首页> 外文期刊>Electron Device Letters, IEEE >Improved NBTI Reliability With Sub-1-Nanometer EOT ${rm ZrO}_{2}$ Gate Dielectric Compared With ${rm HfO}_{2}$
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Improved NBTI Reliability With Sub-1-Nanometer EOT ${rm ZrO}_{2}$ Gate Dielectric Compared With ${rm HfO}_{2}$

机译:低于1纳米EOT的NBTI可靠性得到提高 $ {rm ZrO} _ {2} $ 相比,栅电介质Formulatype =“ inline”> $ {rm HfO} _ {2} $

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The negative bias temperature instability (NBTI) reliability of sub-1-nanometer equivalent oxide thickness (EOT) ${rm ZrO}_{2}$ and ${rm HfO}_{2}$ dielectrics with metal gate is investigated. The threshold voltage shift $(Delta{V}_{rm TH})$ at identical NBTI over-drive stress conditions is observed to be lower in ${rm ZrO}_{2}$ than in ${rm HfO}_{2}$ field-effect transistors. Ring oscillator charge pumping is applied to determine interface trap generation $(Delta{N}_{rm it})$ in the sub-1-nanometer EOT devices, with ${rm ZrO}_{2}$ devices showing about one order of magnitude lower $Delta{N}_{rm it}$ than ${rm HfO}_{2}$ device. However, the $Delta{N}_{rm it}$ contribution to the total $Delta{V}_{rm TH}$ is very limited in sub-1-nanometer EOT devices, as the recoverable component from the pre-existing bulk defects dominates the whole NBTI degradation. Pulsed Id–Vg technique is applied to analyze the pre-existing bulk defects in those sub-1-nanometer EOT devices, and lower pre-existing bulk defect density is shown in ${rm ZrO}_{2}$, which decisively reduces NBTI in ${rm ZrO}_{2}$ gate dielectric.
机译:小于1纳米等效氧化物厚度(EOT)的负偏压温度不稳定性(NBTI)可靠性<分子式> =“ inline”> $ {rm ZrO} _ {2} $ $ {rm HfO} _ {2} $ 电介质。在相同的NBTI过驱动应力条件下,阈值电压偏移<公式公式类型=“ inline”> $(Delta {V} _ {rm TH})$ 为在 $ {rm ZrO} _ {2} $ 中观察到比在 < tex Notation =“ TeX”> $ {rm HfO} _ {2} $ 场效应晶体管。应用环形振荡器电荷泵来确定接口陷阱的生成 $(Delta {N} _ {rm it})$ 1纳米以下EOT设备,其中 $ {rm ZrO} _ {2} $ 设备显示大约一个数量级与 $ Delta {N} _ {rm it} $ TeX“> $ {rm HfO} _ {2} $ 设备。但是, $ Delta {N} _ {rm it} $ 对总的贡献在低于1纳米的EOT设备中, $ Delta {V} _ {rm TH} $ 的限制非常有限,因为它可以从先前存在的大量缺陷中恢复。在整个NBTI降级中占主导地位。脉冲Id–Vg技术用于分析那些在小于1纳米的EOT设备中预先存在的体缺陷,并且较低的预先存在的体缺陷密度显示在<公式Formulatype =“ inline”> $ {rm ZrO} _ {2} $ ,它在 $ {rm ZrO} _ {2 } $ 栅极电介质。

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