2022 IEEE International Symposium on Circuits and Systems (ISCAS) 2022
DOI: 10.1109/iscas48785.2022.9937652
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Characterization of Single Event Upsets of Nanoscale FDSOI Circuits Based on the Simulation and Irradiation Results

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Cited by 5 publications
(3 citation statements)
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“…Micromachines 2023, 14, x FOR PEER REVIEW 7 of 14 Therefore, the RHB-12T-hardened cell has the ability of single-node Q (or QN), S0, S1, and double-node {S0, S1} to upset and recover and can completely suppress SNU and partially tolerate DNU response. The research shows that the charge-sharing effect between two NMOS (or PMOS-NMOS) occurs at 1.62 µm (or 0.6 µm) [28,29]. The physical distance between node Q and nodes S0 and S1 is reasonably designed on the layout to effectively reduce the influence of the charge-sharing effect.…”
Section: Seu Recovery Analysismentioning
confidence: 99%
“…Micromachines 2023, 14, x FOR PEER REVIEW 7 of 14 Therefore, the RHB-12T-hardened cell has the ability of single-node Q (or QN), S0, S1, and double-node {S0, S1} to upset and recover and can completely suppress SNU and partially tolerate DNU response. The research shows that the charge-sharing effect between two NMOS (or PMOS-NMOS) occurs at 1.62 µm (or 0.6 µm) [28,29]. The physical distance between node Q and nodes S0 and S1 is reasonably designed on the layout to effectively reduce the influence of the charge-sharing effect.…”
Section: Seu Recovery Analysismentioning
confidence: 99%
“…Consequently, the use of tools that allow designers to locate sensitive nodes and harden circuits before radiation tests is an interesting approach to increase the robustness of electronics for harsh-radiation environments. Whereas there are exhaustive analyses of charge sharing employing 3D simulation tools such as TCAD [16] or from a more physical perspective [17], this paper focuses on a complementary approach that optimizes the time required to find vulnerabilities against radiation in designed circuits. The proposed methodology is based on a tool, called AFTU [18], which uses electrical models to emulate particle impacts with a certain level of charge, allowing fast analyses based on transient simulations to provide RHbD circuits [19,20].…”
Section: Jinst 18 P10023mentioning
confidence: 99%
“…However, for the top silicon layer, the electrons and holes generated by the incident device can move through the shared active region, enabling charge sharing. Furthermore, experimental results [ 18 ] also demonstrate the existence of charge-sharing effects in FDSOI SRAM. This indicates that the decrease in the LET upset threshold observed in device level simulations of SRAM is a result of the combined effects of charge sharing and bipolar amplification.…”
Section: Sram Device Level See Simulationmentioning
confidence: 99%