介质隔离采用浅层氧化物和多晶硅

J. Raffel, S. Bernacki
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引用次数: 2

摘要

先前对多晶隔离的研究由于扩散增强而限制了密度,这就排除了壁状发射器的几何形状。氧化物隔离方案在深度上受到限制,这是由于在光刻定义中氧化凸起和由此产生的降解而造成的平面度损失。开发了一种集电极的多晶隔离和碱基的浅氧化物隔离相结合的技术。这种方法能够提供深介电隔离,表面平面化和高密度的壁射极几何形状,这是迄今为止任何其他方法无法获得的组合。该隔离方案已用于制造ECL栅链。晶体管位于2.5微米厚的n-epi岛上,周围是5 × 105ω -cm的多晶硅,用氮化硅掩蔽选择性氧化至1微米厚。氮化物掩膜处的氧化物凸点通常为3000 Å,聚层台阶高度小至2600 Å。该电路具有多晶硅电阻,并采用热扩散和离子注入制备。这些电路的速度-功率乘积大约是结隔离电路的一半。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Dielectric isolation using shallow oxide and polycrystalline silicon
Previous work with polycrystalline isolation was limited in density by enhanced diffusion which precluded walled emitter geometries. Oxide isolation schemes are limited in depth by loss of planarity due to oxide bumps and resultant degradation in photolithographic definitions. A technique has been developed which combines polycrystalline isolation of collectors and shallow oxide isolation of bases. This approach is capable of proriding deep dielectric isolation, surface planarity and the high density of walled emitter geometries, a combination heretofore unobtainable by any other means. This isolation scheme has been used to fabricate ECL gate chains. The transistors were located in 2.5 micron thick n-epi islands surrounded by 5 × 105ohm-cm polysilicon selectively oxidized with silicon nitride masking to a thickness of one micron. The oxide bump at the nitride mask was typically 3000 Å and the epipoly step height was as small as 2600 Å. The circuits have polysilicon resistors and were fabricated using both thermal diffusion and ion implantation. The speed-power product of these circuits was approximately one-half that of junction isolated circuits.
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