{"title":"二氧化硅中的电荷储存和电荷衰减","authors":"P. Gunther, G. Sessler","doi":"10.1109/CEIDP.1988.26335","DOIUrl":null,"url":null,"abstract":"SiO/sub 2/ layers with thicknesses between 150 nm and 2.5 mu m were either thermally grown or made by chemical vapour deposition on 2-inch p-type silicon wafers. Positive or negative charging of the samples was performed by liquid-contact, corona, and electron-beam methods. The decay of the surface potential was observed isothermally at room temperature and at 350 degrees C or by a thermally stimulated discharge (TSD) method at linearly increasing temperature. In the isothermal measurements, positively charged samples showed a somewhat faster decay than negatively charged ones. The decays can be interpreted with a simple theory based on carrier drift and compensation by conductivity. TSD peaks of negatively charged material occur at temperatures higher than those of positively charged samples. Activation energies of 1.0 and 1.4 eV for positively charged oxides and 1.9 eV for negatively charged oxides were found.<<ETX>>","PeriodicalId":149735,"journal":{"name":"1988. Annual Report., Conference on Electrical Insulation and Dielectric Phenomena","volume":"28 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1988-10-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Charge storage and charge decay in silicon dioxide\",\"authors\":\"P. Gunther, G. Sessler\",\"doi\":\"10.1109/CEIDP.1988.26335\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"SiO/sub 2/ layers with thicknesses between 150 nm and 2.5 mu m were either thermally grown or made by chemical vapour deposition on 2-inch p-type silicon wafers. Positive or negative charging of the samples was performed by liquid-contact, corona, and electron-beam methods. The decay of the surface potential was observed isothermally at room temperature and at 350 degrees C or by a thermally stimulated discharge (TSD) method at linearly increasing temperature. In the isothermal measurements, positively charged samples showed a somewhat faster decay than negatively charged ones. The decays can be interpreted with a simple theory based on carrier drift and compensation by conductivity. TSD peaks of negatively charged material occur at temperatures higher than those of positively charged samples. Activation energies of 1.0 and 1.4 eV for positively charged oxides and 1.9 eV for negatively charged oxides were found.<<ETX>>\",\"PeriodicalId\":149735,\"journal\":{\"name\":\"1988. Annual Report., Conference on Electrical Insulation and Dielectric Phenomena\",\"volume\":\"28 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1988-10-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"1988. Annual Report., Conference on Electrical Insulation and Dielectric Phenomena\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CEIDP.1988.26335\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"1988. Annual Report., Conference on Electrical Insulation and Dielectric Phenomena","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CEIDP.1988.26335","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Charge storage and charge decay in silicon dioxide
SiO/sub 2/ layers with thicknesses between 150 nm and 2.5 mu m were either thermally grown or made by chemical vapour deposition on 2-inch p-type silicon wafers. Positive or negative charging of the samples was performed by liquid-contact, corona, and electron-beam methods. The decay of the surface potential was observed isothermally at room temperature and at 350 degrees C or by a thermally stimulated discharge (TSD) method at linearly increasing temperature. In the isothermal measurements, positively charged samples showed a somewhat faster decay than negatively charged ones. The decays can be interpreted with a simple theory based on carrier drift and compensation by conductivity. TSD peaks of negatively charged material occur at temperatures higher than those of positively charged samples. Activation energies of 1.0 and 1.4 eV for positively charged oxides and 1.9 eV for negatively charged oxides were found.<>