电沉积温度对碘化亚铜薄膜光学性质的影响(英文)

以ITO导电玻璃衬底,CuSO4、KI为反应溶液,EDTA为络合剂,通过简单的电化学方法分别在40,60,80℃的电沉积温度下成功制备出高定向的γ-CuI薄膜。讨论了不同沉积温度下碘化亚铜薄膜各项性质的差异,作为比较还利用化学沉积方法在室温下合成了碘化亚铜粉末。利用X射线衍射图(XRD)进行结构分析,场发射扫描电子显微镜(SEM)进行形貌观察。实验结果表明:碘化亚铜薄膜由三角形纳米片构成,沿(111)晶相择优生长。随着电沉积温度的升高,颗粒的尺寸从2μm减小到500 nm。不同电沉积温度制备出的碘化亚铜薄膜均在拉曼光谱上呈现出一个强的LO峰和一个微弱的TO峰,峰的强度均随着电沉积温度的升高而增大。同时,光致发光(PL)光谱的分析显示出强的近带边发射峰。CuI粉末在结构及形貌等性质上与CuI薄膜有一定的差异。     

基底温度对α-C:H膜微观结构的影响

使用RF-PECVD法分别在基底温度为60℃、120℃和200℃的N型单晶锗表面制备了α-C:H膜,采用拉曼光谱、傅里叶变换红外吸收光谱和原子力显微镜等技术手段研究分析了α-C:H膜的价键组成及表面形貌,讨论了基底温度对α-C:H膜微结构及部分性能的影响。结果表明,在α-C:H膜沉积过程中,基底温度对膜层微观结构有较大影响,基底温度60℃时,膜层表面光滑、致密无石墨化现象。随着基底温度的升高,α-C:H膜中含H量和微晶石墨量逐渐增多,α-C:H膜层性能也逐步退化。     

A polyene chain of canthaxanthin investigated by temperature-dependent resonance Raman spectra and density functional theory （DFT） calculations

We report on a temperature-dependent resonance Raman spectral characterization of the polyene chain of canthax- anthin. It is observed that all vibrational intensities of the polyene chain are inversely proportional to temperature, which is analyzed by the resonance Raman effect and the coherent weakly damped electron/lattice vibrations. The increase in intensity of the CC overtone/combination relative to the fundamental with temperature decreasing is detected and discussed in terms of electron/phonon coupling and the activation energy Uop. Moreover, the polyene chain studies using the density functional theory B3LYP/6-31 G＊ level reveal a prominent peak at 1525 cm-1 consisting of two closely spaced modes that are both dominated by C=C stretching coordinates of the polyene chain.     

Heat transfer in boundary layer stagnation-point flow towards a shrinking sheet with non-uniform heat flux

In this paper, the effect of non-uniform heat flux on heat transfer in boundary layer stagnation-point flow over a shrinking sheet is studied. The variable boundary heat fluxes are considered of two types: direct power-law variation with the distance along the sheet and inverse power-law variation with the distance. The governing partial differential equations (PDEs) are transformed into non linear self-similar ordinary differential equations (ODEs) by similarity transformations, and then those are solved using very efficient shooting method. The direct variation and inverse variation of heat flux along the sheet have completely different effects on the temperature distribution. Moreover, the heat transfer characteristics in the presence of non-uniform heat flux for several values of physical parameters are also found to be interesting.     

Densification and lithium ion conductivity of garnet-type Li7-xLa3Zr2-xTaxO12 （x=0.25） solid electrolytes

The garnet-type Li7La3Zr2O12 ceramic is a promising solid electrolyte for all-solid-state secondary lithium batteries. However, it faces the problem of lithium volatilization during sintering, which may cause low density and deterioration of ionic conductivity. In this work, the effects of sintering temperature and addition on the density as well as the lithium ion conductivity of Li7-xLa3Zr2-xTaxO12 (LLZTO, x=0.25) ceramics prepared by solid state reaction have been studied. It is found that optimization of the sintering temperature leads to a minor increase in the ceramic density, yielding an optimum ionic conductivity of 2.9×10-4 S·cm-1 at 25℃. Introduction of Li 3 PO 4 addition in an appropriate concentration can obviously increase the density, leading to an optimum ionic conductivity of 7.2×10-4 S·cm-1 at 25℃. This value is superior to the conductivity data in most recent reports on the LLZTO ceramics.     

Optical spectroscopy studies on FeTelxSex and AxFe2uSe2 （A = K, Rb, Cs）： A brief overview

In this short overview, we summarize the optical spectroscopy FeTezxSex and AxFe2-ySe2. We elaborate that optical spectroscopy band structure evolution across the AFM phase transition temperature, studies on iron selenide superconducting systems measurements yield fruitful information about the the electronic correlation effect, the superconduct- ing pairing energy gap, the condensed carrier density or penetration depth, the inhomogeneity and the nanoscale phase separation between superconductivity and antiferromagnetism in those systems.     

