{"title":"利用电荷DLTS实验测定a-SiGe:H合金带隙态","authors":"M. Zeman, V. Nádaždy, E. Pinčík, R. van Swaaij","doi":"10.1109/ASDAM.1998.730156","DOIUrl":null,"url":null,"abstract":"We used the charge deep level transient spectroscopy (DLTS) to determine the midgap density of states (DOS) distribution in undoped a-SiGe:H layers. By applying a bias voltage of -5 V and 0 V on the MIS structures and annealing them 10 minutes at equilibrium temperature of 490 K we moved the position of the Fermi level, E/sub F/, in the a-SiGe:H material, which has led to the different equilibrium distributions of the DOS. In case of applying -5 V, which moves E/sub F/ towards the valence band edge, the DOS distribution is dominated by a peak at 0.61 eV below the conduction band edge and in case of 0 V, when E/sub F/ is around midgap, a peak in the DOS distribution is formed at 0.80 eV. In both cases light soaking leads to an increase in the DOS and a formation of a subband at 0.90 eV.","PeriodicalId":378441,"journal":{"name":"ASDAM '98. Conference Proceedings. Second International Conference on Advanced Semiconductor Devices and Microsystems (Cat. No.98EX172)","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1998-10-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Band gap states in a-SiGe:H alloys determined from charge DLTS experiments\",\"authors\":\"M. Zeman, V. Nádaždy, E. Pinčík, R. van Swaaij\",\"doi\":\"10.1109/ASDAM.1998.730156\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We used the charge deep level transient spectroscopy (DLTS) to determine the midgap density of states (DOS) distribution in undoped a-SiGe:H layers. By applying a bias voltage of -5 V and 0 V on the MIS structures and annealing them 10 minutes at equilibrium temperature of 490 K we moved the position of the Fermi level, E/sub F/, in the a-SiGe:H material, which has led to the different equilibrium distributions of the DOS. In case of applying -5 V, which moves E/sub F/ towards the valence band edge, the DOS distribution is dominated by a peak at 0.61 eV below the conduction band edge and in case of 0 V, when E/sub F/ is around midgap, a peak in the DOS distribution is formed at 0.80 eV. In both cases light soaking leads to an increase in the DOS and a formation of a subband at 0.90 eV.\",\"PeriodicalId\":378441,\"journal\":{\"name\":\"ASDAM '98. Conference Proceedings. Second International Conference on Advanced Semiconductor Devices and Microsystems (Cat. No.98EX172)\",\"volume\":\"1 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1998-10-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"ASDAM '98. Conference Proceedings. Second International Conference on Advanced Semiconductor Devices and Microsystems (Cat. No.98EX172)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ASDAM.1998.730156\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"ASDAM '98. Conference Proceedings. Second International Conference on Advanced Semiconductor Devices and Microsystems (Cat. No.98EX172)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ASDAM.1998.730156","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Band gap states in a-SiGe:H alloys determined from charge DLTS experiments
We used the charge deep level transient spectroscopy (DLTS) to determine the midgap density of states (DOS) distribution in undoped a-SiGe:H layers. By applying a bias voltage of -5 V and 0 V on the MIS structures and annealing them 10 minutes at equilibrium temperature of 490 K we moved the position of the Fermi level, E/sub F/, in the a-SiGe:H material, which has led to the different equilibrium distributions of the DOS. In case of applying -5 V, which moves E/sub F/ towards the valence band edge, the DOS distribution is dominated by a peak at 0.61 eV below the conduction band edge and in case of 0 V, when E/sub F/ is around midgap, a peak in the DOS distribution is formed at 0.80 eV. In both cases light soaking leads to an increase in the DOS and a formation of a subband at 0.90 eV.