A. Mercha, J. M. Rafí, E. Sirnoen, E. Augendre, C. Claeys
{"title":"在0.13 /spl mu/m CMOS技术下的低温寄生导通","authors":"A. Mercha, J. M. Rafí, E. Sirnoen, E. Augendre, C. Claeys","doi":"10.1109/WOLTE.2002.1022451","DOIUrl":null,"url":null,"abstract":"Low temperature measurements at 4.2 K and 77 K are performed on n- and p-MOSFETs of a 0.13 μm CMOS technology. Two parasitic current contributions are identified in the subthreshold regime and strong inversion at 4.2 K. The first one is related to a parasitic parallel conduction inherent to Shallow Trench Isolation. Whereas the second one, resulting in a second peak in the linear transconductance, is discussed in terms of a stronger impact of substrate majority carriers due to a higher substrate resistivity at 4.2K. The measured substrate current in n-MOSFETs is probably originating from electrons tunneling from the substrate valence band to the gate. At 4.2 K, the substrate current induces a reduction of the threshold voltage resulting in the measured kink of the b(V G ) characteristic and the second transconductance peak at low drain bias.","PeriodicalId":338080,"journal":{"name":"Proceedings of the 5th European Workshop on Low Temperature Electronics","volume":"70 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2002-11-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"7","resultStr":"{\"title\":\"Parasitic conduction in a 0.13 /spl mu/m CMOS technology at low temperature\",\"authors\":\"A. Mercha, J. M. Rafí, E. Sirnoen, E. Augendre, C. Claeys\",\"doi\":\"10.1109/WOLTE.2002.1022451\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Low temperature measurements at 4.2 K and 77 K are performed on n- and p-MOSFETs of a 0.13 μm CMOS technology. Two parasitic current contributions are identified in the subthreshold regime and strong inversion at 4.2 K. The first one is related to a parasitic parallel conduction inherent to Shallow Trench Isolation. Whereas the second one, resulting in a second peak in the linear transconductance, is discussed in terms of a stronger impact of substrate majority carriers due to a higher substrate resistivity at 4.2K. The measured substrate current in n-MOSFETs is probably originating from electrons tunneling from the substrate valence band to the gate. At 4.2 K, the substrate current induces a reduction of the threshold voltage resulting in the measured kink of the b(V G ) characteristic and the second transconductance peak at low drain bias.\",\"PeriodicalId\":338080,\"journal\":{\"name\":\"Proceedings of the 5th European Workshop on Low Temperature Electronics\",\"volume\":\"70 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2002-11-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"7\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of the 5th European Workshop on Low Temperature Electronics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/WOLTE.2002.1022451\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the 5th European Workshop on Low Temperature Electronics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/WOLTE.2002.1022451","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Parasitic conduction in a 0.13 /spl mu/m CMOS technology at low temperature
Low temperature measurements at 4.2 K and 77 K are performed on n- and p-MOSFETs of a 0.13 μm CMOS technology. Two parasitic current contributions are identified in the subthreshold regime and strong inversion at 4.2 K. The first one is related to a parasitic parallel conduction inherent to Shallow Trench Isolation. Whereas the second one, resulting in a second peak in the linear transconductance, is discussed in terms of a stronger impact of substrate majority carriers due to a higher substrate resistivity at 4.2K. The measured substrate current in n-MOSFETs is probably originating from electrons tunneling from the substrate valence band to the gate. At 4.2 K, the substrate current induces a reduction of the threshold voltage resulting in the measured kink of the b(V G ) characteristic and the second transconductance peak at low drain bias.