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Recovery behavior in negative bias temperature instability

机译:负偏压温度不稳定性下的恢复行为

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摘要

The recovery mechanism observed in oxynitride gate pMOSFETs after negative bias temperature (NBT) stresses is reviewed. The recovery can be divided into two elements, fast recoverable- and permanent components (R and P). An interesting features, universality, observed in R was examined. In addition, the validity of the empirical equation previously proposed for the universality was confirmed from the perspective of the recovery activation energy distribution or R. Moreover, the origin of the defects responsible for recovery were investigated. R can be due to the annihilation of E′-centers (X_3=Si~++Si=O_3, where. denotes a dangling bond and X is oxygen or nitrogen). During a recovery period, the trapped holes are emitted from E′-centers, resulting in R. The hole emission begins immediately after NBT stresses because the emission energy is shallow. Therefore, the fast recovery, i.e.. R is observed. On the other hand, several defects, interface states (D_(it)), fixed positive charges (D_(pc)), K-centers (N_3=Si) and E′-centers were involved in P. When NBT stresses were light, only D_(it) and D_(pc) were observed. The experimental data support a model where hydrogen emitted from interfacial Si-H bonds by NBT the stresses reacts with adjacent Si-X-Si network in the SiON gate insulator, which leaves silicon dangling bonds (Si_3=Si~- called P_b-centers), i.e., D_(it), and forms the generation of Si-X~+H-Si (overcoordinated oxygen or nitrogen, i.e., D_(pc)), Heavy NBT stresses generated additional defects, K- andE′-centers, which also act as D_(it) and D_(pc). Moreover, these K- and E′-centers that were formed through the breaking of Si-X bonds caused stress induced leakage current. Because the annihilation of P-related defects, D_(it), D_(pc), K-cen-ter and E′-center, requires very high temperature, P behaves as the permanent component under conventional NBT experimental temperature conditions. We reviewed these results and a model for the generation and recovery behaviors of defects.
机译:审查了在负偏置温度(NBT)应力之后在氮氧化物栅极pMOSFET中观察到的恢复机制。恢复可以分为两个部分,快速恢复组件和永久组件(R和P)。研究了在R中观察到的一个有趣的特性,即通用性。此外,从恢复活化能分布或R的角度证实了先前提出的经验性方程的有效性。此外,还研究了造成恢复的缺陷的根源。 R可能是由于E'中心的the灭(X_3 = Si〜++ Si = O_3,其中。表示悬空键,X为氧或氮)。在恢复期间,被困的空穴从E'中心发射,产生R。空穴发射在NBT应力之后立即开始,因为发射能量很浅。因此,观察到快速恢复,即R。另一方面,P中涉及一些缺陷,界面状态(D_(it)),固定正电荷(D_(pc)),K中心(N_3 = Si)和E'中心。当NBT应力较小时,仅观察到D_(it)和D_(pc)。实验数据支持一个模型,其中应力通过NBT从界面Si-H键释放的氢与SiON栅极绝缘体中的相邻Si-X-Si网络反应,从而留下硅悬空键(Si_3 = Si〜-称为P_b-中心) ,即D_(it),并形成Si-X〜+ H-Si(氧或氮的配位过高,即D_(pc)),重NBT应力产生了其他缺陷,即K-和E'-中心。还充当D_(it)和D_(pc)。此外,这些通过Si-X键断裂形成的K和E'中心会引起应力感应的漏电流。因为the灭与P有关的缺陷D_(it),D_(pc),K-中心和E'-center需要非常高的温度,所以P在常规NBT实验温度条件下充当永久成分。我们回顾了这些结果以及缺陷生成和恢复行为的模型。

著录项

  • 来源
    《Microelectronics & Reliability》 |2014年第3期|520-528|共9页
  • 作者

    Yoshiki Yonamoto;

  • 作者单位

    Yokohama Research Laboratory, Hitachi Ltd., Yokohama, Kanagawa 244-0817, Japan;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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