{"title":"重复脉冲电子束二极管中的等离子体特性","authors":"M. Myers, D. Hinshelwood, F. Hegeler, M. Wolford","doi":"10.1109/PPC.2017.8291206","DOIUrl":null,"url":null,"abstract":"Electron beam (e-beam) generation in high power vacuum diodes results in anode and cathode plasma formation. It is well documented that expansion of these plasmas into the A-K gap may adversely affect diode performance during the main e-beam pulse. Ionized gases exist after the main pulse and can limit diode performance. For a given repetitively pulsed driver, diode physics will depend largely on the emitter material used in the cathode, the anode material, the electric field E, dE/dt, current density (J), vacuum pumping speed, the pulse width, and the pulse repetition frequency (PRF). For single shots and at a PRF of 1 pulse per second (PPS) taken on the NRL Solid State Pulser, diode plasmas are investigated using dielectric fiber velvet and graphite cathodes. A fiber laser interferometer is used to measure the line density of plasma at the cathode. A gated camera is fielded for nanosecond resolution of plasma emissions at axial positions across the anode-cathode gap.","PeriodicalId":247019,"journal":{"name":"2017 IEEE 21st International Conference on Pulsed Power (PPC)","volume":"7 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2017-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Plasma characterization in a repetitively pulsed electron beam diode\",\"authors\":\"M. Myers, D. Hinshelwood, F. Hegeler, M. Wolford\",\"doi\":\"10.1109/PPC.2017.8291206\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Electron beam (e-beam) generation in high power vacuum diodes results in anode and cathode plasma formation. It is well documented that expansion of these plasmas into the A-K gap may adversely affect diode performance during the main e-beam pulse. Ionized gases exist after the main pulse and can limit diode performance. For a given repetitively pulsed driver, diode physics will depend largely on the emitter material used in the cathode, the anode material, the electric field E, dE/dt, current density (J), vacuum pumping speed, the pulse width, and the pulse repetition frequency (PRF). For single shots and at a PRF of 1 pulse per second (PPS) taken on the NRL Solid State Pulser, diode plasmas are investigated using dielectric fiber velvet and graphite cathodes. A fiber laser interferometer is used to measure the line density of plasma at the cathode. A gated camera is fielded for nanosecond resolution of plasma emissions at axial positions across the anode-cathode gap.\",\"PeriodicalId\":247019,\"journal\":{\"name\":\"2017 IEEE 21st International Conference on Pulsed Power (PPC)\",\"volume\":\"7 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2017-06-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2017 IEEE 21st International Conference on Pulsed Power (PPC)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/PPC.2017.8291206\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2017 IEEE 21st International Conference on Pulsed Power (PPC)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PPC.2017.8291206","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Plasma characterization in a repetitively pulsed electron beam diode
Electron beam (e-beam) generation in high power vacuum diodes results in anode and cathode plasma formation. It is well documented that expansion of these plasmas into the A-K gap may adversely affect diode performance during the main e-beam pulse. Ionized gases exist after the main pulse and can limit diode performance. For a given repetitively pulsed driver, diode physics will depend largely on the emitter material used in the cathode, the anode material, the electric field E, dE/dt, current density (J), vacuum pumping speed, the pulse width, and the pulse repetition frequency (PRF). For single shots and at a PRF of 1 pulse per second (PPS) taken on the NRL Solid State Pulser, diode plasmas are investigated using dielectric fiber velvet and graphite cathodes. A fiber laser interferometer is used to measure the line density of plasma at the cathode. A gated camera is fielded for nanosecond resolution of plasma emissions at axial positions across the anode-cathode gap.