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作 者:陶芬芬 杨红 唐波 唐兆云 徐烨锋 许静 王卿璞 闫江
机构地区:[1]School of Physics,Shandong University [2]Key Laboratory of Microelectronics Devices and Integrated Technology,Institute of Microelectronics,Chinese Academy of Sciences
出 处:《Journal of Semiconductors》2014年第6期32-37,共6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 of China(No.61306129);the National Found for Fostering Talents of Basic Science(No.J0730318)
摘 要:The characteristics of TDDB (time-dependent dielectric breakdown) and SILC (stress-induced leakage current) for an ultra-thin SiO2/HfO2 gate dielectric stack are studied. The EOT (equivalent-oxide-thickness) of the gate stack (Si/SiO2/HfOz/TiN/TiA1/TiN/W) is 0.91 am. The field acceleration factor extracted in TDDB experi- ments is 1.59 s.cm/MV, and the maximum voltage is 1.06 V when the devices operate at 125 ℃ for ten years. A detailed study on the defect generation mechanism induced by SILC is presented to deeply understand the break- down behavior. The trap energy levels can be calculated by the SILC peaks: one S1LC peak is most likely to be caused by the neutral oxygen vacancy in the HfO2 bulk layer at 0.51 eV below the Si conduction band minimum; another SILC peak is induced by the interface traps, which are aligned with the silicon conduction band edge. Fur- thermore, the great difference between the two SILC peaks demonstrates that the degeneration of the high-k layer dominates the breakdown behavior of the extremely thin gate dielectric.The characteristics of TDDB (time-dependent dielectric breakdown) and SILC (stress-induced leakage current) for an ultra-thin SiO2/HfO2 gate dielectric stack are studied. The EOT (equivalent-oxide-thickness) of the gate stack (Si/SiO2/HfOz/TiN/TiA1/TiN/W) is 0.91 am. The field acceleration factor extracted in TDDB experi- ments is 1.59 s.cm/MV, and the maximum voltage is 1.06 V when the devices operate at 125 ℃ for ten years. A detailed study on the defect generation mechanism induced by SILC is presented to deeply understand the break- down behavior. The trap energy levels can be calculated by the SILC peaks: one S1LC peak is most likely to be caused by the neutral oxygen vacancy in the HfO2 bulk layer at 0.51 eV below the Si conduction band minimum; another SILC peak is induced by the interface traps, which are aligned with the silicon conduction band edge. Fur- thermore, the great difference between the two SILC peaks demonstrates that the degeneration of the high-k layer dominates the breakdown behavior of the extremely thin gate dielectric.
关 键 词:HFO2 TDDB SILC bulk trap interface trap
分 类 号:TN386[电子电信—物理电子学]
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