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首页> 外文期刊>Physica, B. Condensed Matter >Thermal evolution of surface blistering, exfoliation due to ion-implanted hydrogen monomers into Si〈1 1 1〉
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Thermal evolution of surface blistering, exfoliation due to ion-implanted hydrogen monomers into Si〈1 1 1〉

机译:离子注入的氢单体进入Si 〈1 1 1〉引起的表面起泡,剥落的热演化

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摘要

This study investigated the dependence of surface blistering and exfoliation phenomena on post-annealing time in H-implanted Si〈1 1 1〉. Czochralski-grown n-type Si〈1 1 1〉 wafers were room-temperature ion-implanted with 40 keV hydrogen monomers to a fluence of 5×10 ~(16) cm ~(-2), and followed by furnace annealing treatments at 400 and 500 °C for various durations ranging from 0.25 to 3 h. The corresponding analysis results for Si〈1 0 0〉 [1] (Liang et al., 2008); [2] (Bai, 2007) were adopted in order to make comparisons. The evolution of blister formation and growth for Si〈1 1 1〉 at 400 °C has a shorter characteristic time compared to Si〈1 0 0〉. However, there is a longer characteristic time when annealing takes place at 500 °C. In addition, no craters were observed for Si〈1 1 1〉 annealed at 400 °C while the opposite is true for Si〈1 0 0〉. The evolution of crater development for Si〈1 1 1〉 annealed at 500 °C has a longer characteristic time compared to Si〈1 0 0〉. These results are attributed to the fact that compared to Si〈1 0 0〉, Si〈1 1 1〉 has a smaller surface binding energy of silicon atoms and a larger areal number density of silicon atoms on the plane perpendicular to the incident-ion axis. Furthermore, Si〈1 1 1〉 has a greater areal number density, smaller diameter, and a similar covered-area fraction of optically-detectable blisters compared to Si〈1 0 0〉. However, Si〈1 1 1〉 has a lower areal number density and a smaller covered-area fraction of craters than does Si〈1 0 0〉. Increasing post-annealing temperature from low (e.g. 400 °C) to high (e.g. 500 °C) revealed that Si〈1 1 1〉 tends to create more blisters while Si〈1 0 0〉 tends to develop larger blisters as well as create more craters.
机译:本研究研究了注入H的Si <1 1 1>中表面起泡和剥落现象对退火后时间的依赖性。将Czochralski生长的n型Si <1 1 1>晶片室温离子注入40 keV氢单体,注量为5×10〜(16)cm〜(-2),然后在110℃下进行炉退火处理。 400和500°C,持续时间从0.25到3 h。 Si <1 0 0> [1]的相应分析结果(Liang等,2008); [2](Bai,2007)被采用以进行比较。与Si <1 0 0>相比,Si <1 1 1>在400°C的水疱形成和生长演变具有较短的特征时间。但是,在500°C下进行退火时,特征时间较长。另外,在400℃下退火的Si 〈1 1 1〉没有观察到缩孔,而Si 〈1 0 0〉则相反。与Si <1 0 0>相比,在500°C退火的Si <1 1 1>的弹坑发展演变具有更长的特征时间。这些结果归因于以下事实:与Si 〈1 0 0〉相比,Si 〈1 1 1〉在垂直于入射离子的平面上具有较小的硅原子表面结合能和较大的硅原子面数密度。轴。此外,与Si <1 0 0>相比,Si <1 1 1>具有更大的面数密度,更小的直径以及相似的光学可检测水泡覆盖面积分数。然而,与Si <1 0 0>相比,Si <1 1 1>具有更低的面数密度和更小的凹坑覆盖面积分数。将退火后的温度从低(例如400°C)增加到高(例如500°C)表明Si <1 1 1>倾向于产生更多的水泡,而Si <1 0 0>倾向于形成更大的水泡并产生更多的火山口。

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