| 磁控溅射碲镉汞表面钝化模拟研究 |
| 投稿时间：2024-09-23 修订日期：2024-10-09 点此下载全文 |
| 引用本文：高志富,王文,李树杰,耿松,何胤,桂希欢,左大凡,李雄军.磁控溅射碲镉汞表面钝化模拟研究[J].红外,2025,46(2):13~19 |
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| 中文摘要:碲镉汞(HgCdTe)表面钝化层的化学计量比对器件性能具有至关重要的影响。通过SRIM软件模拟了Ar+溅射能量和入射角度对表面钝化层化学计量比的影响。模拟结果表明，在300~500 eV能量范围内，CdTe和ZnS对Ar+的核阻止本领远大于电子阻止本领，且ZnS的核阻止本领优于CdTe；离子入射角在60°附近时CdTe有最大溅射产额，入射角在70°附近时ZnS有最大溅射产额；溅射过程中存在择优溅射现象，Cd、Zn元素为择优溅射元素。基于模拟结果，长波碲镉汞表面钝化层的质量得到明显改善。该方法建立了钝化层计量比与溅射能量、入射角度之间的关系，为实际工艺过程提供了指导方向。这对于高性能碲镉汞红外探测器的研制具有一定的实际意义。 |
| 中文关键词:磁控溅射 阻止本领 表面钝化 溅射产额 择优溅射 |
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| Simulation Study on the Surface Passivation of HgCdTe by Magnetron Sputtering |
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| Abstract:The stoichiometric ratio of the surface passivation layer of mercury cadmium telluride (HgCdTe) has a crucial influence on the device performance. The influence of Ar+ sputtering energy and incident angle on the stoichiometric ratio of the surface passivation layer is simulated by SRIM software. The simulation results show that in the energy range of 300－500 eV, the nuclear stopping power of CdTe and ZnS for Ar+ is much greater than the electron stopping power, and the nuclear stopping power of ZnS is better than that of CdTe; the maximum sputtering yield of CdTe is found near the ion incident angle of 60°, and the maximum sputtering yield of ZnS is found near the incident angle of 70°; there is a preferential sputtering phenomenon in the sputtering process, and Cd and Zn elements are the preferential sputtering elements. Based on the simulation results, the quality of the passivation layer on the long-wave HgCdTe surface is significantly improved. This method establishes the relationship between the stoichiometric ratio of the passivation layer and the sputtering energy as well as the incident angle, which provides a guiding direction for the actual process. This has certain practical significance for the development of high-performance HgCdTe infrared detectors. |
| keywords:magnetron sputtering stopping power surface passivation sputtering yield preferential sputtering |
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