于薄膜均匀性的改进.     

147Pm激发的ZnS：Cu,Cl发光粉的研究

以高纯ZnS粉末为基质,采用高温转相、扩散,以及表面涂敷工艺,制得了¹⁴⁷Pm激发的ZnS:Cu,Cl发光粉。分析了ZnS:Cu,Cl的晶体结构,测量了ZnS:Cu,Cl的激发光谱、发射光谱、发光亮度。其晶体结构主要是六方纤锌矿型结构,激发光谱峰值波长为341nm,发射光谱峰值波长为513nm,初始发光亮度达到312mcd/m₂。由激发光谱的峰值波长341nm推算得到六方ZnS晶体的禁带宽度为3.64eV。分析了¹⁴⁷Pm激发的ZnS:Cu,Cl发光粉的发光寿命,其发光寿命达到5年以上。还探讨了该放射性发光粉的发光机理。¹⁴⁷Pm激发的ZnS:Cu,Cl的稳定发光,实际上是激发过程与复合过程的准平衡。ZnS:Cu,Cl的绿色发光来源于深施主-深受主对的复合发射。实验结果的分析表明,ZnS:Cu,Cl中深施主-深受主之间的能级间隔约为2.42eV。