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英译汉--给高分,急!!

金钥匙卫浴 2007-04-18
Abstract The hollow cathode will be presented as a plasma source for reactive evaporation processes. The hollow cathode generates an arc discharge plasma. This contains a high portion of directed electrons with an enhanced mean energy, the... Abstract The hollow cathode will be presented as a plasma source for reactive evaporation processes. The hollow cathode generates an arc discharge plasma. This contains a high portion of directed electrons with an enhanced mean energy, the so called low voltage electron beam (LVEB). The mean energy of the LVEB, in the range of 11 eV, results in a very effective ionization of the gas and vapor particles. Consequently, very high plasma densities can be achieved, which corresponds to high particle densities in high-rate deposition processes. Furthermore, a high self bias potential of about 16 V is obtained on insulating substrates. For the coating of heat-sensitive substrates with high deposition rates a process with a low ratio between thermal load and deposition rate is necessary. The heat flux on plastic substrates 2 has been measured at the reactive Al evaporation process. The overall thermal load of about 4 W/cm related to a deposition rate of 100nm/ s is low in comparison to other processes. This makes the hollow cathode a favorable tool for the plasma-activated high-rate deposition. The oxide layers deposited by this process show dense and glassy structures even at comparatively low condensation 2 temperatures. This is caused by the high ion current densities in the order of 30 mA/ cm . The low ion energy determined by the self bias potential results in relatively low compressive stress below 100 MPa. The low thermal load and the moderate intrinsic stress of the layers makes the hollow cathode plasma-activated deposition (HAD) process the method of choice for the deposition of oxides as abrasion resistant layers on plastic films and sheets. Ó 1998 Elsevier Science S.A. All rights reserved. 1. Introduction Table 1 shows typical layer materials that have been deposited by the PMS–DMS process and the corre-In recent years, the importance of coating plastic sponding dynamic deposition rates. The dynamic deposisurfaces with oxides and nitrides has increased. Typical tion rate is defined for moving substrates as the product of applications are solar control and low-emissivity multilayer the layer thickness and the substrate transportation speed. systems for window panes and window films, antiabrasion The HAD (hollow cathode-activated deposition) process layers on plastic films, plastic sheets and plastic parts as is the combination of a high-rate evaporation process and a well as barrier layers for packaging films. high-density plasma activation using the hollow cathode
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B安小春
摘要 空心负极将被提出作为血浆来源为易反应的蒸发过程。空心负极引起弧放电血浆。这包含被指挥的电子的一个高部份以改进的卑鄙能量, 所谓的低压电子束(LVEB) 。LVEB 的卑鄙能量, 在11 的范围eV, 导致气体和蒸气微粒的非常有效的电离。 结果, 非常高血浆密度可能达到, 对应于高微粒密度在高率证言过程中。 此外, 大约16 V 高自已偏心潜力被获得在绝缘的基体。为热敏感基体涂层以高证言率一个过程以一个低比率在热量装载和证言率之间是必要的。热涨潮在塑料基体2 被测量了在易反应的Al 蒸发过程。大约4 W/cm 整体热量装载与100nm/ 关系了s 的证言率是降低与其它过程比较。这做空心负极为血浆被激活的高率的一个有利工具 证言。氧化物层数由这个处理展示密集和玻璃状结构放置在比较低结露2 个温度。这由高的离子电流密度造成按30 mA/ cm 的顺序。低离子能量由自已偏心潜在的结果确定在相对地低压缩应力在100 MPa 以下。低热量装载和层数的适度内在重音做空心负极血浆被激活的证言(有) 处理选择方法为氧化物的证言当磨蚀抗性层数在塑料胶膜和板料。3O Elsevier 1998年科学S.A 。版权所有。 1. 介绍 是的表1 展示典型的层数材料 由PMS-DMS 过程放置和corre 在Z近岁月, 涂上塑料的重要性sponding 动态证言率。动态deposisurfaces 与氧化物和氮化物增加了。典型的tion 率被定义为移动的基体因为应用产品是太阳控制和低发射性多层层数厚度和基体运输速度。 系统为窗玻璃和窗口影片, antiabrasion 有的(凹陷负极被激活的证言) 处理层数在塑料胶膜, 塑料板料和塑料零件象高率蒸发过程和井的组合当阻挡层为包装的影片高密度血浆活化作用使用空心负极

分少了点吧 再加点``
3 0 2007-04-19 0条评论 回复
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