单脉冲和再加热正交双脉冲激光诱导击穿光谱对比研究

为了提高激光诱导击穿光谱技术(LIBS)的检测灵敏度和辐射光谱特性,采用再加热正交双脉冲结构对样品中的4种元素Fe,Pb,Ca和Mg以及含有不同浓度重金属元素Cr的土壤样品进行分析。研究了4条特征谱线FeⅠ：404.581 nm,PbⅠ：405.78 nm,CaⅠ：422.67 nm和MgⅠ：518.361 nm的光谱强度和信背比随两激光脉冲之间时间间隔的变化关系,获得了两激光脉冲之间最佳的时间间隔为1.0 μs。在单脉冲和双脉冲条件下,得到了4条特征谱线FeⅠ：404.581 nm,PbⅠ：405.78 nm,CaⅠ：422.67 nm和MgⅠ：518.361 nm光谱强度的增强倍数分别为2.23,2.31,2.42和2.10;分析了特征谱线FeⅠ：404.581 nm和CaⅠ：422.67 nm谱线强度随时间的演化特性以及4条特征谱线信背比随光谱采集延时的变化关系,双脉冲能有效延长光谱强度的衰减时间以及提高特征谱线的信背比;比较分析了等离子体温度和电子密度随时间的演化特性,在双脉冲条件下,等离子体温度最大升高了730 K,电子密度最大增加了1.8×1016 cm-3。单脉冲和双脉冲条件下获得重金属元素Cr的检测限分别为38和20 μg·g-1,再加热正交双脉冲技术使元素检测限下降近2倍。以上结果表明：再加热正交双脉冲能有效地提升LIBS技术的检测灵敏度和光谱特性,为进一步降低元素的检测限提供了有效的方法。     

基于辐射法和原子发射光谱法的转炉口火焰温度测量

转炉炼钢的终点控制包括钢水出钢时温度及其成分的控制,炉口火焰能够反映炉内脱碳速率及转炉运行参数等。工业炉燃烧火焰可见光谱段,普遍存在着钾(K)和钠(Na)等碱金属元素的原子发射谱线,利用K的特征谱线相对比值可以计算火焰温度。基于辐射双色法,三色法和谱线相对强度法对转炉口火焰温度进行了测量;数据处理过程中对特征谱线进行了基线拟合提取,小波脊线拟合提取;特征谱线进行了Gauss函数和Lorenz函数拟合。结果表明,辐射测温法对谱线比较敏感,选择合理的波段能够有效,精确地测量火焰温度;采用谱线相对强度法受制于特征谱线的数学模型、谱线的跃迁机率、能级的简并度及火焰的光学厚度,需要分辨率非常高的光谱仪才能进行高温转炉火焰中电子温度的测量。     

沿面型介质阻挡放电喷枪的发光特性及气体温度研究

利用氩气作为工作气体,采用正弦电压驱动沿面型等离子体喷枪,在大气压空气环境中产生了均匀的等离子体羽。电学和光学测量结果表明,等离子体羽放电只存在于外加峰值电压的正半周期,并且正半周期的放电脉冲个数随气体流量的增加而增加。通过对正半周期不同位置的发光脉冲信号进行比较,发现等离子体羽均按子弹形式传播,其中每一个发光脉冲均对应一次等离子体子弹传播过程。通过对比放电电流和等离子体羽的发光信号,发现等离子体羽的发光脉冲滞后于放电电流脉冲,且该延迟时间基本服从正态分布。该延迟时间随着外加电压峰值及气体流量的增大而减小。利用光纤测温仪测量了等离子体羽的气体温度,发现气体温度随外加峰值电压的增大而升高,随工作气体流量的增大而降低。通过分析放电过程,对上述现象进行了定性解释。     

激光诱导Ti等离子体电子温度的实验研究

室温,常压下,利用Nd∶YAG脉冲激光器产生的波长为1 064 nm, 脉宽12 ns,能量分别180, 230和280 mJ的脉冲激光冲击Ti靶,使用中阶梯光栅光谱仪检测了三种激光能量下对应的光谱。调节延时器DG645的延迟时间,检测了延迟0～500 ns时间范围内Ti等离子体对应激光能量下的发射光谱,分析光谱,可以得到了九条不同的的TiⅠ 和TiⅡ等离子体谱线,证明在该实验条件下,Ti靶能够充分吸收能量电离且离子谱线具有不同的演化速率,利用Saha-Boltzmann法计算并分析Ti等离子体电子温度,实验结果表明：相同的延迟时间,激光能量越大,谱线相对强度越大,电子温度越高,谱线相对强度的变化量随激光能量的变化量增大而增大;在延时0～150 ns内,三种激光能量下的等离子体电子温度和谱线的相对强度都随延迟时间的增加而快速下降,其中280 mJ激光能量下的等离子体电子温度和谱线强度下降速率较快;在150～250 ns范围内,电子温度和谱线强度均随延迟时间的增加有一个缓慢的上升,180 mJ激光能量下的等离子体电子温度和谱线强度的上升速率较快。250～500 ns范围内,三种激光能量下的电子温度和谱线强度均随延迟时间的增加而缓慢下降。