S. Ochiai, A. Maeda, T. Ogawa, T. Takagi, M. Ieda, T. Mizutani
{"title":"超薄蒸发聚丙烯薄膜的电性能","authors":"S. Ochiai, A. Maeda, T. Ogawa, T. Takagi, M. Ieda, T. Mizutani","doi":"10.1109/CEIDP.1993.378956","DOIUrl":null,"url":null,"abstract":"A ultrathin polypropylene film (PP film) is deposited on a glass substrate from an evaporating source in vacuum. The temperature of the glass substrate is kept at 100/spl deg/C during the deposition. The thin PP film is about 100/spl Aring/ in thickness. The film shows a self-healing breakdown in the high field region, and the electrode area gradually decreases. The electric strength of the film was 12.2MV/cm after self-healing breakdown. Its value is higher by a factor 1.7 than that of a conventional film. The conduction current in the ultrathin film is ohmic in the low field region and increases steeply by tunneling injection in the high field region.<<ETX>>","PeriodicalId":149803,"journal":{"name":"Proceedings of IEEE Conference on Electrical Insulation and Dielectric Phenomena - (CEIDP '93)","volume":"11 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1993-10-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Electrical properties of ultra thin evaporated polypropylene films\",\"authors\":\"S. Ochiai, A. Maeda, T. Ogawa, T. Takagi, M. Ieda, T. Mizutani\",\"doi\":\"10.1109/CEIDP.1993.378956\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A ultrathin polypropylene film (PP film) is deposited on a glass substrate from an evaporating source in vacuum. The temperature of the glass substrate is kept at 100/spl deg/C during the deposition. The thin PP film is about 100/spl Aring/ in thickness. The film shows a self-healing breakdown in the high field region, and the electrode area gradually decreases. The electric strength of the film was 12.2MV/cm after self-healing breakdown. Its value is higher by a factor 1.7 than that of a conventional film. The conduction current in the ultrathin film is ohmic in the low field region and increases steeply by tunneling injection in the high field region.<<ETX>>\",\"PeriodicalId\":149803,\"journal\":{\"name\":\"Proceedings of IEEE Conference on Electrical Insulation and Dielectric Phenomena - (CEIDP '93)\",\"volume\":\"11 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1993-10-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of IEEE Conference on Electrical Insulation and Dielectric Phenomena - (CEIDP '93)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/CEIDP.1993.378956\",\"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 IEEE Conference on Electrical Insulation and Dielectric Phenomena - (CEIDP '93)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CEIDP.1993.378956","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Electrical properties of ultra thin evaporated polypropylene films
A ultrathin polypropylene film (PP film) is deposited on a glass substrate from an evaporating source in vacuum. The temperature of the glass substrate is kept at 100/spl deg/C during the deposition. The thin PP film is about 100/spl Aring/ in thickness. The film shows a self-healing breakdown in the high field region, and the electrode area gradually decreases. The electric strength of the film was 12.2MV/cm after self-healing breakdown. Its value is higher by a factor 1.7 than that of a conventional film. The conduction current in the ultrathin film is ohmic in the low field region and increases steeply by tunneling injection in the high field region.<>