{"title":"低压射频放电中鞘层动力学","authors":"M. Lieberman","doi":"10.1109/PLASMA.1989.166201","DOIUrl":null,"url":null,"abstract":"Low-pressure RF discharges are widely used for materials processing. Typical parameters are pressure of 1-100 mtorr, frequency of 13.56 MHz, and RF voltage of 50-1000 V. A reasonably complete picture of the dynamics of these sheaths has been developed. Some typical results for a high-voltage sheath driven by a sinusoidal current source, under the assumptions of time-independent, collisionless ion motion and inertialess electrons, are: (1) the ion sheath thickness s/sub m/ is square root 50/27 larger than a Child's law sheath for the same DC voltage and ion current density; (2) the sheath capacitance per unit area for the fundamental voltage harmonic is 1.226 epsilon /sub 0//s/sub m/, where epsilon /sub 0/ is the free space permittivity; (3) the ratio of the DC to the peak value of the oscillating voltage is 54/125; (4) the second and third voltage harmonics are, respectively, 12.3% and 4.2% of the fundamental; and (5) the conductance per unit area for stochastic heating by the oscillating sheath is 2.98 ( lambda /sub D//s/sub m/)/sup 2/3/ ( epsilon /sup 2/n/sub 0//mu/sub e/), where n/sub 0/ is the ion density, lambda /sub D/ is the Debye length at the plasma-sheath edge, and u/sub e/=(8eT/sub e// pi m)/sup 1/2/ is the mean electron speed.<<ETX>>","PeriodicalId":165717,"journal":{"name":"IEEE 1989 International Conference on Plasma Science","volume":"17 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1989-05-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Dynamics of sheaths in low pressure RF discharges\",\"authors\":\"M. Lieberman\",\"doi\":\"10.1109/PLASMA.1989.166201\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Low-pressure RF discharges are widely used for materials processing. Typical parameters are pressure of 1-100 mtorr, frequency of 13.56 MHz, and RF voltage of 50-1000 V. A reasonably complete picture of the dynamics of these sheaths has been developed. Some typical results for a high-voltage sheath driven by a sinusoidal current source, under the assumptions of time-independent, collisionless ion motion and inertialess electrons, are: (1) the ion sheath thickness s/sub m/ is square root 50/27 larger than a Child's law sheath for the same DC voltage and ion current density; (2) the sheath capacitance per unit area for the fundamental voltage harmonic is 1.226 epsilon /sub 0//s/sub m/, where epsilon /sub 0/ is the free space permittivity; (3) the ratio of the DC to the peak value of the oscillating voltage is 54/125; (4) the second and third voltage harmonics are, respectively, 12.3% and 4.2% of the fundamental; and (5) the conductance per unit area for stochastic heating by the oscillating sheath is 2.98 ( lambda /sub D//s/sub m/)/sup 2/3/ ( epsilon /sup 2/n/sub 0//mu/sub e/), where n/sub 0/ is the ion density, lambda /sub D/ is the Debye length at the plasma-sheath edge, and u/sub e/=(8eT/sub e// pi m)/sup 1/2/ is the mean electron speed.<<ETX>>\",\"PeriodicalId\":165717,\"journal\":{\"name\":\"IEEE 1989 International Conference on Plasma Science\",\"volume\":\"17 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1989-05-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE 1989 International Conference on Plasma Science\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/PLASMA.1989.166201\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE 1989 International Conference on Plasma Science","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PLASMA.1989.166201","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Low-pressure RF discharges are widely used for materials processing. Typical parameters are pressure of 1-100 mtorr, frequency of 13.56 MHz, and RF voltage of 50-1000 V. A reasonably complete picture of the dynamics of these sheaths has been developed. Some typical results for a high-voltage sheath driven by a sinusoidal current source, under the assumptions of time-independent, collisionless ion motion and inertialess electrons, are: (1) the ion sheath thickness s/sub m/ is square root 50/27 larger than a Child's law sheath for the same DC voltage and ion current density; (2) the sheath capacitance per unit area for the fundamental voltage harmonic is 1.226 epsilon /sub 0//s/sub m/, where epsilon /sub 0/ is the free space permittivity; (3) the ratio of the DC to the peak value of the oscillating voltage is 54/125; (4) the second and third voltage harmonics are, respectively, 12.3% and 4.2% of the fundamental; and (5) the conductance per unit area for stochastic heating by the oscillating sheath is 2.98 ( lambda /sub D//s/sub m/)/sup 2/3/ ( epsilon /sup 2/n/sub 0//mu/sub e/), where n/sub 0/ is the ion density, lambda /sub D/ is the Debye length at the plasma-sheath edge, and u/sub e/=(8eT/sub e// pi m)/sup 1/2/ is the mean electron speed.<>