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"NBTI"

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"NBTI"

Comparative Analysis of Channel Length Dependence of NBTI and CHC Characteristics in PMOSFETs
Jae Nam Yu, Sung Kyu Kwon, Jong Kwan Shin, Sun Ho Oh, Sung Yong Jang, Hyung Sub Song, Ga Won Lee, Hi Deok Lee
J Korean Inst Electr Electron Mater Eng 2014;27(7):438-442.   Published online July 1, 2014
DOI: https://doi.org/10.4313/JKEM.2014.27.7.438
Channel length dependence of NBTI (negative bias temperature instablilty) and CHC (channel hot carrier) characteristics in PMOSFET is studied. It has been considered that HC lifetime of PMOSFET is larger than NBTI lifetime. However, it is shown that CHC degradation is greater than NBTI degradation for PMOSFET with short channel length. 1/f noise and charge pumping measurement are used for analysis of these degradations.
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Effect of SiO2 Buffer Layer Thickness on the Device Reliability of the Amorphous InGaZnO Pseudo-MOS Field Effect Transistor
Se Won Lee, Yeong Hyeon Hwang, Won Ju Cho
J Korean Inst Electr Electron Mater Eng 2012;25(1):24-28.   Published online January 1, 2012
DOI: https://doi.org/10.4313/JKEM.2012.25.1.24
In this study, we fabricated an amorphous InGaZnO pseudo-MOS transistor (a-IGZO Ψ -MOSFET) with a stacked Si3N4/SiO2 (NO) gate dielectric and evaluated reliability of the devices with various thicknesses of a SiO2 buffer layer. The roles of a SiO2 buffer layer are improving the interface states and preventing degradation caused by the injection of photo-created holes because of a small valance band offset of amorphous IGZO and Si3N4. Meanwhile, excellent electrical properties were obtained for a device with 10-nm-thick SiO2 buffer layer of a NO stacked dielectric. The threshold voltage shift of a device, however, was drastically increased because of its thin SiO2 buffer layer which highlighted bias and light-induced hole trapping into the Si3N4 layer. As a results, the pseudo-MOS transistor with a 20-nm-thick SiO2 buffer layer exhibited improved electrical characteristics and device reliability; field effective mobility(μFE) of 12.3 cm2/V·s, subthreshold slope (SS) of 148 mV/dec, trap density (Nt) of 4.52× 1011 cm-2, negative bias illumination stress (NBIS) ΔVth of 1.23 V, and negative bias temperature illumination stress (NBTIS) ΔVth of 2.06 V.
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Dependency of the Device Characteristics on Plasma Nitrided Oxide for Nano-scale PMOSFET
J Korean Inst Electr Electron Mater Eng 2007;20(7):569-574.   Published online July 1, 2007
DOI: https://doi.org/10.4313/JKEM.2007.20.7.569
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Improvement of Negative Bias Temperature Instability by Decoupled Plasma Nitridation Process
J Korean Inst Electr Electron Mater Eng 2005;18(10):883-890.   Published online October 1, 2005
DOI: https://doi.org/10.4313/JKEM.2005.18.10.883
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Impact of Post Gate Oxidation Anneal on Negatlve Bias Temperature Instability of Deep Submicron PMOSFETs
Young Min Kim
J Korean Inst Electr Electron Mater Eng 2003;16(3):181-185.   Published online March 1, 2003
DOI: https://doi.org/10.4313/JKEM.2003.16.3.181
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