Surface potential distribution of resist exposed by electron beam and the non-charging exposure conditions.

Masatoshi Kotera, Yoshinobu Kono
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Abstract

In this study, we experimentally analyzed the charging phenomenon when an insulating resist film on a conductive layer formed on bulk glass is irradiated by electron beams (EBs). To quantify the charging potential induced, an electrostatic force microscope device was installed in the scanning electron microscope sample chamber, and potential distributions formed under various exposure conditions were obtained. Based on the results obtained, a model for charge accumulation within the sample, explaining positive and negative charging and their transitions, was developed. At an EB acceleration voltage of 30 kV, the following observations were made: 'global charging' could be avoided by applying -5 V to the sample. Regarding 'local charging' near the exposure area of the EB, at low exposure doses, emission of secondary electrons from the sample surface induced positive charging, while the accumulation of incident electrons within the sample induced negative charging. At exposure doses where the effects of both are balanced, the sample exhibited zero potential, revealing the appearance of the 'first zero-cross exposure dose'. At higher exposure doses, the sample transitions from negative to positive as the exposure dose increases due to the electron-beam-induced conduction, resulting in the so-called second zero-cross exposure dose. The exposure dose dependence of the charging potential distribution at various acceleration voltages was obtained. In particular, we found that at an acceleration voltage of 0.6 kV, the sample surface is not charged even when exposed to small to very large doses of EBs.

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电子束和非充电曝光条件下光刻胶的表面电位分布。
在这项研究中,我们通过实验分析了在大块玻璃上形成的导电层上的绝缘抗蚀膜在电子束照射下的充电现象。为了量化引起的充电电势,我们在扫描电子显微镜样品室中安装了静电力显微镜装置,并获得了在不同照射条件下形成的电势分布。根据所获得的结果,建立了样品内部的电荷积累模型,解释了正负电荷及其转换。在 30 千伏的电子束加速电压下,得出了以下结论:对样品施加 -5V 电压可避免 "整体充电"。至于电子束照射区域附近的 "局部充电",在低照射剂量下,样品表面发射的二次电子会引起正充电,而入射电子在样品内部的积累则会引起负充电。在两者影响平衡的曝光剂量下,样品显示出零电位,出现了 "第一个零交叉曝光剂量"。在较高的曝光剂量下,由于电子束诱导传导,随着曝光剂量的增加,样品会从负电位转变为正电位,这就是所谓的 "第二次零交叉曝光剂量"。我们获得了不同加速电压下充电电势分布的曝光剂量依赖性。我们特别发现,在加速电压为0.6千伏时,即使暴露在小剂量到超大剂量的电子束中,样品表面也不会带电。
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