半导体Si上电沉积Cu-Co颗粒膜及其巨磁电阻效应

采用电化学沉积方法在半导体Si上制备Cu-Co金属颗粒膜. XRD测试结果表明制备态的薄膜形成了单相亚稳态面心合金结构, 薄膜经退火后, XRD谱图中出现了析出的纯金属Co的衍射峰, 这表明薄膜在退火过程中发生了相分离. TEM测试结果也进一步证实了磁性的Co颗粒从非磁性的铜基体中析出. 随着退火温度的增加, 颗粒膜巨磁电阻(GMR)效应不断增大, 当退火温度为450 ℃时, Co0.20Cu0.80薄膜的巨磁电阻效应达到最大, 磁阻率为8.21％. 之后, 磁阻率又随退火温度的升高而降低. 退火前后样品磁滞回线的变化表明薄膜中发生了从超顺磁性到铁磁性的转变, 矫顽力、剩余磁化强度和饱和磁化强度均随退火温度的增高而逐渐增大. 超顺磁性颗粒的作用导致了GMR－H与M－H曲线的不同.     

铜在储氢合金表面包铜电极中的行为

在密封的电池体系中，包铜储氢合金电极具有较好的抗氧化能国和；而在强碱性溶淤 中，铜在电极工作的电位范围内具有一定的稳定性，但当扩展扫描范围，将出现铜的氧化不这原反应。     

ρ-Si上电沉积制备镍-磷非晶薄膜催化剂

非品态合金作为一类新型催化材料，越来越引起人们的广泛关注．Ni－P非晶态合金催化剂的催化加氢性能研究尤为活跃［‘，’］，研究结果表明其活性明显高于Ni－P晶态合金和比表面积相当的Ni粉L＼从而具有实用价值．传统的非品态合金催化剂的制备方法，如真空蒸镀、真空溅射、液相急冷及离子注入等，存在设备复杂、耗能大，难以批量生产等缺点；化学法可制备粒度均匀的催化剂＊；但给提纯带来了一定困难，而电沉积制备非晶薄膜催化剂由于具有纯度高、能耗低、制作方便等优势而倍受青睐问利用半导体做载体沉积Ni－P非晶态合金，在光电催化…     

离子液体在电化学中的应用

离子液体作为绿色替代溶剂在电化学中的应用涉及电解、电镀、电催化、电池和电容技术等 ,在全球环境问题日益严峻的今天 ,电化学及其技术将显示重要作用。本文就离子液体这一新型的反应介质及其在电化学中的应用和研究进展加以阐述     

非晶Co-Pt合金纳米线有序阵列的制备及其磁学性质

通过直流电沉积方法，以多孔阳极氧化铝(AAO)为模板，在室温下成功制备出一维非晶态Co-Pt合金纳米线有序阵列. SEM和TEM分析表明：纳米线长度均约10 μm，直径35 nm；纳米线在阳极氧化铝模板孔内互相平行. XRD结果表明，制备的纳米线为非晶态结构，经过700 ℃退火处理后则转变为面心立方(FCC)多晶结构. 采用VSM(振动样品磁强计)对退火处理前后样品的矫顽力和剩磁比进行研究，结果表明：当外加磁场与纳米线平行时，非晶态Co-Pt合金纳米线的矫顽力高达1700 Oe，剩磁比为0.83，表现出明显的垂直磁各向异性；而退火处理则使其优秀的磁学性质消失. 退火前后不同的磁学性质源于其不同的微观结构. 非晶态的Co-Pt合金纳米线由于无磁晶各向异性竞争，进而使得由纳米线一维形态引起的形状各向异性起主导作用，使其显示了很好的垂直磁各向异性；而多晶样品由于磁晶各向异性与形状各向异性竞争，导致矫顽力和剩磁比迅速降低.     

