激光功率密度对Al膜靶后表面快电子发射的影响

 报道了在20 TW皮秒激光器上完成的p偏振激光与等离子体相互作用过程中产生的快电子的角分布和能谱测量结果。实验得到：当激光功率密度小于10¹⁷ W/cm²时,电子发射没有明显定向性,在激光入射面内多峰发射;当激光功率密度大于10¹⁷ W/cm2,小于10¹⁸ W/cm²时,电子主要沿靶面法线方向发射;当激光功率密度达到相对论强度时,电子主要沿激光传播方向发射;激光功率密度未达到相对论强度时,靶后表面法线方向快电子能谱拟合平均温度符合共振吸收温度定标率;激光功率密度达相对论强度以上时,靶后表面法线方向快电子能谱拟合平均温度高于已有的温度定标率。     

电子束激励KrF激光放大器稳定运行的重要技术问题

 介绍了用于天光一号高功率氟化氪(KrF)准分子激光系统中的电子束双向激励主放大器稳定运行中必须解决的一些重要技术问题：水介质脉冲传输线中的绝缘支撑击穿问题；大面积电子束二极管阳极膜的安装；与压力膜接触处Hibachi筋的形状；二极管后脉冲的形成及其对阳极膜和阴极发射体造成的损害等问题。还着重描述了主开关导通时刻对二极管后脉冲的影响及最佳导通时刻的确定。     

Excitation functions of alpha particle induced reactions on aluminium and copper

Cross-sections for the reactions with product nuclei²⁴Na,²²Na,⁶⁸Ga and⁶⁷Ga were investigated over the energy range of 30 to 75 MeV for alpha particle induced reactions on natural aluminium and copper, using stacked-foil activation technique. The measured excitation functions were analysed with special reference to their suitability for monitoring beam energy and intensity. The experimental results were compared with the predictions of hybrid model of Blann. The assumption of initial exciton numbern ₀=4(4p0h) best satisfies the measured excitation functions in the present work.     

用网格衰减膜相对标定SIOFM─5FW软X光底片

点聚焦激光等离子体发出的Ｘ射线经晶体色散形成均匀的单色Ｘ射线源，在此基础上，用单层网格作为衰减膜，得到未经衰减和经过衰减的Ｘ射线谱，对无保护膜ＳＩＯＦＭ５ＦＷ软Ｘ光底片作了试验性的相对标定，得到了０．９１ｎｍ波长的特性曲线     

Measurement and analysis of excitation functions for alpha induced reactions on iodine and cesium

The excitation functions for the reactions¹²⁷I(α, 2n)¹²⁹Cs,¹²⁷I(α, 4n)¹²⁷Cs,¹³³Cs(α, 2n)¹³⁵La and¹³³Cs(α, 4n)¹³³La have been measured up to ≈50 MeVα-particle energy using the stacked foil activation technique. Measured excitation functions are compared with pre-equilibrium geometry dependent hybrid model calculations. It has been found that theoretical calculations using an initial exciton numbern ₀=4 (2p+2n+0h) give good agreement with experimental excitation functions.     

Determination of nickel in water by electrothermal atomic absorption spectrometry with preconcentration on a tungsten foil

A preconcentration method for nickel in waters involving adsorption on tungsten foil, followed by electrothermal atomic absorption spectrometry (ETAAS) with a tungsten tube atomizer is described. The most suitable pH for nickel adsorption was 5 and the optimum immersion time was 2 min. Severe interferences from co-existing elements (Al, Ca, Cu, Fe, K, Mg, Na, Pb and Zn) on the Ni AA signal were observed. Under optimal conditions, the preconcentration of nickel on W foil could eliminate interferences from these elements. The detection limit of nickel by preconcentration-ETAAS was 0.1 ng/ml (3S/N). The method with preconcentration on tungsten foil was applied to the determination of nickel in river water. The recovery of spiked nickel was 93–102%. The tungsten foil preconcentration method is sensitive, simple, and convenient. This adsorption method can be utilized inin situ-sampling of ultra-trace nickel in environmental samples (water). Furthermore, after sampling it is easy to carry and store the W-foil without contamination for long time.     

Reduced graphene oxide foils for ion stripping applications

ABSTRACT

Reduced graphene oxide (rGO) films can be employed as ion strippers in an accelerator. They show some advantages with respect to the graphite foils, due to their high thermal and electrical conductivity, low density, high mechanical resistance and high stability. Thin graphene oxide (GO) films with a sub-micron thickness have been synthesized and transformed into reduced GO (rGO) by ion beam irradiations. Physical characterizations of the pristine and ion irradiated GO films have been performed. Measurements of stripping efficiency have been carried out by using helium, lithium, carbon and oxygen ion beams. The rGO stripper films demonstrate a significantly high charge production, comparable to that of the graphite films but with the advantage of a longer lifetime.     

电解铜箔添加剂研究进展

介绍了电解铜箔添加剂的研究现状和进展;指出随着信息产业的不断发展,对电子产品印刷电路板(PCB)制作的要求不断提高,而对关键的电解铜箔技术所用的添加剂的要求也日益苛刻.同时就电解铜箔添加剂的发展趋势进行了展望,以期为今后国内电解铜箔行业的发展提供参考.     

超短激光与金薄膜靶相互作用产生的质子能谱

在能量11 mJ、波长744 nm、脉宽120 fs、功率密度61016 W/cm2的超短脉冲装置上,开展了超短脉冲激光与2.1 m和5.0 m金薄膜靶相互作用产生质子束的实验研究。利用Thomson谱仪测量了产生的质子能谱,发现利用2.1 m金薄膜靶时,质子能谱由于质子源数量不足而在74 keV附近出现单能峰,5.0 m的金薄膜靶产生的质子计数和能谱均比2.1 m的金薄膜靶产生的低,主要原因是超热电子穿过薄膜靶时出现的能量损失和几何倾斜降低了电子回流所致。     

ZnO Nanobelts and Hollow Microspheres Grown on Cu Foil

采用低温热蒸发法在铜箔衬底上制备了大量ZnO纳米带、空心微米球和“海胆”状球．采用XRD、激光拉曼光谱仪、SEM和荧光光谱仪分别对ZnO纳米结构的微结构、形貌和光致发光性质进行研究．分析表明,纳米带的宽度大约为500 nm且长度超过10μm,而空心微米球的直径为5～10μm;ZnO纳米结构的发光主要是较强的蓝绿缺陷态发光,以及弱的紫外带隙态发光．铜衬底上ZnO纳米结构的制备使得ZnO纳米结构和导电衬底之间具有良好黏着性和电接触性．