氧化铟锡氩离子束溅射二次离子的能量分布

C. Bundesmann, A. Hellmich
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引用次数: 1

摘要

利用能量选择质谱法测量了氧化铟锡氩离子束溅射过程中二次离子的能量分布与几何参数(离子入射角、极性发射角、散射角)、离子能量和o2背景压力的关系。最常见的离子种类是O +、o2 +、Ar +、In +和Sn +。O +、In +和Sn +离子的能量分布在10 ~ 20 eV之间呈现低能最大值,当散射角为γ > 90°时呈幂律衰减。如果γ < 90°,则会形成一个额外的高能结构,该结构被分配给各向异性效应,即直接溅射粒子。Ar +离子的能量分布呈现出一个低能的最大值,并且与散射角有关,最多可达两个附加的高能结构,这些结构也被分配给各向异性效应。这里它与直接散射事件有关。所有附加结构都与散射角和离子能量有系统的相关性。o2 +离子的能量分布表现为低能量最大值,随后信号突然下降。散射角和离子能量几乎没有变化。一般来说,增加o2背景压力会导致粒子能量的降低,这是由于在与背景气体粒子相互作用时能量损失所致。实验结果与基于弹性双粒子碰撞理论的srim计算和SDTrimSP蒙特卡罗模拟进行了比较和讨论。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Energy distributions of secondary ions for the Ar ion beam sputtering of indium tin oxide
The energy distributions of secondary ions for the Ar ion beam sputtering of indium tin oxide were measured in dependence on geometric parameters (ion incidence angle, polar emission angle, scattering angle), ion energy, and O 2 background pressure using energy-selective mass spectrometry. The most prevalent ion species were identified to be O +, O 2 +, Ar +, In +, and Sn +. The energy distributions of O +, In +, and Sn + ions show a low-energy maximum between 10 and 20 eV, followed by a power-law decay if the scattering angle is γ > 90 °. If γ < 90 °, an additional high-energy structure evolves, which is assigned to anisotropy effects, namely, directly sputtered particles. The energy distributions of the Ar + ions show a low-energy maximum and, in dependence on the scattering angle, up to two additional high-energy structures, which are also assigned to anisotropy effects. Here it is related to direct scattering events. All additional structures show systematic correlations with scattering angle and ion energy. The energy distributions of the O 2 + ions exhibit a low-energy maximum followed by a sudden signal drop. There is almost no variation with scattering angle or ion energy. In general, increasing the O 2 background pressure results in a decrease of the particle energy due to an energy loss upon interaction with background gas particles. The experimental results are compared and discussed with calculations based on elastic two-particle collision theory and using srim, and Monte Carlo simulations using SDTrimSP.
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