Pub Date : 2024-06-28DOI: 10.1109/tdmr.2024.3420759
G.C. Lyu, X.P. Zhang, M.B. Zhou, C.B. Ke, Y.W. Mai
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Pub Date : 2024-06-28DOI: 10.1109/TDMR.2024.3420391
Chonghao Chen;Jiang Xu;Zhuojun Chen
Lateral diffused metal-oxide-semiconductor (LDMOS) devices are vulnerable to single-event burnout (SEB) in radiation environments, potentially leading to catastrophic failure in high-voltage integrated circuits (HVICs). Pulsed-laser experiments have demonstrated that the SEB triggering voltage of n-type LDMOS (nLDMOS) is significantly lower than that of p-type LDMOS (pLDMOS), which limits the applications of complementary LDMOS devices in aerospace electronic systems. This work investigates the SEB mechanism in both nLDMOS and pLDMOS through technology computer-aided design (TCAD) simulations. The analysis reveals that differences in the current gain of parasitic bipolar transistors and well resistance between pLDMOS and nLDMOS result in varying SEB triggering voltages. Additionally, a radiation-hardening technique is employed to improve the SEB triggering voltage of nLDMOS, aligning it closely with that of pLDMOS. This research provides insight into the design of radiation-hardened high-voltage integrated circuits, such as DC-DC converters and motor drivers, using a standard Bipolar-CMOS-DMOS (BCD) fabrication process.
{"title":"Single-Event Burnout Effects of Complementary LDMOS Devices in High-Voltage Integrated Circuits","authors":"Chonghao Chen;Jiang Xu;Zhuojun Chen","doi":"10.1109/TDMR.2024.3420391","DOIUrl":"10.1109/TDMR.2024.3420391","url":null,"abstract":"Lateral diffused metal-oxide-semiconductor (LDMOS) devices are vulnerable to single-event burnout (SEB) in radiation environments, potentially leading to catastrophic failure in high-voltage integrated circuits (HVICs). Pulsed-laser experiments have demonstrated that the SEB triggering voltage of n-type LDMOS (nLDMOS) is significantly lower than that of p-type LDMOS (pLDMOS), which limits the applications of complementary LDMOS devices in aerospace electronic systems. This work investigates the SEB mechanism in both nLDMOS and pLDMOS through technology computer-aided design (TCAD) simulations. The analysis reveals that differences in the current gain of parasitic bipolar transistors and well resistance between pLDMOS and nLDMOS result in varying SEB triggering voltages. Additionally, a radiation-hardening technique is employed to improve the SEB triggering voltage of nLDMOS, aligning it closely with that of pLDMOS. This research provides insight into the design of radiation-hardened high-voltage integrated circuits, such as DC-DC converters and motor drivers, using a standard Bipolar-CMOS-DMOS (BCD) fabrication process.","PeriodicalId":448,"journal":{"name":"IEEE Transactions on Device and Materials Reliability","volume":"24 3","pages":"401-406"},"PeriodicalIF":2.5,"publicationDate":"2024-06-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141506378","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The node upset may occur in the memory cell if the charged particle from cosmos rays or packaging materials strikes the integrated circuit. Radiation-hardened-by-design (RHBD) techniques introduce redundant transistors in the SRAM cell to improve its ability of recovering from the undesired node upset. However, the extra redundant transistors may increase the number of sensitive nodes in the SRAM cell, which decreases its capability of node-upset tolerance in turn. This work proposes an RHBD 14T SRAM cell and an RHBD 16T SRAM cell. Both the proposed SRAM cells only have two sensitive nodes. The proposed SRAM cells are able to recover from all the SNU cases. The layout harden technique is used to protect the proposed cells from SEMNU, and the blank of the hardened layout is reused so the proposed 14T and 16T SRAM cells consume the same area. Although the proposed cells have more transistors, the hardened layout areas of NS-10T/ PS-10T/ RHD-12T/ RHBD-10T/ RHBD-10T[VLSI]/ QUCCE-12T are respectively $1.78times $