电位活化现象与金属电沉积初始过程的研究

进行了恒电流电位-时间曲线和循环伏安曲线的测定，显示了铁电极进行氰化物镀铜时，镀层沉积前铁表面的电位活化过程. 对铁电极上焦磷酸盐镀铜的初始过程研究表明，由于铜的析出电位较正，铜是在未活化的电极表面上沉积的，因此镀层的结合强度很差.采用氩离子溅射和X射线光电子能谱相结合的方法，检测焦磷酸盐镀铜层和铁基体界面区含氧量的变化，证明了氧化层的存在. 通过添加辅助络合剂和控制起始电流密度的方法，可以增强无氰电镀时阴极的极化. 当铜的析出电位负于铁基体的活化电位时，可显示出铁表面的电位活化过程，定量测量镀层的结合强度也与氰化物电镀相近.     

Electrodeposition of a nickel-based hydrotalcite on Pt nanoparticles for ethanol and glucose sensing

Two different substrates, GC and graphite electrodes, have been coated with electrodeposited Pt nanoparticles (PtNPs) of different morphologies and sizes (from 2 μm to 20 nm). The electrochemical behavior of the platinised GC electrodes has been mainly evaluated in terms of the increase of the real surface area. A nickel-based hydrotalcite-like compound (HT) has been electrosynthesised on the GC platinised electrodes, by the cathodic reduction of a 0.03 M Ni and Al nitrates solution, and the cyclic voltammetric responses to these electrodes have been measured in a 0.1 M NaOH solution. Finally, the electrocatalytic performances of the GC–PtNPs–HT electrodes to ethanol and glucose have been investigated and compared with the performances of HT electrodeposited onto bare Pt, in the same conditions.     

Electrodeposition of Lead at Boron‐Doped Diamond Film Electrodes: Effect of Temperature

The electrodeposition of lead on boron‐doped diamond has been studied with a view to identifying the fundamental parameters controlling the sensitivity and lower detection limit in anodic stripping voltammetry. Chronoamperometric transients are used to explore the deposition, indicating a progressive growth mechanism confirmed by ex situ AFM images. Linear sweep ASV experiments show a threshold concentration of ca 10^?6 M below which no lead is detected; this is attributed to the need for nucleation of the solid phase on the electrode. Experiments with variable temperature show that this threshold can be usefully lowered at elevated temperatures.     

Properties of Co-Mo coatings obtained by electrodeposition at pH 6.6

Cobalt-molybdenum coatings were prepared by electrodeposition in a sulfate-citrate bath and their morphology, structure and magnetic properties were analysed. Concentrations of 0.1 mol dm^–3 CoSO₄ and 0.005 mol dm^–3 Na₂MoO₄ at pH 6.6 led to Co-Mo deposits of 20–23% Mo that can be grown to several microns over graphite or copper substrates. At low deposition potentials or current densities, the deposits presented a close-packed hexagonal structure (hcp) that evolved to a (100)+(110) preferred orientation and acicular morphology as the deposit thickness increased. When the deposition potential or the current density was made more negative, a mixed crystalline+amorphous structure was obtained. The degree of crystallinity depended on the thickness: thin films were more amorphous than the thicker ones. Co-Mo deposits showed lower saturation magnetization (M_s) and coercivity (H_c) than the pure cobalt deposits. The crystalline+amorphous films showed the lowest H_c values (around 40 Oe).     

Electrochemical deposition and properties of PbO2 + Co3O4 composites

Electrolysis of suspensions of Co₃O₄ particles in Pb²⁺-containing electrolytes has been used for depositing PbO₂ + Co₃O₄ composite layers on Ni rotating dise anodes. A sufficiently high angular speed of the electrode is necessary to obtain layers of homogeneous thickness and Co₃O₄ concentration. The volume fraction of Co₃O₄ particles in the deposit α reaches a limiting value of ca. 0.1 when the volume fraction of particles in suspension C exceeds 0.008. The current density j has little effect on α as long as it is in the range 1 to 20 mA cm⁻²; if j increases further, α decreases.PbO₂ + Co₃O₄ composite layers have been studied as electrode materials for the oxygen evolution reaction (mainly in NaOH solution). The overpotential and Tafel slope decrease upon increasing α. At a fixed potential, j is roughly proportional to OH⁻ concentration. The PbO₂ + Co₃O₄ electrode performance is fairly stable at 25°C but declines with time at higher temperature.