{"title":"真空放电击穿阶段阴极点等离子体参数","authors":"A. Batrakov, S. Popov, E. Dubrovskaya","doi":"10.1109/DEIV.2016.7748674","DOIUrl":null,"url":null,"abstract":"Ion energy distributions of different ion species in cathode-spot plasma were measured with using the HIDEN EQP300 analyzer in both the breakdown and arc modes of discharge in a vacuum gap with the Ga-In liquid-metal cathode simplifying repetitive discharge ignition. In the arc mode of discharge, the average charge of ions rises with increase of discharge current. This trend was found to be absent in the breakdown mode of discharge.","PeriodicalId":296641,"journal":{"name":"2016 27th International Symposium on Discharges and Electrical Insulation in Vacuum (ISDEIV)","volume":"8 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2016-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":"{\"title\":\"Cathode spot plasma parameters in the breakdown stage of vacuum discharge\",\"authors\":\"A. Batrakov, S. Popov, E. Dubrovskaya\",\"doi\":\"10.1109/DEIV.2016.7748674\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Ion energy distributions of different ion species in cathode-spot plasma were measured with using the HIDEN EQP300 analyzer in both the breakdown and arc modes of discharge in a vacuum gap with the Ga-In liquid-metal cathode simplifying repetitive discharge ignition. In the arc mode of discharge, the average charge of ions rises with increase of discharge current. This trend was found to be absent in the breakdown mode of discharge.\",\"PeriodicalId\":296641,\"journal\":{\"name\":\"2016 27th International Symposium on Discharges and Electrical Insulation in Vacuum (ISDEIV)\",\"volume\":\"8 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2016-09-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"4\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2016 27th International Symposium on Discharges and Electrical Insulation in Vacuum (ISDEIV)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/DEIV.2016.7748674\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2016 27th International Symposium on Discharges and Electrical Insulation in Vacuum (ISDEIV)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/DEIV.2016.7748674","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Cathode spot plasma parameters in the breakdown stage of vacuum discharge
Ion energy distributions of different ion species in cathode-spot plasma were measured with using the HIDEN EQP300 analyzer in both the breakdown and arc modes of discharge in a vacuum gap with the Ga-In liquid-metal cathode simplifying repetitive discharge ignition. In the arc mode of discharge, the average charge of ions rises with increase of discharge current. This trend was found to be absent in the breakdown mode of discharge.