首页> 外文期刊>IEEE Transactions on Plasma Science >Ion Charge State Distributions of Al and Cr in Cathodic Arc Plasmas From Composite Cathodes in Vacuum, Argon, Nitrogen, and Oxygen
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Ion Charge State Distributions of Al and Cr in Cathodic Arc Plasmas From Composite Cathodes in Vacuum, Argon, Nitrogen, and Oxygen

机译:真空,氩气,氮气和氧气中复合阴极在阴极电弧等离子体中Al和Cr的离子电荷态分布

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Multielement cathodes are increasingly used for advanced coatings, yet most cathodic arc plasma measurements have been reported for pure element cathodes. In this contribution, we measure the charge state distributions of aluminum and chromium ions from Al–Cr composite cathodes of different Al to Cr ratios. The arc discharges are pulsed, with pulse duration of around 300 $mu{rm s}$ and currents of 175 A, operated at high vacuum and in gases with a pressure of up to 1.3 Pa of Ar, ${rm N}_{2}$, and ${rm O}_{2}$. For comparison with literature data, the measurements also included the plasma compositions of discharges using pure Al and Cr cathodes. As expected, the charge distributions are found to be affected by the cathode conditions, the type of gas, and the pressure of the gas into which the arc spot plasma is expanding. Generally, large effects of gas are observed when the pressure exceeded 0.1 Pa, which can be mainly associated with the ions' mean-free path with respect to charge exchange collisions. Differences between ions can be attributed to the energy- and species-dependent charge-exchange cross sections. Considering different cathode compositions, we found that Cr ions tend to have lower charge states from the composite cathodes compared with the pure element cathode, whereas Al ions are relatively unaffected by the cathode composition. Despite the wealth of detailed experimental results, it is difficult to discern trends and rules that could be generalized because measured data involve a convolution of cathode phenomena and gas collisional effects.
机译:多元素阴极越来越多地用于高级涂料,但据报道大多数阴极电弧等离子体测量均用于纯元素阴极。在这一贡献中,我们测量了不同铝对铬比率的铝铬复合阴极中铝离子和铬离子的电荷态分布。电弧放电是脉冲的,其脉冲持续时间约为300 $ mu {rm s} $ ,并且电流为175 A在高真空和Ar压力高达1.3 Pa的气体中, $ {rm N} _ {2} $ $ {rm O} _ {2} $ 。为了与文献数据进行比较,测量还包括使用纯Al和Cr阴极的放电等离子体成分。正如预期的那样,发现电荷分布受阴极条件,气体类型和电弧点等离子体向其中膨胀的气体压力的影响。通常,当压力超过0.1 Pa时会观察到很大的气体影响,这可能主要与离子在电荷交换碰撞方面的平均自由程有关。离子之间的差异可归因于能量和物种相关的电荷交换截面。考虑到不同的阴极组成,我们发现与纯元素阴极相比,Cr离子倾向于具有较低的复合阴极电荷态,而Al离子相对不受阴极组成的影响。尽管有大量详细的实验结果,但是由于测量数据涉及阴极现象和气体碰撞效应的卷积,因此很难辨别可以概括的趋势和规则。

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