{"title":"Space-charge distributions in electron-beam charged Mylar and Kapton films","authors":"J. West, H. Wintle, A. Berraissoul, G. Sessler","doi":"10.1109/ISE.1988.38526","DOIUrl":null,"url":null,"abstract":"The method of laser-induced pressure pulses (LIPPs) was used to determine space-charge distributions in 22- mu m Mylar and Kapton 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 the case of Kapton, is located deeper in the material than for smaller charge densities. Heating of the samples to 100 degrees C causes a decrease of the charge density without broadening of the charge layers.<<ETX>>","PeriodicalId":199976,"journal":{"name":"6th International Symposium on Electrets,(ISE 6) Proceedings.","volume":"19 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1988-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"24","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"6th International Symposium on Electrets,(ISE 6) Proceedings.","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ISE.1988.38526","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 24
Abstract
The method of laser-induced pressure pulses (LIPPs) was used to determine space-charge distributions in 22- mu m Mylar and Kapton 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 the case of Kapton, is located deeper in the material than for smaller charge densities. Heating of the samples to 100 degrees C causes a decrease of the charge density without broadening of the charge layers.<>