D. Ielmini, A.S. Spinellii, A. Lacaita, G. Ghidini
{"title":"Evidence for recombination at oxide defects and new SILC model","authors":"D. Ielmini, A.S. Spinellii, A. Lacaita, G. Ghidini","doi":"10.1109/RELPHY.2000.843891","DOIUrl":null,"url":null,"abstract":"This work presents experimental and computational investigations on the physical mechanisms of SILC. Carrier separation measurements are carried out on MOS samples with oxide thickness 6-8 nm, highlighting the electron and hole contributions to the SILC. We have investigated the relation between these components by means of time-relaxation. It is found that a linear relationship holds between electron SILC and hole SILC, measured at different times after the initial high-field stress. The same linearity has been observed for increasing fluences of injected electrons, at fixed stressing field. A correlation between electron and hole ILC is found also from a comparison between carrier separation data obtained in n/sup +/- and p/sup +/- polysilicon devices. These experimental data entails that hole SILC is due to a recombination current. As a result of these experimental findings, a new model for the SILC is developed. This model is based on trap-assisted tunneling, but also accounts for hole tunneling and includes Shockley-Hall-Read recombination process in the bulk oxide as a new leakage mechanism. Simulations in the oxide thickness range 5.9-8.2 nm show excellent agreement with I-V measurements and carrier-separation data. The resulting defect concentration scales with the oxide thickness, in agreement with published results. The energy distribution of defects responsible for the steady-state leakage is located 0.7-1.3 eV below the Si conduction-band minimum. Capture cross sections of 10/sup -13/ and 10/sup -16/ cm/sup 2/ have been assumed for electrons and holes respectively, compatible with a donor charge state of the SILC-related defect centers. Simulations are finally shown for oxide thickness t/sub 0x/=2.8 nm. The mechanism of recombination in the bulk oxide accounts very well for the observation of low-voltage SILC in ultrathin oxide, showing the effectiveness of the proposed SILC model.","PeriodicalId":6387,"journal":{"name":"2000 IEEE International Reliability Physics Symposium Proceedings. 38th Annual (Cat. No.00CH37059)","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2000-04-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"10","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2000 IEEE International Reliability Physics Symposium Proceedings. 38th Annual (Cat. No.00CH37059)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/RELPHY.2000.843891","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 10
Abstract
This work presents experimental and computational investigations on the physical mechanisms of SILC. Carrier separation measurements are carried out on MOS samples with oxide thickness 6-8 nm, highlighting the electron and hole contributions to the SILC. We have investigated the relation between these components by means of time-relaxation. It is found that a linear relationship holds between electron SILC and hole SILC, measured at different times after the initial high-field stress. The same linearity has been observed for increasing fluences of injected electrons, at fixed stressing field. A correlation between electron and hole ILC is found also from a comparison between carrier separation data obtained in n/sup +/- and p/sup +/- polysilicon devices. These experimental data entails that hole SILC is due to a recombination current. As a result of these experimental findings, a new model for the SILC is developed. This model is based on trap-assisted tunneling, but also accounts for hole tunneling and includes Shockley-Hall-Read recombination process in the bulk oxide as a new leakage mechanism. Simulations in the oxide thickness range 5.9-8.2 nm show excellent agreement with I-V measurements and carrier-separation data. The resulting defect concentration scales with the oxide thickness, in agreement with published results. The energy distribution of defects responsible for the steady-state leakage is located 0.7-1.3 eV below the Si conduction-band minimum. Capture cross sections of 10/sup -13/ and 10/sup -16/ cm/sup 2/ have been assumed for electrons and holes respectively, compatible with a donor charge state of the SILC-related defect centers. Simulations are finally shown for oxide thickness t/sub 0x/=2.8 nm. The mechanism of recombination in the bulk oxide accounts very well for the observation of low-voltage SILC in ultrathin oxide, showing the effectiveness of the proposed SILC model.