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Kinetics of the pulsed erosion deposition process induced by high intensity plasma beams

机译:高强度等离子体束引起的脉冲腐蚀沉积过程的动力学

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摘要

Intense pulsed ion and/or plasma beams can modify the surface properties of materials by melting their near surface region and doping and/or coating with foreign atoms reaching doses in the order of 10{sup}17 cm{sup}(-2) in a single pulse. Such processes can be performed using a Rod Plasma Injector (RPI), where plasma pulses are generated as a result of a low-pressure, high current discharge between two concentric, cylindrical sets of rod-type electrodes. The discharge is initiated by a HV pulse applied with a delay time τ{sub}d after the moment of injection of working gas into the inter-electrode space. Depending onτ{sub}d, two modes of operation are possible. Ifτ{sub}d is sufficiently long, the plasma contains almost exclusively the elements of the working gas (PID mode). For shortτ{sub}d in addition to the generation of plasma of the working gas rapid erosion of the metallic electrodes also occurs (DPE mode). This metal is deposited and in some cases mixed into the substrate. The aim of the present work was to get insight into the kinetics of the DPE process. Several experiments with different working gases (N, Ar, and Xe), different electrode materials (Ti, W) and substrates (Al{sub}2O{sub}3, Cu) were performed. Energy density was approximately 5-7 J/cm{sup}2 and pulse duration was approximately 1μs, respectively. The two main conclusions have been derived. (a) Metal atoms eroded from electrodes do not undergo ionization and acceleration during the discharge (as it is the case with the working gas). Vapor and low energy ions reach the surface when it is already solidified after being melted first by the working gas plasma. The metallic coating is molten and mixed into the substrate during the subsequent pulse. (b) Erosion of electrodes is caused by some thermal effects as a result of heating by ions and electrons - but not by sputtering.
机译:强脉冲离子束和/或等离子束可以通过熔化材料的近表面区域并掺杂和/或涂覆外来原子,达到约10 {sup} 17 cm {sup}(-2)的剂量,从而改变材料的表面性能。一个脉冲。可以使用杆式等离子注入器(RPI)来执行此类过程,其中,由于在两组同心,圆柱形的杆式电极组之间进行低压高电流放电而产生了等离子体脉冲。在将工作气体注入电极间空间之后,通过施加延迟时间τ{sub} d的HV脉冲开始放电。取决于τ{d} d,两种操作模式是可能的。如果τd足够长,则等离子体几乎仅包含工作气体的元素(PID模式)。除了产生工作气体的等离子体以外,还短时间产生金属电极的快速腐蚀(DPE模式)。沉积该金属,在某些情况下,将其混合到基材中。本工作的目的是深入了解DPE工艺的动力学。使用不同的工作气体(N,Ar和Xe),不同的电极材料(Ti,W)和衬底(Al {sub} 2O {sub} 3,Cu)进行了几次实验。能量密度分别约为5-7 J / cm {sup} 2,脉冲持续时间约为1μs。得出了两个主要结论。 (a)从电极腐蚀掉的金属原子在放电过程中不会发生电离和加速作用(工作气体就是这种情况)。当蒸汽和低能离子在被工作气体等离子体首先熔化后已经固化时,它们会到达表面。在随后的脉冲期间,金属涂层被熔化并混合到基底中。 (b)电极的腐蚀是由于离子和电子加热而产生的一些热效应引起的,而不是溅射引起的。

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