飞秒激光-金属薄膜靶相互作用中靶前后超热电子能谱的比较

采用电子谱仪测量了飞秒激光-金属薄膜靶相互作用中靶前和靶后产生的超热电子能谱.结果显示：靶前超热电子能谱的峰出现在约430 keV处，靶后超热电子能谱的峰出现在约175 keV处；靶前超热电子的有效温度分别为218 keV和425 keV，靶后超热电子能谱出现“软化”现象，其有效温度分别为96 keV和347 keV.靶前和靶后超热电子能谱明显不同是由于超热电子输运穿越过密等离子体和冷材料的靶，并在靶后建立Debye鞘，鞘电场使靶后超热电子能谱峰向低能端移动，鞘电场和自生磁场导致靶后超热电子能谱产生“软化”，估算出的鞘电场小于激光电场.     

多层板材料的技术动向

概述了多层板材料的技术动向和特性。     

Formation of Al-Si Composite Oxide Film by Hydrolysis Precipitation and Anodizing

This paper presents a new technique in the high dielectric constant composite oxide film preparation.On the basis of nanocompsite high dielectric constant aluminum oxide film growth technology, a new idea of adulterating Si oxide species into the aluminum composite film was proposed. As a result, the specific capacitance and withstanding voltage of the composite oxide film formed at the anodizing voltage of 20V are enhanced, and the leakage current of the aluminum composite oxide film is reduced through incorporation of Si oxide species.     

Excited atomic state of Li

An optical transition of 3489 A has been shown to arise from Li using beam foil spectroscopic technique. The mean life of the state emitting this radiation has been measured to be 2.23 ä 0.08 n sec.     

固体薄层纵深分析研究——Ⅱ.钢、铝合金和钛合金溅射速率的测定

用PHI 600型扫描俄歇探针、200型台阶仪和Q-920型图象分析仪,测定了35Cr Ni3MoV钢、Al-5.5 Zn-1.4Mg合金和Ti-5Al-2.5Sn合金的溅射速率,提出了对蚀坑分部位确定溅射速率的方法。文中给出了详细的测定结果。     

辐射烧蚀铝箔数值模拟研究

 利用一维多群辐射输运程序RDMG数值模拟神光II条件下辐射烧蚀铝箔的实验研究,详细描述了X光在铝箔中的辐射输运过程,清楚地显示了辐射热波在铝箔中的传播,给出铝等离子体温度密度的时空分布、铝箔背面出射的X光能谱及出射X光各能区能流随时间的变化,分析出射X光的能区对测量结果的影响,对神光II条件下辐射烧蚀铝箔的厚度范围进行初步的探讨。数值结果与实验结果相吻合。     

Optical parameters and work function of Zn–In–Sn–O films

The work function behavior of Zn–In–Sn–O (ZITO) films with various Zn and Sn contents were studied. The work function increased with addition of Zn content. With further increase of Zn contents, the work function gradually decreased. The work function behavior can be investigated by (1) Fermi level position relative the carrier concentration, (2) ionization potential by the surface dipole change. The Fermi level position related the carrier concentration was calculated by Drude parameters, and ionization potential measured by UPS. As results, we confirmed that the work function of ZITO may be linked to changes in ionization potential, not carrier concentration.     

Demonstration of enhanced the photocatalytic effect with PtSe2 and TiO2 treated large area graphene obtained by CVD method

Here, we report our method on enhancing the photocatalytic effect with PtSe₂ and TiO₂ treated large area graphene (LAG). The LAG was growth on copper foil at a low temperature (500 °C) under atmospheric pressure by chemical vapor deposition (CVD) method. A facile, fast ultrasonic method was then used to successfully synthesize PtSe₂-LAG/TiO₂ nanocomposites. The composites that were obtained were characterized using X-ray diffraction (XRD) spectroscopy, scanning electron microscopy (SEM) with energy dispersive X-ray (EDX) spectroscopy, transmission electron microscopy (TEM), Raman spectroscopic analysis, and X-ray photoelectron spectroscopy (XPS). UV–vis diffuse reflectance spectra (DRS) analyses were also performed, and the catalytic behavior was investigated by the decomposition of methylene blue (MB).The as-prepared LAG with a Raman D band was obtained, and graphene layers can be clearly seen in High-Resolution Transmission Electron Microscopy (HRTEM) images. The degradation performance of the MB solution was determined via UV–vis spectrophotometry. This improved photocatalytic activity is a result of the positive synergetic effect between PtSe₂ and LAG in the heterogeneous photocatalyst. In this study, the LAG behaves as an electron transfer agent, contributor, collector, and source of active adsorption sites. The optical properties were also observed to be affected by the different weight ratios of the LAG in the composites by observing their respective band gaps from diffuse reflectance spectra.     

Hydrodynamics of a biologically inspired tandem flapping foil configuration

Numerical simulations have been used to analyze the effect that vortices, shed from one flapping foil, have on the thrust of another flapping foil placed directly downstream. The simulations attempt to model the dorsal–tail fin interaction observed in a swimming bluegill sunfish. The simulations have been carried out using a Cartesian grid method that allows us to simulate flows with complex moving boundaries on stationary Cartesian grids. The simulations indicate that vortex shedding from the upstream (dorsal) fin is indeed capable of increasing the thrust of the downstream (tail) fin significantly. Vortex structures shed by the upstream dorsal fin increase the effective angle-of-attack of the flow seen by the tail fin and initiate the formation of a strong leading edge stall vortex on the downstream fin. This stall vortex convects down the surface of the tail and the low pressure associated with this vortex increases the thrust on the downstream tail fin. However, this thrust augmentation is found to be quite sensitive to the phase relationship between the two flapping fins. The numerical simulations allows us to examine in detail, the underlying physical mechanism for this thrust augmentation.      

气体爆轰波在声学吸收壁下游的再加强过程

实验研究了爆轰波在声学吸收段下游发生的再恢复过程。利用声学吸收段首先将一个稳定的爆轰波衰减,于是产生一个非稳定爆轰波,速度降为 45% ~60?J。该非稳定爆轰波传出声学吸收段后再次加强,并在距声学吸收段出口端一定距离处突然发展成超驱动爆轰。实验利用烟迹技术捕捉了爆轰波从发生衰减到再次加强的全过程,获得了爆轰波再加强距离随初压变化的实验规律。由此,本文建立了再加强段内加速传播火焰的理论模型,称为激波 -爆燃波复合态,并解释了火焰加速和超驱动爆轰形成的机理。