{"title":"Space-charge distributions in electron-beam charged Mylar and Kapton films","authors":"J. West, H. Wintle, A. Berraissoul, G. Sessler","doi":"10.1109/CEIDP.1988.26337","DOIUrl":null,"url":null,"abstract":"The laser-induced pressure pulse method was used to determine space-charge distributions in 22- mu m films charged with 10 to 40 keV electron beams. For relatively low deposited-charge densities corresponding to surface potentials below 300 V, two charge layers develop, one at the surface of the samples and one at a depth corresponding approximately to the electron range. For higher deposited-charge densities, when breakdown in the surrounding air occurs during pressurization, the surface-charge layer is positive. For deposited-charge densities in excess of 1 mu C/cm/sup 2/, the space-charge layer is broader and, in Kapton, located deeper than for smaller charge densities. Heating of the samples to 110 degrees C reduced the charge without broadening the charge layers.<<ETX>>","PeriodicalId":149735,"journal":{"name":"1988. Annual Report., Conference on Electrical Insulation and Dielectric Phenomena","volume":"28 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1988-10-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"1988. Annual Report., Conference on Electrical Insulation and Dielectric Phenomena","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/CEIDP.1988.26337","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
The laser-induced pressure pulse method was used to determine space-charge distributions in 22- mu m films charged with 10 to 40 keV electron beams. For relatively low deposited-charge densities corresponding to surface potentials below 300 V, two charge layers develop, one at the surface of the samples and one at a depth corresponding approximately to the electron range. For higher deposited-charge densities, when breakdown in the surrounding air occurs during pressurization, the surface-charge layer is positive. For deposited-charge densities in excess of 1 mu C/cm/sup 2/, the space-charge layer is broader and, in Kapton, located deeper than for smaller charge densities. Heating of the samples to 110 degrees C reduced the charge without broadening the charge layers.<>