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作 者:任尚清 杨红 唐波 徐昊 罗维春 唐兆云 徐烨锋 许静 王大海 李俊峰 闫江 赵超 陈大鹏 叶甜春 王文武
出 处:《Journal of Semiconductors》2015年第1期86-89,共4页半导体学报(英文版)
基 金:Project supported by the Important National Science&Technology Specific Projects(No.2009ZX02035);the National Natural Science Foundation of China(Nos.61176091,61306129)
摘 要:Positive bias temperature instability(PBTI) characteristics and degradation mechanisms of NMOSFET with high-k/metal gate last process have been systematically investigated. The time evolution of threshold voltage shift during PBTI stress still follows a power law. However, the exponent n decreases from 0.26 to 0.16 linearly as the gate stress voltage increases from 0.6 to 1.2 V. There is no interface state generation during stress because of the negligible sub-threshold swing change. Moreover, the activation energy is 0.1 e V, which implies that electrons directly tunnel into high-k bulk and are trapped by pre-existing traps resulting into PBTI degradation. During recovery the threshold voltage shift is linear in lgt, and a mathematical model is proposed to express threshold voltage shift.Positive bias temperature instability(PBTI) characteristics and degradation mechanisms of NMOSFET with high-k/metal gate last process have been systematically investigated. The time evolution of threshold voltage shift during PBTI stress still follows a power law. However, the exponent n decreases from 0.26 to 0.16 linearly as the gate stress voltage increases from 0.6 to 1.2 V. There is no interface state generation during stress because of the negligible sub-threshold swing change. Moreover, the activation energy is 0.1 e V, which implies that electrons directly tunnel into high-k bulk and are trapped by pre-existing traps resulting into PBTI degradation. During recovery the threshold voltage shift is linear in lgt, and a mathematical model is proposed to express threshold voltage shift.
关 键 词:positive bias temperature instability(PBTI) high-k metal gate
分 类 号:TN386[电子电信—物理电子学]
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