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首页> 外文期刊>Surface & Coatings Technology >Optical emission diagnostics of cathodic arc plasmas used for deposition of TiN and Ti(C, N) coatings
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Optical emission diagnostics of cathodic arc plasmas used for deposition of TiN and Ti(C, N) coatings

机译:用于沉积TiN和Ti(C,N)涂层的阴极电弧等离子体的光发射诊断

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The interelectrode region of titanium arc discharge in various atmospheres (N-2, C2H2, mixtures of N-2 + C2H2 and vacuum) has been investigated by optical emission spectroscopy. A multi-source, industrial arc vacuum device was used to generate the discharges. It was found that the temperatures determined by applying the Boltzmann and coupled Saha-Boltzmann equations for lines of Ti I, Ti II and Ti III were very close together, with exception of those connected with low-lying energy levels of Ti I. The temperatures were dependent on the atmosphere composition. The interelectrode plasma was observed to be in a partial local thermodynamic equilibrium (p-LTE) state. The N-2 pressure (between 0.2 and 2 Pa) and the N-2/C2H2 ratio (between 5 and 30%) changed the relative abundance of various excited species in the plasma. The electron impact processes were suggested to be here mainly responsible for the excitation and ionization of plasma components in the interelectrode area. The effect of plasma cooling in the presence of higher C2H2 concentration was observed. (C) 2003 Elsevier B.V. All rights reserved.
机译:通过光发射光谱法研究了在各种气氛(N-2,C2H2,N-2 + C2H2的混合物和真空)下钛电弧放电的电极间区域。使用多源工业电弧真空装置产生放电。发现通过应用玻尔兹曼和耦合的Saha-Boltzmann方程对Ti I,Ti II和Ti III的线确定的温度非常接近,除了那些与Ti I的低能级有关的温度。取决于大气成分。观察到电极间等离子体处于局部局部热力学平衡(p-LTE)状态。 N-2压力(介于0.2和2 Pa之间)和N-2 / C2H2比率(介于5和30%之间)改变了等离子体中各种激发物质的相对丰度。在这里,电子碰撞过程被认为主要是引起电极间区域中等离子体成分的激发和电离的原因。观察到在较高的C2H2浓度下等离子冷却的效果。 (C)2003 Elsevier B.V.保留所有权利。

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