1. 中国科学院大学,北京,100049
2. 中国科学院特殊环境功能材料与器件重点实验室
3. 中国科学院新疆理化技术研究所,新疆,乌鲁木齐,830011
4. 新疆电子信息材料与器件重点实验室,新疆,乌鲁木齐,830011
网络出版:2019-05-25,
纸质出版:2019
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席善学, 陆妩, 郑齐文, 等. 体效应对超深亚微米SOI器件总剂量效应的影响[J]. 电子学报, 2019,47(5):1065-1069.
XI Shan-xue, LU Wu, ZHENG Qi-wen, et al. The Impact of Body Effect on TID of Ultra Deep Sub Micron SOI Devices[J]. Acta Electronica Sinica, 2019, 47(5): 1065-1069.
席善学, 陆妩, 郑齐文, 等. 体效应对超深亚微米SOI器件总剂量效应的影响[J]. 电子学报, 2019,47(5):1065-1069. DOI: 10.3969/j.issn.0372-2112.2019.05.013.
XI Shan-xue, LU Wu, ZHENG Qi-wen, et al. The Impact of Body Effect on TID of Ultra Deep Sub Micron SOI Devices[J]. Acta Electronica Sinica, 2019, 47(5): 1065-1069. DOI: 10.3969/j.issn.0372-2112.2019.05.013.
研究体偏置效应对超深亚微米绝缘体上硅(SOI,Silicon-on-insulator)器件总剂量效应的影响.在TG偏置下,辐照130nm PD(部分耗尽,partially depleted)SOI NMOSFET(N型金属-氧化物半导体场效应晶体管,n-type Metal-Oxide-Semiconductor Field-Effect Transistor)器件,监测辐照前后在不同体偏压下器件的电学参数.短沟道器件受到总剂量辐照影响更敏感,且宽长比越大,辐射导致的器件损伤亦更大.在辐射一定剂量后,部分耗尽器件将转变为全耗尽器件,并且可以观察到辐射诱导的耦合效应.对于10m/0.35m的器件,辐照后出现了明显的阈值电压漂移和大的泄漏电流.辐照前体偏压为负时的转移特性曲线相比于体电压为零时发生了正向漂移.当体电压
Vb
=-1.1V时部分耗尽器件变为全耗尽器件,|
Vb
|的继续增加无法导致耗尽区宽度的继续增加,说明体区负偏压已经无法实现耗尽区宽度的调制,因此器件的转移特性曲线也没有出现类似辐照前的正向漂移.
The impact of body effect on the total dose effect of ultra deep sub micron SOI devices is studied.130nm SOI NMOSFET devices were irradiated in TG bias state
the electrical parameters of devices before and after irradiation were monitored under different body bias.The short channel PD SOI NMOS devices are more sensitive to total dose radiation
and the larger channel width to length ratio of devices will cause more damage.After a certain dose of radiation
the partially depleted devices will turn into fully depleted devices
and the radiation-
induced coupling effect can be observed.Significant threshold voltage shifts and large leakage currents can be observed after irradiation of 10 m/0.35 m devices.The transfer characteristic curve at negative body bias is positively shifted compared with it at zero body bias before the device is irradiated.When the body voltage
Vb
=-1.1V
then partially depleted devices become full-depletion devices.And continued increase in|Vb|will not result in continued increase in the width of the depletion area
which shows that the negative body bias can no longer adjust the width of the depletion region
so the transfer characteristic curve of the device does not show a positive shift similar to that before irradiation.
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